Roy L. Clough Jr. - Svenskt Modellflyg
Transcription
Roy L. Clough Jr. - Svenskt Modellflyg
Model air car skims the ground By ROY L. CLOUGH, JR. Working model of a ground-effect vehicle rides on a cushion of air from a model-airplane engine Tethered to a stake, the car will skim half an inch or so off the ground, around and around until it runs out of fuel WITH A hollow whistling note audible over the whine of its tiny engine, this advanced working model of a ground-effect vehicle skims across the floor supported on a cushion of air. What makes it go? Air is supplied by a prop to a peripheral slot, which produces a high-speed wall of air around the edge of the model to retain the lift. A separate propulsion-system tube bleeds off air for reactive propulsion---from the blower section, not the skirt. Supporting pressure is not reduced --- a major fault of ground-effect vehicles which propel by dumping air pressure and lifting the skirt on the opposite side from the desired direction of travel. Stabilizers on each side act somewhat like the dihedralled wings of an airplane— if the model tilts to either side, air pressure escaping from the skirt builds up under the vane and returns it to even keel. The result is a model, which can buzz along at a good clip on any level surface with a minimum of sideslip due to minor irregularities on the surface. Attached to a tether it will whiz merrily around in a circle until the fuel runs out. It rides a half-inch or so off the floor even when running free. Any small airplane engine can be used to power it. If you use the engine installed in the original model, which is supplied with a three-blade prop, you won't have to make a prop of sheet metal, a pattern of which is given. If the engine is new, break it in by running on a test stand for 15 or 20 minutes. Top and rear views above and below show the engine mounted in the intake duct and the propulsion tube outlet at the rear. Note the wire hook on the door for tethering. A squeeze bulb feeds fuel through the plastic fuel line connected to the tank. The dry cell plugs into the phono jack First study the cutaway drawings given to become familiar with the various parts. Then begin construction by making up the base, top and diaphragm plate from edge-glued 3/32-in. balsa sheet. Use stiffeners where shown and allow to dry on a flat surface. Make up the 3 1/2in. intake duct from art paper and use this as the first structural member to hold the top and base together. When dry, add the 3/16-in. uprights, which form the supports for the side covering. Next install the paper propulsion tube. Note the vane to direct airflow within it. The skirt is vertical grained 3/32-in. stock glued around the bottom edge of the base. Use basswood or balsawood and there will be no difficulty in making the bends. Cover the framework of the car body with art paper, one section at a time, beginning at the rear. Add dummy headlights and fin, stabilizing vanes and handrails. Windows may be glazed with sheet acetate or left open. Finally turn the model over and install stator vanes. Coat the interior with at least two coats of hot fuel proof dope (clear). Dope the exterior in your favorite color. The original was painted light blue outside, fire red inside. Make up the engine pedestal, mount the engine and cement the pedestal to the wires to the glow plug. Cut out a 3 1/4-in. disk of cardboard and use this as a guide in centering the engine. Actual installation is made by cementing the diaphragm plate to the stators. Use a slow drying cement to allow time to even up the slot around the skirt and center the engine shaft. Run out the fuel filler tubes and engine lead out wires and make up a needle valve extension shaft. The glow-plug wires lead to a phonograph jack---a great convenience in starting. A recoil spring starter is a must and is installed before the prop. A length of 1/8-in. cord is cemented around the skirt as a buffer. (A round shoestring works very nicely.) Suspend the model by the engine shaft and balance it so that it hangs evenly. Small bits of solder, coated with cement and dropped inside the body on the light side or end will do the trick. If tethered operation is desired, cement a wire hook through the covering to the upright on the centerline. Scanned from: Popular Mechanics Do it yourself Encyclopedia MODEL CAR RACING AT ITS SIMPLEST Deceptively simple in appearance, every line on his car has been carefully planned to make it easy to build and maintain and fun to race By ROY L. CLOUGH, JR. WIND • Here is the perfect project to absorb your old three-port .19-.29 engine that still has a few kicks left in it despite being outmoded for flying use by newer and hotter engines. We wanted to find out if a really good air-drive car could be built to look like a real race car and not a runaway fuselage. The results were surprisingly good. With an old O&R side-port .19 it hit a zooming 62.8 mph. Even a beaten-up .14 diesel engine kicked it up to 40 mph. This compares very favorably with wheel-drive cars, and Wind Wagon is a lot simpler to operate and cheaper to build. The plan should be followed fairly closely. Making an air-drive race car is not just a matter of sticking a motor and prop on a wheeled platform; balance and dynamic loadings are important. There are a couple of angles designed into this one which are essential to good performance. For example, the wide underchassis is not a matter of taste in style, but is made that way to create an airflow pattern to prevent fine abrasive dust, present on concrete surfaces, from being thrown up to the engine intake; the washer arrangement which holds the model plane type wheels came about because other arrangements wore out aluminum hubs in WAGON nothing flat. Begin construction with the chassis. This is carved from white pine or equivalent. The wheel axles are 1/8" steel landing gear wire. It is not difficult to drill holes in the chassis for these by hand if care is used, but a drill press makes the job a cinch. Don't try to drill all the way through from one side; drill in from each side so the holes meet in the middle. Note how the axles are held by soldered washers. It is not essential that the axles be held so firmly they cannot rotate, but there should be no end-play. Do not put the wheels on yet. The body is carved from soft pine. Some originality of line is permissible here, but don't depart too far from the plan and be sure the thrust line comes as shown. The motor mount is 1/2" plywood, cut to fit your particular engine. Chassis, body and mount are assembled with 11/2" flat head wood screws and good wood glue—do not use model cement. The cockpit details add realism. The driver is a ping pong ball, painted to look like a helmeted head and the rim of the pit is padded with heavy twine cemented in place. The fuel tank can be anything handy that suits the engine. Several types have been used on the original and all worked well provided the usual U-control fuel feed to the outside was observed. Be sure it is anchored firmly. Next bore a ballast hole, put in the screweyes and bridle and make a trial fit of the engine and tank and check the balance. The model should hang the slightest trifle nose-down when suspended by the bridle, so pour in melted lead or old bearing metal to balance. Pull the engine and tank and finish the model with fuel-proof dope or enamel—incidentally, it seems easier to clock a bright-colored car. When the paint job suits you install the wheels, using the washer arrangement shown to minimize wear on the hubs. Install the motor and tank and check it over to make sure the wheels spin freely and track and foot well. Put a little #50 oil on the axles every other run and clean them off whenever they seem to be picking up dirt. Because the engine is pushing instead of pulling you must now check the shaft end play to make sure the push doesn't move the shaft in so far that it puts a strain on the connecting rod or allows the crank throw to strike the back of the crankcase. Usually on such engines as the O&R .19 and .23 side-port jobs the hard steel propeller back plate running against the end of the bronze main bearing is all the thrust bearing required. If, however, there is considerable end play, or gap, fill this in with thin brass or surface ground steel shim washers until the play is just perceptible. Do not run the shaft tight and be sure to oil the shims well before the first run—see page will take care of lubrication after that. 39 We found that maximum speeds came from careful selection of propellers and by setting the car off a bit rich so that it would start to lean out by about the tenth lap—presumably because the rich start prevented the pusher engine from overheating before the car got going fast enough for the slipstream to provide sufficient cooling. While this vehicle will never set the world on fire from either the appearance or performance standpoint, it does bring auto racing within the reach of the average miniature engine owner who may not have access to a lathe or the other specialized equipment so vital to AMRCA followers. By limiting a group of racing enthusiasts to same size or maximum power plants any hobby shop or model club can come up with a fleet of cars in jig-time for some informal, strictly-for-fun racing. Almost any smoothly surfaced parking lot will suffice (school yards frequently provide the type of running surface most desirable). A portable center post sandbagged in place and mounting a skate wheel well bolted to a sturdy timber or piece of piping is about all that's needed for "Sunday" drivers. A steel wire connects from the pivoting center piece to the car bridle; be super sure that your lines are all of sufficient size and free of nicks. As with all projects presented in this publication, the editors welcome your comments and photos of completed models. Let your fellow hobby fans see your handiwork; send along your model pictures Air Trails HOBBIES for Young Men By ROY L CLOUGH JR. Unique gyrocopter-kite design launches itself without towing, costs less than $1 to build there's not enough room WHEN to run with a kite or too Amt. Req. 1 1 1 1 2 1 1 1 3 1 2 1 2 Misc. 74 MATERIALS LIST—WHIRLYBIRD KITE Size and Description Use 1/8 x 3 x 36" sheet balsa rotors 1/4 x 3 x 20" sheet balsa fuselage 1/16 x 3 x 20" sheet balsa vane, stabilizer 1/8 x 3/4 x 5" pine or basswood landing gear support 1 1/4" Dia wooden wheels main wheels 3/4" Dia wooden wheel nose wheel 10" x .030 wire axles 9" length coat hanger wire rotor mast #6-32 brass hex nuts rotor spacers 3/32" id brass washer thread washer 3/32" id x 3/4" brass tube rotor bearings 2 x 4" tin can stock rotor hubs 3/16" id brass eyelets tether eye model airplane cement, red, black, and silver dope; and kite string much wind to fly model airplanes, it's a perfect time and place to test fly this newly designed rotary-wing kite. All materials you'll need are available at your local hobby shop and in one evening's time you can have your 'copter-kite ready to fly. First, layout the fuselage, stabilizer, rotors, and vanes (Fig. 3) on balsa stock and cut them out with a sharp hobby knife or razor blade. To shape the rotors and stabilizer, first crack them along scored lines as in Fig. 3A, then fill the crack with cement and prop up the end of the part until the cement dries. Note that the rotors are not identical, but are a pair, having opposite pitch for counterrotation and are oppositely coned. Now cement the stabilizer and landing gear support (Fig. SB) to the fuselage, reinforcing the joints with a fillet cut from the 1/4-in. balsa stock. Next cut the rotor mast from coat hanger wire and cement this to the right side of the fuselage, 12 3/4 in. from the aft end. Reinforce by sewing it to the balsa with a needle and heavy thread, then coat the threads" with more cement. After installing the eyelet to which the tether attaches, sand the assembly with fine sandpaper and paint as in Fig. 3C, with model airplane dope. Do not apply dope to the rotors or vane. The rotor bearings and hubs (Fig. 3D) are made of 3/4-in. lengths of tubing soldered to strips of tin can metal. Make two of these, form them over the blades, and cement them to the rotors as in Fig. 3E. SCIENCE and MECHANICS by ROY L. CLOUGH, Jr. ONE evening of fairly intensive work will put this little whirligig-type helicopter aloft. The construction is quite simple and offers no problems to the builder who is handy with a soldering iron. Good balance without excessive weight is the primary consideration, and care along this line will result in good flight performance. A Campus Bee was used for the original and proved to be very reliable. A bit 34 of cellulose tape which can be flipped over the filler hole after charging, to keep dirt out, is good performance insurance because of the exposed nature of the model. Begin construction by unscrewing the filler valve. Put this in some safe place until again needed, taking care not to lose the tiny rubber plug which serves as a check valve. Unsolder the feed line at the tank end. A 2-56 or 3-48 stud, an inch long, is tapped, and then soldered in the hole. Layout the motor mounting holes on a 3/4" disk of tin can stock, punch or drill them and solder the disk to the lower end of the tank. Next mount the engine with common pins, which are bent over and soldered securely in place. While doing this, carefully check the alignment of the crankshaft with the tank and the stud. A bit of 1/16" rod is soldered to the tin disk opposite the cylinder, the end of this being wrapped with a few turns of tinned copper wire to serve as a counterweight. The counter-weighting may be done very exactly, as follows: wrap the wire on fairly tight until it seems correct; then slide the wrapping a bit one way or the other for fine balance. When you find it, heat the end of the rod briefly and the wire will "tin on" and stay put. Drill a new hole for the feed line near the top of the tank and on the opposite side from the filler valve. Solder the line in place carefully, to prevent leakage. The big rotor is made from a good springy variety of balsa, which may be finger-doped for added toughness. It is of left-hand pitch to permit the interchange of various easy-to-obtain righthand propellers on the motor end. We have used the Hillcrest adjustable plasticblade prop and also Monogram kit props with fairly good results but top performance will come from a wood propeller carved to fit the individual machine. The fairly small total area of the rotor system results in a rather rapid descent, but is necessary because the engine must turn up quite rapidly in order to develop enough power to fly the machine. There is, of course, a very favorable heat-exchange setup because of the rapid motion of the cylinder through the air as the tank rotates, but set the motor at near maximum output to get the best results altitude-wise. One word of caution: be absolutely certain the motor is running in the right direction when released! MODEL AIRPLANE NEWS • April. 1950 WHAT'S THE SCORE ON helicopters? By ROY L. CLOUGH, JR. • Easily the most fascinating thing that flies, the helicopter is making a name for itself in peace and war as the marvelous machine that can land or take off anywhere, hover over one spot or tuck its nose down and scoot away in any direction the pilot chooses. It is only natural then that model builders have been attracted to the type, for here is a flying machine which does its stuff close in where it may be observed and enjoyed, does not require huge tracts over which to fly, and which should give more solid hours of model fun than anything ever invented. Or so it would seem at first glance. However, as many a model builder who has tried it will testify, it isn't quite that simple. To some who have tried it, at first it appears a rather straightforward proposition—merely arrange a prop to pull upward, provide some method of torque nullification, presto, there is a helicopter. And several bitter disappointments later, the model builder sweeps up the shattered balsa wood, lays aside his tools and tries to dig up some information on the type. In many cases a study of the problems involved makes the whole thing look so impossibly complex that there seems to be little point in trying it at all. The envisioning of complicated controls, pushrods, flap hinges, dampers, complicated power transmissions, hairline adjustments and impossibly complex and delicate structures places the designing and building of a successful free flying model helicopter on the level of a major engineering feat—so the modeler puts the whole thing aside and starts sketching a new pylon job. The truth of the matter, as in most cases, lies somewhere between the two extremes of utter simplicity and impossible complexity. A fair statement of the case is that a good model helicopter is no more difficult to build and fly than any other type of fairly advanced model aircraft. What may appear to be difficult at first becomes at second glance merely different. This is because there is very little in the way of carry-over analogy from fixed-wing models. Roughly speaking, the differences are of the same order as those between building a hot engine into a speed job and building the same engine into a boat. The principles are approximately the same, but the factors are different. Helicopter information, in the empirical form in which it is most useful to model builders, has unfortunately been neither complete nor widely available. Therefore the design picture has been a bit clouded. Any up-to-date aviation fan, if he scratches his memory a bit, will recall having read that "articulation" is a good thing, that helicopters are inherently "unstable," that there are a great number of things like "cyclic" pitch and gyroscopic precessive forces to be dealt with. All of which contains elements of truth, yet just how these things apply to sitting down and actually building a flying model helicopter has been obscure. The writer scored considerable success in rubber-powered helicopter models with his development of the cage drive co-axial system, which allowed two rotors to revolve in opposite directions about a common center, thus canceling out both torque and gyroscopic effects. With this system, which first appeared in Air Trails some time ago, incorporated into the model, stable power-on free flight was possible for the first time without the use of complex control arrangements. Extremely steady in flight, the machine and a later variation of it were capable of rather surprising duration when winder-wound. However, these flights were very largely vertical; it was not possible to secure any marked forward flight with the machine, barring the use of extreme nose-heavy trim. Later a further development, a kit design manufactured in limited numbers, featured a stabilizing or "damper" fin which permitted a fair degree of forward flight, with great steadiness and every indication of stability. So consistent was this type that by counting the number of turns stored in the motor the model could be flown from one table-top to another, time after time alighting within an inch or two of the desired spot. Several further variations of this machine were built, performing well. Now, note that no blade articulation of any sort was used in these models. There was no provision for cyclic, pitch changes and gyroscopic action did not enter the picture. Yet they flew very well under rubber power. Keeping that empirical fact in mind, let us further examine the co-axial system. This system—meaning two rotors revolving in opposite directions, about a common center—is one of the oldest designers' answers to the question of what to do about torque reaction. Further, it appears to be ideal in many respects because it would seem that any disturbances, either aerodynamic or gyroscopic, which occur in one rotor would be balanced immediately by the reverse of that reaction in the other. Now then, why, if this system is so theoretically ideal, with equalized thrust, cycling and gyroscopic moments, has it not appeared in any machine which has demonstrated itself to be of practical commercial importance? The answer lies in the fact that coaxial systems have two major requirements, and, from a practical standpoint, these requirements tend to be mutually exclusive. First, it is desirable that the two rotors be mounted close together. The reason for this is that widely spaced rotors introduce great stresses in the mast and rotor system when the blades are cycled for forward flight, that is, when the blade angle is increased at the rear and reduced at the front each revolution of the rotor. The uppermost blade will require a greater pitch change than the lower blade in order to equalize the couple between the points of applied force and the center of gravity. Thus, if we wish to avoid excessive stressing of the rotor and mast system, the rotors must be quite close together. Second, the rotor blades of a co-axial machine must be spaced with a large gap from one set to the other because otherwise they may clash together due to the flexibility of the rotors. Blade deflection due to gusts or even normal cycling pitch changes is great enough, ordinarily speaking, to make any spacing of the rotors less than one third rotor diameter apart definitely hazardous. Thus, the rotors must be far apart. From these two requirements it can be seen that the only way out of the problem is not actually an "out" at all, for it will mean building the rotor systems impossibly heavy and rugged and thus losing many, if not all, of the advantages of the co-axial system. In the practical sense, then, this means that co-axial systems are limited in use to such cases as where it may be possible to stress the system all out of proportion to its size—models and tiny man-carrying jobs. Now, what is this business about cyclic pitch? Did we not just describe rubber models, which flew well without it? Why not merely eliminate cycling pitch from the co-axial system and fly forward by shifting the C.G. ahead? The rubber models did fly forward by means of the stabilizing fin and C.G. shift. But don't overlook the fact that a rubber model flies with continuously diminishing power after the rotors come up to speed. This is very important because it meant the writer could eliminate cycling controls because of a characteristic of the power plant. Just why this was so may be explained as follows: Picture a purely hypothetical co-axial model helicopter in which the thrust does not vary, which has stiff, fixed-pitch rotors, and which is trimmed nose heavy to make it fly forward. All set? The machine, because of the unequal loading of the disk (area covered by the rotors) begins to slide forward. It will not tip to either side since the advancing blade of one rotor, creating more lift as it encounters a relative wind due to forward motion has a balancing counterpart in the blade, which is rotating forward on the opposite side. This, incidentally, is a major advantage of the co-axial configuration. Now, as the machine gains speed we find that the front edge of the rotor disk is entering the wind while the rear edge is leaving it. This means that the rotor is lifting more at the front than at the back, and it will tilt upward, moving the machine into what is actually a stall—one of the few analogies which occur between fixed and rotating wing craft. Now this will happen no matter how much weight is placed in the nose, consistent of course with the ability of the machine to lift it. Now, when this stall occurs, the helicopter will slide backward increasing the lift at the rear of the rotor disk until the model stalls tail up, whereupon it repeats the trick, oscillating back and forth with increasing amplitude and violence until it finally crashes. The reason the rubber-powered models flew steadily ahead under C.G. shift is that the power gradually decreased as the machine flew forward and the damping fin provided a stabilizing surface, which served to maintain the proper angle. Thus it might be said with considerable accuracy that the rubber models actually made use of the oscillating tendency of stiff rotors to secure forward flight and that they were successful in doing this because the oscillation was damped at proper time by the motor running out. Or, to put it a bit differently, the coaxial rubber model helicopters with damper fins as developed by the writer were simply highly modified co-axially driven planes flown vertically. Have you ever seen Jim Walker do the Saber dance? The principle is the same. Thus, to fly forward in a co-axial machine, as in any other, requires that the pitch of the blades decrease in front and increase at the rear of the rotor disk. And, since we must be able to control the pitch of the rotor blade around the circumference of its sweep, we may as well abandon the co-axial configuration and its power transmission problems and go over to something simpler, the single rotor and torque prop. Either that, or power the rotor itself by means of tip jets or motors which eliminate torque effects entirely. For most model work, and at this stage of the game, we will find the torque prop type more practical, since this gives us a heading and trim control and the boom helps to round out the design by balancing the weight of the power plant, which will be forward in most cases. Which means we promptly dive head first into the rotor head business—but don't let it scare you. The earliest successful helicopters used a refinement of what is known as the flapping, drag link rotor originated by Juan de Cierva, the autogiro inventor. To Cierva's basic invention were added mechanisms to secure collective and cyclic pitch control and with such an arrangement the first man-carrying machines flew. This system (Fig. 2) makes use of a hinge between the blade root and rotor mast. This allows the blade to flap up and down relative to the plane of rotation and was originally introduced in the autogiro to permit the machine to fly forward without tipping over due to relative wind differentials. Soon after this was invented it was found necessary to add another hinge which would allow the blade to swing fore and aft, since, as the blade coned upward on the advancing side it would tend to lag behind the retreating blade, thus setting up terrific stresses in the flap hinge. This drag hinge then had to be fitted with a dynamic damper—a gadget similar to the device which closes doors without slamming —to absorb the jolts and shocks that such a system was heir to and to assure a correct nominal circumferential position of the blade. This system is in wide use among fullscale helicopter makers but it has some limitations in that it is not truly stable, although quite flyable with a competent pilot. As far as model helicoptering is concerned the system is of interest chiefly as background material. In practice it proves tricky to build, fragile and easily misaligned, and it falls down on a most important model requirement in that it will not fly "hands off." As a matter of fact, it is not even a satisfactory free flight autogiro arrangement as the writer discovered some years ago, and this lack of satisfactory flight characteristics started a series of experiments, which led into contact with a type of rotor arrangement that would perform satisfactorily on an autogiro. Initial experiments with articulated rotors on rubber model autogiros resulted consistently in dismal crackups at the end of erratic flights of a few feet. Apparently the fault was somehow connected with the articulation that was supposed to promote flight stability. So we committed heresy. We stopped articulating the rotor blades.* This was better, but still not good, and then came the inspiration—why not articulate the blades in some other fashion, so that the effect would be the same, but the big bounce would be taken out? Why not, instead of allowing the blade to flap upward, allow it to rotate span wise— that is, instead of letting the tip fly up, let the trailing edge flap upward? A new rotor was built with the blades spring-loaded against their span wise axis at zero pitch, and since the rotor was stiff, tip-to-tip, the mast, which held the rotor, was jointed, or articulated to the fuselage to prevent the transmission of disturbances back and forth. Aerodynamic pressures would result in the slight negative pitch angle necessary for autorotation, and a sort of automatic cycling pitch would be obtained as the advancing blade flattened to the relative wind, which would flip the trailing edge down as the blade passed in front and started back dh the downwind side. It worked. *Louis Garami built a successful nonarticulated, non-feathering giro at about the same time which flew by using torque of the motor to counteract the progressive tipping of his stiff four-bladed rotor. This appeared in Air Trails.—RLC. (To be continued in subsequent issue.) AIR TRAILS SEPTEMBER 1952 (Continued from previous issue) This initial model was soon followed by others, simplified greatly by eliminating the springs and mast rubbers, and using thin wood blades attached to a stiff spar and a flexible wire mast. Models built here and in England proved the soundness of the system. Fig. A. The articulated rotor mast was fine for autogiros, with due restrictions on the articulation to prevent clipping the prop or the tail, because it permitted the initial tilting, which starts the gyroscopic wobble, to* damp out without running through a cycle of self-excitation back and forth through the mast. But, for model helicopter work a flexible mast seems impractical. If rotation is supplied by the rotor, as in the case of the autogiro, it will run concentric and true if in balance. But, if one tries to feed power into the rotor through a flexible mast the whole thing will jump out of line and wobble violently with the whole system acting as an eccentric. In the practical sense, then, this means that a flexible mast cannot be used on model helicopters except, possibly, where the propulsive force originates in the rotor, as for example, tip-jet propulsion. At this point the writer became acquainted with the work done by Arthur Young, who designed the Bell helicopters, and this takes us into a discussion of the so-called "feathering rotor" system in which the blades neither cone upward nor drag back, and in which, for the first time, we begin to see inherent stability introduced into rotary wing flight. In order to understand the differences between the fully articulated and feathering systems it is necessary to look a bit more closely at gyroscopics, the seemingly puzzling, but actually rather simple set of shenanigans which take place when a rotating system is disturbed. Any rotating system, and this applies with particular emphasis to helicopter rotors, is a gyroscope, and jointing, hinging or springing it will not make it anything else; it will still observe the natural laws which govern gyroscopic action. This is probably the most puzzling and least understood factor in rotary wing flight, and the reader will find it of value if at this, point he takes the trouble to make up a small "understanding tool" and follow along with the text. Cut out a six-inch circle of heavy cardboard and mount it with a pin through the center in the end of a short length of 1/4" stock which has its sides numbered consecutively: 1, 2, 3, 4. This represents a rotor—and a gyroscope. If you wish, mark the disk with an arrow showing left hand rotation (most model helicopter rotors will be left hand in rotation because of mechanical considerations which will develop later on). First, flick the disk with the fingers to make it spin rapidly, then poke gently under the rim of the spinning disk on the side of the stick marked 1. . What happens? The edge of the disk rises, not where you poked at it, but at 90 degrees, the side, marked 4. Repeat the experiment, only this time - poke it at 3. It rises at 2. What is happening? Simply this: the deflecting force is modified by a factor of 90 degrees. This is the first rule: that a gyroscope, if deflected, reacts with a displacement proportional to the deflection at 90 degrees in the direction of rotation from the impingement of the deflecting force. (Of course it also deflects an equal amount in an opposite direction 90 degrees back from point of impingement, but we're trying to keep this thing simple.) With the understanding tool at hand this becomes quite easy to understand, or think of it this way: if a rotor blade is deflected at one point in its circumferential travel, it will tend to pop up 90 degrees further along in the direction of rotation. Now, spin the disk again and gently tilt the stick. Note that while the gyroscope initially tends to remain in its original plane, it will now gradually readjust itself until it is spinning with its plane perpendicular to its axis (the stick). If the disk were mounted on a universal joint and driven by rotation of the stick this effect would be even more pronounced. This occurs because it is a function of centrifugal force to' cause the rim of the disk to recede as far as possible from the axis, and this condition is satisfied at. 90 degrees. These two related phenomena are of extreme importance to helicopter designers: first, a deflection reacts at 90 degrees; second, a gyro seeks rotation perpendicular to its axis. Now remove the stick and take the disk outside and scale it through the air with a quick spinning motion. Note how it tips over toward the advancing side. Two factors are responsible for this behavior. The first is related to the Magnus effect and is due to differing pressure gradients on the surface of the spinning disk, and the second, which is our primary interest helicopter-wise, is that the air pressure at the entering edge of the disk is producing a gyroscopic resultant at 90 degrees, thus turning the disk over. Bear in mind these vital functions as we consider the requirements of a stable helicopter rotor. One thing should be evident, that forward flight produces a problem in tip speed differentials, the advancing blade in meeting a faster relative wind than the receding blade tends to tip the machine toward the retreating blade side due to, aerodynamic forces, but these aerodynamic forces are balanced to a large extent by gyroscopic forces, provided the blades do no flap upward or drag back circumference-wise and are free to rotate, within limits, about their span-wise axis. And, if the rotor head is mounted in a gimbal, rotor deflections will not be transmitted back and forth between rotor and fuselage through the mast, which means that the helicopter will be stable. By the addition of a stabilizing fly-bar between mast and fuselage connected by linkages, which can alter its plane of rotation, the rotor can be made to take up any position desired by the pilot. In other words, then, if we use a flapping blade with drag links we must also include a device to alter the pitch of the blades cyclically, mechanically; but, if we eliminate the flap hinges and drag links and allow the blades to "feather" as it rotates, cyclic pitch is automatic in accordance with the gyrodynamics of the system. This basic discovery about the helicopter rotor was made by Arthur D. Young of Bell helicopter fame. In this writer's opinion, based on literally scores of experiments with flying models, this discovery is one of the great aerodynamic advances of the century. Not only for the mechanism which Young worked out, which is remarkably effective, but for the principles his work outlines, which it is not extravagant to state mark the greatest single contribution to rotary wing flight. From these principles we can arrive at a stable rotor for model helicopter work. Fig. B illustrates such a rotor. The simplicity of the thing is its beauty. With a little study of the sketch no reader will have trouble duplicating it. Note that the fly-bar is moved up level with the blades. This is simply a length of wire with a few turns of solder on the ends to provide operating momentum—not much weight is needed. Note that the function of the fly-bar is to steer the rotor blades back into the proper position with respect to the mast through a damping interval, hence cyclic control may be had by arranging the fly-bar in such fashion that it can be deflected into a new plane of rotation— but, very important, the fly-bar must not be rigidly attached to the mast because this will cause rapid following; that is, the mast will tend to swing immediately the rotor is displaced, because the independent nature of the system will have been destroyed. In Fig. C we see a system developed by the writer, which uses the independent rotor principle together with control "trailers" similar to the Kaman system. The advantages of this system for model work is that it provides automatic-rotation in addition to the stability of the Young system, plus the fact that cyclic control by trailer deflection (only one trailer need be connected) is very easy to arrange with a line up through a hollow mast and out to a "loaded" trailer. The other end of the line being attached to a cam ring which may be set to produce the cyclic deflection at any desired point. The drag of this system is higher than others and it must be designed carefully if maximum lift is to be obtained, yet its many advantages make it attractive and it is certainly capable of much greater development, particularly since it is possible, with trailers, to make use of high lift sections with less regard for pitching moments. This system is particularly attractive for jet work, and it should be noted that by placing the line of thrust of the jet motor a bit below the center of the span-wise hinge the blade pitch will be controlled by the thrust output of the engine. However, this factor must be used judiciously because too great a moment here will result in the blade mushing around slowly at a very high pitch, which will produce no lift at all. Remember too that trailers, in operation, should drop down into the rotor plane— don't seek to drive them either above or below the plane, since this puts them at a great, mechanical disadvantage and may result in their control over blade pitch becoming ineffectual and the drag of the system very high. Note, of course, that it is possible to use H series stable airfoils and eliminate the trailers entirely; however, if this is done the rotor system may show a tendency to tip back in forward flight, and cyclic control installation may be more difficult. But for straight hovering or vertical flight this system is unmatched for stability. I have been asked, "How does the Jetex kit helicopter work?" This model is a good performer with a very fair duration for this type of craft and in flight exhibits stability. If we examine the machine we can find the answer. Two blades are used which are articulated to a supporting beam. These depend, as does the Cierva system, upon centrifugal force to keep them at the proper angle in flight, without a rigid connector. Underneath the rotor is a thrust beam to which are mounted two Jetex engines and the machine is driven by the reaction of these units. Now, please note that the mass of the jet motors is quite high in-regard to the total mass of the ship; that is, it has a sort of high-momentum flywheel beneath an articulated rotor with the mass of the pod, or fuselage being quite negligible. Thus we see here a combination of the articulated blade system with the flybar stabilizer, which operates well if we confine activity to vertical flight. In essence this machine is dynamically similar to the writer's little Infant job of a couple years back, but being jet powered it requires no damping fins or fuselage-rotor-mast brake to retain proper heading. However, in its present form forward, flight by changing the C.G. trim will be found unreliable; the machine isn't designed for that sort of thing. It should prove a very interesting experiment to move the power beam up level with the rotor blades, and rebuild the rotor along the lines shown in Fig. B. This should produce a model capable of forward flight, as well as vertical, but the problem of autorotational letdown will have to be solved with some new mechanism to alter blade pitch. Also it may prove necessary to introduce a small amount of friction between the motor-fly-bar and its gimbal connection to the mast in order that adding weight to the nose will make it go forward and not just alter the angle of dangle of the fuselage from the rotor. On the basis of experiment the writer suggests that configurations for first experiments be kept as simple as possible. The first helicopter should be rubber powered, something along the lines of a simple stick model, probably direct drive. It won't fly for very long with this limited power, but it can be fooled with indoors at great length and the rotor set-up ironed out. After you get the "feel" of the rotor set-up and a bit of experience in handling rotary wings, try something in gas or jet power. The best bet for gas engines is the single rotor, or tandem rotor type—like the Piasecki jobs with a rotor at each end of a long fuselage. Coaxials, or rather composite rotor jobs, such as the writer's little Infant machine, are very simple and okay for direct vertical flight, but they won't do well in forward flight and will return to earth with quite a thump unless some free-wheeling arrangement, other than spin-in-reverse is used. Better than freewheeling, which will mean pitch change too, is engine twospeed control. Have a timer rigged to drop a partial obstruction into the venturi after a certain interval. This will bring the model down under power, quite gently. The really ambitious may use spark ignition in conjunction with timer control—but watch the weight. It takes power to fly helicopters. It is impossible of course, in a 2-part article to cover all phases of helicopter design. However, it is quite possible and the writer hopes he has been successful in this respect, to outline some primary essentials. In answer to the question, then: "What's the score on the helicopters?" the reply is this: you can build them and fly them successfully if you understand the basic dynamics. In this report are shown two stable rotor designs. They work, they have been flown, they do not hop and jump madly about and there is no element of luck about it; they can be duplicated by any average modeler who will take the time to understand just what forces are involved and how they react. If, in times past, the reader has tried unsuccessfully to design his own, or has purchased kits which did not perform as well as expected, he should re-examine his experience in the light of the material he has just read, make a couple more experiments and decide for himself that practical model helicopters are not only possible but downright fascinating. In general, then, we may sum it up as follows: It is better to use a shallow pitch and run the rotor at a good clip; make the blades of high aspect ratio—and thin section. Be sure the pitch is equal on both blades; mount the torque prop as far aft as practical—it will absorb less power, and keep the design of the model as simple as possible and the bearings as near perfect as you can get them. There are several things to watch out for. For one thing, the rotor blades should be quite stiff. Balsa wood if hard is pretty fair, but pine or even birch is better. Because of the thin sections, which must be used, and the high rotor speeds, an overly flexible rotor blade may develop "whip" due to resonance. This will make the blades run out of track, absorb a terrific amount of power and may result in tearing the model apart, particularly if a whipping blade connects with the drive string to the torque rotor. Some of the writer's early models used exceptionally flexible blades without articulation or feathering features, yet flew. How? By adding quite a bit of weight to the tips. Thus as the rotor was spinning up for take-off as the model sat on its wheels a gyroscopic plane or reference was established which held the model fairly steady for the brief duration of the rubber power. This won't work well if power is continuous, as for a gas motor; the model will gradually tip over a bit to one side and then jump violently at 90 degrees. The reason for this behavior is that a sort of cycling occurs due to blade flexibility, at the first small tilt, and this condition is rapidly excited back and forth until something disastrous happens. With single rotor and torque prop models a change of heading may be noticeable immediately after jump-off. This may be only a few degrees or a quarter circle, even if the balance of thrust is correct. The way to minimize this is to hold the model for a second or two to allow the rotors to come up to speed. For gas jobs use old friend "stooge" to hold the model down until ready. Theoretically the axis of the torque prop should lie in the plane of rotation of the rotor. Practically it must be somewhat below this plane. This is due to fuselage effects, aerodynamically speaking, and to the mechanical consideration that we must keep the prop drive string (or shaft) well clear of the rotor tips. Empirically it works out rather well, because design considerations necessary for power location, landing gear, lateral areas, etc., work out so as to make it possible to locate the torque prop axis well down out of the way. Assuming a left hand rotor, it will be noted that if the axis of the torque prop is too high the machine will fly sidewise to the left, and if the axis is too low it will fly to the right. Properly located, the model shows no tendency to slide off in either direction. This is a very happy circumstance because it means that by combining a few factors, such as level of the torque prop-axis with C.G. we may make a model of very simple design fly in any desired direction without a separate cyclic control mechanism. This statement reads rather simply, but go back and look it over again, for it contains the essential elements 'of practical model helicopter flying in that we see how that adjustment of the model helicopter, and the mechanism to make that adjustment possible, are not a complicated mess of pushrods, cams and levers, but are in fact no more complicated than the adjustment of an ordinary free flight model of the conventional type, and in many ways simpler. And, incidentally this is no condemnation of cyclic controls, as such, for they have much to offer the purist and the researcher. However, and analogically, the writer must point out that we do not find it necessary to build operating ailerons, rudder, elevator and flaps into a conventional free flight model in order to enjoy it tremendously. Power transmission may scare the uninitiated at first, particularly the bevel gear drive shown in one of the pictures. It shouldn't. It does present a new problem, true, yet a simple drive of this nature is but the work of a few minutes to produce, requiring far less effort than the control system of, say, a team racer. The gears are readily obtainable in any toy store; for 20 cents two toy eggbeaters yield six gears, four small and two large ones. You can't even buy a good bell-crank for that. There are dozens of ready sources of small gears, toys, old alarm clocks, etc. Fuel line (brass) and landing gear wire takes care of the shaft and bearing problems nicely and adequately. To drive the torque prop use balsa wood pulleys faced with #1 sandpaper and a string belt. About 2½-to 3-1 is a practical ratio and slippage with this system is nil. Gas power requires heavy reductions in speed and some sort of shock clutch or take-up may be necessary if any considerable weight or power is to be used. We hope to cover this phase more fully at a later date and show some simple gas motor hook-ups, which require no machining or difficult work. One pitfall to avoid is the idea that a large, high pitch, slow moving rotor will produce longer and better flights. It won't. Power requirements will be tremendous, which means a thicker motor will be required, meaning more weight, meaning it can't be wound as many turns, meaning a great deal more power will be needed for torque correction—a vicious circle that adds up fast. Rotor blades should be of fairly high density, thin in section and operated fairly fast at low angles of attack. For the present, helical pitch should be shelved in the interests of simplicity; use flat blades of uniform pitch until you build up a little experience at helicopter flying. The sketches show general proportions and sound design practice. Stick pretty closely to these layouts, at least for your first machine, then strike out on your own. ROY L. CLOUGH, JR. AIR TRAILS SEPTEMBER and NOVEMBER, 1952 Water Bug By ROY L. CLOUGH, JR. INSPIRED BY those little aquatic insects called "water striders," this unusual model boat flits along the surface of the water on three flipper shaped planing feet mounted at the ends of long legs. Although it travels fastest on calm water, Water Bug can run through 4 to 5 in. ripples— the scale equivalent of 5-ft.waves---with no trouble. The struts simply slice through the wavelets and keep going. The boat is very stable and can be run with a guideline or turned loose in small ponds where recovery is easy. The original model showed no tendency to trip or tip over, even with the rudder bent sharply for free-running turns. The hull is a simple box structure of 1/8-in. sheet balsa. It should offer no problems, but remember to soak the sheeting, which covers the front section in hot water before bending. Finish the boat with a couple of coats of sanding sealer and one of dope, or cover the bare wood with a layer of lightweight model tissue laid on with heavy dope. The motor mount is a disc of plywood pinned and cemented to the rear leg. Drill for the engine mounting bolts, set the engine in place and build up the fairing on the rear of the bulkhead with scrap balsa left over from the hull planking. Don't worry about access to the rear of the bulkhead to tighten up the nuts. If built-in blind this way, they'll stay put. The thrust line of the motor should be almost parallel to the bottom of the boat, but pointed slightly downward. Cut the planing feet out of .019 sheet metal, then make up the holders and rudder and solder them to the feet at the angles shown. Attach the feet to the struts by lashing and cementing securely. Finish off the model with scale radio masts, running lights and foghorn. A couple of screw eyes are used for the restraining bridle. If you use a tether, attach it in such a fashion that the boat dangles level when suspended by it. If you don't have a model boat basin with tether post, you can run Water Bug off a spinning rod from a rowboat. To launch the boat hold it by the motor mount and give a gentle push. It should climb out of the water in about 6 ft. with an immediate increase in speed. If it doesn't, turn up the front edges of the forward planing feet slightly. Scanned from: Popular Mechanics Do it yourself Encyclopedia 'TYPHOON-STEAM OR AIR EXPANSION ENGINE By Roy L. Clough Jr. Of all the gadgets a hobbyist can make, few offer greater kick than a homemade steam engine that really hums along smoothly. Usually, however, making even a simple oscillating type engine entails considerable machine work, lots of know-how and experience—which keeps many from trying it. This little expansion engine, which runs beautifully on air or steam pressure, was designed especially for the hobbyist who would like to try this phase of model building with good assurance of success, without a well-equipped machine shop at his disposal. All difficult parts are adapted from readily obtainable things; the rest are odds and ends that everybody has kicking around. For instance the crankcase is made from a couple of catsup or chili-sauce bottle caps, the piston and cylinder from an old fish-rod ferrule, bearings from odd bits of brass tubing. A little rummaging around in the scrap box will probably turn up most of the rest in nearly finished shape. You don't have to stick very closely to the dimensions either; just watch the proportions so you arrive at enough clearance between the con rod and cylinder sides at quarterstroke. The completed engine fills the gap between gas engines and clockwork drive for model boats, or if you're really ambitious and want to see what it was like back in the compressed-air flying model days, make up an air tank and fly a plane with it. Despite its extreme simplicity the engine is very efficient and powerful, due chiefly to unique valve system worked out by the author after much experimenting with rotary, ball valve and oscillating cylinder engines. This system has all the simplicity of the latter and none of its drawbacks. Cylinder is stationary and valving is taken care of by simple flat valve rocked back and forth by means of slotted drive over crankpin. Feed line is flexible neoprene tubing, which moves with valve. Hunt up, or buy, a mating pair of 9/16" fish-rod ferrules, cut to proper length and lap with fine pumice and oil to smooth slide fit. (Alternatively you may use 9/16" tubing and turn a piston from aluminum or brass.) Next locate a couple of bottle caps of right size and cut out for cylinder, which is then soldered in place in one. Other cap is cut back on rim for about 1/4" to provide valve clearance and two 4-40 bolts soldered in place to act as mounting studs. Put this aside. Crankshaft is built up from length of steel rod, threaded into heavy brass washer and soldered. Bearing is any handy bit of brass or copper tubing, which fits or can be reamed to size. Cut hole in front case and solder it in. Make up wristpin bracket from scrap of .024 stock and set aside. Find two bits of brass tubing for con rod bearings, one to fit machine screw (around 6-32 size), which forms crankpin. On smooth board, measure off con rod length and with appropriately sized nails hold bearings to board. Then bend length of 1/16" brass or soft iron rod around two bearings in shape shown on plan and solder in place. Melt a little solder into inside of piston, heavily tin con-rod bracket, put rod in bracket, push pin through, then dangle bracket into piston, apply heat to piston until solder fuses. Drop piston into cylinder; poke crank pin into crankpin bearing and screw lightly in Typhoon Engine (Continued from page 26) place. Rotate shaft to check for sticks and binds. Now remove piston, shaft, etc. Make up a valve plate from scrap of sheet brass, threading and soldering valve rocker stud in place and filing off even so as not to project against cylinder. Drill inlet hole. Now wire valve plate to cylinder in a couple of places with enameled copper wire (which won't stick), line it up carefully and run solder along both sides to hold in place. Remove wire tie-down and drill through cylinder wall through valve plate inlet hole. (Doing it in this order prevents distorting thin cylinder tubing.) Carefully scrape off rough edges. Now reassemble shaft and piston workings and recheck for sticks or binds. Make up valve—but do not drill intake hole yet, just rocker shaft hole. Put valve in place, holding with spring, washer and nut, and rotate shaft to quarter-stroke in direction you wish engine to run. (Note valve can be turned over at this point for left-hand rotation.) With a scribe mark valve for drilling through intake hole in cylinder. Then turn shaft 180° and make certain inlet hole is now open, the edge of the valve having slid past it. Remove valve, drill marked spot, then with wood peg in hole solder on short length of brass tubing for feed line. Polish valve face by rubbing lightly on fine file, oil up and reassemble the works. The cylinder head, a disk of tin can metal or .024 brass, should fit quite well with a push fit. Then rotate shaft so piston is at bottom stroke and carefully solder head in place. Attach 5" length of black neoprene tubing to intake line (clear tubing is not satisfactory—steam hardens it and it works too stiffly for air) and put on flywheel or prop and apply a little pressure. A flip is necessary to start it, or else simply rotate to valve "on" position for self-starting. If everything works right, and it should, you may now solder rear case in place. Use lots of oil for first few runs; when run in a bit, a few drops on valve plate and crankshaft bearing are sufficient. Air pressure up to 100 p.s.i. may be used, steam to 60-70 p.s.i. American Modeler — September I960 Try TURBINE It's not too hard to convert your regular glow plug engine into a passable jet power plant! By ROY L. CLOUGH, JR. COMING ATTRACTION: scheduled for next "AT" is Roy's "Blow Bug" pressure jet basic F/F The increasing importance of jet and rocket aircraft has focused interest on power plants which can be used to propel their scale model counterparts without the ear-splitting racket of a pulse jet, and with longer duration than is provided by current rocket motors. In an effort to achieve this, a number of builders have been experimenting with various arrangements whereby a conventional model engine is used to produce a jet blast. Although less thrust can be produced in this fashion with any given engine than that same engine would put out with a propeller, the results can often be satisfactory if the weight of the model is kept low due to the terrific power to weight ratio of small glow, plug engines. There are at least three types of possible piston-engine operated jet motors. These are 1) ducted fan, 2) pressure jet, 3) jets operated by means of a positive displacement, or Rootes-type blower. Since initial experimentation has been along the lines of the ducted fan system this type is best known. Basically the ducted fan is simply a model engine and propeller placed inside a tube. For optimum efficiency the tube should be so shaped that the ambient pressure is about the same on both sides of the propeller, or fan. This means that the ducted fan should produce a great increase in velocity of air flowing through it without producing a corresponding great increase in pressure. This is accomplished by proportioning the tail pipe and the intake pipe so that their difference in size matches the pressure/velocity of the air flow within each to the other, and by locating the fan in the necked-down portion between the two sections. In other words, the airflow behind the fan will be much faster than the flow ahead of the fan, so the tail pipe diameter will be proportionately less than the intake diameter, and the fan will be located at the transition point, or, where the air is speeded up. The sketch illustrates this. The reason for this proportioning is that pressures within the tube are functions of air velocity, and, the faster the air is moving, the less pressure it exerts on the walls. If we tried to build a ducted fan with the same diameter from intake to exhaust end we would find it very inefficient because the intake end would be operating at a much higher pressure than the exhaust end, the engine would tend to starve, race, and possibly overheat, and the thrust from the efflux would be small. The ducted fan obtains reactive propulsion by accelerating the column of air within it; it is the inertia of this column of air to being set in motion, which provides the thrust. Thus anything that impedes the flow of air within the system tends to reduce thrust. It is better, then, to have tail pipe a bit on the small side than too large, and, from the empirical approach, which is generally the best m model sizes, a variable area exhaust nozzle can be used to advantage. A very simple instrument which can be made from a two foot length of transparent fuel line and an oil bubble is helpful in determining pressures at various points within the duct. This is called a manometer. To work it simply suck up a slug of light oil an inch or two into the line and hold the other end first at the intake, then at the exhaust end. By comparing the behavior of the bubble in both positions a good idea can be gained of the pressure pattern. Even better, tap into the duct in several places and compare pressures. The tail pipe pressure should be higher than the intake pressure, but not a great amount higher, for ducted fan designs. Too great a pressure difference means that the fan is working against back pressure and is not handling all the air it can; which is in direct opposition to the basic philosophy of the ducted fan to move the greatest mass of air possible in the shortest possible tune. Simplicity is a great advantage of ducted fans, and of course, the tube can be used as the keel or central member of the airframe AIR TRAILS 26 JETS for your Models which supports the other assemblies. The tube may be constructed of steamed sheet balsa or stiff hard-finished paper. The writer has found that aluminum foil makes the best interior finish; being smooth and nonabsorbent it is easily wiped clean of oil from the engine. Stick it in place with hot fuel proof dope which has been allowed to thicken a bit The necked down portion of the tube could mean making a layout for each new motor built, but this can be avoided by building this portion using a dime store funnel for a form and trimming the section where it fits. The angle is just about right and the bother of laying out a conic section is bypassed with plenty of trim allowance. Standard practice with ducted fans is to angle the motor supports to act as stator vanes to straighten out the airflow and reduce, or eliminate torque effects. In some cases it may be necessary to add a vane or two to do the job. These should be adjustable to permit interchange of fans without losing torque trim. Small sheet metal "flower petal" fans are generally used in ducted jobs, but try carving small wide-bladed props of correct helical pitch for added thrust A carefully carved fourblader will move more air than metal fans A spinner is another aid to accelerated flow Actually, the ideal ducted fan would be a wheel-type plastic job with a well-shaped rim to prevent tip losses and to provide a good flywheel effect. Perhaps some manufacturer will read this and produce one Generally speaking, to get the most out of a ducted fan use as large a diameter as possible for any given model, cutting down on the number of blades and pitch where necessary to maintain correct engine speed. Be sure to streamline the backside of the engine mount and lead-out glow plug wires and needle valve extension for convenience in operation. If the engine can be fueled and started without using a removable section in the tube, so much the better. An external fuel supply, or filler line, depending upon engine used will simplify this part of operation, and a starting rod, JULY. 1953 which can be poked down the intake to flip the engine over will eliminate fiddling with strings or risking chopped fingertips to get the thing going. The ducted fan motor works best in scale-type models flown at moderate speeds and may be used singly, as a fuselage member, or mounted in external pods. If pod mounts are used, keep them as close together as possible. Some adaptation to helicopter use is possible, but the bulk and clumsiness of this type of model jet makes it less practical for rotary wing craft than our next consideration, the pressure jet The pressure jet system has not been widely employed in conjunction with model engines. This is quite a different affair from a ducted fan The pressure jet consists essentially of an impeller, or blower, which keeps a reservoir or plenum chamber stuffed with compressed air, and from this reservoir lines are bled off to feed jet reaction nozzles which may be located some distance away from, or at least angles to, the blower. Unlike the ducted fan, the idea is not to provide a large mass of air with velocity, but to supply a smaller mass of air at a relatively high pressure, to high velocity discharge nozzles (or afterburners). Pressure jet systems may use either an axial flow (propeller) fan, or a centrifugal blower, depending upon the general layout and designer's discretion. They could also use positive displacement blowers of the Rootes type, as mentioned above. The chief objection to use of this type blower is that there is none light enough for model use, and in any event they operate at a slower shaft speed than model engines provide, which seems to suggest infinite complication, hence impracticality for our purpose. Pressure jets offer intriguing possibilities for buried installations, experiments with multiple jets, boundary layer control, helicopter propulsion, etc. We may use a simple box with a tightly fitting rotor for the plenum chamber and bleed off jet tubes wherever we wish. (Continued on page 69) 27 Turbine Jets Since high internal velocities are of less concern, internal streamlining of the system is relatively unimportant within reasonable limits. We may simply seal up a fuselage, or wing," and use it as the plenum chamber, locating the jets at handy points and placing the air pickup, or intake, either at the top (at or slightly behind the CG) the front, or split to the sides. Whether we use axial or centrifugal blowers will depend upon various considerations A centrifugal blower is good where the air intake is "dead," that is, open to the inside of a ventilated fuselage, it may also leak less air under high pressures. It can, however, be used in podtype jet motors as shown in the sketch It is a characteristic of a centrifugal blower that air rammed into it puts a load on the engine, just the opposite of what happens with an axial or fan blower, which speeds up when rammed This means that in applications where a centrifugal blower is to be used in conjunction with ram air, the motor should run at its optimum rpm under ram, which means it may race when the model is not in motion. Since it is usually better to locate the engine within the plenum chamber to take advantage of its heat and exhaust gases this means that it will operate in a supercharged condition The way a glow motor will wind up under such conditions may surprise the builder the first time he tries it. Operating well above atmospheric pressure, the engine really stuffs itself with air and water condensation and it can get very hot in the process. For this reason it is a very good idea to use cold plugs and fuel in engines put to this use. Pressure jets work to best advantage where mechanical advantage can be taken of their unique characteristics, one of the best applications being driving helicopter rotors, where a stream of high speed air emerging from a blade tip can produce considerable rotational speed and lift. For scale type models of fighters they are not quite as good as ducted fans, except where highly streamlined and fast jobs are to be used, or where used in conjunction with a thrust augmenter, which we'll discuss in a moment From the above material the reader should be able to arrive at workable jet propulsion with a standard engine for his jet project As best thrust will not be as high with a propeller, so the weight must be kept down. But nevertheless, workable scale type jet models can be built and flown if a little attention is given to detail, and surprisingly "hot" models can be built by anybody willing to take a little extra care with internal finish and experiment a bit with intake and exhaust diameters Our interest in model jets is largely limited to such uses as scale model power-methods of the big ships, and for special model uses, such as helicopters, where, by sacrificing some mechanical efficiency we can do away with a great deal of mechanical complexity (.Continued from page 27) This does not mean that extremely good performance lies beyond the reach of our engine driven jets. Attention to the factors involved, minor adjustments, care in detailing and improved operational experience can result in greatly improved thrust figures over what we are able to obtain at present. Such angles as variable tail cones (in flight?), improved ram scoops and fans of improved design should be exploited more fully, and possibly the use of afterburners and the many problems they present can be licked A good rule for the experimenter to remember is that the propulsive efficiency of any system is highest when the exhaust efflux velocity most nearly matches the forward speed That is, the air should be blown backward about as fast as the model moves forward Practically speaking, this means it is more efficient to move a large mass of air at a moderate speed than it is to move a small mass of air at a very high speed, because moving the larger mass gives us the advantage of inertia. In the concrete application we can improve propulsion efficiency in those systems where the exhaust velocity is several times higher than the forward speed of the model by using augmenters, that is, devices which will introduce more air into the efflux, increasing its reaction mass and slowing it down. A tail pipe shroud, as shown in one of the sketches, is a good way to do this. Another method, useful in ducted fan systems suspected of having low tail pipe pressures is the simple clapper valve—a reed of tough paper, which admits more air to the tail pipe if its internal pressure drops below atmospheric The essential thing to remember in designing engineoperated jets is that the basic problem is to put a gas (air plus combustion products) in motion, in order to get the opposite reaction (propulsion) produced by doing work upon that selfsame gas. A good rule of thumb for empirical model jet design is "The greater the gob of gas you can grab, the less 'give' it's got and the more got you'll get " TRIAD...A Radial-Wing Flying Model By ROY L. CLOUGH, Jr. An interesting experiment in radial-wing ships, this model is incapable of stalling out of a climbing turn. DESIGNED with radially mounted wings as found on some robot bombs, this novel model has brought favorable comment wherever it has been flown. Its surprising stability is due directly to the vertical wing. In straight and level flight, the two lower wings provide lift. Should the model tend to bank in either direction, the vertical wing will exert lift and return the ship to an even keel. In 156 POPULAR SCIENCE fact, turning and banking can be controlled entirely by warping the single aileron on this vertical wing. Construction is extremely simple. The fuselage is built up of three sheets of 1/32" medium-hard balsa, all cut to the same shape. Stiffeners of 1/16" square balsa are cemented to the inner faces of these sheets. The nose end is reinforced with plates of 1/16" balsa, cemented on after assembly. Cut three identical wing frames from 1/16" medium soft balsa and install the 15 ribs, trimming a little from the trailing edges of the outer ribs to make them fit. Cover with regular model tissue and water-shrink, but do not dope. Wing design makes for speedy construction. The aileron shown on the plan is fitted to the vertical wing only. Other wings have landing wheels at their tips. A shallow groove cut chord-wise in the butt edge or root of each wing will make a stronger joint. Use cement liberally to attach the wings to the fuselage. The two lower wings, which take up the shock of landing, are reinforced with wire crosspieces as shown on the plans. A notch in the elevator, reinforced by an additional thickness of stock, retains the rear rubber hook. Mount a wide-bladed prop of fairly high pitch and make test flights over tall grass on a calm day. The sturdy fuselage permits use of a powerful enough rubber motor to give the ship a skyrocket climb. A nose wheel helps preserve the prop from damage. Performing much like a high-pylon design, the plane climbs to the right and glides to the left. SEPTEMBER 1946 WHIRLIGIG By Roy L. Clough Jr. Two views of the whirligig in actual flight. Note the flexing of the rotors under power. EXPERIMENTING CAN BE FUN WITH THIS VERY SIMPLE HELICOPTER PROJECT THIS direct-lift model utilizes a simple and foolproof counter-rotational system based on the familiar principle of the contest "whirligig." Due to the nature of the rubber motor hook-up the two rotors are constantly and automatically in balance with each other, effectually neutralizing the torque element without gearing of any kind. This model is the 73d helicopter built by the writer and experience gleaned from the first 72 is incorporated in its construction. Counter-rotation is considered the best approach to the torque problem, due to the fact that as long as some power must be used to offset rotor torque that power might just as well be turned to additional lift. The length of a rubber motor is in any case limited (barring the use of gearing) in a model of this type and it is therefore essential that the best possible use be made of the power that is available. Two-bladed rotors were used on the original because they may be placed in line with the fuselage making the model a rather "flat package" and easily portable, a somewhat important factor in cramped city quarters. Three-bladed rotors would probably be okay if you wish to try them. More power would be needed and slightly less pitch would doubtless increase the soaring qualities of the model. Start construction with the coaxial unit. Study the plans until there is no doubt as to the action of the unit. The motor tube is 1 1/4" in diameter and is constructed of either balsa sheet or stiff drawing paper. The thrust bearing is located at the bottom of the tube and consists of a pin-washer-bead arrangement. This bearing should rotate freely but should have very little "play." Strive to get the bearing as close to the dead center of former "C" as possible. The pin-shaft is bent at this point to keep it from falling inside the tube, but it is attached to its crosspiece only after the fuselage is completed. Cement former "B" into the other end of the tube leaving a 1/8" rim to accommodate "A." If you have chosen drawing paper for the construction of the motor tube, dope it now for additional strength. Allow plenty of time for the dope to dry before cutting holes in it for access to the rubber motor. The shaft, which turns the lower rotor, is made from either thin-wall brass or aluminum tubing. 1/8" O.D. The tubing is split two ways for about 1/2" and the split ends flattened at right angles to the tube. Now "soak" the tubing for at least five minutes in dope thinner to remove all grease and/or dirt. If this is done no difficulty will be experienced in making cement stick to it. Push the tube through the hole in former "A" (it should fit snugly), coat liberally with cement and push the whole assembly down into the "cup" formed by former "B" and the end of the motor tube. Allow a few minutes for the glue to set a little, then true up the shaft with the tube. That is, make certain the motor tube and the hollow shaft rotate in the same plane. The upper bearing is an odd piece of aluminum tubing, 1/4" long, slipped over the hollow shaft and mounted in the 1/4" by 3/8" crosspiece in the top of the fuselage. It simplifies matters to put the crosspiece with the bearing in it on at this point, because it is impossible to slide it on after the tube-shaft is flared to take a bead bearing. The lower rotor hub is mounted next. Drill the shaft hole a little undersize and force the hub on the tube. If it feels a bit loose, wedge it tightly with short lengths of toothpick. Apply plenty of cement, let the whole thing dry for a couple of hours, and go over it with cement again. Hundreds of flights on the original model failed to loose a hub attached in this manner. After the rear prop hub is well set, flare the end of the tube slightly to hold a glass bead, the thrust bearing for the upper rotor. Insert the propshaft through one of the access holes cut in the motor tube (tweezers are a great help) and slide a bead and washer and the upper rotor hub over the shaft. Use your favorite free-wheeler. The rotor blades are cut from 1/20" sheet and sanded over a bottle to produce a slight camber. Note that the angle of the lower rotor blades is slightly more than that of the upper. This is done because the upper blade "bites" into dead air and the air forced downward by the lower blade is already in motion. A higher blade angle on the lower blade, in theory at least, prevents compression between the rotors, and consequent instability. The fuselage of the helicopter model is built up of 1/16" strip, and is quite conventional, except for the sharp curves in the forepart of the longerons. If the longerons are soaked thoroughly in hot water before any attempt is made to bend them into place, no difficulty will be encountered. Because of the light nature of the construction it will be necessary to install internal cross-braces at the points marked on the plans. Where the landing gear legs are attached on the bottom of the fuselage it is a good idea to cover in a couple of sections with 1/32" sheet balsa. Tail fin is of 1/32" sheet. The cabin section is cellophaned in before the balance of the fuselage is covered. The original was covered with orange tissue and water-shrunk, not doped. Weight is an important factor in a model of this type; try to keep it down. The top section of the fuselage should be left uncovered until the coaxial unit is mounted. The bottom of the tube is anchored to a 1/8" crosspiece and the upper crosspiece is mounted directly into the fuselage. Check and make certain that no part of the rotating tube binds on the inside of the fuselage. AIR TRAILS Power will vary according to the weight of the model. Start with a double loop of 1/8" flat brown (four strands) and build it up from there. The original model flew well on this power until stepped upon and re-built, after which another loop had to be added to take care of increased weight. The tailskid, which is not shown in the photograph, was added later to avoid the necessity of holding the tail up in position in ROG flying. The model should balance 1/4" ahead of the rotor axis for straight vertical flight. Hand launching is accomplished by letting the ship take off from the hand with the nose pointed slightly downward. This model can be made to fly forward as it climbs by adding a small weight to the nose. The free-wheeler is to let it down easy. A few pertinent facts on model helicopter design should be mentioned at this point. The first and holiest commandment of model helicopter design is: Rotor blades absolutely must balance. Lack of balance induces vibration and loss of power. Vibration induces instability and the average helicopter is, by reason of the principles involved, not overly stable to begin with. Rotor blades should have a certain amount of "flex" to them. Rigid blades and instability are, in models of this type at least, synonymous. The center of lateral area should be high, otherwise the flat fuselage sides will act as a fin, causing the model to spill over at the top of its flight and descend upside down. The center of gravity should be as low as possible for the same reason. About 75 percent of lateral area should be behind the axis of the rotors; otherwise the model may fly tail-first in "forward" flight. Stub-wings, elevators, flaps, and whatnot are just so much junk on helicopters. Any unnecessary object sticking out into the slipstream of the rotors is a good bid for instability. Do not expect a model helicopter to turn in performance comparable to a conventional model of similar weight. Don't forget rubber length is limited and that the lift of the model is produced entirely by rotating vanes. Good performance, however, can be had as a result of careful construction and half-minute flights should not be uncommon with this model. If the free-wheeler works smoothly, a certain amount of soaring ability will be noticeable if the ship gets caught in a thermal. Use fresh rubber, as the model is hand-wound, or go us one better and figure out a way to use a winder on this ship. Making the bottom end of the coaxial tube and the bottom section of the fuselage under it, removable, might do this. OCTOBER, 1946 THE MODEL 'COPTER By ROY L. CLOUGH, JR. Roy's Little Infant job (AT Sept. '52) in flight. Damper fins have been removed and rudder turned over. Model will fly steadily forward, descends via auto-rotation pitch changes. Roy's continued research into the whirlybirds has produced some fine models including the first truly successful stable co-axial type. This is fascinating stuff, In our previous series of articles, ("What's the Score on Helicopters?") the writer tried to present a simple basic understanding of the major forces involved in a rotary wing flying machine. We saw that the problem of flight stability largely resolves into integrating the natural gyroscopic forces of a rotating system with its aerodynamic characteristics in such fashion that a reaction by either tends to maintain the positional integrity of the system with respect to the rotor mast. This, in the practical application, requires a certain amount of independence between mast and rotor in order to prevent immediate displacements from setting up a chain reaction of self-aggravated wobbling, and a certain amount of interdependence in order that control may be effected, or imposed upon the rotor, and that the mast shall serve as a 28 reference point, ruling the me of rotation of the rotor. Thus it becomes quite simple to design a vertical-lofting or hovering model, by simply arranging the rotor to feather along its longitudinal, or span wise axis and by hanging the hub in a gimbal which permits a seesawing action, and positioning the blades by means of a flyweight or paddle bar so they will not roll over or develop flutter in a chord-wise plane A rotor such as this is said to be independent, for if all bearings are free it will rotate in its own optimum plane regardless of the position of the fuselage, or mast. This is fine for an indoor model where gusts are not a factor, and when it is not desired to obtain forward flight. However, the completely independent rotor is not desirable, even for model work, because it has no reference point from which control can be effected. (In the practical sense it is well to point out that a completely independent rotor does not exist; there is always some friction in the pivots and gimbals which tends to position the blades at 90 degrees to the mast, but this residual friction is seldom much in a model) Therefore, we must build in a small amount of friction, either by making the gimbal fittings a bit stiff to begin with, or by providing a drag of some sort, which can be adjusted. When this is done the model will fly forward by simply changing the C.G slightly, since the reaction of the rotor, in seeking to justify its position with respect to the angle of the mast and aerodynamic pressures, will result in cycling pitch. This is the simple way of doing it and it works quite well for models. By judicious use of a small weight arranged to slide fore and aft, the model will climb vertically or by forward at a fast clip in satisfactory fashion. By reference to the previous articles, note that sidewise flight can be obtained by raising or lowering the torque prop axis, or alternatively the weight can be attached to a wheel strut Keep this trick in mind, later, when building gas models, you may wish to position the gas tank in such fashion that the attitude of the model changes in flight; as for example, take-off directly into forward flight with the speed decreasing as fuel is consumed and with let-down in autorotation vertical. Cyclic control of the rotor is a bit more complicated, but not greatly so, and undoubtedly it will eventually replace C.G shift control except in the simplest models. This is particularly true when we consider the advantages of such a system in contest flying. A cyclic control system means having a control which can be moved to secure flight in any desired direction, without changing ballast, by altering the pitch of the rotor blades for a segment of their sweep around the circumference of the "disc " The type of cyclic control we are interested in for model work is the socalled "indirect" or reactive control, in which the linkage is not directly attached to the rotor, but to an intermediary point from which the rotor is controlled. If we tried to attach the cyclic mechanism directly to the blade roots, and connected the other end of it to the fuselage, we would find that this AIR TRAILS would freeze the system, resulting in a stiff rotor and destroying the stability we gained by freeing the rotor from the mast in the first place Therefore we must control the rotor from some point not rigidly attached to the fuselage. With the Bell system, this is the Young fly-bar control (see sketch). To work this connect the flybar to the longitudinal pivot with a jointed lever which can be cyclically pulled inward at the joint, thus changing the angle between the fly-bar and the blades, for a segment of each revolution The reaction of the blades to this deflection gives cyclic control. The Hiller Paddle system (see "Rotor-matic" sketch) uses two short wings set upon a cross-arm, which is attached to the central pivot. The angle of these wings or paddles may be changed through a simple scissors type linkage, which is attached to a swash plate. When the swash plate is tilted the angles of the paddles change in rhythmic cyclic fashion with each revolution, and the rotor blades' reaction to this produces a longitudinal rolling of the rotor, which results as cyclic pitch. This system is very simple, as is the Bell, but in both cases avoid any considerable play in the linkages since this may result in excessive wobbling and erratic control. However, for most small models this may not be critical because of the strong damping effect (scale effect) present in models. As a footnote to these two systems we can add that it isn't strictly necessary to duplicate the control systems of the originals in order to get satisfactory performance. Here is a simple dodge, which judiciously applied works most effectively Build the rotor, with its paddle beam or fly-bar in the simplest fashion and simply stick a wire up from the fuselage in such a way that the cross-arm bumps it gently at the same point every revolution Presto' The reaction gives you cyclic control. Remember, however, that this is control by unstabling—the bumper wire should be quite flexible or the fuselage may sway excessively, and. while it sounds very simple, and it is, it can get out of hand by displacing the rotor too far if the jolts are too heavy. OCTOBER, 29 I953 Tandem rubber job. Rotors are Young fly-bar type; Power transmitted through bevel gears at each end of long motor which equalizes thrust. Brake on one rotor permits forward flight. Co-ax close up. Dimensions not critical, but if large version is built top rotor should be hung In gimbal since tension of heavy rubber motor may not allow sufficient see-saw. In an effort to develop a system, which would lend particular emphasis to the qualities desirable in model helicopter work, we have designed a two-part series of rotors, which we term the "bungee-dynamic series." These rotors cover a wide field of application and include power delivered at the hub and power applied at the tip, which means the series covers rubber, internal combustion, rocket, pressure jet and ducted fan configurations In the middle of the series is our special pride and joy—a system which we believe to be the first truly successful, inherently stable, co-axial rotor arrangement, which positively controls the ancient problem of rotor clash The basic rotor and its derivations are shown in the drawings accompanying this article We start with a two-bladed rotor (see sketch "Basic Rotor Design—Cyclic Control") which is see-saw mounted in gimbals and free to pivot, within limits in a span wise fashion This rotor is of the first part of the series, which we term "locked " By this is meant that the pitch of the rotor blades relative to each other is Axed at all times (as in the Hiller) except as subject to collective pitch control. The blades are stabilized by means of dynamic weights, which protrude tangentially, about one chord length ahead of the Blades' leading edge. There is no fly-bar or paddle-beam; instead, we have a double horn to which are affixed two snubbers, or "bungees" which run to a swash plate which may be tilted to secure cyclic control. These elastic connectors replace the inertial damping forces of the fly-bar, or the aerodynamic damping of the paddle beam, and are simpler to work with than either of these. Because of the concentration of mass in the rotor tips we can use much lighter blades successfully— meaning balsa instead of birch or pine, and the corrective force is balanced at all times, exerting a positive, yet gentle steering action upon the system. This is the cyclic control version. And if we desire extreme simplicity we just move the bungee connections 90 degrees, that is, amx them to the span wise pivot to exert a continuous corrective force upon the seesaw axis, and the machine becomes controllable through C.G. shift 30 From this point of departure we proceed to multi-blade applications —we may build a four bladed rotor simply by doubling up what has just been described, except that of course only one mast attachment, or swash plate will be required. In order to build a stable co-axial machine, using rubber power as an example, we merely construct the lower rotor attachment with span wise pivots and attach it rigidly, that is, without see-saw gimbal to the drive tube with a bent wire "lead-around" interconnecting the blades. The upper rotor must be free to see-saw about ten degrees up and down, which allows plenty of leeway against clashing with moderate gap, and this may be accomplished, in a rubber model, by simply rounding the edges of the thrust button—the tension of the rubber motor being sufficient "bungee" action. If we build a gas model, with shafting, then of course the upper rotor must be mounted in a gimbal and snubbed with rubber bands, permitting damped motion between stops. Now with such an arrangement as this we secure forward flight by trimming slightly nose-heavy. No other cyclic control is required. For heading control a simple fin, as shown, corrects for the downwash, which may tend to rotate the fuselage the same way as the lower rotor. The sketch ("Basic Coaxial 'Bungee' Dynamic"), incidentally, is all the plan needed by any reasonably able builder to turn out his own machine in short order. One note on adjustment: The down wash’s tendency to rotate the fuselage is corrected by bending the fin. However, after doing so the machine may show a tendency to drift sidewise. This is due to the reaction of the air against the fin, so just move the rotor mast a trifle off-center to correct it, countering the side thrust with a bit of off-center lift. The second part of the series includes the unlocked rotors. These rotors may be built in any number of blades, from one, with counterweight, through two, three, four, five, or as many as desired. In the unlocked blade series (final sketch) we run into "dynamic pitch." By this is meant that the blades have no particular fixed pitch relative to each other or the mast, but seek pitch angles individually according to the speed of rotation. This is AIR TRAILS accomplished by positioning, the dynamic balances well below and ahead of the leading edge of the blades, which causes them to ride up under the action of centrifugal force until a balance is reached between the force exerted by the up-thrust of the counterweights and the aerodynamic pressure on the blades. It is important with this system to locate the hinge line knowingly to obtain high efficiency, but in the practical application we find it works well even with rough approximation of position. The hub attachment of this system to the mast may be quite varied, from a simple rubber disc which functions as a universal joint, to separate snubbers for each blade pivot. This system gives us a built-in and fully automatic cyclic and collective control. Auto-rotational letdown is fully automatic (with a simple ride-out dog release on the mast) which solves a mechanical problem that can be knotty, and cyclic control is merely a matter of shifting the C.G. There is just one precaution to be observed with this system in securing forward flight by C.G. shift. It is better to have the snubbers a bit too limp than a bit too tight, and don't overdo the noseheaviness. The reason for this is that a condition of "over-cycling" will occur if the snubbers are too tight, that is, the blade pitch will adjust itself too rapidly, accelerating the cyclic action, meaning the model will nose down and dive into the ground. If the snubbers are too limp the worst that will happen is that the rotor will tilt backward and forward flight will proceed at a snail's pace. This adjustment is by no means highly critical—the admonition just given is of the same order as instructing a builder of conventional planes not to tilt up the leading edge of the stabilizer too far if he doesn't want the model to dive in. Whatever system you elect to use, try to make your selection knowingly, based OCTOBER, 1953 This machine believed to be fist truly successful stable co-axial type to solve problem of control by C. G. shift and eliminate problem of blade clash. Could be flown with bungee cyclic control to lower rotor only. Model has been kept simple, no collective pitch used; hence letdown must be under residual power. Dimensions: Disc: 24". Mean chord; 1½ ". Tube: 7½ " x 1" dia. (1/32" sheet). Fuselage: 3/32" sq. stock 18" long. Weight: 2 oz. Performance: Altitude: 20 ft. Forward flight: 25-30 ft. at 5-6 ft. altitude (Hand-wound). That's high performance on three loops of 3/16" flat! on what you want to do with it, compared with its characteristics. For example, the unlocked bungee-dynamic rotor is perfect for jet power, quite good for gas engine, and a complete bust for rubber—because it wastes too many revolutions in getting started. Rubber is a special case anyway, since the number of turns is always strictly limited by dimension, which isn't at all true in the case of jet or gas power. For rubber models the best bet is to skip autorotation and bring the model down under residual power, or if you are the ambitious type, fly with a locked rotor, which unlocks and de-pitches itself when the power is exhausted. Once again, we strongly recommend that the first model should be rubber power—it will give you a wonderful opportunity to get the "feel" of rotor wing flying, without introducing a lot of distracting complications. (To be continued) 31 Once the reader has flown a rubber job successfully and wants to build a model capable of really big performance, it will be necessary to switch to gas engine or jet power. Let's deal with jets first. The Jetex motor is an excellent source of power for model helicopters; generally speaking two will be used, although it might prove practical to use up to four, although this complicates the problem or getting a number of motors ignited at the same time in order that the charges bum evenly to preserve the balance of the rotor. For that matter a one-bladed rotor, with the blade balanced by the motor, can be used very successfully—which I know sounds a bit contradictory, but the practical fact is that the burning charge getting out of balance in a one-bladed system is considerably less critical than, say, two or three charges consuming at an uneven rate in a multi-blade system. The reason for this seems to be that the thrust output of the Jetex varies according to the amount of fuel left at any given instant, and peaks at the last few seconds. Thus in a multi-bladed system we have several thrust peaks, and if they do not closely approximate each other the thrust load on each blade may vary widely, meaning considerable pitch variations in a dynamic pitch rotor. In a one-bladed, single-motor job, the thrust variation is inherently "in gear" with the single rotor blade. Unbalanced centrifugal loads due to fuel, charge consumption result in a narrow period of oscillation of the rotor mast, but since this vibration lies in a span wise plane the practical effect is not serious—for a model. The jets replace the dynamic weights of the unlocked type rotor, being mounted below and ahead of the* rotor tips. The angle of thrust should be slightly downward, and it may be necessary to provide up-pitch limit stops to facilitate getting the rotor going. The balance of the rotor blade on its pivot should be slightly nose heavy with fuel charge aboard. Note this, because of the position and forces exerted in this type of rotor it is not necessary to use stable blade sections— use the highest lift cambered section you deem practical and don't worry about pitching moments; the orbiting of the tip weight clamps the blade firmly at whatever pitch the speed and dynamic settings call for, and transition into auto-rotation after burnout is smooth and easy with a good let-down. The adapting of a tiny internal combustion engine that screams out its very high power rating at speeds in excess of 10,000 rpm to rotors, which run under 2,000 rpm, offers an interesting challenge. This may be achieved in a number of ways. The classical method is to reduce the speed and increase the torque through reduction gears. These should be of at least 5-1 ratio and there must be some sort of clutching arrangement between the gears and the rotor, otherwise it may prove to be impossible to start the motor, or gear teeth will be stripped by the high starting loads. A clutch satisfactory for this purpose should en- NOVEMBER, I953 With full size choppers more and more in the news this informative series will get you started off on the right foot in building your own model helicopter CLOUGH’S CONCLUDING COMMENTS CONCERING 'COPTERS By ROY L. CLOUGH, JR. 25 gage smoothly and positively, and may be either of the manual engaging type, in which the release of a lever holding two faces apart permits them to be forced together under spring compression, or of the centrifugal type which engages automatically with an increase in speed. See center sketch on this page. Clutches require access to tools and a knowledge of machining operations, but this should not deter a really determined builder. The ideal thing, of course, will 1% for some hep manufacturer to read this and produce a small lightweight clutch-reduction-gear unit at a reasonable price. Experience in the model racecar field indicates this can be done. Reduction can be had by means of pulleys and belts, with a sliding engine mount serving as a "clutch," but belting is not the most satisfactory power transmission. I have flown a K&B .049 job with belt reduction, briefly. The belt begins to slip after a time and the model descends. For this job I used a round belt running over wood pulleys at 4.5:1 with a heavy application of a good belt dressing. The problem seems to be that the high speed of the engine pulley soon glazes the belt, causing excessive slippage. Howard G. McEntee has suggested using small Vee belts. This might work a lot better due to the better traction offered by such a belt, but obtaining Vee belts and pulleys small enough for the purpose has been a poser. When using belt drive with gas engines, great precautions must be taken to keep fuel spray 06 the belt and pulley. A baffle between the shaft and intake tube and exhaust ports is highly necessary, and frequent wiping of oozed oil from the end of the main bearing is a must. Another angle, which I’ve been experimenting with lately, is to use a torque converter between engine and rotor. A torque converter is simply a specialized type of fluid clutch and operates without any direct connection. I use a small high-speed rotor connected directly to the engine shaft, running inside a larger rotor, which is connected, to the helicopter end. The casing is filled with castor oil. This device, in bench tests, appears to transmit a fair amount of power—with redesigning and a bit of finagling it should be quite evident. However, I have had a lot of trouble due to overheating, which causes some of the oil to ooze out past the bearings, and that results in lowered efficiency of power transmitted. In any event power for the torque prop isn't hard to arrange. Turn this about two to three times as fast as the main rotor by means of a simple string belt running over sandpaper-faced pulleys. Remember that the torque prop should stop when the model goes into autorotation in order that it won't swing the tail around in a circle on the way down. Simply attach the driving pulley between the clutch and the ride-out dog of the rotor. We mentioned this before, the rotor release. Whether or not you plan for autorotation you must have a rotor release, which permits the rotor to override when the power quits. (Continued on page 66) 26 AIR TRAILS Clough on 'Copters (Continued from page 26) Otherwise the great amount of kinetic energy stored in the spinning rotor may twist off a shaft or strip gears or even shatter the blades if the system suddenly freezes when the motor stops. This unit can be incorporated in the function of the clutch or may be a separate item in the rotor hub: I prefer it to be separate since this simplifies the operation of stopping the torque prop when the motor quits. Now, how about really simple gas motor hook-ups, requiring no gears or clutches? Sure, it is possible and practical, and may be accomplished in several ways. One way is to use torque reaction drive—such as in the little Infant powered job of the previous article. However, don't use the primitive semi-articulate rotor system of that model, but build your rotor along the lines discussed in the previous issue for the rubber co-axial job, except use unlocked blades on the big rotor to get a good auto-rotational descent, and locked, but feathering blades on the small rotor attached to the engine shaft, say in a rubber mount, to permit a small amount of see-saw action. Because of the strong downwash of the small rotor a brake or fin is required to prevent fuselage rotation, but for simplicity this is hard to beat. Propelling the rotors at the tips by means of propellers has been suggested many times by many people. It seems simple, but it can be very troublesome. The reason is two-fold. First, the props act as gyros running in a tight circle— meaning the engine shaft tends to twist upward or downward, depending upon rotational direction of the blade to which it is AIR TRAILS affixed; second, torque effects may add a bit of complication. You can, however, make such an arrangement work if you use my rotor configuration, the unlocked system, and play off torque and gyro effects against centrifugal loads. Use very light driving props of as high a pitch and small a diameter as possible, and place the thrust line of the engine angled toward, or away from, the chord parallel, depending upon which way you run the rotor; to help compensate for gyroscopic twist. In connection with this, note that the props can be shrouded, converted into ducted fans, with stator vanes to eliminate torque effects. This makes a neat looking job, but auto-rotation suffers heavily from any bulky excrescence at the rotor tips. Another method of drive is to use a pressure-jet configuration. Mount the engine in the fuselage, or in the rotor, as a blower supplying air under pressure to jet nozzle* in the tips of the blades. This system isn’t terribly efficient, but the great power-to-weight ratio of modem small engines will let you get away with it if you are careful. This produces very dean structures, smooth blades, and excellent auto-rotational and control characteristics—so in a way it might be said that the system is efficient after all. There is one angle in designing pressure jet jobs, which I am not too happy about. From the standpoint of efficiency it is a fine thing to have the cylinder head and exhaust opening inside the duct, that is, behind the fan, in order that the motor may cool better, run faster from the supercharging effect of air being rammed into the intake, and the pressure augmented by the heat of the cylinder and exhaust gas efflux. However, the oil sprayed by a 2-cycle engine tends to gum up the works and mess up the blower ducts. Tentatively I run my jobs that way anyhow and clean the ducts after each flight with a wad of cotton tied on a string, which is pulled through. Old-fashioned but effective. I have a grave suspicion, nevertheless, that the drag of the air against oil-coated tubes may cancel out the gain produced by exhaust heat-gases. Have you, for example, ever noted the ripples and ridges that develop on the surface of an oil-coated wing exposed to prop blast? That means quite a bit of drag, and it seems logical to assume that the same condition obtains within the pressure ducts of a blower jet system. While it is true that a lot of the oil is blown out with the air and by centrifugal force, a lot of it still sticks to the inside. And that isn't so good. Probably, in the interests of tidiness, it might be well to advise piping the exhaust into the open, and eschew the theoretical benefits in favor of the practical considerations. I have tried to present as many applications, suggestions, and observations as space will allow, in the belief that model builders win find more of value in something like this than they would in an article which dealt with the construction of one particular model and consisted largely of instructions to glue stick A to stick B and so forth. This 2-part article, together with the previous series covers, I fondly believe, enough of the basics of helicopter principles to permit anybody to turn out a very satisfactory job with a minimum experiment. Try it and see for yourself! NOVEMBER 1953 36 Air Trails, HOBBIES For Young Men "This is one of my all-time bests," says the designer who has been acclaimed as one of the country's most original men of modeling. No fancy gimmicks here, no frills, just a little easy construction, and then lots of fascinating flying ahead The Control-Line Gyro-Copter By ROY L. CLOUGH, JR. You'll stop the show when you put this spectacular rotary-wing job aloft. In flight it looks just like a big tandem rotor helicopter with lines reminiscent of the Piasecki and Bristol machines. Although the appearance of the model is very close to the double-ended helicopter types it is really more closely related to the gyro-dyne family—rotary wing machines which may rise up vertically, like a helicopter, but which depend upon a propeller for forward motion. In this respect it is somewhat similar to an autogyro. To avoid mechanical complication our model uses a short ground run instead of vertical take-off. With this system it is not necessary to power the rotors and taking off with forward speed is more practical in a controlled model because it keep the lines tight. Okay, it sound great, but how does it handle? Is it hard to fly? How does it behave in a breeze? The answers are that this model is actually easier to fly than the average sport job. The control response is very smooth and positive and it stays right out at the end of 50 foot lines with any good .19, as high as you'd care to fly any non-stunt type model of this weight, and the wind bothers it less than fixed wing models. There is a barely perceptible cyclic slap from the rotors, but, far from being a nuisance, this gives the "feel" of real rotary wing flying. You do not require any particular knowledge of rotary-wing craft to build and fly it successfully. Begin with the fuselage which consists of two 3/32" x 3" x 36" sheet sides cut to shape. The bulkheads are 1/8" sheet and the two rotor mast carrying bulkheads should be cut from very hard stock, or else substitute plywood. You will note that the fuselage follows very conventional construction lines for sheet balsa building and requires little or no explanation except at the front end. This model differs from usual controlliners in that the elevating surfaces are at the front end instead of the tail. Therefore study the control hook-up and be sure you understand it—the elevators are depressed to raise the nose, and lifted up to lower it, just the reverse of SEPTEMBER. 1955 usual. The landing gear arrangement should be followed; if you use a radial mount engine, for example, put in a plywood floor to bolt the landing gear firmly in place. Note the L.G. wire should not be firmly attached to the elevator cross-arm piece, but is held to it by rubber bands which act as shock absorbers. The motor mount depends upon the engine. We used a McCoy Sportsman .19 with rear rotor valving. This is about the top power which should be put in this model—in fact, if you go down to 35foot lines, a good hot .09 engine might prove quite adequate. The rotors are very simple to build, but a good touch with a soldering iron is necessary. These rotors are not rigid as they may appear at a glance, but semiflexible, which takes the cyclic jar and shock out and greatly increases the operating life. We mention this so you will not substitute a heavier wire than specified for the arms, or try to by-pass the soldering job by gluing up a solid wood rotor head. A glued-up rotor head seems simple and easy, and it is, but the catch is that if you equip the model 37 with rotors like this you can expect cracked blades after the first flight and somewhere along about the third flight you will get an interesting shower of broken balsa as the rotors shatter under cyclic pounding. Clean metal and acid-core solder and an iron a bit hotter than necessary will insure a good job. You do not have to use bottle caps of the exact size shown, for anything similar which will fit is okay. Be sure to leave at least one inch of wire between the blade root and the hub for flexing. The cone angle should be as shown; if no cone angle is used the model will not fly well in level flight, but will have to be nosed up, which is sloppy. Be sure the rotor masts tilt at the correct angle; the rear rotor operates at a greater angle of attack than the front to compensate for downwash effects. This will not make the model nose in. When you assemble the rotors to the mast make sure they rotate freely; there should not be any great difference in the ease with which each bearing turns. Flying the model is not much different than flying any sport job. The four-wheel gear produces exceptionally good ground stability, but do not neglect the usual down-wind take-off precaution—you have two big rotors here, plus a propeller, and if you flub a stall-off in a strong wind and the model rolls up in the lines it will take five years to untangle. After a couple of normal take-offs under normal conditions you will learn the trick of yanking the nose up immediately after your helper releases the model, and then letting it drop back. This trick sets the rotors spinning very quickly and reduces an otherwise 15-20 feet take-off run by half. Spinning the rotors by hand before releasing the model does not work well and should be avoided. Near the end of the run, when the motor starts to sputter, bring the model down to five or six feet. When the motor dies bring it in gradually. Full-size plans for the Tan-Giro are part of Group Plan # 9 5 5 Hobby Helpers, 770 Hunts Point Ave., New York 59, N. Y. (50c). A SURE FIRE AUTOGIRO Autogiros are usually tricky, but this one IS a sure fire performer by ROY L. CLOUGH JR. A DISTINCTLY rare item—the free flight model autogiro—has the reputation of being an extremely difficult thing to build and fly. Demonstrating that this reputation is quite undeserved, this model is simple enough to be knocked out in an evening and is no more difficult to fly than a conventional ship. In fact, it is not even necessary to set the rotor in motion before launching This model climbs at a steep angle and when power is exhausted floats gently back to earth on its spinning rotor, thus eliminating the chief cause of destruction of flying models—a headon glide into a solid object Begin construction with the fuselage, which is built up from 1/32" medium sheet balsa. Stiffened are used at appropriate intervals and the thin covering is backed up with 1/16" sheet at the point where the landing gear is attached Nose and tail plug openings are reinforced with strips of 1/16" x 1/8" stock. The bubble canopy is carved from a block of soft balsa Tail surfaces are 1/16" sheet and are cemented in place with no offsets of any kind Carve two end plugs; adapt one as a tail hook and the other as a thrust bearing for the propeller The prop may be sanded down from a purchased pre-sawed blank or built up as was the original. The prop should be of medium low pitch, and diameter should not exceed 9 inches Freewheeling would be of no particular advantage in this model Bend the landing gear from 1/20" steel wire and cement it to the reinforced underside of the fuselage Wheels are 1 1/4" in diameter and must be hardwood. The rotor and rotor mast, while quite simple, must be made exactly according to plan to obtain optimum performance. The mast is bent from a length of 1/20" steel wire and is anchored to a plate of 3/32" hard balsa which is cemented to -the top of the fuselage. A short length of drilled hardwood dowel is slipped over the mast and cemented to the plate for added strength. The rotor is acted upon by highly complex forces in flight and must be highly flexible to permit these forces to be damped out without upsetting the model The hub is a piece of dowel which is drilled to permit a loose fit on the mast The spars are 1/16" x 1/8" hardwood, pushed into slots in the hub at the angle shown on the plan, and cemented. Two short pieces of 1/16" x 1/8" balsa are cemented to the upper sides of the spars next to the hub. Rotor ribs are simply toothpicks. Cover the blade sections with a strip of smooth typing paper, 2 3/8" x 11" for each side. Note that the rotor has 0 degrees incidence and will spin in the proper direction regardless of the direction from which the relative wind comes. This is very important! Drill out two short pieces of dowel; slip one over the rotor mast, then put on the rotor, using the other bit of dowel to hold it in place. The proper height of the rotor above the fuselage is the shortest distance, which will give good propeller clearance. The retainers are cemented in place after testing. To test fly: install an 8-strand motor and balance the model at the rotor axis. Drop it from shoulder level a few times to make sure the rotor works well, then try short powered flights in calm air The model should climb without deviating right or left and is performing best when it gains a foot of altitude for every foot of forward flight Whatever minor adjustments may be required can be made by slightly bending the rotor mast MODEL AIRPLANE NEWS MARCH 1948 BEFORE YOU conclude that this is a model of a helicopter, take another look. It's a model plane with a spinning wing, or rotor, that windmills in the slipstream of a conventional propeller to provide the lift necessary for flight. The rotor is self-spinning and that's where the autogiro or gyroplane, as it is now called, differs from the airplane and the helicopter in appearance, in flying characteristics and also in construction. And on the end of a control line it is a new experience for model-plane fans. Control-line gyros have been built, of course, and flown with fair success. But none could be considered spectacular performers. Some showed a persistent tendency to roll up in the control lines and some that performed satisfactorily otherwise developed an arm-shaking vibration. This appears to have been largely due to use of a rigid motor, which tended to develop a condition of unbalance while in flight. The rocker-type, or seesaw, rotor used in this model starts spinning quickly and easily and the gyro lifts off and flies smoothly without dipping, diving or rolling. It pulls hard, but not too hard, on the control lines and settles as lightly as an autumn leaf when the motor fades. The fuselage is simply an elongated balsa box made mostly from 3/32-in. material except the bulkheads, A, B and C, and the stabilizer which Mount engine on the firewall with four small bolts, using washers under left mounting to provide offset Remember the spinning-wing autogiro? By ROY L. CLOUGH, JR. are 1/8-in. stock. Although the over-all size of the bulkhead, C, is given, you may have to do some fitting of this member to assure a true fairing of the fuselage sides and top piece. The fuselage is fitted with a conventional engine, propeller, landing gear and a standard controlline elevator for controlling the gyro in flight. The rotor mast centers 4-1/4 in. from the forward end of the fuselage. In assembly it passes through the bottom of the fuselage, the bend at the end being seated and cemented in a notch cut in the bottom of the fuselage. Note that it also passes through the control strut and the bell crank. Washers are soldered above and below the crank, permitting the latter to swing freely on the mast. After installing the controls and the reinforcing strips at the forward end of the fuselage, cement the fuselage top pieces in place, then the pilot's head and the fairing. Study the rotor drawing closely. Note that the blades operate at a negative pitch and that the rotor, although stiff from tip to tip, is pivoted POPULAR MECHANICS at the center to permit a seesaw motion. Stops on the hub pivot, limits vertical motion so that the blades won't strike the tail. This type of rotor mount allows the blades to rock without transferring motion to the fuselage, yet keeps the rotor tracking evenly. Give the model a coat or two of sealer before applying pigmented dope. Make certain that everything runs freely, and that the center of gravity is either right on, or just ahead of the control crank or bell-crank axis. If the center of gravity (CG) is behind the control-crank axis, the model may not pull hard enough on the lines to give good control. After you get the feel of it, you can make jump takeoffs by letting the model roll about 6 ft., giving it full up and dumping the-elevator quickly to bring it into a normal flight attitude. Incidentally, that machine-gun-like popping you hear in flight is common to all rotorcraft. It's caused by the rotor blades running into their own tip vortices. JULY, 1962 Torque Reaction Helicopter Models-further experiments By: Roy L. Clough Jr. Thus far in discussions of model helicopters most reports have stuck pretty closely to single rotor machines, or those in which a rotor, or pair of rotors support the weight symmetrically. However, for model work we find that duplicating the rotor arrangements of the big craft is not very practical except in rubber or jet power configurations, both types being unfortunately of short-lived duration. If we wish to use gas engine power, at this stage of the art, we must find some method of using a power plant, which grinds out several thousand rpm without getting into too much complication. One method of doing this is by designing our ships to the torque-reaction drive specifics, the system whereby the engine torque spins a large rotor in opposition to the rotation of a smaller prop on its shaft. (This, incidentally, should not be confused with true co-axial systems, which utilize equal-sized rotors turning in opposite directions.) Very good performance is possible with torquereaction drive although it has two major drawbacks: 1) it is not very efficient because of low mechanical advantage; 2) the system does not behave in classical fashion—that is, we have a new and different set of forces and reactions to deal with. Objection #2 is not serious if we remember to keep the reactions of this type isolated in our minds from the reactions of standard types and not confuse them. Torque-reaction drive helicopters are queer birds. They are almost as removed from conventional helicopters as, for example, an autogiro. The reason for this is that torque-reaction drive helicopters split flight duties between a large, slow-moving rotor and a prop attached to the engine shaft. The engine shaft prop is generally standard and it has one main function-it provides 99% of the lift. In some cases it may be used to contribute to stability as well, but the primary function is to lift the machine. Its gyroscopic effects are completely negated by the much larger mass of the engine and big rotor whirling around in the opposite direction underneath it. The function of the large rotor is to provide a torque drag on the engine, a device with which to secure stability and control, and finally, to serve as a parachute to let the machine down without damage when the power stops. This division of labor produces an unusual condition because, under power, the large rotor is operating in a substantially unloaded condition. Its blades are not damped by a strong aerodynamic pressure as they would be if the weight of the machine was being supported by them. As a result, control and stabilizing reactions assume an altered aspect. The builder who does not understand this may find his model crashing repeatedly despite his efforts to re-rig it for normal flight, because the control reactions, in most flight regimes, are actually reversed. If we build a very simple helicopter, with rigid, un-pivoted blades without tip weights and adjust it to fly forward we find that it starts to slide ahead, then noses upward sharply, slides back and repeats the pattern with increasing amplitude until it crashes. The reason for this is that the advancing blade produces a high lift force when it encounters the relative wind; this lift processes 90 degrees forward tilting the nose up, which kills forward speed, then the model slides back with what was the retreating side of the rotor now producing a lift which will move 90 degrees, or to the tail, riding the tail up then sliding back, etc., etc. So we now pivot the blades and fit them with dynamic balances. Now when the model moves ahead the air pressure on the front of the disc makes the rotor blade twist its pitch angle upward, 90 degrees ahead that is the retreating side, and downward, that is 90 degrees behind on the advancing side. When this happens the change in pitch 90 degrees to the side produces a force that is moved another 90 degrees, so that the rotor disk tends to tilt up at the rear and down at the front. When the model is in a state of balance the forces cancel out and the machine flies forward without riding up at the nose or going into a dive. This is due to the upward force of the relative wind striking the advancing blade being leveled out by the precessive pitch shift in the blades produced by the pressure of the relative wind, which tends to nose the rotor disk down. This is the way it should work, and does work when the CG is properly located. However, if the CG is improperly located trouble develops, and this trouble is usually a dive. Why? Suppose the builder flies his model once or twice and it works quite well, moving forward steadily. He then wishes to see it rise vertically. It would seem reasonable then, to add a bit of ballast to the tail to kill off the forward motion? Unfortunately it does seem very reasonable. We have the past precedent of fixed wing models; we have the precedent of single rotor helicopters, which fly forward if the weight is moved forward and back if the weight is moved back. Seems reasonable. So weight is added to the tail, the model rises up, starts forward faster than ever, noses down and crashes. Why was this? We just said that torque-reaction helicopters are a special case because of the unloaded condition of the rotor, which does the controlling. Here is what happens: We have noted that air pressure on the rotor results in a cyclic action which resolves to cancel the nose up effects of that pressure, that is, relative wind effects are self-nullifying. But, any force applied to the rotor reacts in cyclic control, the blades shift in an effort to nullify the applied force. Now, when we add weight to the tail we are placing a steady pressure on each pivot blade as it passes over the tail-the CG has shifted—and by reference to gyroscopic precession laws we see that this force will result 90 degrees further on, or at the side. Thus the blade advancing tilts down and the blade which is retreating on the other side, tilts up. This tends to twist the rotor laterally, but again referring to gyroscopic rules we can see that this twist, moving 90 degrees, resolves to push the nose down! Thus if we take a helicopter which is adjusted to rise vertically, and move the CG aft a little bit the model will now fly forward—BUT if we move the CG too far aft the model will overdo it and dive into the ground. This is because we have two cyclic instigators working, the CG imbalance, plus the normal cycling produced by forward flight. A model of this sort therefore is fairly sensitive to CG location, too sensitive, as a matter of fact, so it is customary to build in a safeguard which will allow a wider altitude of CG travel before diving or tail sliding occurs. A good example of this is the Berkeley kits, which use two different methods of obtaining the same result. In the D model we note that two of the blades are fixed in pitch. Thus, as the model moves forward the lift build, caused by increased relative wind meeting the stiff blades tends to push the nose up, while the cyclic action tends to push it down. Since the up couple is a bit stronger we also have a drogue on this job, which increases the cyclic reaction of the pivot blades, and, secondarily slows the model down. ' Thus, within allowable CG travel the tilt angle of the machine is self-governing. If it slows down the cycling action, which is fully automatic, tends to speed it up, if it goes faster, the stiff blades bring the nose up, slowing it down. This governing action is pronounced enough to permit flight in surprisingly high winds and gusts without getting into trouble. However, if the CG is moved too far aft, the balance of forces is upset and the model will dive in. Ordinarily the model D gives no trouble—except where the builder has put on several heavy coats of dope and has not re-checked his CG afterward. The CG position shown on the plan, incidentally, is for absolute maximum top speed. To climb vertically it must be moved ahead with ballast. The other model, the TR, has four pivoted blades and uses a swivel prop to provide a recovery couple. When the tilt is to the right, changing the lift vector, which puts a side load on the rotor which induces a cyclic shift which pushes the nose upward. This model has a tail rotor to control heading, and a few words on this: A rudder will not make a helicopter turn. A positive side thrust is required; hence a tail prop is needed to push the tail around or to hold it steady. A rudder will only crab the ship slightly while it continues in substantially the same direction. Another method of obtaining turn without a tail rotor is to tilt the rotor mast toward the side toward which turn is desired. Don't get confused on this, the model does not slide that way, but the downwash rebounds from the side of the fuselage at a different angle, tending to roll the model over—but again by gyroscopic reference, the roll is resolved at 90 degrees into turn. There are many ways in which a torque-reaction helicopter can be set up. One thing, which is quite important, is to respect the fact that the fuselage lies in the downwash of the small prop, and exposed areas should balance, or very nearly so or there may be serious trouble. The use of small fins in the prop wash to obtain turn, or to reflect the wash' backward for reactive forward propulsion meets with some success and one can use a twisted stabilizer which tends to put torsion on the fuselage with increased forward speed, to induce nose-up cycling, relative wind strikes the prop edge it as a corrective force couple. When designing originals it is a very good idea to include always some governing factor on forward speed. Rig it either with a swivel prop, a stiff, alternate set of blades, or torsion fins. Speed of forward flight will vary with the design and power plant, and will not be as high as a fixed wing model— a good fast walking pace is about right with present designs. —ROY L. CLOUGH, JR. THE USE OF TORSION FINS "A" must clear rotor disk. Fins may be either horizontal or vertical. As forward speed builds up, fins tend to roll fuselage to right, which induces nose-up cycling moment. FORCES ACTING ON TYPICAL HELICOPTER Barred lines: drag of drogue tail produces down pressure on balance weight of pivoted blades which induces cycling action which tilts blade down at side and pushes nose down. Dash lines: fixed pitch of this blade encountering relative wind produces lift at side, but since rotor functions as a gyro the reaction moves 90 degrees, producing nose-up tendency. Solid line: wind pressure on pivot blades reacts at 90 degrees to make pitch change shown to hold nose down. Thus, if CG is too far aft it induces cycling in the pivoted blades which reinforces down control of drogue tail and wind impingement on pivoting blades and overrides nose-up tendency of fixed blades and the model will dive in. Centered CG has no cyclic effect and model will rise vertically. CG too far to front will cause model to back up or tail-slide. NOTE: CG is usually slightly aft of mast CL in order to balance fuselage effect and promote forward flight. FORCES ACTING UPON TYPICAL SEE-SAW PROP HELICOPTER A) CG rigged tail heavy induces cycling in pivoting blades which causes nose-down forward motion (barred lines). B) With CG centered, model rises vertically. C) Nose-heavy CG will cycle blades into backward flight (dash lines). Wind pressure on blades produces precessive pitch change at side position preventing nosing-up (solid lines). Role of the swivel prop: wind pressure on front of see-saw prop, by gyro precession, causes it to tilt to model's right, which angles lift vector to right. Side thrust on rotor system produces cycling which makes nose of model ride upward, thus limiting forward speed and preventing dive (assuming CG is correct). Seesaw prop must be mounted to rock freely for best results. (Seesaw prop can be eliminated if two opposite blades are fixed pitch with counterweights removed. Air Trails Model Annual - 1956 Snapper By Roy L. Clough Jr Ever since the first half-A engines appeared we've thought it would be a riot to stick one on a ten-inch wing and turn the contraption loose. We finally pared some wings down to mere stubs on an old free flighter and tried it. It was a riot . . . a short-lived one. After we swept up the balsa wood (never leave the pieces in a hayfield—it's bad for cows) and cleaned the turf out of the engine we came to the conclusion that a free flight speed job would have to be a carefully tailored affair. The wild corkscrew gilhooley and painful thump of the clipped down free flighter had given us a lot to think about. A model intended to reach high speeds in free flight must have (1) a high degree of directional stability, (2) a sharply limited motor run, (3) no tendency to climb or dive under slight variations in power output, and (4) be light and very rugged. In order to obtain these characteristics we must (A) find some way of managing a whale of a lot of torque with a small Author Roy L. Clough Jr. wants you to admire that ultra simple, surgefree, positive-duration fuel tank! Full size working Drawings are on Hobby Helpers’ group plan #1162 American Modeler --November 1962 wingspan, (B) limiting the motor, run reliably without a timer mechanism, (C) making the model insensitive to gusty weather, and (D) using the lightest and most simple geometry consistent with adequate strength. "Snapper" is the answer. It is a reliable little ship. It will fly in calm or windy weather with anything from a Cox .010 to an Atwood .049. With a good hot .049 it will hit close to 100mph. Snapper is rakish, but, except for the cockpit, styling had nothing to do with its appearance. It's designed that way because that is the shape that will best do the job. Any built-in offsets in thrust line, wings or control surfaces are out. It doesn't take an engineering degree to figure out the reason. The model is light and it goes like a devil with his tail on fire. You'd never get a chance to balance off wing incidence by varying down thrust or to use any of the usual free flight adjustment tricks. The wings, stabilizers, fin and thrust line must be substantially parallel to each other. Dihedral angle raises the tips of the wings and this raises the center of resistance. We have to counter it by raising the thrust line a little above the wing. We require a special fuel tank and it has (Continued on page 47) 29 to be on the bottom of the plane. This pretty clearly calls for an inverted engine mounting. So, we start the motor with the plane held upside down where we can check the fuel flow. Don't try to use a timer tank or fuel shut-off. This little job will chew off about 100 feet of airspace a second when it gets rolling. That means it could be well over a mile away in less than a minute if you forgot, or if something stuck. Somebody is sure to ask why we included a landing gear on a handlaunched speed job that lands in the grass. The answer is: it helps to keep dirt out of the engine. But don't expect any wheels-on landings. 47 All that torque and no rudder? Just elevators? That's correct. Because of the small span of the model the elevators act as ailerons. This means we correct for torque effect by giving the elevators a differential twist. The left one slightly down, the right one slightly up. The less one has to monkey with on a high-speed rig like Snapper the better. Cut off the needle valve about a sixteenth of an inch outside the needle valve body, file a slot in it and do your adjusting-with a screwdriver. If necessary, jam the needle valve body a little out of round to get the necessary friction. Needle valve settings (on the Atwood) vary about half a turn around the "ideal" position. Model is started with a heavy prime and the first tankful is run out to warm it up. It doesn't seem to be practical to connect the open end of the coiled fuel line to a tank then detach it before flight. This changes the suction pattern and the needle valve, would be in need of adjustment before launching. With the arrangement shown the motor turns over for about 12 seconds. That gives you about 8 seconds to detach battery wires, straighten up your aching back and give the model a solid heave. Plenty of time, once you get used to it. The model will whizz for a couple hundred feet before running out of juice. When it does it will slow up like it hit a brick wall and roll to the right. Don't expect much of a glide. Pre-flight adjustments call for an arrow-straight "glide" with a fair amount of roll to the right. Make your first test hops over deep grass with low pitch props; step up the pitch, and the speed as you – become accustomed to the adjustments. Snapper should fly 10 to 15 feet up, No thermal worries here! American Modeler -- November 1962 Skyhook... By ROY L. CLOUGH, JR. DRAWING boards and in secret test ONhangars of at least a dozen major companies and scores of smaller ones the helicopter of the near future is being evolved. Rotating-wing craft have caught the public fancy, and manufacturers are hurrying to perfect their direct-lift wares for the postwar market. Already at least three distinct types have flown successfully. In the helicopter, torque effect is one of the major problems. If a single rotor were attached to a power source with no provision for this effect the entire fuselage would spin around and around. Two rotors revolving in opposite directions around a common center overcome this tendency. Counter rotation is employed in Skyhook, a model that flies straight up like the real thing and, when the power is expended, descends in a spiral and lands on its wheels. Skyhook is best flown indoors, but may be sent aloft outdoors on calm days. It will be noted that the motor tube, which also serves as a shaft for the lower rotor, is attached only by a simple bearing at the 148 lower end. The upper end rotates freely in a hole in the top of the fuselage with 1/8" clearance all around. Power absorption in one rotor is constantly balanced by that of the other and an unbalanced torque condition cannot occur. Elimination of torque is not enough, however, to obtain satisfactory flights in this type of model; hence the directional vane pointing rearward from the top of the fuselage. As the downwash of air leaves the lower rotor, it does so with a rotary motion and tends to impart this motion to the fuselage and cause it to revolve in the direction of rotation of the lower set of blades. To forestall this effect, the vane is attached at approximately the same angle as the upper rotor, and in this position acts to exert a push in the opposite direction and keep the fuselage pointed straight. The tips of the lower rotor are bent downward at a 30-deg. angle to give adequate air flow over the directional vane. A word of caution: A free-flight model helicopter is not an easy thing to build because of the number of "bugs" inherent in the helicopter idea. In fact, it might be said that if a model helicopter flies at all, it's good! Therefore, it is recommended that the plans be followed closely. Try to keep the weight down. Do not dope or add unnecessary detail to the model. Excessive weight means more power will be required to fly it, and more power means more rubber, fewer winds, and more weight. This can develop into a vicious circle. Notice mounting strip for the front wheel between the bottom longerons of this unfinished fuselage. A cross brace midway at the rear adds strength. A FLYING MODEL HELICOPTER It is best to form the motor tube of 1/20" medium-soft sheet balsa, but if this is not obtainable use 1/16" stock, well sanded. To avoid splitting, soak the wood in hot water before bending it around a circular form and wrapping in place with gauze. If a form of the size indicated is not available, the diameter of the tube may be safely altered, taut remember to change the hole in the motor guide plate accordingly to retain the 1/8" clearance. When the tube is thoroughly dry, slip it from the form and cement the edges together. Near one end of the tube Two rotors revolving in opposite directions overcome torque. cut two small holes in opposite sides for a short length of 1/8" dowel to hold the Build one side of the fuselage upon the other as in end of the rubber motor. Run a bead of cement a conventional model, using 3/32" square medium around the edges of these holes to prevent the wood balsa strip. Soak the upper longerons in hot water from splitting. before bending. Crosspieces are required at the points From 1/16" medium stock cut three disks to fit marked "X" in the plan, and another may be placed closely inside the tube. Cement one flush with the between the upper longerons near the rear for greater upper end of the tube and another about 1/8" inside strength. The floor the lower end. Keep the third for future use. Motive parts include six rotor blades, motor tube, and top rotor hub. Note lower blades are cut shorter. plate shown in one photo is 3/32" by 2-1/4" by 2-3/4". Center a 1/32" by 1/4" strip between the lower longerons from the floor plate to the nose to support the front wheel. Cover the windows with cellophane or light celluloid and place dark-blue tissue on the rest of the fuselage, except for the space occupied by the motor guide plate on top and the floor below. Water-shrink, but do not dope, the covering. Form the landing gear from 1/32" hard balsa sheet, cement it to the lower longerons as indicated, and mount 1-3/4" balsa or celluloid wheels on its ends with pins. Attach the 11/2" front wheel with a wire strut. Cut the six rotor blades from 1/20" balsa, well sanded. Notice that the plan below shows the top surface of the upper blades and the bottom surface of the lower, since the upper rotor moves counter-clockwise and the lower clockwise when viewed from above. Also notice the shape of the cross section. Do not dope these blades. Carve the upper rotor hub from soft balsa and install the motor hook through a standard thrust-plug and bearing as shown. The motor ring may be cut from 1/8" balsa, but two 1/16" sheets glued together with the grain crosswise have greater strength. Cement the ring to the motor tube about 1/2" from the upper end. Attach the upper blades to the rotor hub at a pitch of 25 deg., with a 2" dihedral under the tips. Mount the lower blades on the ring at 25 deg. but with no dihedral. Bend 150 down the tips as shown. Make certain that all blades balance and track evenly. Now bend a paper clip to the shape shown on the plan so that it will stand upright. Thrust the stem through the third disk cut for the motor tube until the bent part rests flat against one side. Put plenty of cement into the recess at the lower end of the tube and push the disk with wire attached inside. The lower bearing is a 1/2" length of 1/16" OD. brass tubing soldered into a 1/2" by 1/2" piece of tin plate. Cement the latter to the center of the floor plate. Next cut the directional vane from 1/20" sheet and cement it to the motor plate at the point indicated on the plan. Wet the wood at the thin part and twist until the vane has approximately the same pitch in the same direction as the upper rotor. Now install the rubber motor. About four loops, or eight strands, of 1//8" flat rubber are required. Slip the tube through the motor guide plate and lower it into the fuselage. Poke the lower shaft through the bottom bearing. Solder a washer to the end to hold it, or bend over the end of the shaft, and Skyhook is ready for a trial flight. All take-offs should be from a level surface. Hold the circular lower rotor hub stationary and wind the upper blades. Set the model on the ground with upper and lower rotors between forked thumb and forefinger and release both simultaneously. Above: A shot of the full-scale Sikorsky S-51 helicopter in flight. About the only real difference between the real one and the model is that the aft rotor on the model does not turn. Instead, it is replaced by a celluloid disc that supplies ample stability to keep the model flying straight. Left: A still shot of the model hanging from a string. The prop was held rigid for this shot so as not to tilt the model: The working prop is mounted so that it will swivel on the prop shaft, as shown on the plans. The ship is made of sheet balsa sides cemented to sheet balsa formers, with a simulated cockpit. SIKORSKY S-51 by Roy L Clough, Jr. In answer to many requests for a realistic helicopter that actually flies, we offer this semi-scale Sikorsky. A good action shot showing the model in actual flight. Performance is realistic with no danger of hard landings when the engine cuts as freewheeling vanes ease the model down. FLYING MODELS FEBRUARY 1953 • Probably the most famous design of pioneer helicopter builder Igor Sikorsky, the S-51 helicopter has racked up an impressive record in life-saving and rescue operations, both at home and abroad. It is the standard unit of Los Angeles Airways, first airline with scheduled helicopter operation, and has been manufactured in England by Westland under license from the parent company. In addition to its performance record, it is generally agreed to be the most beautiful rotary wing craft ever built, with clean flowing lines that adapt themselves readily to scale model practice. The big ship uses a three-bladed rotor of the type known in the trade as the "flapping blade" or articulated system. This rotor type has an extreme degree of maneuverability with rapid control reactions and is quite stable in normal cruising flight. The torque effect of the (Please turn to Page 34) 15 SIKORSKY (Continued from Page 16) rotor is nullified by a small rotor attached to the tail boom which produces a counteractive side thrust and is used as a heading control. This arrangement is fine for a full-scale craft, but the unstable hovering characteristics of an articulated rotor limits its usefulness to piloted craft— it is not the best system to use on a model which must fly independently and has no pilot aboard to correct disturbances due to gusts or roughness in the air which are present under even the most ideal conditions. Therefore we must use a rotor, which has a degree of automatic stability if we wish our model to fly for more than a few seconds without skating wildly in all directions and finally crashing. Our first S-51 model, therefore, used a dynamically stabilized rotor of the so-called "feathering" type. That is, the blades did not flap up and down, but rotated within limits in a span-wise plane, allowing flight deflections to register as pitch changes instead of flapping movements. The pitch changes served to maintain the stability of the machine by adjusting the lift of the rotor from sideto-side as required, since the blades were independent of each other and, to a limited extent, of the rotor shaft. Pitch was determined by rotational speed (centrifugal force) and the model used a rear torque correcting propeller. The power was rubber and thrust was transmitted through a bevel gear drive to the main rotor and by pulley to the tail rotor. This model flew very well, was stable and able to cope with rough air without upsetting or going into a wild dance. However, the duration was very limited and the altitude attained was not very great, due to the complexity of the machinery required and the rather sharply limited output of twisted rubber bands. We decided to scrap this design in favor of something that could be powered by a ½A engine, on the theory that builders would rather have a much simpler model with greater performance, and would be willing to sacrifice a bit of scale appearance to get it. By using the torque-reaction drive, we eliminated gearing and clutches and the need for a torque prop. The dynamic stabilizers, which govern individual blade pitch, were retained, giving a good, positive and fully automatic auto-rotational let-down when the motor quit—an important factor in models having any considerable weight and power. The torque prop, an outstanding feature of the original, was replaced with a clear disk of plastic, which serves as a fin. The result is a model which is quite realistic in flight, more rugged in construction, and actually much simpler to build than the original rubber-powered version. Construction: The fuselage is a straightforward semi-monocoque keel-type affair. Build one side over the keel on a flat surface to insure good alignment, then put on the half-bulkheads on the other side and finish the job. Attachment of the landing gear and rotor 34 shaft should be quite clear from the plans. Note that the landing gear struts have been omitted since we want a springy gear to absorb landing jars. Window details are best painted on with a contrasting color—plastics do not take kindly to the spray of fuel and oil from the engine (yes, you can use a 1/4" sheet profile fuselage if you want extreme simplicity—but move the CG ahead about 3/8" to allow for altered fuselage effects). The rotor mechanism and engine hook-up is quite a simple affair, but study the plans carefully and make certain you know how it works before tackling it. The hub is tin-can stock, the blade arms 1/16" steel wire soldered carefully in place. All bearings and bushings may be made of brass tubing, or simply rolled around a music wire form with flat nose pliers, using thin brass or tin-can stock material. Make the rotor blades from a good tough variety of 3/32" sheet balsa and be sure the rotor blades' tip weights (dynamic stabilizers) are securely cemented in place and bent to the proper angle. The amount of weight should be just enough on each blade so that the blade will tip forward to maximum "down" pitch when at rest. This weight will vary somewhat from model to model, but is not critical within wide limits as long as only a reasonable amount is used. Understand how these weights operate—under centrifugal force they ride up, increasing blade pitch, if the model tilts they alter the blade pitch to provide a corrective side thrust and, lastly, when the engine runs out of fuel they govern collective pitch and throw the rotor in auto-rotation to bring the machine down safely and slowly. The recommended engine for this model is the K&B .049. It is recommended because of the ability of this engine, which has a longer stroke than some, to carry a very large prop without killing out—a very important consideration in torque-reaction-drive helicopter models. It also has a very handy mount and the gas tank comes in the right place for this sort of model. Balance the cylinder with a blob of solder on the blade holder arm opposite the tank. The finished weight is of much greater importance in a helicopter than in any other type of model. This model should weigh at least 4.5 ounces and less than 5.5 ounces for best scale-type performance. If it is too light it will zoom up much too rapidly to be properly enjoyed, and if it is too heavy it may be sluggish about rising— particularly on hot days. When the model is finished (up as far as the special engine shaft rotor, and we're saving that to describe last for a good reason), check it over for good blade tracking and alignment. This model flies not only vertical, but forward as well. In order to get it to do this without incorporating a cyclic control mechanism we took advantage of the shape of the thing. Forward flight is produced by the reaction of the downwash from the engine prop against the flat front of the rotor pylon which creates a force which tends to tilt the nose down, and the reaction to this tendency to tilt by the main rotor blades results in an automatic shift of pitch which propels the model forward. FLYING MODELS FEBRUARY 1953 SIKORSKY (Continued from Page 34) Now, when the model is finished up as far as the special see-saw engine rotor, it may be a strong temptation to stick a prop on it and turn it loose— just to see what will happen. If you try this stunt be sure to have a dustpan with you because you may need it. It it quite true that you can fly the model this way, and if your balance is good you may get away with it for half a dozen flights in dead air. But, just about as you are deciding that Clough is an overcautious old fuddyduddy, your model may tilt over on its nose and end its career in one glorious full-throttle plunge into the ground. The reason for this happening (with a stiff center prop) is that the main rotor blades "feather" or adjust pitch angles relative to the air pressure on them at any given rotational speed. This is a condition of neutral stability which means that the model will fly stably unless disturbed by some external force—all things being equal. Unfortunately all things are not equal in actual practice. A gust may hit the model, or a bubble in the feed line may make the motor kick -or bump, which may set up a jiggle or tilt which will cause the rotor to shift its position. Study the rotor a bit. Note that it functions as a gyroscope. If a condition of excessive forward speed or sidewise skid occurs, we have a strong pressure upon the tip of the lead blade (the blade which at any given moment is perpendicular to airflow on the upwind side), and this pressure produces a resultant force 90° behind the point of impingement, which is the characteristic gyroscopic reaction. This force resolves into altered blade pitch as the weight seeks to justify its inertial forces, and this pitch alteration causes another reaction back to the front of the rotor disk which pushes the nose of the model down into a dive. Since this condition is self-propagating, there is no hope of recovery from such an attitude barring a miraculous gust of wind or engine stoppage which, by pulling power from the rotor, kills off the precessive cycle allowing the nose to ride up again as the blade shifts into auto-rotation. At this point somebody is sure to ask: why not add little dihedral sections to the tip of the rotor ahead of the pivot line, so that air pressure in forward (or any directional) flight will impinge upon the tip of the leading blade, forcing it to assume a greater pitch and lifting it upward to return the model to even keel? It won't work that way. If we try it we find that the model, instead of diving, now rolls over on its 44 side, because when the blade pitch changes at one spot—in this case the front of the model —the reaction comes 90° behind the alteration and the model tilts sidewise and crashes (Factually there is a reverse reaction 90° ahead of the deflection in addition, since if one side tilts down the other must tilt up). Thus the solution of this knotty little problem calls, in this case, for an automatically regulating counterreaction that will at all times interact with the forces of the main rotor to provide recovery couples. We do this by installing on the engine shaft a special type of rotor or propeller which is pivoted to "see-saw" gimbals. This isn't very difficult to build. Simply carve out a prop to the dimensions shown and, instead of mounting it with a hole through the center, mount it in a U-shaped pivot bearing, using a length of 1/16" steel wire for a pivot shaft, which runs through the side of the prop. What have we here? Well, this prop has fixed pitch, it does not feather as does the big one beneath it, but it can see-saw on its trunnions. When the motor is running, it "planes" and runs flat and true. When the model starts to slide, this see-saw prop tilts back opposite to the direction of sliding. This produces a complex of forces, but essentially it serves as a drag in that the faster the model goes the more it tilts back, producing a counter-reaction and an opposing gyroscopic deflection that limits the speed of the slide to practically zero. The model, which was neutrally stable with a stiff center prop, now becomes inherently stable with a seesaw prop because a positive reaction is obtained which produces automatic correction. This means the model will simply hover in one spot unless some other factor is added to make it fly forward, and the flat front surface of the rotor pylon takes care of that. If you want more speed in forward flight, gradually shift the CG ahead a little at a time until you get what you want. In our experience, few things offer the satisfaction and enjoyment of a good model helicopter. This model is a good one. Build it carefully, according to plan, and it will give you performance you may have believed impossible, particularly if you have tried unsuccessfully in times past to adapt model engines to helicopter practice. BILL OF MATERIALS (Balsa unless otherwise specified) 3-3" x 1/32" x 36" (medium)………….Fuselage sides 1-3" x 1/16" x 36" (medium hard)..…..Fuselage keel 1-5/8" x 7" x 1/8" (hardwood)…………..Prop blank 1-4 ¼" dia. .012 thick (plastic)……………………….Fin 12" length of soft iron wire 1/16" O.D.; clean discarded tin can; loop of rosin core solder; 2, 1" dia. rubber wheels; 1, ¾" dia. rubber wheel; leather or fibre; small washers; dope, cement, fuel proofer and decorations; K&B .049 engine. FLYING MODELS FEBRUARY 1953 This mini whirly-bird is a lot closer to scale configuration-wise than you'd think; big difference is way rotors are constructed and how they work. Semi-Scale Sikorsky R-6 One of history's most significant 'copters by one of modeling's most unorthodox designers; it's a mighty happy combo! In flight the model R-6 is a majestic sight. You'll really stop traffic with this one. Easy to build and a real thrill to fly as a free flight job. By ROY L. CLOUGH, JR. •The Sikorsky R-6 helicopter is historically important for several reasons. As a design it marked the beginning of a trend away from unlovely steeltube box structures, demonstrating that a helicopter could be beautiful as well as efficient. It was one of the first to be operationally fitted out as a flying ambulance— it could carry two external pods, each holding two stretchers on either side—and it took part in many early military experiments designed to test the utility and application of rotary wing craft. The model R-6 follows in the historical tradition by introducing a new model helicopter rotor system, the "multi-phase rotor" which permits use of true mechanical cyclic control in addition to the automatic cyclic and collective pitch normally used in models. The "multi-phase" rotor system is based on the idea that it is possible to build three distinct types of rotors which occupy the same space at the same time, so that the reactions of one rotor are modified by the others, etc. This is an extension of the co-axial system previously published in which one rotor was a rigid-feathering affair with the other a see-sawfeathering type, the interaction resulting in an automatically stable co-axial system. The multiphase system uses three rotor blades, each with a different characteristic dynamic reaction. Thus we include the desirable features of each blade type, while suppressing the undesirable reactions in the composite meld. (The reader should be cautioned that simply tossing together a number of different types of blades in one rotor is no guarantee that the good features will emerge and the bad features be suppressed—it can come out the other way around.) Air Trails Model Annual '55 For example: A rigid, non-feathering blade produces a nose-up resultant in forward flight, it does not autorotate; a Clough-type tip weighted blade produces a nose-down resultant in forward flight, and it autorotates beautifully; an angled hinge blade will tend to adjust pitching motions, it autorotates fairly well, but it is very critical in adjustment. In the multi-phase system we use the rigid blade to counter the nose-down tendency of the feathering blade (as in the Berkeley model D). What does the angled hinge blade do? On this particular model we wanted to use a manually set cyclic control, which flips the feathering blade to produce forward flight by mechanical cycling, as in full scale, rather than by induced or C.G. shift cycling as is generally done in models. But, if we use a fixed cyclic deflection on the feathering blade, in conjunction with a fixed pitch stabilizing blade, we discover that as the speed of the model increases in forward flight we have two cyclic forces: first, the fixed mechanical cycling which will always be the same, and second, the dynamic cycling caused by air pressure on the entering edge of the rotor disk. This induced cycling increases with forward speed at about the same rate as the nose-up cycling effect produced by the fixed pitch blade; therefore, if we add mechanical cycling to it we find that the model will accelerate and go into a dive. We could prevent this by using larger fixed blades operating at greater pitch—but this would spoil the autorotation. So we add an angled hinge blade to the system. This will autorotate, and as forward speed increases the air pressure in front of the disk causes it to bend downward and increase its pitch on the advancing 47 side, and bend upward and decrease its pitch on the retreating side. Now we can pre-set the rotor system with a fixed amount of cyclic deflection on the feathering blade and the model will accelerate up to the point where the induced reverse cycling of the anglehinge blade cancels out both the pre-set and induced cycling in the feathering blade and will go no faster. If air conditions, gusts, tend to speed up the model the rotor system increases it’s cycling momentarily to kill off the speed, then resumes normal operations. If, in calm air, we launch the model sharply nose down, it slides forward, slows down, then finds its own optimum speed, and proceeds at that rate. When the power stops the model descends in autorotation, the rate of descent being governed by the fixed pitch blade, which acts as a governor upon the two automatic blades. This incidentally does not produce a wobbling descent, provided any reasonable autorotational speed is maintained—90 rpm or a little better. Construction The model is a keel job; lay out and bulkhead in the usual manner. Note how the landing gear struts are cemented in position between blocks. Make sure these are dry before covering. The rotor mast should not be hard steel wire—use something fairly soft so it can be adjusted easily. The nose block goes on after covering. The covering may be 1/32" sheet balsa, or fairly stiff double-calendered paper miking about .008. If you use paper, start at the tail and work forward, lapping each joint 1/8" on the bulkheads. This paper covering trick produces an extremely smooth sheet-metal appearance and finishes with a minimum of doping, but it is slightly heavier. Whichever cover is used, note that the top area between bulkhead C and B must be covered before the pylon is sheathed in. This provides a working base to which to trim the pylon covering. Also be sure to cut a slot for the rear wheel strut. The tail rotor is simulated by a plastic disk. Edge it with a circle of rattan or reed to keep its shape. It functions purely as keel surface. Cabin detail is painted on in a contrasting color—silver blue makes a good "glass"—and the front of the machine may be doped as much as desired since additional ballast will be needed in any event to balance the tail boom. Before tangling with the rotor mechanism study the plan carefully. Sheet metal parts may be cut from tin can stock or secured from a Berkeley kit where applicable. The big idea here is to have everything tight that should be tight and freely-working on pivots and hinges. The rotor mast bearing should be very free, almost sloppy, but the pivots should work easily without any play for best results. The rotor blades are very simple, and while you're at it make a couple of spares, just in case. Assemble Sikorsky R-6 built in 1943 was the first military high-performance helicopter. It would climb to 5000 ft. in 7 minutes, could carry bombs. 48 the works and check the blade balance next. It won't ordinarily happen, but it is possible that the rotor assembly may balance perfectly by accident due to wood density variations. If this should happen, don't fly the model this way because a little extra mass is required on the tips of the fixed and angled hinge blades—about equal to a dime. If in the balancing operation more weight is required on the feathering blade with the tip weight, add this extra weight on the hinge line, not on the counterweight arm. Do not put the cyclic mechanism on yet. The original model used a Wasp with its fuel tank modified as shown on the plans so it would operate without throwing fuel out of the vents. Let's fly it. Check the C.G. location by holding the model sidewise by the engine shaft. If the tail dips down it is tail heavy and may dive; the best trial position is very slightly nose heavy or balanced on the mast axis. Fire up the engine and make sure it is delivering full power before releasing the model—a ragged 2-4 cycling engine is poison. Release the model from a level position and watch it! If you have followed directions- closely the machine will rise up steadily, move forward very slowly and will probably circle rather tightly to the left—probably a bit tighter than you may desire, so bend the rotor mast slightly to the model's right, which will make it fly straight, or turn to the right, depending upon degree of bend. This, by the way, is your combined rudder-aileron control on this type model. Fore and aft trim is accommodated by shifting the ballast—in reverse fashion, that is, more weight forward to kill off a dive, more weight aft to stop tailsliding. Once the trim settings are mastered the model can be flown that way if desired, but the cyclic control is more fun since it allows a choice of vertical ascent or horizontal flight at the flip of a lever (or more accurately, the bending of a wire!). Trim the model to rise vertically with a minimum of forward motion, then install the cyclic control. Simply cement a length of paper clip wire to the side of the pylon, as shown, and solder a short length of springy steel wire to the arm holding the feathering blade and blend it so the blade is flipped gently each revolution. Vary the position of the tripper by bending it up or down to regulate the cyclic deflection—not much is needed. Now, with this control, and by varying the rotor tilt you can make it climb straight, fly forward, cruise in circles or any combination desired. Nearhovering can be obtained by cutting the fuel with a straight 3-1 mix of alky and castor oil. . Guide to Helicopter Adjustment Model helicopter flyers may find it easier to reGlidden Doman of Doman Helicopters, Inc., used an R-6 to experiment with his dynamically balanced rotor system (no vibration). Air Trails Model Annual '55 The cabin ol the R-6 was built of molded plastic impregnated Fiberglass, probably the first use of this material in production aircraft. member helicopter model adjustments by making an analogy to fixed wing practice, thus: Conventional Equivalent Helicopter Horizontal Stabilizer Fixed pitch rotor blade or See-saw engine prop or Torsion tail surf ace (s) Ailerons (wash-in—out) Lateral mast tilt Rudder Tail rotor, mast brake, downwash fins under motor. Thrust Line Center of gravity location moving aft increases D.Th. Glide Angle Speed in Vertical FPM in Autorotation Therefore we note that increasing the pitch of the fixed blade (s) reacts similarly to increasing the angle (negative) of a horizontal stabilizer, bringing the nose up under power, or, decreasing the gliding speed (rate of descent, power off). The rudder function, yaw, is obtained by a tail rotor, by a brake on the spinning main rotor, or by means of fins tending to promote or stop rotation of the fuselage in the slipstream. Aileron control, or bank-turn is by tilting the rotor laterally so the engine shaft inclines toward the desired direction, and altering the dynamic pressure on the feathering blades by moving the C.G. aft (or forward) resolves out as down-thrust or up-thrust respectively. Air Trails Model Annual '55 Full-size plans for the Sikorsky R-6 are part of Group Plan # 55A from Hobby Helpers, 770 Hunts Point Ave., New York 59, N. Y. (50¢) 49 30 YOUNG MEN FLY THE ALL-ALUMINUM PLANE! SHEET METAL SUSIE By ROY L. CLOUGH, JR. No hot fuel problems here; Susie's unique vibration isolation assembly means a long-lasting model • Suzie looks like a rather complex bit of sheet metal work, but actually this gleaming aluminum beauty can be yours at a cost of so little time and effort that you won't believe it until you try. The trick is the use of simple basic geometry which will distort naturally into the shape we desire. We squeeze the ends of a cylinder and there is our fuselage; we draw together the sides of a right angle and there is our wing section. The main disadvantage of sheet metal models is the effect that high frequency engine vibration has upon metal-to-metal junctures. This punishing vibration will erode or fatigue the toughest metal in a short time. Add to this the rough shocks of repeated landings and it is easy to understand why the operating life of MARCH, 1956 metal models of the past has been brief. Suzie was designed with the elimination of this weakness as a major point of effort. Note: there are no direct metalto-metal component junctures; no points where metal can chatter against metal, and no points where heavy mass or flight loads fall upon flat, or unsupported sheet metal areas, in concentrated fashion. Engine vibration is isolated and absorbed by a wood bulkhead, which also takes landing shocks; the wings are attached to a wooden spar, as are the tail surfaces, the wood in turn being attached to the fuselage. The result of this type of construction is a model which will still be flying years from the time you build it—provided you don't run it into stonewalls too often. How about the weight? We won't kid you. Suzie is fabricated from .019 aluminum sheet and this stuff isn't microfilm. She squats on the takeoff line with a full tank at 24 oz., and uses up one-third to half a circle to get airborne with a Cub .14—the smallest engine you should use. Once aloft, however, she flies as good as any sport-type model with an elevator response, climb and dive, which belies its weight. When the engine quits Suzie whistles into a high-momentum glide as flat as a tabletop and keeps pulling on the lines until she stops rolling. You'll like her. Construction: Stop in at your local building material outlet and ask for a couple feet of 24" aluminum flashing. This shouldn't cost over 75c. This stuff should mike about .019; don't get the heavy-duty .024 grade. Note that this material has a "grain," that is the long way and you'll get a better and easier job by observing the lay of the metal. Cut out a piece 18" x 10" and roll this into a cylinder, then get your perimeter dimension by setting the bulkhead in place in one end, mark and then remove the bulkhead, line up the cylinder, prick and drill and bolt the edges together with ¼" round head 4-40 bolts and nuts. (Riveting is okay if you have the equipment.) Now observe the inside edge of the lap joint; this must come at the bottom right (outside) fuselage. With this in mind gently squeeze the tube into shape to receive the tailpiece, the wood rudder, and bolt this in place. Run a #3 drill through the sides, taking care to be perpendicular to the rudder piece and then carefully slit the fuselage as shown and bend the resulting tab upward on each side. Drill and bolt the hardwood stabilizer to these tabs—a modicum of bending is permissible if necessary for good alignment. Set the fuselage aside and make up the engine - mount - bulkhead - tank - landing gear assembly. This is a separate and independent unit and note that the engine shaft will be off-center to the left; regardless of what engine you use, the shaft position will be dictated by having just the glow plug tip project beyond the fuselage side. This permits use of the popular "flat-opposed" type of engine cowl. Next take the nose assembly and stick it into the open fuselage end—line your assemblies up simply by twisting one way or the other, and when you are satisfied with the alignment notch out the fuselage end—line your assemblies up simply by twisting one way or the other, and when you are satisfied with the alignment notch out the fuselage metal around the landing gear legs—this will maintain the arrangement. You may wish to drill for the wood screws now and put them in place temporarily. With a straightedge draw pencil lines down each side from the stabilizer center to the centering marks on the bulkhead. Balance the assembly between fingertips and mark at this point. (This will vary somewhat between the ultralight Cub .14 and something heavier, like an O&R .23). Do not make any allowances for missing elevators or prop, but cut for the spar at this point in similar fashion as for the stabilizer-spar, except that the tabs here are on the bottom. Poke the wing spar into place, drill and bolt temporarily. Only at this time do we cut out the cockpit. Use a coping saw and leave the edges rough, smear with Pliobond cement, slit a 12½" length of heavy-wall black neoprene tubing and push it in place as moulding around the cockpit rim. (Continued on page 81) Full-size plans for Sheet Metal Susie are found on Group Plan #356 by Hobby Helpers, 770 Hunts Point Ave., New York 59, N. Y. (35c) Sheet Metal Susie (Continued from page 31) Now for the wings. These are simply cut out and bent to shape with the trailing edges bolted or riveted together— there is a little trick that makes it easier and more foolproof, however. Clamp the metal along the leading edge line between a couple of stout sticks and bend it to 90 degrees, then remove the sticks and finish bending by hand to a nice "natural" symmetrical section. Then hold the trailing edges together with the sticks while you drill and fasten them together—this prevents a wavy edge from developing. Remove the spar bolt from one side, slip the wing over the spar, spot the inboard hole and the one near the end of the spar and drill them. Dig up a couple of "J" bolts and drill into the underside of the wing and the side of the fuselage and install the "J" bolt with a fiber washer between wing root and fuselage as shown on the plan view. Do not omit this! Now do the other wing, spotting the "J" bolthole so as to provide a slight amount of washout effect on the outboard wing. Next put in the balsa end caps, sticking them in place with Plio-bond. The cowling is simply a strip of aluminum wrapped around the nose, slotted for the landing gear legs and the glow plug tip and held together with a couple of bolts or rivets at the bottom. You will find it easy to bump a nice edge on the cowl using an inkbottle form (one of the oval ones) and a plastic mallet. (From my experience I suggest you use an empty inkbottle!) Add an extension to the needle valve and lead this through the cowling. Four nickel-plated wood screws hold the whole front end together. The elevators are next. Use a stitched bias tape hinge and roll an inter-connector of 1/16" wire into the flippers as shown—it is fairly easy, but maybe you would like to practice rolling a bit of scrap with wide flat nose pliers first. (This is a good trick to know—once you learn it you'll never be caught short for a bit of tubing for any purpose!) The elevator horn is simply an integral tab on the left side. Make up the tailskid and bolt this in place. We put the control quadrant under the left wing, pivoting on the inboard bolt for simplicity, but you can pick up a little speed by putting it inside the fuselage, on the spar, if you wish to take the extra trouble. If an external horn is used, make up a wire line-guide and bolt this in place with the spar tip bolt. The deep tail and the skid places the model in proper take-off position, just let it taxi—it’ll take off by itself as the proper speed is reached. Check all bolts for tightness after the first flight and occasionally after that until you are sure she has snugged down to business. Never wipe sand or dirt away with a rag, wash it off with kerosene to prevent scratching the metal. FULL SIZE PLANS YOUNG MEN & AIR TRAILS MODEL ANNUAL Group No. 256 50¢ ENCLOSE COIN OR MONEY ORDER "BUNKER BOAT" by Cal Smith and Frank Lashelt. The long awaited fishing boat model for electric power, can be radio controlled Scaled 5/16" to foot, 35¼" long, 6¾" beam First shown on June 1955 cover of ATHFYM Group No. 356 35¢ ENCLOSE COIN OR MONEY ORDER "SHEET METAL SUSIE" by Roy L Clough, Jr. Aluminum covered control line model that's easy to make and a snap to fly. Extremely durable model. Spans 27 Inches; overall length 21 inches Uses 14 to 23 power plants FOR SPECIAL HANDLING( Add 9¢ per plan—1st class ) of Plans Only ( Add 18* per plan — Air mall NEW 1956 CATALOG 12-5 28 PAGE, FULLY ILLUSTRATED. SEND 10¢ TO COVER HANDLING . HOBBY HELPERS 770 HUNTS POINT AVENUE NEW YORK 59, N. Y By ROY L. CLOUGH, JR. Saturnian SPACE SKIMMER • This ultra-weird and flashy, U-control looks like it just zoomed out of the pages of a science-fiction magazine. A startling eye-catcher, our vane-winged dreamboat has a lot to recommend it besides its unusual looks It is easy to build, easy to fly and never breaks a prop. Odd as it may seem, lift is excellent despite the unusual fore and aft arrangement of the lifting surfaces This permits a very good glide and nice handling charactestics. The huge dorsal and ventral fins which flare forth so rakishly are not just decorative, they're functional. They provide lift to hold the model out when flown near the vertical, an idea we may see adapted t o future stunt jobs The construction, although specialized to fit the unusual geometry, is quite ordinary in method. Start with the cabin or pod. which is built up on the plywood cross beam. This may be covered with 1/32" sheet balsa, or stiff tag stock Take particular care with the engine installation since the thrust and surface incident lines must be parallel. We used a Space Bug Jr. running backwards. A left-hand Wasp would also do the trick, or the ambitious could carve a left-hand prop for any .049. Regardless of the engine used, note that the tank, if integral, must be arranged so the fuel will feed properly. Generally this will mean running the engine on its side with plastic lines attached to the filler and vent and brought above fuel level. Make up the wing vanes, joined at the rear with the stabilizer and elevator and stiffened with the long fins. Note how the joint goes together between the cross beam and the wing vanes, stiffened by the projection of the long fins. Use plenty of cement and give it plenty of time to dry. Check the thrust line against the wing plane and add the struts next. Tie control system hardly requires explanation, except to note that unlike most models, your Skimmer has no lead-out wire. The control lines attach directly to the control quadrant. A wheel landing gear may be added if desired, We built one into the original in order to locate the correct placement for those who wanted a wheel. However, there is a lot to be said in favor of flying the model hand-launched or with a U-Reely, and it looks even more "unearthly" without it. Much of the charm of this model is i t s co l o r scheme, the flasher, the better. Modeling a rotor sailing ship By ROY L. Anton flettner's famous rotor ship Buckau was propelled by spinning drums upon which the wind acted to produce thrust. While it required a small motor to spin these rotors, the main source of power was the wind harnessed through the Magnus effect—if a drum is set to spinning in a wind, a thrust vector is produced at 90 deg. from wind impingement. Unlike the original rotor ship, this little model uses an un-powered modified rotor CLOUGH, JR which also provides rotary shaft power to spin an underwater propeller. It's actually a Magnus windmill that will spin regardless of the wind direction. The thrust produced by the rotor is in direct proportion to the speed at which it turns. However, you will note that this rotor has been loaded with a rather large propeller which holds down its speed, since the propeller thrust must be greater than the rotor thrust. The reason for this is actually quite simple. When the model has the wind on its port beam, the thrust of the clockwise rotor is dead ahead, but when the wind is on the starboard beam, the rotor thrust is toward the rear of the ship. In the first instance, the rotor thrust is added to the propeller thrust, but in the second it is subtracted. Thus, the greater prop thrust makes it possible for the model to tack either way. The graceful little hull will go together as easily as a box if you allow the cement to dry well between assembly steps, Solder the shaft-log bearing into a bit of tin-can stock and cement it into the hull. The deep keel (pine) should be cemented and nailed to the hail. Drill an. undersized lead hole in this and drive in the 1/8" wire mast. Ballast can be a length of old shafting, solder, Babbitt or type metal, soak the balsa. To shape the vanes of the rotor, soak the balsa until it's pliable, and then bind the two sheets around a 2-1/4" mailing tube which you have covered with wax paper. When dry, you can make minor dimensional corrections by springing them slightly during assembly. Next, roil up a tube of stiff paper, soak it well in model airplane dope and mount it between the rotor end disks on locating plugs. Finally, glue the curved vanes in place. It's particularly important that the gearing and shaft in the power tram work freely, flattened egg-beater gears were used in the model illustrated, but many similar gears would have worked just as well. Be careful to align the cross member which supports the upper part of the propeller shaft. This should mesh perfectly with the gears. You can adjust the location of the rotor gear by slipping washers or bits of tubing over the rotor mast so that this gear engages the prop shaft gear favorably. The shaft-log bearing may be very loose and still not leak water, since a couple of drops of lubricating oil will be enough to keep the water from entering. The two sides should be attached at the stem and stern block, and then sprung apart so that the bulkheads may be inserted. Pin the guide strip to the keel so that different sections of the bottom planking may be aligned easily A rotor sailor makes the best speed when the wind is on the port beam. At varying angles in front of the wind the speed will vary with the thrust vector resultant Gears which link the rotor to the propeller may be salvaged from any clockwork mechanism. However, be sure to mount them so they mesh perfectly and work easily Roy Clough PDF files (Rock collection) Air Car Basic Design Problems of Model Helicopters Blow-Bug Build Your Own FLYING SAUCER Channel Winger Cloud-Copter TR CLOUD-COPTER-D CLOUD-COPTER-TR Clough Helicopter From Toys and Games Clough autobiography Expansion Engines Gyro Kite Hoopskirt Hover Bug Hydro jet Powers Little Speedster LITTLE DRAGON b LITTLE DRAGON original Martian Space Ship More on Helicopters New Model Helicopter Original Channel Winger Parasol Plane Peter 0'Dactyl Saturian Sheet Metal Susie Sikorsky R-6 Sikorsky S-51 Slat Wing Snapper Spinning Disc Saucer Spinning-Wing Sure Fire Tan-Giro FULL Tan-Giro Tiled The Model Copter The Whirligig TRIAD Try a Turbine Typhoon Engine Venusian Scout Water Bug What's the score on helicopters? WhirliC02pter Whirly Bird Kite b Yankee Flea Build it... and watch it soar 1,000 feet in the sky: New Model Helicopter: By Roy L. Clough Jr. EVER since the first helicopter got off the ground, model-makers have been trying to design a miniature version that would do the same. Here's one of the first model-helicopter designs to succeed really well. Its secret? Most early models were such complicated contraptions that they sometimes worked-but more often didn't. The new one is ingeniously simple in construction, yet makes "HERE'S a radically new free-flight helicopter,” says noted model-airplane authority Howard G. McEntee, shown at left flighttesting the model for POPULAR SCIENCE. "Its ingenious engine-on-rotor-blade design is the first such I know of. It gives the model a stable, soaring flight, uncomplicated by the many problems that have plagued other copter designers for so long." Why It Flies use of half a dozen complex principles of flight. The result is a fascinating study of aerodynamic problems that have plagued designers of both real and model copters for years. The power plant is a glow-plug engine. at the rim of a spinning gyroscope 1Poke and it immediately tilts. But not where you touch it—instead at point 90 degrees past where you touch it. Scientists call this "precession." In the PS helicopter, the whirling rotor acts like a horizontal gyroscope and the propeller blade a vertical gyroscope. To keep a copter level, rotor blades must Whirling blade-tip weights react 90 degrees 2decrease 3later pitch on forward stroke to balance to the force at the tail by twisting reduced lift of rearward stroke—called "cyclic pitch." This is done by weighting the model tail-heavy so it pulls down on the blades at the rear—like pushing on rim of a gyroscope. blades down on copter's right side. This reduces lift as blades advance into the wind. At same time, air pressure against the downtilted blades exerts a new force on the rotor. tips, again acting as a gyroscope, 4Blade react 90 degrees later to force of air on spring back up on left side to take 5Blades full bite of air. Since lift is less on rearward the right side by tilting down in front. This tips the nose down so the copter, while tailheavy, tilts forward for straight-ahead flight. stroke away from the wind, the full-pitched blades now balance reduced-pitch blades on opposite side, and the copter flies level. CONTINUED 147 How you can build the gas-model helicopter Underside of rotor hub shows how spider forces two nonpowered blades to tilt at the same angle as powered blade. Wire blade stems are bent at right angles to engage holes in spider plate. Solder parts with hub held flat, upside down, to insure uniform alignment of the blades. 148 POPULAR SCIENCE MAY 1962 like that used in most model planes. But instead of being mounted inside the fuselage, the engine is attached directly to one of the copter's three rotor blades. In most conventional copters, both real and model, the engine drives the rotor from a central shaft. In turning the rotor forward, it "braces its feet" against the fuselage and also pushes backward. This backward torque keeps attempting to spin the fuselage in the opposite direction from the rotor. In full-size copters, torque must be offset by a separate stabilizing tail rotor or other special devices to keep the craft flying straight. In the model shown here, the blade-mounted engine pulls the rotor around instead of pushing it. It creates no torque and thus needs nothing to counteract it. The model is a whopper, too—nearly 4' across the rotor tips. Yet, despite its size, it's so efficient that it flies on a tiny .020 Cox engine— one of the smallest made. Designed for free flight, it has hit altitudes of 1,000 feet on two minutes of fuel, giving it a rate of climb of 500 feet a minute. Earlier models have required much bigger engines to achieve the same lifting power. How the model flies. The three rotor blades are pivoted loosely at the hub, leaving them free to tilt up or down like the elevator on an airplane. The blades are also linked together at the hub by a bell-crank mechanism so that whatever one blade does, the other two do likewise. Unlike a conventional helicopter, however, no special controls are needed to tilt the blades up or down for takeoff or landing, or to provide complicated changes, known as cyclic pitch, during flight. They're automatic. The trick is based on the fact that the whirling rotor and the spinning propeller [Continued on page 186] How the model climbs Whirling propeller acts like a gyroscope in the same way as the rotor, but this time in a vertical plane. It reacts at 90 degrees to the sideward twist on it by tilting upward. This tilts up the rotor blade (and the other two blades linked to it), giving the helicopter lift for climbing. How the model lands When the engine quits, the upward gyroscopic twist on the rotor blades also stops, and they pivot freely. Upward air pressure on the trailing edges forces the blades to tilt down, and the helicopter glides slowly to earth. New Model Helicopter: Why It Flies [Continued from page 149] attached to the rotor both act like gyroscopes. As the drawings show, a gyroscope reacts to a force placed on it by tilting at 90 degrees, or sideways, to the original point of force. This is used in several ways to provide stable flight. The upward gyroscopic twist of the propeller tilts the rotor blades up to give the copter lift for taking off and climbing. A similar gyroscopic reaction is given to the rotor by weighting the copter tail-heavy. This causes weights fastened to the leading edges of the blades to twist the blades downward and reduce lift as they advance into the air stream—just like the cyclicpitch mechanism on big copters. An additional gyroscopic reaction in the rotor forces it to tilt downward at the nose to keep the model flying forward. Earlier attempts to make a model copter fly forward by simply weighting it nose-heavy proved disastrous. The rotor, pulled down at the front, reacted like a gyroscope and flipped over, on its side, sending the craft crashing to the ground upside down. Earlier models had another fault: Blade pitch was fixed at an upward angle for climbing. To provide the downward pitch for landing, the rotor had to come to a stop, then reverse its direction. This time lag caused the copter to drop a long distance before the reversed rotor got up enough speed to break its fall. In the new design, the pivoted rotor blades continue to turn in the same direction, but automatically tilt downward when the engine stops to let the model glide gently to earth. Only the rotor is tricky, the copter's fuselage is a simple sheet-balsa job. But the rotor, the heart of the craft, must be carefully balanced to provide correct blade pitch and avoid vibration. The blade-tip weights are blobs of solder, each equal to the weight of three nickels. They are used only on the two non-powered blades as the engine supplies the weight on the third blade. After the weights are mounted, gradually shave off bits of solder until the rotor remains balanced in any position. Weight the fuselage with clay until it balances at a point 1/2" behind the rotor's axis. This will make the ship slightly tailheavy as required for proper flight. Blade pitch is controlled by a spidershaped plate on the underside of the hub. This works like a three-way bell crank. (86 POPULAR SCIENCE MAY 1962 When the plate is twisted by the stem on the power blade, it in turn twists the stems on the other two blades to a like angle. The U-shaped stop bracket should limit the plate's movement to provide a maximum of 12 degrees upward blade pitch for climbing. Downward or negative pitch should be set as shallow as possible for a slow, leisurely descent. Note that the engine is mounted at an angle on the rotor blade, rather than straight-ahead. This puts its thrust line at a tangent to its circle of rotation. If it pointed straight ahead, it would exert a side thrust on the rotor as it whirled around. Note, too, that it is turned partially on its side, with its cylinder tilted inward toward the rotor hub. This puts its fuel reservoir in line with centrifugal force so the gravity feed will continue to operate even though the engine is being slung around sideways by the rotor. The engine must also be tilted slightly downward to minimize the force of its slipstream. The slipstream tends to turn the copter's fuselage to the right, but is offset by the rotor's downwash and bearing friction, which tend to swing the fuselage to the left. The engine can be mounted on the metal bracket shown in the construction drawing or, for a neater appearance, can be faired into the rotor blade with a shaped balsa block, as shown in the photos. If a larger engine than the .020 Cox is used, it will require additional counter weighting of the rotor blades. In this case, add the extra weight to the tips of the blades themselves, not to the tip weights, which must remain the same. Flight-testing the copter. An ROG (riseoff-ground) takeoff is slower but safer at the start since you can see what's happening. When all adjustments are perfect, you can go to the faster handlaunch. Begin with a 6"-diarneter, 3"-pitch plastic prop and trim it a little at a time until the engine reaches maximum r.p.m. Hold the ship by the tail until the rotor gains speed, and duck out of the way. The model should rise slowly, then tuck its nose down and climb in a right-hand spiral of 20' to 30' in diameter. During trials and on windy days, let some of the fuel flow/ through before letting go—or you may wish the copter didn't fly so well. • ....MORE ON HELICOPTERS by R. L. CLOUGH JR. Twin spool drive of tail prop is used on this model THE design of a helicopter poses many problems which often cannot be solved by analogy to fixed-wing practice. In "Basic Design Problems of the Model Helicopter" (M.A.N. Sept. 1945), the writer endeavored to present briefly, and in general terms, several types of flying model helicopter arrangements together with their characteristics. Since that time two new types of helicopters have appeared, both of which offer interesting possibilities to the model experimenter. Also during this interval, the writer found time to conduct further investigation into the subject and has reached a few conclusions, which should be illuminating. Many incidental mechanisms were tried, many discarded and a few retained. Fig. 1 represents the dual rotor intermeshing machines. The Kellett and Flettner helicopters utilize this form of torque nullification. On full scale machines the rotors are meshed by gearing, but in models it is possible to construct the rotors in such fashion that they mesh of themselves. Use of piano wire sections near the hubs is a fairly good substitute for gearing as well as providing a desirable degree of blade articulation. Both rubber motors should be of the same tension, and winding is best accomplished from the underside. Rotors must be of equal degree of pitch and very well balanced for good results. Fig. 2 is a single rotor helicopter with torque effect compensation obtained by means of an airfoil shaped tail vane, which is provided with an adjustable flap. This type is particularly well adapted to models and will probably be the favorite in future duration contests. It has the disadvantage of over-correcting for torque when fully wound and undercorrecting when nearly exhausted, but is MODEL AIRPLANE NEWS May, 1947 Coaxial rotors eliminate torque propeller otherwise very satisfactory once the proper relationship has been worked out. Rotor speed should be high enough to provide a good slipstream over the vane and slow enough to permit a fair duration. Theoretically the rotor should be as small as possible and of very low pitch. It is necessary to incorporate a cyclic pitch mechanism if forward flight is desired. The CG should come slightly forward of the rotor axis in order to balance the drag of the vane. To understand thoroughly the difference between helicopters and conventional aircraft—and this understanding is the difference between success and failure—it must be realized that, unlike the airplane, the helicopter is a machine of variables. By way of illustration let us consider a conventional model plane. The performance of such a machine is fixed and does not vary; thus at a certain speed a certain amount of lift is produced. The fundamental performance is the same whether the machine is under power or gliding; this is because the machine is one distinct mass in motion. Now, in the helicopter we have the rather paradoxical situation of part of an airborne mass being exposed to a relative wind (the rotors); and part of the mass (fuselage) having no relative wind or greatly varying degrees of relative wind depending on the velocity of the mechanism as a whole through the air. Let us repeat the above, substituting "kinetic energy" for relative wind. The kinetic energy of a flying machine is the product of its speed times its mass, minus air friction or drag. Thus a helicopter in hovering flight, in calm air, has a relative wind over the rotors, a much smaller amount over the fuselage, and no kinetic energy of the mass as a whole. When hovering into a strong breeze the above factors are the same, except that the fuselage now possesses a stronger relative wind; it is in effect flying into the wind at the speed of the wind, but with the important difference that no momentum is produced as a result of this forward flight. Therefore, it may be seen that "groundspeed" is an important factor in reckoning performance characteristics of helicopters. If a helicopter is hovering into a stiff breeze and that breeze suddenly ceases, the machine is apt to drop to the ground (such accidents have occurred) But, if the machine is flying forward at a good rate of speed into the wind and the wind ceases, the momentum of the mass will accelerate it as the air resistance drops and "carry over" loss of altitude will be negligible. The effects of this differential of inertias are quite marked in helicopters and in some maneuvers can become very complex. In the practical application to our problem of designing stable model helicopters it serves to remind us that it is not wise to go overboard on the matter of "pendulum stability." Too great a distance between rotors and fuselage is likely to accentuate swinging moments rather than minimize them. Relative wind differentials must be borne in mind as well when designing rotary wing craft. When the fact that the relative wind over the rotors and over the fuselage have different effects, is thoroughly digested, many seemingly baffling problems are made clear at one stroke. Power, the degree of power that is, is another important factor. A rubber band motor's output varies with every revolution of whatever mechanism it drives. This humpbacked power curve of rubber has considerable influence upon the design of models so propelled. Often it is 39 necessary to alter a design to a considerable degree from what it "should" be in order that stable flight be obtained through all phases of the power curve. The over-powered model helicopter is lifted rapidly and stops climbing very suddenly—with the effect that inertia may carry the machine a bit higher after lift ceases, permitting the machine to fall free until it attains sufficient velocity for the fuselage area to act as fin surface and invert the model. The properly powered model rises more slowly, perhaps to a slightly lower altitude, and performs the transition from climb to controlled descent without the weight of the machine being removed from the rotors and transferred to the fuselage at any time. It may be stated that the ideal power loading for any given model helicopter is the highest which can be achieved without sacrificing desired flight characteristics. More simply: use the smallest possible amount of rubber. There are several types of flight performance possible: (1) power climb, power braked descent; (2) power climb, free-fall descent; (3) power climb, reverse free-wheeling descent; (4) power climb, over-riding freewheeling descent: (5) horizontal flight, landing being accomplished while the machine is still under power, (It is almost impossible to secure hovering flight in rubber powered helicopters without using a very tricky automatic pitch rotor head.) Of these types No. 4 is the most desirable, and often No. 1 is the most practical. Fig. 3 shows a method of obtaining overriding free wheeling (and, incidentally, automatic pitch). This method can be adapted to either co-axial or single rotor designs, and produces very realistic nights. If greater simplicity is desired, two 40 methods of obtaining freewheeling by reversing direction of rotation are shown in Fig. 4. Both these methods are adaptable to various types of rotor arrangements. Of the two, the coil spring is the most positive, but in some situations the friction disk setup is more practical. Friction disks should be alternately inner tube rubber and coarse emery cloth or sandpaper. In the previous helicopter article the writer laid great stress on the necessity for well-articulated rotor blades to minimize forces set up by gyroscopic action. At this point something called "cyclic pitch" should be explored in some detail. Cyclic pitch means independent control of the pitch of individual rotor blades at various positions as the rotor turns. By means of cyclic pitch mechanisms the angle of any blade may be increased or decreased as it passes through any segment of the rotor disk. Thus it is possible to increase the lift produced by the rotor on one side and decrease it on the other. This causes the rotor to tilt toward the side on which lift is decreased. Increasing the lift of each blade as it passes through the rear of the disk causes the machine to move forward; increased lift at the front causes it to move backward. Thus the force which is applied to single rotor helicopters to secure forward flight is not a constant thrust as in the case of propeller driven planes but is like a series of "jiggles" which nudge the machine along. This accounts for much of the vibration incident to machines of this type. Now it would seem that forward flight could be attained as easily by shifting the center of gravity in relation to the rotor axis, as is done in many co-axial machines, and avoid the vibration caused by cyclic pitch. To a casual observer this appears to be quite logical, but unfortu- nately the solution is not that simple. Picture a two-blade rotor spinning in a horizontal plane. When hovering, the lift of each blade is equal that is each blade is moving a similar mass of air downward. Let's assign an arbitrary tip speed to the rotor of, say 100 mph. Now, by shifting the CG of the rotor we cause it to move forward at 50 mph. What happens? The blade advancing into the slipstream encounters a relative wind of 150 mph, its own speed, plus the speed of forward motion; the blade receding from the slipstream encounters a relative wind of 50 mph, its own speed, minus forward speed. Such a difference in lift makes the arrangement unflyable; it simply wouldn't remain right side up. Therefore, in order to make a single rotor stable in forward flight it is necessary to incorporate a mechanism that will decrease the pitch of the advancing blade and increase the pitch of the receding blade to an extent which will equalize the all-over lift of the rotor disk. A mechanism for producing cyclic pitch in models is shown in Fig. 5. This is quite simple and produces less friction than some methods that have been suggested. The rotor hub is thin brass tubing through which is slid the blade holder before the blades are affixed. Cyclic control is obtained by means of an eccentric mounted disk, which may be shifted about and pinned to secure horizontal flight in all directions. This disk controls the movements of a small wheel or roller, which in turn transmits its movements to the rotor by means of a simple linkage. It is desirable to have a pin and hole setup in the plate upon which the cam is mounted in order to prevent it from shifting while the model is in flight. A light coil spring between the roller arm and rotor shaft is necessary to prevent (Turn to page 64) MODEL AIRPLANE NEWS . Moy, 1947 ... More on Helicopters (Continued from page 40) "floating." Sometimes, depending on the size of the rotor, static balance weights ahead of each blade will give a smoother performance. The rotor head of the model with tail prop illustrated herewith is an attempt to secure fully automatic cycling. This model is flown forward by adding a small weight to the nose, the angle of the blades on each side of the rotor being controlled by air pressure on them. This method shows promise, although the-writer has had only indifferent success with it to date. The crux of the matter seems to be obtaining the proper static balance. Now the question is sure to be raised: "Is it possible to obtain forward flight in machines of this type without using cyclic pitch?" The answer is "Yes," but in a rather weak voice. If the rotor speed is high enough and the forward speed of the machine slow enough, a fairly decent horizontal flight can be obtained—but the rotor must be highly articulated. If the speed increases above a certain critical point, however, the model will tilt and begin to fly sideways at the same time, which condition will soon resolve itself into the helicopter's equivalent of a nose dive. Several methods of transmitting power to. the torque prop are shown in Fig. 6. "A" is the common sandpaper-faced pulley and string belt arrangement, "B" is the flexible shaft drive which uses aluminum and neoprene tubing and a friction roller at the rotor head; and "C" is the wind-up, wind-down string and spool system in which the string winds both ways at once and rewinds itself automatically as the main rotor is turned. In any case the blades of the torque prop should be adjustable. In dealing with the problems of control of co-axial model helicopters we find there are several methods that give good results. Because there are two rotors turning in opposite directions in co-axial machines, it is possible to make these fly forward by adding weight to the nose or by shifting the angle of the rotor axis. In models there are two good methods of obtaining forward flight by CG shift: the simplest is to add weights to a hook in the nose. This works well on experimental machines and is very convenient. A model using this method should be slightly, tail heavy without weights making it possible to obtain reverse, 64 vertical and forward flight by flying with or without various small weights. A slightly more complicated method is shown in Fig. 7. With this setup the motor tube is moved fore and aft along an arc by means of a movable guide plate and pivoted thrust bearing. A friction holder is required on the movable plate to prevent shifting in flight. When laying out a model of this type, be sure to allow ample clearance for the rotors at both extremes of movement so they won't hit fuselage or tail surfaces. Slipstream controls may be used to turn the nose of the model right or left (or correct turning tendencies), secure forward flight, or may be used in conjunction with CG shift to obtain extremely accurate trim. Several types of slipstream controls are shown in Fig. 8. Control surfaces of this type on a helicopter differ in function from that of a conventional plane, and it is important that this difference be understood. In a conventional plane, control surfaces are used to set up or arrest turning moments around one or several axes. (Flaps and slots are no exception; neither are they true controls.) In the helicopter, only one control surface effects a turning moment, that is the heading surface which points the machine in the desired direction. The other surfaces are not as much control surfaces as they are secondary propelling surfaces and act by reaction to direct slipstream in a direction opposite to that in which forward motion is desired. This is the function of the "elevator" shown in Fig. 8, as should be quite clear from the drawing. It. must be noted that the resistance of these control surfaces at a distance from the rotor axis has a tendency to produce a condition similar to that of CG shift, and this effect must be taken into consideration when designing this type of model. A question, not covered exhaustively in the previous article, is that of "coning angle." Coning angle is the helicopter's dihedral angle. It is_ the angle of "dish," positive or negative, of a spinning rotor. From the writer's experience it seems difficult to lay down any hard and fast rule regarding it. Apparently it is wise to use positive cone on single rotor and dual rotor machines. With co-axial machines negative cone seems to give the best forward flight characteristics. At any rate either one appears to be better than a perfectly flat disk, and the writer suggests that builders try both and decide for themselves. Much can be said in favor of either. Sometimes, after carefully designing and building a helicopter of his own design, the experimenter finds that despite all his efforts the machine will not perform as intended. What is wrong? First, check the model for gyro effect. The procedure is relative in nature and must be learned but is not difficult. Wind up the rotors and hold the machine nose down. Releasing the rotors but not the fuselage, move the machine around in various directions about its longitudinal axis. If there is considerable resistance to such movements, the chances are that the blades are gyroscoping. This calls for more sandpapering to add flexibility or easing up of the articulation system if the rotor is of that type. If the machine rises but shows a tendency to oscillate, the trouble may be caused by an unintentional pitch differential between two or more blades of the same rotor. Check the pitch carefully, using a template to insure uniformity. Plain and simple wobbling is usually caused by unbalanced blades or uneven tracking. Another type of wobble difficult to correct is caused by "puffs" of air striking the top of the fuselage aft of the rotor axis and ahead -of it at different times. This effect is most often noticed in machines employing a three-blade rotor. For this reason the writer recommends that rotors having two or four blades be used. This may sound like a small thing, but in helicopters it is often the small things that count. The helicopter experimenter should never take it for granted that something which is good practice in airplanes will work equally well on rotary wing craft. Usually it will not. However, if there is ever any theoretical doubt as to whether or not a thing will work, try it! Some of the most important inventions have been accidental discoveries. Such discoveries are the rewards of providence to an inquiring mind—and certainly nothing to be ashamed of. Good luck! MODEL AIRPLANE NEWS . May, 1947 Conventional model-plane power plant pushes little craft over water, and standard model-plane tech- niques are used to build the craft from balsa. The nacelle accepts most .020-049 radial-mount engines. MODEL HYDROPLANE Skims Pusher prop spun by model-plane engine gives high performance. Construction is easy and fast By ROY L. CLOUGH JR. H ydrofoils have been around for some time, but even so, nothing on the boating scene draws every eye like a hydroplane lifting out of the water as it gains speed. Even the U.S. Navy has been attracted to foils, and has tested them on its fast PT boats. The PS model shown here can be completed in a couple of work sessions. Surface-piercing foils and air-prop drive give it speed and stability with minimum complexity. Construction is far simpler than you'd guess from the performance. Basically, these craft deliver greater speed because resistance against several small areas (foils) is considerably lower than against a complete, submerged hull. Resistance declines as the craft rises. Completely submerged foils are the most efficient, but they require sensing 140 POPULAR SCIENCE and control systems to keep them at proper depth. Surface-piercing foils automatically adjust for depth—but they also have a tendency to create air bubbles that reduce lift. The PS model uses a foil design that minimizes this undesirable side effect. Instabilities can develop in either type of foil. This is particularly true of models. Simply put, the angle necessary to make the foils "fly" at low speed can also make them hop out of the water at high speed and spill the boat. The model has a designed-in, relatively steep foil incidence and a high thrust line to minimize the possibility of this happening. Building the model. Typical modelplane construction techniques are used. But keep in mind two important construction hints: Cut all parts very accurately. Use ordinary pins to hold the components while the glue dries. Build the cabin first, complete with tail boom and rear foils. Cover the lower half of the cabin with lightweight model tissue before doping, for a smooth and watertight finish. The windows are simply clear plastic (I cut mine from bubbletype packaging). Next, make up the front foils, floats, the Water and crossbeam as a unit, and cut them into the cabin floor at the correct angle. Shape and fasten the motor-mount nacelle; the one shown on the blueprint w i l l accept most .020-.049 radial-mount engines. To be safe, check your engine before shaping the part. large lake or a broad river will serve as a suitable playground for Mount the engine to the A the model. Run it on a tether around your boat, or turn it loose for plywood firewall during as- a "free flight" if there's enough water area to do so safely. sembly; epoxy cement is best here and a good-size dab on the nuts holding the mounting control heading and raise or lower the nose, much like the elevators on an airscrews is recommended. The pusher engine. If you use a reed- plane. For your shakedown cruise, bend the valve type you can use a standard p r o p but be sure to put it on backward. If t r i m tabs up at the rear edge until the your engine has a rotary valve, use a model rises up on its foils and scoots. left-hand pusher prop of the type used To get maximum speed, bend the tabs upward to the minimum that w i l l make for air-drive model race cars. Important: The model should balance the craft "fly." Direction is controlled by when fingertip-held between the points differential bending of the tabs. I flew the model on a large lake, chasshown on the blueprint. Though a little tail heaviness is allowable, a nose-heavy ing it w i t h a boat. But you might also fly it on a tether around a boat. model puts you out of business. Double-check all foil angles before making a test run. The rear, inverted-V Turn the page for PS lie-flat blueprint foil is fitted with bendable tabs, which MAY 1969 141 LITTLE DRAGON Part One by ROY L CLOUGH, JR. Little Dragon glow engine is a project any amateur THE machinist can tackle with full confidence of good results. It does not require any special tools, special talents, or extreme precision. A large part of the total time spent in developing the design was devoted to eliminating awkward machining jobs, delicate operations, and tricky assemblies. If the reader owns a small lathe and can center a piece of stock with 1/64", he need have no qualms about being able to turn out the job. On the other hand, the skilled builder who has a good "touch" for this sort of thing will discover he has an engine, which requires absolutely no apologies on the score of being homemade. The motor is a basic design, as old-engine hands will recognize by the drawings. It has great amounts of leeway at every step of construction. This means there is plenty of room for the correction of errors, which should appeal to the amateur, and equally of importance, it allows the experienced motor builder to "soup-up" the design as he sees fit. For example, the weight of the original came out at 2 oz., complete with plug and prop. Skillful shaving-down by experienced machinists can reduce this figure greatly, but this has nothing to do with the operating characteristics. Port areas and valve timing are laid out with an eye to obtaining maximum start ability and a good rate of speed with average construction and internal fits, but the experienced worker who is capable of doing very good work will find it possible to increase the porting and degree of valve opening to obtain an extremely hot engine. The original Little Dragon was turning the plastic prop shown in the photo at 8,000 rpm, 5 minutes after it was assembled. It did this on a break-in mix of 3 parts O & R No. 2 and 1 part castor oil. This is the performance the average builder can reasonably expect. For experts, and with one of the hot Francisco Lab fuels, 10,000 rpm is a reasonably conservative estimate. The mounting of any engine uses up time and energy and in too many cases is finicky and bothersome. We have tried to get around this and come up with something that is simple, quick, and practical. The two-stud mount is our answer. Simply press the studs against a piece of plywood to mark it for drilling, set the engine in place and run on a couple of nuts. No muss, no fuss, and no bother. A bore of approximately 7/16" with a 3/8" stroke fixes the displacement at about .06. By selecting these dimensions, it was possible to take advantage of material sizes which sim- An ordinary book of matches dwarfs our tiny engine MODEL AIRPLANE NEWS • October, 1950 Little Dragon all ready to roar! This engine is really "on the square" plified construction considerably and is one of the reasons you will find dimensions indicated in 32nds of an inch instead of thousandths. (Editors note: Cad drawing in thousandths.) However, those who wish to build the engine to conform to AMA 1/2A regulation can use a 1/2" O.D. cylinder liner instead of the 9/16" specified on the plans. This will bring the displacement down to about .049, safely within the rules for engines of .05 or less. This will require slight alterations in the width of the con rod for adequate clearance, and of course the liner hole, piston size and head are changed accordingly. Conversely, a skillful builder can increase the displacement to more than .070 if he desires. To those who think an elaborate machine outlay is required in order to build engines, a glance through the list of tools used to make the original should prove refreshing. These were: small lathe, hack saw, hand drill, two files, two taps, one die, and a pocket scale graduated in 64ths. A micrometer was used to check sizes, but actually could have been dispensed with. And the big news, of course, is that no milling operations are required. The Little Dragon employs what is known as the "sleeve-inblock" style of construction. Instead of having separate cylinder and crankcase, one blends into the other, eliminating cylinder tie downs, heat dams, and two more places for errors to accumulate. The engine block serves the same purpose as the "keel" frequently used in model airplane construction, being a basic member, which when laid out correctly serves as an accurate basis for the remainder of the construction. The block is the easiest part to make, in terms of tolerances, and serves the amateur builder the purpose of getting his hand in as he goes along. Once the block is made the rest of the engine falls right into line. Cut off about 1-7/8" of 3/4" sq. hard aluminum alloy bar stock, center it accurately in the four-jaw and face off the end. This gives a plane surface to set against the chuck face. Remove the piece, re-center, and face it down to the proper size. Next, outline the cylinder block. Here is a good rule to remember: always keep as much stock between the end of the piece and the chuck as possible; in other words, make the first cuts out near the end to leave a maximum diameter of supporting metal. By this rule, we see that the fins are machined first. If your lathe is a light one, use the back gears and feed the finning tool in slowly, particularly at the start of each cut where it is chopping at the square corners of the stock. The first fin is extra heavy because this must carry the screws, which will hold the head in place. If you have cut the piece a bit short by accident, you may take the error out of the first fin. For example, if the piece is 1/32" shorter than it should be, the first fin would be 3/32" deep instead of 1/8". This is all right, but don't make it any thinner. There are three fins below this, each 1/32" deep with a 1/16" gap between all fins. Since the lowest fin must come in exactly the right position because of the exhaust port, cut this one after you have made the top fin. If your finning tool isn't quite the correct width, split the difference to fix the location of the middle two fins. Do not cut the fins too deeply and weaken the block. A fin depth of 1/32" measured from the flat of the stock is entirely adequate. Turn down the "barrel" and buff it with a crocus cloth. A good shine here increases (Turn to page 48) 23 Little Dragon (Continued from page 23) the eye appeal; rough tool marks give the engine the appearance of having been whittled out of a stove bolt with a cold chisel! The block is drilled out to an I.D. of a shy 9/16" and brought up to size with a boring tool, or reamer. Getting the correct depth is important, not because it will prevent the engine from running, but because you will have to go over the whole thing changing other dimensions to make it come out right. Note how a shoulder is left to support the liner. This liner must fit closely in order to prevent blowby around the exhaust port and at the head. This does not mean a piston-type fit by any means, but it should be tight enough so that it is just about possible to pull the piece out with the fingers. A dummy sleeve cut from the steel tube stock is a great help here. If by some mischance the hole is oversize, don't scrap the job, just tin the sleeve and resize it to fit the hole. (But you won't be able to harden the sleeve if you do this, and then you will have to use an aluminum or cast iron piston.) Remove the piece and re-chuck it in order to bore out the front of the case. Open this up part way with a drill and bring to final size with a boring tool. The inside rear must be faced off smoothly because the rotor valve will ride against it. The rotor pin hole is drilled out by holding a 3/32" drill in the tailstock. At this point lay the piece aside and make up the crankcase front section. Do a good job here and no gasket will be needed; in any case a short piece of thread wrapped around the plug portion of this part will serve very well as a gasket. If the inside end is turned first and fitted to the block, the job is easier, as this leaves something to chuck with. Next, reverse the piece and bore out to 3/16" I.D. and bring the outside down to size. No bearing is used other than the metal itself. If you want to be ritzy about it, the hole can be bored oversize and bronze, or Oilite bearing material pressed in. In practice, the writer has found aluminum to serve very well, but the coefficient of friction of Oilite material is undoubtedly more favorable if the end in view is extreme performance. For that matter, ball bearings small enough to be used in this engine can be obtained, and we are indebted to Malcolm D. Whitman, Jr., of Carmel, Calif., for that information. If you use ball bearings, the crankshaft diameter must be reduced or the outboard end of the bearing increased to accommodate the ball race, should double ball suspension be desired. The crankshaft belongs to a breed of cats that seems able to scare a lot of people. Don't worry about it. Put the three-jaw chuck on your lathe and insert the piece of 9/16" drill rod. Bring this down to size with light cuts and power feed. Finish the journal with a fine file, crocus cloth and common sense. If you happen to have a tool post grinder, by all means use it. Custom fit the shaft to the crankcase front section, double checking to be certain the thrust washer clearance is adequate, then mark the spot and turn down to the size you have selected for the threaded portion. We call for an 8-32 thread, but this is a matter of choice and whatever die you have handy. The threads may be cut on the lathe, but some will find it less trouble to back off the tail stock and use an ordinary die. Be sure to start it straight; back the die off every half turn to break the chips and insure a good thread. A few drops of light oil makes the cut easier. Near the end of the cut it is a good idea to reverse the die in order to cut the threads up close to the journal. The thrust washer is simply a threaded disc. The writer has used threaded drive washers on a number of engines with good results and why no commercial engine uses them is something of a mystery since it is certainly easier than milling splines or grinding flats. Now, remove the piece and put on the four-jaw. Chuck up the shaft by the journal and off-center the piece 3/16" by adjusting the jaws. It is possible to hold the piece adequately without marring the journal, but the cautious may wish to push the shaft into a length of brass tubing and squeeze the jaws down on this. If this is done, be sure to use only a gentle tapping to put it in place, because the journal must be knocked out again afterward. The whole secret of turning off-centers is setting the lathe tool on center, feeding in slowly, and using power feed to drag the tool along the work. In addition, be willing to take a little time to do the job. The pin should be brought to a good surface finish. The crank disc may be ground or filed away as indicated by the dotted lines on the plan for a sort of counterbalance effect, but this is not critical. The rotor comes next. Most people seem to have the opinion that disc valves must be tricky since they come in the more expensive engines, so we'll give a little background on this. When the original Little Dragon was being laid out, a great deal of consideration was given to the induction method. It had to be very simple and very effective. Three-port induction seemed simple, but it meant tapping into the block and cutting another hole in the liner. Besides this it did not allow much leeway for error and would not produce the best power output. Shaft rotary looked good at first glance, but this would mean less than optimum strength for the crankshaft, chances for errors in both the port hole and the hollow shaft, and the added difficulty of setting the intake tube into the front case. So that was out. Next we toyed with the idea of flutter valve induction; these arrangements are simple, and since they work on crankcase pressure, very effective. However, a speck of dirt, or oil hardening in the valve makes them inoperable with a vengeance. Further difficulty was foreseen due to the great powers of fuel meniscus in these small sizes. Fuel meniscus? That did it! So we used a disc rotor and made it free-floating. Five minutes after assembly we knew we had it. Only two smooth faces are needed, and one of them is already inside the crankcase. Best of all the intake hole can be spotted easily, and if missed, it can be tried again with a new rotor. In addition to all these advantages, the thickness of the rotor is not critical and this gives the amateur machinist another place to pick up and correct accumulated error. Chuck up the 5/8" aluminum rod and turn down the rotor shaft to fit the hole in the rear of the engine block. This should not be a tight fit, but smooth running and a bit loose if anything. Bring the O.D. of the rotor down to size and face it with a gentle cut, making certain there is no shoulder next to the shaft as this will prevent seating. Cutting loose from the stock should be halted about halfway through and all sharp edges broken, then complete the severance. Locate and drill the drive hole. This should be a bit oversize, but do not drill all the way through the disc, just enough for good clearance. Mark the outline of the port and file away the indicated area. The rotor may be held between two thin bits of wood or fibre in a vise for this operation. Break any edges that develop. Now, take up the block and put the rotor shaft into the hole from the outside rear of the case and scratch the outline of the round portion as shown on the plan. Split the difference between this line and the edge of the shaft hole and drill a 1/8" hole along the diagonal. The intake tube is a 'length of 5/32" thin wall brass tube. Taper one end slightly (this taper is emphasized on the drawings) and press the tube firmly into the case. The needle valve assembly may be from a Baby Spitfire or other small engine. The crankcase front section must now be drilled; set it in the engine block and spot the holes for drilling. These holes are drilled and tapped 2-56. The original engine used 348 screws throughout, but the larger size is not needed. However, it may be comforting to know that if you ruin the No. 2 hole you can always re-tap it for 3-48. Tapping is easier if the holes are first filled with kerosene and the tap backed off at frequent intervals. Tap in the mounting studs next. At this point, clean up all the parts and make a trial assembly to be sure everything fits smoothly and turns freely. If the rotor valve shows a tendency to creep forward on the pin, don't worry about it—it won't when the engine is running. The important thing is that it seats well and does not bind at any point. MODEL AIRPLANE NEWS • October, 1950 (Next month we'll bring you the concluding part of the Little Dragon construction article, giving instructions for con rod, cylinder head, and the amazingly simple sleeve and piston arrangement which eliminates the need of conventional milled or cast-in by-pass. Details of fuel, starting and running will also be covered.) BILL OF MATERIALS (for entire engine) 8" of 3/4" sq. hard aluminum alloy rod 2" of 5/8" round hard aluminum alloy rod 3" of 1/2" round 17ST rod 3" of 9/16" seamless steel tubing 3" of 9/16" drill rod 1" of 1/8" O.D. heavy wall brass tube 1" of 5/32" O.D. thin wall brass tube Scrap of 1/8" thick dural sheet (hard) for con rod 2—3-48 studs 5/8" long 8—2-56 or 3-48 screws, fillister head, 3/8" long 2—No. 4 hole washers 2—3-48 nuts l"-sq. thin gasket material 1 Baby Spitfire needle valve assembly 1 McCoy Hot Point Plug 49 little dragon part two by ROY L. CLOUGH JR. Here are details for finishing testing, and troubleshooting; let us know your results with this simple but efficient power plant THE Little Dragon shapes up rapidly once the block and lower assemblies are completed. The cylinder liner is made from a length of 9/16" seamless steel tubing which has a wall thickness of about 1/16". Use great care in cutting it to size. Hold it by means of a leather strap in a vise and use a fine hack saw blade (put in the frame backwards). Take light strokes. The final sizing is done in the lathe three-jaw chuck. Once again please note, here is an opportunity to adjust for previous error. The internal finish of cold drawn tubing is quite good to begin with. It can be brought to a fair running finish by means of lapping. If the builder has access to a hone, so much the better; if not, make up a brass lap and polish out the inside of the tube. This can be done easily by holding the sleeve in the three-jaw chuck, running the lathe slowly and working the lap back and forth evenly. Always run the lap into the sleeve from the same end; it is a good idea to daub a bit of red dope on this end to keep track of it. This will be the lower end of the sleeve. When the lapping has been finished, clean all traces of lapping compound from the liner. At this stage of the construction it may be helpful to read over either of the two previously published engine articles, the Simplex 25 (M. A. N. March and April, 1947,) and "Build Your Own Diesel" (M. A. N. May and June, 1948,) on the subject of piston and cylinder fits. This ground has been covered very thoroughly. The state of the fit, the material and degree of hardness of the piston, have great bearing upon the life of your motor, and to a lesser degree, its original performance. The best piston as far as wearing qualities are concerned is hardened and centerless-ground steel. The next best is cast iron ground on centers. Both of these methods offer difficulties to the homebuilder, but there is no question of their excellence. If either of these two methods is elected, there is little, if anything, the writer can add, as the Little Dragon piston design is about as straightforward as they come, and requires no special instructions. If, on the other hand, the reader is anxious to get his motor running and wants a method of fitting a piston that will produce quick results, although it will not last as long, he can make up a hard aluminum piston in very short order by means of the "cold broach" method. If the internal liner surface is in good condition to begin with, aluminum pistons sometimes last for a surprisingly long time, and several commercially produced engines have used aluminum pistons with good results. Here is the method: chuck up a piece of 1/2" 17ST, about 3" long in the three-jaw. Do not support the tail end. Using power feed and very light cuts, bring the O.D. down so that the piece will barely fit in the lower end of the liner. Because of the length of the piece and its unsupported condition the finest cuts that can be managed will still produce a slight taper. The surface must be very bright and free of tool marks. Bore out the piston, cut it loose, and drill the wrist-pin holes. We now have the following condition: the skirt of the piston will go into the lower end of the liner about 1/8". This is backward from the way it will run. Set the liner on a block of wood, dip the piston in castor oil, set it into the liner, and making certain it is square, take a drift and drive it right through. After a couple of trips through the cylinder liner backwards, the piston can be re30 versed and driven through the right way. Always drive it in from the lower end of the liner and turn the piston slightly from its last position. Use plenty of castor oil and keep the piston wiped clean. After a time it will be found possible to rotate the piston without a great deal of resistance and a fairly good fit will have been established. The conn rod is worked up from 1/8" hard dural stock. Check with the plans against what you have built, before drilling the rod holes. The piston skirt must not hit on the front case plug at bottom stroke. If you require a longer rod due to small errors, make it longer—you can take the difference out of the head. The wrist pin is simply a short length of 1/8" heavy-wall brass tube. Assemble the engine, using light oil on all bearing surfaces, and turn it over by hand. The piston will (or should) have quite a bit of resistance, but no real "sticks" should develop anywhere. If they do, correct them. Check the position of the piston relative to the liner at top and bottom center. If these positions are within 1/64" of the positions shown on the plan, congratulate yourself on a job well done. If not, you will have to make allowances for the liner ports. The exhaust port and intake by-pass are cut into the liner with a small, medium-fine file. Support the liner endwise between two thin pieces of wood in the jaws of a vise. This operation is very simple as can be seen by the plan, but care and accuracy can return big dividends here. Carefully remove any burrs that develop. The piston deflector is now filed on. Check this against both the plan and the liner. The exhaust port must open first, and leads the intake port by 1/32" of piston travel. File through the barrel of the engine block below the last fin, put the liner in place and check the alignment. The block slot should be slightly larger than the liner slot, but no smaller. Take a scribe and mark the portion of the liner supporting rim below the by-pass slot, remove the liner and cut away this portion of the rim with a fine metal chisel or hand grinder. This licks the by-pass problem. The cylinder head is of the "plug" variety and also has a slight gasket-retaining groove. The combination makes it leakproof even with very indifferent machining. Ideally, the plug should be a smooth push fit into the liner. The plug portion is extra long to facilitate final assembly. Tap a 1/4" x 32 hole into the head for the glow plug. The head is mounted the same way as the front case section, that is, drill the head holes first and use these as guides for drilling the holes in the engine block. These are tapped 2-56 all the way through the first fin. Clean up everything, wipe castor oil on all contacting surfaces and assemble the engine except for the head. Put a prop on the shaft and turn it over a few times. There will probably be quite a bit of piston resistance, but this is all right. The thing to watch out for is jamming, though this is not likely to occur due to the general design of the engine. If it should happen, take the engine apart and look for surfaces that appear unnaturally bright, or scored-looking. Fix them up. The internal clearance between rotor, rod and crankshaft need be no more than 1/32". If the clearance is as much as 1/16 the meniscus effect will be lost on the rotor plate. This will not prevent running, but it will make starting a bit harder. MODEL AIRPLANE NEWS • November, 1950 a half dozen bursts, the parts will "find" and the motor will run out the fuel. Don't hook it up to a tank and lean it out until it has run off a few minutes of four-cycling. The fuel you will use depends to a great extent upon the piston fit. It is loose, more oil will be required, but if very good it can be run on straight O & R No. 2. Don't jump to conclusions about the compression ratio if it doesn't run correctly. Try altering the fuel mixture (oil ratio) because it may be a case of poor piston fit. If you're certain the piston fit is good, then increase the ratio by deepening the gasket groove. This engine has quite a wide range of glow C.R. because of good thermal characteristics and will operate well between 7- and 10-1, with 8 being about optimum. Once the engine is running properly don't take it apart unless absolutely necessary, as this disturbs the run-in. This is particularly true if the aluminum piston is used. The Little Dragon is the result of about three months of design consideration by the writer, in an effort to obtain a layout in the ½A size, which could be, quite literally, all things to all men. A basically simple construction which could return good results to the beginner, yet give the old motor hand a design which would permit him full exercise of his skill and require no apologies for the fact of being homemade. If you like it, let's hear about it. If you run into difficulties, don't hesitate to write the author. Good luck. Set the head in place (without glow plug) and turn the piston up to top center, and see how much the head lifts off. Then rechuck the head and face off the plug portion enough to allow 1/32" clearance between it and the piston, at top dead center. Don't break the sharp edge of the cut—it's too handy to cut holes in gaskets with. Use it now to cut a gasket, and trim around the edges enough to allow the head screws to go through. Dip the gasket in castor oil and assemble the head to the engine. Pull the screws down "cross corner" fashion, a little at a time. They should be snug and fairly tight, but don't strip the threads out of the block. Mount the engine on a piece of wood, which can be screwed down to something solid, and put on a four- or five-inch length of fuel line. Turn the engine over by hand for a few minutes and get used to its grunts and groans. Don't put the glow plug in yet. Get to know the various wheezes and pops and what they mean. Note the soft "tunk!" made by the intake port opening into the cylinder, the gurgle of the intake rotor. These sounds are usually masked by the louder pop of released compression when the motor is flipped over. Turn the motor over slowly several times and the intake port noise may disappear. This means the rotor has ridden off its seat. A quick flip backward reseats it. Repeat this trick with the glow plug in place (McCoy Hot Point plug is recommended). When the rotor unseats there will seem to be a loss of compression. Again flip the prop backwards and the "compression" reappears. Unless you are familiar with this stunt, you may think the head gasket has blown, or there is dirt under the rotor, and tear the motor down to find the "trouble." Mix up a break-in mix of three parts O & R No. 2 and one part castor oil. Fill the fuel line and squirt a couple of drops into the exhaust port. Hook up the wires and give it a flip. After MODEL AIRPLANE NEWS • November, 1950 GLOW PLUG DIAGNOSTICS SYMPTOM: Starts readily, revs up well, rpm drops off when plug wire is removed. Indication: Compression ratio is too low. Cure: Add oil and/or nitrate to fuel, deepen gasket groove to decrease head space. SYMPTOM: Starts very hard with much flashback, but runs well once started. Indication: Exhaust port not opening soon enough before intake transfer. Cure: Check liner slots against plan, file more "lead" into exhaust. SYMPTOM: Must be flooded to start and will run only on rich mixture. Indication: Cylinder head, or glow plug gasket is leaking. Cure: Replace gaskets, check surfaces for damage. SYMPTOM: Kicks violently, runs in short high speed bursts, kicks off prop, stops suddenly. Indication: Compression ratio is too high. Cure: Reduce compression ratio by shaving down inserted "plug" portion of cylinder head, or try high compression fuels with a cold glow plug. SYMPTOM: Starts easily, holds up speed when wire is removed, leans out well, then gradually dies out. Indication: Motor is not yet broken-in, probably overheating. Cure: Use heavy, low pitch prop and run motor as rich as it will take for ten to fifteen minutes, then try it again. General: Watch for the usual bugs, clogged fuel line or needle, tanks not vented correctly, loose prop, bad plug, loose wires, insecure mounting, evaporation weakened fuel. Use a port prime to start engine. 31 LITTLE DRAGON Part One by ROY L CLOUGH, JR. Little Dragon glow engine is a project any amateur THE machinist can tackle with full confidence of good results. It does not require any special tools, special talents, or extreme precision. A large part of the total time spent in developing the design was devoted to eliminating awkward machining jobs, delicate operations, and tricky assemblies. If the reader owns a small lathe and can center a piece of stock with 1/64", he need have no qualms about being able to turn out the job. On the other hand, the skilled builder who has a good "touch" for this sort of thing will discover he has an engine, which requires absolutely no apologies on the score of being homemade. The motor is a basic design, as old-engine hands will recognize by the drawings. It has great amounts of leeway at every step of construction. This means there is plenty of room for the correction of errors, which should appeal to the amateur, and equally of importance, it allows the experienced motor builder to "soup-up" the design as he sees fit. For example, the weight of the original came out at 2 oz., complete with plug and prop. Skillful shaving-down by experienced machinists can reduce this figure greatly, but this has nothing to do with the operating characteristics. Port areas and valve timing are laid out with an eye to obtaining maximum start ability and a good rate of speed with average construction and internal fits, but the experienced worker who is capable of doing very good work will find it possible to increase the porting and degree of valve opening to obtain an extremely hot engine. The original Little Dragon was turning the plastic prop shown in the photo at 8,000 rpm, 5 minutes after it was assembled. It did this on a break-in mix of 3 parts O & R No. 2 and 1 part castor oil. This is the performance the average builder can reasonably expect. For experts, and with one of the hot Francisco Lab fuels, 10,000 rpm is a reasonably conservative estimate. The mounting of any engine uses up time and energy and in too many cases is finicky and bothersome. We have tried to get around this and come up with something that is simple, quick, and practical. The two-stud mount is our answer. Simply press the studs against a piece of plywood to mark it for drilling, set the engine in place and run on a couple of nuts. No muss, no fuss, and no bother. A bore of approximately 7/16" with a 3/8" stroke fixes the displacement at about .06. By selecting these dimensions, it was possible to take advantage of material sizes which sim- An ordinary book of matches dwarfs our tiny engine MODEL AIRPLANE NEWS • October, 1950 Little Dragon all ready to roar! This engine is really "on the square" plified construction considerably and is one of the reasons you will find dimensions indicated in 32nds of an inch instead of thousandths. (Editors note: Cad drawing in thousandths.) However, those who wish to build the engine to conform to AMA 1/2A regulation can use a 1/2" O.D. cylinder liner instead of the 9/16" specified on the plans. This will bring the displacement down to about .049, safely within the rules for engines of .05 or less. This will require slight alterations in the width of the con rod for adequate clearance, and of course the liner hole, piston size and head are changed accordingly. Conversely, a skillful builder can increase the displacement to more than .070 if he desires. To those who think an elaborate machine outlay is required in order to build engines, a glance through the list of tools used to make the original should prove refreshing. These were: small lathe, hack saw, hand drill, two files, two taps, one die, and a pocket scale graduated in 64ths. A micrometer was used to check sizes, but actually could have been dispensed with. And the big news, of course, is that no milling operations are required. The Little Dragon employs what is known as the "sleeve-inblock" style of construction. Instead of having separate cylinder and crankcase, one blends into the other, eliminating cylinder tie downs, heat dams, and two more places for errors to accumulate. The engine block serves the same purpose as the "keel" frequently used in model airplane construction, being a basic member, which when laid out correctly serves as an accurate basis for the remainder of the construction. The block is the easiest part to make, in terms of tolerances, and serves the amateur builder the purpose of getting his hand in as he goes along. Once the block is made the rest of the engine falls right into line. Cut off about 1-7/8" of 3/4" sq. hard aluminum alloy bar stock, center it accurately in the four-jaw and face off the end. This gives a plane surface to set against the chuck face. Remove the piece, re-center, and face it down to the proper size. Next, outline the cylinder block. Here is a good rule to remember: always keep as much stock between the end of the piece and the chuck as possible; in other words, make the first cuts out near the end to leave a maximum diameter of supporting metal. By this rule, we see that the fins are machined first. If your lathe is a light one, use the back gears and feed the finning tool in slowly, particularly at the start of each cut where it is chopping at the square corners of the stock. The first fin is extra heavy because this must carry the screws, which will hold the head in place. If you have cut the piece a bit short by accident, you may take the error out of the first fin. For example, if the piece is 1/32" shorter than it should be, the first fin would be 3/32" deep instead of 1/8". This is all right, but don't make it any thinner. There are three fins below this, each 1/32" deep with a 1/16" gap between all fins. Since the lowest fin must come in exactly the right position because of the exhaust port, cut this one after you have made the top fin. If your finning tool isn't quite the correct width, split the difference to fix the location of the middle two fins. Do not cut the fins too deeply and weaken the block. A fin depth of 1/32" measured from the flat of the stock is entirely adequate. Turn down the "barrel" and buff it with a crocus cloth. A good shine here increases (Turn to page 48) 23 Little Dragon (Continued from page 23) the eye appeal; rough tool marks give the engine the appearance of having been whittled out of a stove bolt with a cold chisel! The block is drilled out to an I.D. of a shy 9/16" and brought up to size with a boring tool, or reamer. Getting the correct depth is important, not because it will prevent the engine from running, but because you will have to go over the whole thing changing other dimensions to make it come out right. Note how a shoulder is left to support the liner. This liner must fit closely in order to prevent blowby around the exhaust port and at the head. This does not mean a piston-type fit by any means, but it should be tight enough so that it is just about possible to pull the piece out with the fingers. A dummy sleeve cut from the steel tube stock is a great help here. If by some mischance the hole is oversize, don't scrap the job, just tin the sleeve and resize it to fit the hole. (But you won't be able to harden the sleeve if you do this, and then you will have to use an aluminum or cast iron piston.) Remove the piece and re-chuck it in order to bore out the front of the case. Open this up part way with a drill and bring to final size with a boring tool. The inside rear must be faced off smoothly because the rotor valve will ride against it. The rotor pin hole is drilled out by holding a 3/32" drill in the tailstock. At this point lay the piece aside and make up the crankcase front section. Do a good job here and no gasket will be needed; in any case a short piece of thread wrapped around the plug portion of this part will serve very well as a gasket. If the inside end is turned first and fitted to the block, the job is easier, as this leaves something to chuck with. Next, reverse the piece and bore out to 3/16" I.D. and bring the outside down to size. No bearing is used other than the metal itself. If you want to be ritzy about it, the hole can be bored oversize and bronze, or Oilite bearing material pressed in. In practice, the writer has found aluminum to serve very well, but the coefficient of friction of Oilite material is undoubtedly more favorable if the end in view is extreme performance. For that matter, ball bearings small enough to be used in this engine can be obtained, and we are indebted to Malcolm D. Whitman, Jr., of Carmel, Calif., for that information. If you use ball bearings, the crankshaft diameter must be reduced or the outboard end of the bearing increased to accommodate the ball race, should double ball suspension be desired. The crankshaft belongs to a breed of cats that seems able to scare a lot of people. Don't worry about it. Put the three-jaw chuck on your lathe and insert the piece of 9/16" drill rod. Bring this down to size with light cuts and power feed. Finish the journal with a fine file, crocus cloth and common sense. If you happen to have a tool post grinder, by all means use it. Custom fit the shaft to the crankcase front section, double checking to be certain the thrust washer clearance is adequate, then mark the spot and turn down to the size you have selected for the threaded portion. We call for an 8-32 thread, but this is a matter of choice and whatever die you have handy. The threads may be cut on the lathe, but some will find it less trouble to back off the tail stock and use an ordinary die. Be sure to start it straight; back the die off every half turn to break the chips and insure a good thread. A few drops of light oil makes the cut easier. Near the end of the cut it is a good idea to reverse the die in order to cut the threads up close to the journal. The thrust washer is simply a threaded disc. The writer has used threaded drive washers on a number of engines with good results and why no commercial engine uses them is something of a mystery since it is certainly easier than milling splines or grinding flats. Now, remove the piece and put on the four-jaw. Chuck up the shaft by the journal and off-center the piece 3/16" by adjusting the jaws. It is possible to hold the piece adequately without marring the journal, but the cautious may wish to push the shaft into a length of brass tubing and squeeze the jaws down on this. If this is done, be sure to use only a gentle tapping to put it in place, because the journal must be knocked out again afterward. The whole secret of turning off-centers is setting the lathe tool on center, feeding in slowly, and using power feed to drag the tool along the work. In addition, be willing to take a little time to do the job. The pin should be brought to a good surface finish. The crank disc may be ground or filed away as indicated by the dotted lines on the plan for a sort of counterbalance effect, but this is not critical. The rotor comes next. Most people seem to have the opinion that disc valves must be tricky since they come in the more expensive engines, so we'll give a little background on this. When the original Little Dragon was being laid out, a great deal of consideration was given to the induction method. It had to be very simple and very effective. Three-port induction seemed simple, but it meant tapping into the block and cutting another hole in the liner. Besides this it did not allow much leeway for error and would not produce the best power output. Shaft rotary looked good at first glance, but this would mean less than optimum strength for the crankshaft, chances for errors in both the port hole and the hollow shaft, and the added difficulty of setting the intake tube into the front case. So that was out. Next we toyed with the idea of flutter valve induction; these arrangements are simple, and since they work on crankcase pressure, very effective. However, a speck of dirt, or oil hardening in the valve makes them inoperable with a vengeance. Further difficulty was foreseen due to the great powers of fuel meniscus in these small sizes. Fuel meniscus? That did it! So we used a disc rotor and made it free-floating. Five minutes after assembly we knew we had it. Only two smooth faces are needed, and one of them is already inside the crankcase. Best of all the intake hole can be spotted easily, and if missed, it can be tried again with a new rotor. In addition to all these advantages, the thickness of the rotor is not critical and this gives the amateur machinist another place to pick up and correct accumulated error. Chuck up the 5/8" aluminum rod and turn down the rotor shaft to fit the hole in the rear of the engine block. This should not be a tight fit, but smooth running and a bit loose if anything. Bring the O.D. of the rotor down to size and face it with a gentle cut, making certain there is no shoulder next to the shaft as this will prevent seating. Cutting loose from the stock should be halted about halfway through and all sharp edges broken, then complete the severance. Locate and drill the drive hole. This should be a bit oversize, but do not drill all the way through the disc, just enough for good clearance. Mark the outline of the port and file away the indicated area. The rotor may be held between two thin bits of wood or fibre in a vise for this operation. Break any edges that develop. Now, take up the block and put the rotor shaft into the hole from the outside rear of the case and scratch the outline of the round portion as shown on the plan. Split the difference between this line and the edge of the shaft hole and drill a 1/8" hole along the diagonal. The intake tube is a 'length of 5/32" thin wall brass tube. Taper one end slightly (this taper is emphasized on the drawings) and press the tube firmly into the case. The needle valve assembly may be from a Baby Spitfire or other small engine. The crankcase front section must now be drilled; set it in the engine block and spot the holes for drilling. These holes are drilled and tapped 2-56. The original engine used 348 screws throughout, but the larger size is not needed. However, it may be comforting to know that if you ruin the No. 2 hole you can always re-tap it for 3-48. Tapping is easier if the holes are first filled with kerosene and the tap backed off at frequent intervals. Tap in the mounting studs next. At this point, clean up all the parts and make a trial assembly to be sure everything fits smoothly and turns freely. If the rotor valve shows a tendency to creep forward on the pin, don't worry about it—it won't when the engine is running. The important thing is that it seats well and does not bind at any point. MODEL AIRPLANE NEWS • October, 1950 (Next month we'll bring you the concluding part of the Little Dragon construction article, giving instructions for con rod, cylinder head, and the amazingly simple sleeve and piston arrangement which eliminates the need of conventional milled or cast-in by-pass. Details of fuel, starting and running will also be covered.) BILL OF MATERIALS (for entire engine) 8" of 3/4" sq. hard aluminum alloy rod 2" of 5/8" round hard aluminum alloy rod 3" of 1/2" round 17ST rod 3" of 9/16" seamless steel tubing 3" of 9/16" drill rod 1" of 1/8" O.D. heavy wall brass tube 1" of 5/32" O.D. thin wall brass tube Scrap of 1/8" thick dural sheet (hard) for con rod 2—3-48 studs 5/8" long 8—2-56 or 3-48 screws, fillister head, 3/8" long 2—No. 4 hole washers 2—3-48 nuts l"-sq. thin gasket material 1 Baby Spitfire needle valve assembly 1 McCoy Hot Point Plug 49 little dragon part two by ROY L. CLOUGH JR. Here are details for finishing testing, and troubleshooting; let us know your results with this simple but efficient power plant THE Little Dragon shapes up rapidly once the block and lower assemblies are completed. The cylinder liner is made from a length of 9/16" seamless steel tubing which has a wall thickness of about 1/16". Use great care in cutting it to size. Hold it by means of a leather strap in a vise and use a fine hack saw blade (put in the frame backwards). Take light strokes. The final sizing is done in the lathe three-jaw chuck. Once again please note, here is an opportunity to adjust for previous error. The internal finish of cold drawn tubing is quite good to begin with. It can be brought to a fair running finish by means of lapping. If the builder has access to a hone, so much the better; if not, make up a brass lap and polish out the inside of the tube. This can be done easily by holding the sleeve in the three-jaw chuck, running the lathe slowly and working the lap back and forth evenly. Always run the lap into the sleeve from the same end; it is a good idea to daub a bit of red dope on this end to keep track of it. This will be the lower end of the sleeve. When the lapping has been finished, clean all traces of lapping compound from the liner. At this stage of the construction it may be helpful to read over either of the two previously published engine articles, the Simplex 25 (M. A. N. March and April, 1947,) and "Build Your Own Diesel" (M. A. N. May and June, 1948,) on the subject of piston and cylinder fits. This ground has been covered very thoroughly. The state of the fit, the material and degree of hardness of the piston, have great bearing upon the life of your motor, and to a lesser degree, its original performance. The best piston as far as wearing qualities are concerned is hardened and centerless-ground steel. The next best is cast iron ground on centers. Both of these methods offer difficulties to the homebuilder, but there is no question of their excellence. If either of these two methods is elected, there is little, if anything, the writer can add, as the Little Dragon piston design is about as straightforward as they come, and requires no special instructions. If, on the other hand, the reader is anxious to get his motor running and wants a method of fitting a piston that will produce quick results, although it will not last as long, he can make up a hard aluminum piston in very short order by means of the "cold broach" method. If the internal liner surface is in good condition to begin with, aluminum pistons sometimes last for a surprisingly long time, and several commercially produced engines have used aluminum pistons with good results. Here is the method: chuck up a piece of 1/2" 17ST, about 3" long in the three-jaw. Do not support the tail end. Using power feed and very light cuts, bring the O.D. down so that the piece will barely fit in the lower end of the liner. Because of the length of the piece and its unsupported condition the finest cuts that can be managed will still produce a slight taper. The surface must be very bright and free of tool marks. Bore out the piston, cut it loose, and drill the wrist-pin holes. We now have the following condition: the skirt of the piston will go into the lower end of the liner about 1/8". This is backward from the way it will run. Set the liner on a block of wood, dip the piston in castor oil, set it into the liner, and making certain it is square, take a drift and drive it right through. After a couple of trips through the cylinder liner backwards, the piston can be re30 versed and driven through the right way. Always drive it in from the lower end of the liner and turn the piston slightly from its last position. Use plenty of castor oil and keep the piston wiped clean. After a time it will be found possible to rotate the piston without a great deal of resistance and a fairly good fit will have been established. The conn rod is worked up from 1/8" hard dural stock. Check with the plans against what you have built, before drilling the rod holes. The piston skirt must not hit on the front case plug at bottom stroke. If you require a longer rod due to small errors, make it longer—you can take the difference out of the head. The wrist pin is simply a short length of 1/8" heavy-wall brass tube. Assemble the engine, using light oil on all bearing surfaces, and turn it over by hand. The piston will (or should) have quite a bit of resistance, but no real "sticks" should develop anywhere. If they do, correct them. Check the position of the piston relative to the liner at top and bottom center. If these positions are within 1/64" of the positions shown on the plan, congratulate yourself on a job well done. If not, you will have to make allowances for the liner ports. The exhaust port and intake by-pass are cut into the liner with a small, medium-fine file. Support the liner endwise between two thin pieces of wood in the jaws of a vise. This operation is very simple as can be seen by the plan, but care and accuracy can return big dividends here. Carefully remove any burrs that develop. The piston deflector is now filed on. Check this against both the plan and the liner. The exhaust port must open first, and leads the intake port by 1/32" of piston travel. File through the barrel of the engine block below the last fin, put the liner in place and check the alignment. The block slot should be slightly larger than the liner slot, but no smaller. Take a scribe and mark the portion of the liner supporting rim below the by-pass slot, remove the liner and cut away this portion of the rim with a fine metal chisel or hand grinder. This licks the by-pass problem. The cylinder head is of the "plug" variety and also has a slight gasket-retaining groove. The combination makes it leakproof even with very indifferent machining. Ideally, the plug should be a smooth push fit into the liner. The plug portion is extra long to facilitate final assembly. Tap a 1/4" x 32 hole into the head for the glow plug. The head is mounted the same way as the front case section, that is, drill the head holes first and use these as guides for drilling the holes in the engine block. These are tapped 2-56 all the way through the first fin. Clean up everything, wipe castor oil on all contacting surfaces and assemble the engine except for the head. Put a prop on the shaft and turn it over a few times. There will probably be quite a bit of piston resistance, but this is all right. The thing to watch out for is jamming, though this is not likely to occur due to the general design of the engine. If it should happen, take the engine apart and look for surfaces that appear unnaturally bright, or scored-looking. Fix them up. The internal clearance between rotor, rod and crankshaft need be no more than 1/32". If the clearance is as much as 1/16 the meniscus effect will be lost on the rotor plate. This will not prevent running, but it will make starting a bit harder. MODEL AIRPLANE NEWS • November, 1950 a half dozen bursts, the parts will "find" and the motor will run out the fuel. Don't hook it up to a tank and lean it out until it has run off a few minutes of four-cycling. The fuel you will use depends to a great extent upon the piston fit. It is loose, more oil will be required, but if very good it can be run on straight O & R No. 2. Don't jump to conclusions about the compression ratio if it doesn't run correctly. Try altering the fuel mixture (oil ratio) because it may be a case of poor piston fit. If you're certain the piston fit is good, then increase the ratio by deepening the gasket groove. This engine has quite a wide range of glow C.R. because of good thermal characteristics and will operate well between 7- and 10-1, with 8 being about optimum. Once the engine is running properly don't take it apart unless absolutely necessary, as this disturbs the run-in. This is particularly true if the aluminum piston is used. The Little Dragon is the result of about three months of design consideration by the writer, in an effort to obtain a layout in the ½A size, which could be, quite literally, all things to all men. A basically simple construction which could return good results to the beginner, yet give the old motor hand a design which would permit him full exercise of his skill and require no apologies for the fact of being homemade. If you like it, let's hear about it. If you run into difficulties, don't hesitate to write the author. Good luck. Set the head in place (without glow plug) and turn the piston up to top center, and see how much the head lifts off. Then rechuck the head and face off the plug portion enough to allow 1/32" clearance between it and the piston, at top dead center. Don't break the sharp edge of the cut—it's too handy to cut holes in gaskets with. Use it now to cut a gasket, and trim around the edges enough to allow the head screws to go through. Dip the gasket in castor oil and assemble the head to the engine. Pull the screws down "cross corner" fashion, a little at a time. They should be snug and fairly tight, but don't strip the threads out of the block. Mount the engine on a piece of wood, which can be screwed down to something solid, and put on a four- or five-inch length of fuel line. Turn the engine over by hand for a few minutes and get used to its grunts and groans. Don't put the glow plug in yet. Get to know the various wheezes and pops and what they mean. Note the soft "tunk!" made by the intake port opening into the cylinder, the gurgle of the intake rotor. These sounds are usually masked by the louder pop of released compression when the motor is flipped over. Turn the motor over slowly several times and the intake port noise may disappear. This means the rotor has ridden off its seat. A quick flip backward reseats it. Repeat this trick with the glow plug in place (McCoy Hot Point plug is recommended). When the rotor unseats there will seem to be a loss of compression. Again flip the prop backwards and the "compression" reappears. Unless you are familiar with this stunt, you may think the head gasket has blown, or there is dirt under the rotor, and tear the motor down to find the "trouble." Mix up a break-in mix of three parts O & R No. 2 and one part castor oil. Fill the fuel line and squirt a couple of drops into the exhaust port. Hook up the wires and give it a flip. After MODEL AIRPLANE NEWS • November, 1950 GLOW PLUG DIAGNOSTICS SYMPTOM: Starts readily, revs up well, rpm drops off when plug wire is removed. Indication: Compression ratio is too low. Cure: Add oil and/or nitrate to fuel, deepen gasket groove to decrease head space. SYMPTOM: Starts very hard with much flashback, but runs well once started. Indication: Exhaust port not opening soon enough before intake transfer. Cure: Check liner slots against plan, file more "lead" into exhaust. SYMPTOM: Must be flooded to start and will run only on rich mixture. Indication: Cylinder head, or glow plug gasket is leaking. Cure: Replace gaskets, check surfaces for damage. SYMPTOM: Kicks violently, runs in short high speed bursts, kicks off prop, stops suddenly. Indication: Compression ratio is too high. Cure: Reduce compression ratio by shaving down inserted "plug" portion of cylinder head, or try high compression fuels with a cold glow plug. SYMPTOM: Starts easily, holds up speed when wire is removed, leans out well, then gradually dies out. Indication: Motor is not yet broken-in, probably overheating. Cure: Use heavy, low pitch prop and run motor as rich as it will take for ten to fifteen minutes, then try it again. General: Watch for the usual bugs, clogged fuel line or needle, tanks not vented correctly, loose prop, bad plug, loose wires, insecure mounting, evaporation weakened fuel. Use a port prime to start engine. 31 Hydrojet Powers Little Newest thing in nautical propulsion, this clever midget boat has no weed-snagging paddles or prop—won't nip unwary fingers. By Roy Clough a little boat that skims over the HERE'S water like a speedy sea sled, riding high on two rocket-like chine planes. Yet when you pick it up you'll find no fingernipping propeller underneath. The only clue to its hidden power is the intake port on the bottom, and an exhaust port directly behind 170 POPULAR SCIENCE it at the stern. Housed in a casing between them is a rotary pump, which draws in water and kicks it backward at high speed. Reaction to this stream drives the boat. The hull. Use 1/8" sheet balsa for the sides, bulkhead, transom (stern), pilot'shead support and chine planes. Thinner balsa serves for the bottom, deck and gunwales. Before decking in the bow be sure to Speedster cement a couple of ounces of ballast to the front of the bulkhead. A ping-pong ball forms the pilot's head, and the windshield is a scrap of acetate sheeting edged with tin. To finish off the hull, sand down the assembly and cover it with model tissue, then paint with hot-fuel-proof dope. Pump and housing. Before building an engine mount, the driving unit should be OFF TO A FLYING START, the hydrojet speedster is already climbing. Top and side ele vations on opposite page are half size for a boat powered by an .047 displacement engine. The upper detail drawing at left indicates the planing angle; the exploded section below it, the pump-housing pattern and impeller-and-shaft assembly. AUGUST 1954 171 OPENING AT BOTTOM OF PUMP HOUSING takes in water, which is kicked back through rectangular port at the stern. The planing angle of the hull eliminates need for a water scoop. assembled and placed in the hull. The pump housing is made from a single piece of tin-can stock (see detail drawing). Dotted lines are right-angle bends, and the tab extension between the pear-shaped bottom and top sections is curved around the rotor end to form a continuation of the sides. Butting edges are soldered, starting at the nozzle to insure good alignment. Make sure that the bearing hole is centered with the larger water-intake hole. A short piece of tubing should be soldered over the bearing hole to keep the impeller shaft aligned. This impeller shaft has a slot sawed in one end to receive the blade, which is a strip of thin brass stock curved in the form of a shallow S. 172 POPULAR SCIENCE Before mounting the blade in the housing, solder a short arm, or "dog," to the top of the impeller shaft. Then tin both the slotted end of the shaft and the blade, scraping off just enough solder to let the notch slip firmly over the center of the blade. To mount, turn the housing upside down and press the shaft through the bearing from below. Drop a small washer through the water-intake hole and over the notched shaft end. Slip the blade through the nozzle with tweezers and press it onto the shaft. Rotate the shaft to make sure the blade doesn't scrape against the housing, then solder it in position. Engine. The power plant is a miniature gas engine, suspended in a U frame of /s" sheet balsa directly above the impeller shaft. For the slightly angled coupling between the engine and shaft, a pin on a flywheel engages the shaft dog. The flywheel is a large iron washer backed up by a small Vgroove pulley turned from hardwood. Mount the fuel tank on one side of the cockpit floor and connect it to the engine with plastic hose. Operation. The hydrojet boat is started by winding a number of turns of string around the grooved pulley and then hauling the twine sharply back through the engine frame. If you don't want to chase the craft with a rowboat, tether it to a line from five to six feet long. One end of the line is attached to an upright post, the other to the side of the bull nearest the fuel tank. Otherwise centrifugal force would starve the engine. END by ROY L. CLOUGH. JR. This stable model gives true helicopter performance DESIGNED to fly vertically, forward or back, this rubber powered helicopter is easy to build and certain to give good results. Instead of individual rotor blade articulation, which is usually necessary to secure steady flight, the entire rotor mechanism of this machine is permitted relatively free motion about its point of attachment. This motion must be limited in order to obtain forward flight; therefore there is only 1/8" clearance between the rotor tube and the fore and aft cross-members. Side motion is permitted up to the width of the fuselage, about 1/2 in each direction. A long fuselage is used on this model to spread its mass over a large area, thus minimizing disturbing effects, which may occur in the rotor. A high tail fin performs the function of maintaining proper heading and brings the CLA into a favorable position relative to CG. Despite appearances, the vertical control surface employed on this model does not create an untoward amount of drag in forward flight. This is because the actual relative wind is largely downward in the immediate vicinity of the ship. As shown in the photographs this surface is cambered, but further experiments made after the pictures were taken indicate that it is more effective if built flat; therefore it is recommended that it be made this way. A simple push-rod linkage is used to hold it in any desired position. A word of caution: It is frequently desirable to enlarge plans of conventional model planes above the size recommended by the designer and this is often done with good results. But this procedure or any other alteration of the plans must be discouraged by the writer as regards to Hoverbug because, to do so, may result in an unflyable machine. This is because weight distribution, articulation problems, and power requirements may be greatly modified by a size increase. Begin construction with the fuselage, which is built on the plans (presented full size). The structure is strictly conventional except that it becomes tri-angular aft of the rotor tube location. The fin may be integral or built separately. Use 1/16" hard balsa strip for all members. The rotor tube mounting plate is a bit of sheet balsa to which a reinforcing washer has been centered and cemented. Cover windows with cellophane, and balance of the fuselage with tissue. Water shrink but do not dope. The control surface is next. For the lower spar, which is also the wheel axle, use a length of 1/8" sq. basswood or very hard balsa, as this piece must sustain landing shocks. Tissue cover and pin flat when shrinking. A small hardwood block is fastened to the center of this piece with a liberal quantity of cement. (See detail sketches.) This block is pierced with a pin and linked to a similar block cemented to a length of 1/16" hardwood dowel. Attach the control surface to the rotor base plate with cloth hinges as shown. A small block of soft balsa is drilled to fit the 1/16" dowel tightly; it is then slid over the dowel and cemented to the fuselage. The control is adjusted by sliding the dowel fore or aft and the control surface should depart 45° from the vertical in either direction. Use pin axles to attach two hardwood wheels to the ends of the control vane. Cementing together two more wheels of the same size and attaching them to the nose block by means of a wire yoke make the front wheel. The rotor tube is formed from a 6" length of 1/16" medium soft balsa sheet, soaked in hot water, wrapped around a dowel, and held in place with gauze. Permit it to dry thoroughly before removing and cementing up the seam. The upper end of the tube is plugged with a disk of 1/8" hard balsa drilled to accommodate a standard hardwood thrust button. Cut out and reinforce two notches in the lower end of the tube to hold the lower rubber anchor, which is a short length of hardwood dowel. Center a pin or piece of wire in another disk of 1/8" hard balsa, cement firmly in place and attach the disk to the bottom of the tube. Next cut four rotor blades from 1/16" medium sheet and sand them over a bottle to produce a slight camber. The lower rotor blades are cemented directly to the motor tube at a pitch of 30° and with a slight negative coning (or dihedral) angle. Don't spare the cement on this assembly. The unit just assembled is tested for balance separately. Build up the top rotor by cementing the two blades over the 1/4" sq. hard balsa hub piece at an angle of 35°. A wire hook, washer and thrust plug complete the assembly. Six strands of 1/8" flat rubber comprise the motor. Drop the completed motor tube into place in the fuselage, poking the pin-axle of the tube through the reinforcing washer in the mounting plate and bending it over to hold in place. Since there is no freewheeling device, this model is flown under power at all times, using residual power to brake its descent. It is best flown indoors and first hops should be of short duration. Balance should come just ahead of the rotor tube axis, but to secure maximum distance in forward flight it may be necessary to make the machine slightly nose-heavy. For forward flight slant the control surface rearward, just the reverse to fly backward. Experiment with varying degrees of power for best results. For outdoor flying greater duration can be obtained by using considerably more rubber and incorporating one of the reversing free-wheelers described in the writer's previous helicopter article in the May issue. MODEL AIRPLANE NEWS September. 1947 airplane models For a real eyestopper, build "Hoopskirt" By ROY L. CLOUGH, JR. Flying barrels have been in the air since Bleriot, but this model proves they can still turn in a top performance TROT THIS MODEL out on the field at your next meet and watch the eyes bug. If anybody snickers, put 'em in their place by reminding them that the annular wing is a very old aeronautical principle. Then launch your Hoopskirt. If its tradition hasn't impressed them, its performance is certain to! At least a half-dozen full-scale planes (plus innumerable kites and gliders) have been built on the "flying barrel" design. One of the initial aircraft made by Ellehammer— the first Dane to fly—took this form. Louis Bleriot, the daring Frenchman who was the first to fly the English Channel, perched one on floats and tried, with indifferent success, to get it off the water. The French are still at it; their latest attempt at annular-winged aircraft is a tail sitting jet. One of the big advantages of this design is its propulsive efficiency. Efficiency in a flying system is highest when the velocity of the discharged air is almost as great as the forward speed of the plane. This means that it's better to 46 move a lot of air relatively slowly than a small amount at high speed. (It's rather like matching impedances.) The annular wing with a propeller ahead of it functions as an effective aspirator to increase the amount of air thrust backward. Such a wing has more lift than you might think. The closed-circuit nature of the airfoil eliminates wing-tip vortices. Theoretically, a hoop-wing plane shouldn't have to bank in order to turn. This model does, however, because of the vertical stabilizing fin at the top of the wing. This was added to produce an effect comparable to dihedral. The Hoopskirt is an extremely stable flying machine. It'll teach you a lot about this offbeat configuration. Don't let the circular wing scare you—it's quite easy to build. Any cylinder with a diameter of about 10 in. (a half inch either way won't hurt) can serve as a mold for the two spars. I used a straight-sided layer-cake pan. The spars can be of any lightwood that bends easily when soaked in hot water. Bind these around the mold with a strip of rag. When dry, trim the ends in long, matching bevels to form the lap shown in the sketch; cement and bind with sewing thread. You can trace the wing-rib pattern directly onto your balsa, stacking blanks to cut as many at once as you can manage. The slots in each end are 3/32 in. wide and 1/4 in. deep. The width should provide a snug fit over the spars. When these hoops are seated in the notches, their outer edges will protrude 1/16 in. for rounding off. An easy way to space the ribs accurately is to set the spar-mold cylinder on a piece of cardboard and scribe around it to produce a circle the same diameter as the spars. Mark off sixteen rib positions by means of radius lines and assemble the wing vertically over this pattern. Cover the frame one section at a time with light model-plane tissue. Sections into which the strut, fin or booms will pass can be left uncovered until assembly is completed—or you can cover the entire wing and then slit the paper of these sections when you install parts that must be cemented to the ribs. Water-shrink the paper; when dry, give it a coat of clear dope. Careful alignment of all balsa parts pays off in good performance. Don't diminish the strength of the rockhard-balsa booms by sanding off the corners—leave them square. The tail plane has a deeply notched trailing edge, backed up with parallel pieces of soft wire cemented to the wood. These wires—which can be snipped from a paper clip— will hold any flight-adjustment bends you may give the two elevator sections after trial runs. An annular wing operates at zero incidence, so you'll have to bend the elevators up two or three degrees to get an angle of attack for climb. Bending one elevator up more than the other makes the model turn in that direction. The rudders 47 have no adjustments, and are simply cemented to the sides of the booms after the tail plane is in place. The engine-pilot nacelle is given a coat of pigmented dope after the motor is fastened on its plywood mount. The color scheme of the model shown is: red nacelle, rudders and fin: natural white wing; silver booms, strut and tail plane—a highly visible combination against a blue sky. For best performance, be sure the model balances at a point about 1-1/4-in. ahead of the trailing edge of the wing. An easy way to balance the plane is to stick straight pins into both booms 1-1/4-in. ahead of the trailing edges. Support the plane on these pins between two stacks of books, and add weight—in the form of bits of clay, small pieces of lead, etc.—to either the nose or the tail until the plane is suspended between the books in a level flight position. Hand launch the model over tall grass until, by bending the elevators up a little at a time, you get a flat glide. As a check on these adjustments try a flight with the motor running rich, then lean it out and watch your model zoom. This is a free-flying model, and has not been adapted for control-line operation. It is a stable flyer, and when out of fuel, it will glide gracefully to a landing if you balanced it carefully. If you're flying it in a limited space, it's a good idea to burn off some of the fuel before turning it loose, because the model travels at a good clip. In any event, you'll draw a good many curious glances— and perhaps a few snorts of derision —when you take Hoopskirt out for its first flight. Any snickers in your direction, though, will quickly change to whistles of admiration when onlookers see the stability of the "flying barrel," one of the earliest of all aircraft designs. POPULAR MECHANICS APRIL, 1963 Fig. 1 V-4 motor with gas generator was made in Japan Fig. 2 Compressed air plant offered clean, quiet power but took lots of pumping Expansion Engines By ROY L. CLOUGH JR. The author feels these power units have been neglected--get busy, experimenters! Fig. 3 Business end of successful steam-powered controlliner THE re-introduction and acceptance of expansion engines as model airplane power plants must bring a definite "I told you so" grin to the faces of oldtimers. For here is a category of prime mover sadly neglected up to now by builders and manufacturers alike, yet which is in many ways more suited to free and controlled flight than the presently popular gas and diesel engines. At this writing there are 2 expansion engines on the market, both CO2 powered. Their quiet operation, nonexistent starting troubles, reliability and cleanliness are appealing to many. Expansion engines are those in which the gases which drive the piston are brought in from an outside source instead of being generated in the cylinder. Engines of this type were the first dynamic power plants used in model planes. They fall into 2 main categories: reservoir and generator engines. Reservoir engines operate from a tank or cartridge of compressed gas; generator engines from a generator or boiler, which produces the energizing gas. The small CO2 engines available today are reservoir engines. The performance of this type is similar to a rubber, or spring motor, the greatest thrust being exerted as soon as the propeller comes up to speed, with output continuously dropping off as the energy (temperature and pressure) of the gas decreases. There are at present no generator engines on the market. An olden example of this type is shown in Fig. 1—the Imp Tornado, offered by International Models during the 30's. It was produced in 2 models, of 2 and 4 cylinders. One of the most powerful pre-gasoline power plants, the Imp gave many a good flight to those who could find a convenient source of the dry ice propellant. The engine in the picture is the 4-cylinder model. The cylinders are arranged in "Vee," 2 cylinders to a bank, with a slide valve for each bank, which operates from a throw at the rear of the crankshaft. The engine is very lightly built of soft brass and light sheet steel stampings, soft soldered and bolted together. The pistons are a good fit and the crankshaft is a very neat job of precision bending. Provision is made to oil the slide valves through screw caps on each bank and the crankcase holds 1/2 oz. of 3 in 1 or mineral oil for lubrication. The gas generator at the right is an ingenious mechanism. It requires small lumps of dry ice and carbide plus water to operate. It is designed to be removed from the plane for loading and cleaning and the feed line detaches from the tank for this purpose. Here there is some leakage in evidence. The inside of the tank is compartmented to hold the 3 requisite fuels. Water is used to heat up the dry ice to Fig. 4 The author's version of a "hot" compressed air engine. MODEL AIRPLANE NEWS. June. 1948 13 cause it to evolve into gas, and the heat developed by the carbide added to the water prevents the water from, freezing in the process. A dumping lever is used to bring the components together, after which the gas is produced very rapidly. Frankly, we never start this thing up without a bit of fear and trembling because we have heard of similar mechanisms exploding violently when overloaded. However, it does have ample power to fly a 6-foot model and is reliable and consistent in operation when one can obtain the all-essential dry ice. The compressed air unit shown in Fig. 2 is typical of the engines of this type offered during the late 20's and early 30's. The tank is (apparently) phosphor bronze about .005" thick, and wrapped with .010" steel wire for extra strength. The ends are closed with .012" spun brass caps and a standard tire valve is used for inflation. The motor, of the rotary valve type, is mounted to the tank with soft solder. This part of the unit is rather poorly constructed; a three-cylinder affairs, the crankcase is of spun brass, cylinders of brass tubing, slotted aluminum pistons with leather compression rings and the connecting rods are merely hard copper. The crankshaft is a 2-piece assembly with a machine screw crankpin. The fit between crankshaft and main bearing, which forms the rotary valve intake and exhaust arrangement, is very poor and leaks badly. Soft solder is used as an assembly medium throughout. The tank, we discovered accidentally, will hold 100 Ibs. pressure safely—how much more is problematical. At this pressure the motor will swing a 12D 10P Pawlownia prop for 45 sec. The first burst of power when the valve is opened is rather surprising, but within 15 sec. the thrust begins to fall off rapidly. After 30 sec. the thrust is negligible. The efficiency of this engine is very low due to excessive leakage of the rotary valve; with the prop held still and the admission valve open a full tank of air will leak out in just under a minute! In order to evaluate properly the worth of compressed air in an efficient engine we built a single cylinder, poppet-valve motor of .20 cu. in. displacement and with the above tank obtained runs of over a minute and a half with power output equal to the 3 cylinder engine originally supplied with the tank. With this arrangement mounted in a 48" span free flight job we obtained flights of 1000 feet and up, with 20 to 30 strokes of a tire pump. A relatively constant pressure supply to the engine was established by use of an Austin flight timer connected to gradually open the feed valve as the tank pressure lessened. We found best results came when the engine was made to carry as much propeller as possible, smaller props at high speed resulting only in a needless waste of pressure. One of the most interesting expansion engine experiments made by the writer is shown in Fig. 3, a steam engine control line plane. The engine, boiler and burner are built as an integral unit, which bolts to the front of the plane. About 4 min. is required to get up steam after which the burner is doused, refueled and relit for flight. This engine has never been checked with a Strobotac but the best estimate of its rpm would not be over 2000 on the ground. Thus the trick is to get it airborne, which requires a smooth takeoff surface and a bit of leading. Once in the air, however, the engine picks up and puts out enough power to fly the ship at about 40 mph on 20 ft. lines, without whipping. This is because of the small size of the burner and boiler, which requires a considerable blast of air into the intake scoop to build up a good pressure. With naptha fuel the engine has quite a bit more pep, but since this soots up badly in the burner employed we have had to stick to denatured alcohol, which burns cleanly. The engine is an inverted oscillating cylinder type with a 1/2" bore and 3/4" stroke. It swings an 11 dia. 9" pitch balsa, or an 8-8 Pawlownia prop with about equal thrust output. A fairly heavy counterweight is used which makes operation nearly vibration-free. Weight (fueled and watered) is a shade over 8 oz. The boiler, incidentally, is stuffed with copper wool to prevent sloshing and improve thermal efficiency. A molded asbestos cap, removed for the picture, keeps the slipstream from hitting the cylinder in flight; otherwise condensation of the steam would lower efficiency. Fig. 4 illustrates an interesting but rather impractical experiment—a "hot" expansion motor, sort of a "McCoy" among compressed air engines. This develops more power than any of the other engines shown. It has 1/2" bore, 7/16" stroke and is constructed of hard brass tubing, except for the crankshaft, which is steel. The piston is hand-lapped to fit and connects to the connecting rod with a ball and socket joint. Full counter- (Turn to page 38) Fig. 5 Below are shown six different valve mechanisms, applicable to various types of expansion engines 14 MODEL AIRPLANE NEWS • June 1948 Expansion Engines (Continued from page 14) weighting is used and a splash oiler with breather vent provides lubrication. At bottom, of the stroke, air is exhausted not only through the very large port but also through a pressure release slot in the rotary valve. This motor turns up 10,000 rpm with a 2 oz. flywheel at 90 Ibs. pressure, but consumption of air is terrific. We loaned it to a friend who tried it at 200 Ibs. pressure on a factory airline, and he gave a speed estimate of 20,000 rpm, which seems a bit overenthusiastic. After about 2 hours running time (much of it spent in getting it synchronized with an electric motor—so we could put a revolution counter on the motor and see what speed we were getting), the motor shows considerable wear of piston and cylinder and the rotary valve no longer fits as snugly as it should. However, at lower speeds and particularly with steam we have found brass to be quite a satisfactory material. All expansion engines have 2 main requirements: a good smooth valve action, and a source of pressure. There are many types of valve gear, which give good results, and a few, with appropriate comments included here, are shown in Fig. 5. (A) The first is the oscillating cylinder valve, which is adaptable to steam, compressed air or other pressure. This is about the simplest and most positive valve gear since it requires no cams, cranks or levers and wear tends to improve the seal. Since much of the operating stress of the engine comes upon the cylinder stud it is essential that this part be well anchored. This engine may be reversed by simply switching the intake line from one tube to the other. (B) is the rotary valve. This, too, is a very simple form of valve and operates with minimum drag. However, a rotary valve is subject to leakage with wear, is limited to relatively low pressures and is not particularly suited to steam. If carefully made it is a fair compressed air valve, but its efficiency is not as high as the more positively sealing types. (C) the piston valve is very positive in action but has the disadvantage of requiring a separate linkage to operate, and it does put some extra load on the engine since the valve closes against line pressure. It is however practically leak-proof if well made, and this feature alone makes it worthwhile. (D) the slide valve is perhaps the most widely employed expansion engine gear. It wears well, seats without leakage and offers a comparatively minor drag on the engine. It is equally good for steam, air, or CO2, but should have some provision for lubrication if the latter 2 "dry" gases are used. Leakage is apt to occur around the gland where the activating rod enters the pressure chest. (E) poppet valves offer fast action with minimum leakage and good wearing characteristics. Excellent for steam or compressed air, they may tend to stick if high-pressure CO2 is used, due to the great refrigerating quality of this gas. (F) the ball valve requires no external drive, seats well and gives little trouble. However, this type of admission works well at high speeds and pressures only. Because of the great amount of "lead" (gas enters the cylinder before the piston reaches top dead-center) a considerable amount of flywheel effect is necessary. If this is not supplied the engine may refuse to start, or may oscillate back and forth without turning a full revolution. This is probably the best type for high pressure CO2 work and both present day CO2 engines use this principle, but we do not recommend it for low pressure or steam engines. Efficient exhaust porting, of expansion engines offers a special problem. Usually it is not enough merely to cut a hole in the cylinder as is done in 2 cycle engines where the piston itself acts as an exhaust valve* This is because the cylinder will exhaust only down to atmospheric pressure, the portion of gases remaining offering considerable resistance to the piston on the way up again. Drag of this sort can absorb a high proportion of the potential power of a low-pressure engine. *Although this practice is permissible where very high pressures are employed, such as in the popular CO2 engines with their four large ports, and in some types of annular ported steam engines where the sudden drop in pressure causes "condensation vacuum." To obtain optimum efficiency the exhaust valve should operate from the head of the cylinder and remain open until the piston is nearly at top of the stroke, closing before or if possible at the same instant the inlet valve is opened. Thus far we have not mentioned double acting engines; a word about them is in order. A double acting engine is one in which the operating gases push the piston both ways by means of a duplication of valves at lower end of the cylinder. This necessitates some sort of packing gland around the connecting rod, a heavier structure and complication of the valve gear. It is, in effect, a 2-cylinder engine in 1 cylinder. On the basis of our experiments we do not recommend this type for aircraft use, although it may be advantageous for model automotive and marine installations. Instead we suggest the use of multiple cylinders, 3 being ideal, since there is no "dead center." In radial "ex-pension engines, any number of cylinders may be employed, odd or even, with the power output becoming smoother as the number of cylinders is increased. Now, how can we obtain pressure? There are several methods of storing gas under pressure to drive an expansion engine. The simplest, oldest and in many ways most satisfactory method is to compress air in a light tank by means of a and pump. For those who dislike pumping operations the tank may be filled from a seltzer cartridge by means of a little gadget used to secure emergency inflation of bike tires. We once used an old high-pressure truck tire, inflated to 80 Ibs. at a local service station; rolled to the flying site it provided, by means of a detachable air-chuck, about a dozen flights. (Surplus oxygen tanks now available quite cheaply are light, strong, and would serve this purpose well. —Ed.) The gas generator engine offers literally dozen of methods of securing pressure. Dry ice can be heated in a tank by means of a tiny, well shielded alcohol flame; CO2-evolving chemicals can be mixed with a small quantity of water, and a small quantity of air and gasoline exploded by an electric spark into a larger amount of dry air will produce instantaneous pressure. However, do not attempt any of these methods without using a reliable safety-valve, and in particular do not try the gasoline exploding stunt without first calculating very carefully the proportions of the generator. If you don't know how, don't try it! Steam is probably the safest thing to generate and the easiest to handle. The boiler should be strongly constructed of non-corroding metals, and baffles of some sort are needed to prevent sloshing around in flight. The steam line should be attached to the tank in such fashion that it cannot pick up water if the plane should bank sharply. The burner is best fueled with alcohol. The safest type we have found is simply a pad of asbestos wicking soaked in fuel. This removes practically all fire hazards since the fuel stays put and there are no feed lines to overheat, fracture, or otherwise cause the model to ignite. Air scoops can be used to increase the heat of the burner and, by strategic placement, carry away all heat, which might be transmitted to the plane's framework. A carefully designed steam plane is perfectly safe for free flight since it will not descend until the burner goes out. Smooth operation makes it possible to use lighter construction to improve soaring qualities. The possibilities of steam have never been fully realized. In view of the results obtained with comparatively crude constructions we venture to suggest that if somebody with the time, money and ambition put as much engineering effort into developing a good airplane model steam engine, as has been put into development of present day gasoline engines, the steam engine would give internal^ combustion a good run for its money. There are many sound reasons for this premise. First, there is absolutely no question of whether or not it will run. If you can scratch a match you can start a steam engine. Second, there are no electrical problems, no wiring, and no switches. Third, steam is quieter, cleaner, and generally easier to handle than internal combustion with its special fuel mixtures, variable compression (in the case of diesels) point clearances, cowling problems, and oil-throwing disposition. But is steam capable of offering as much power? We think it is, and with weights comparing favorably with internal combustion. The reasons are: Although the steam power plant is not as efficient—interims of B.T.U. converted to mechanical energy—as the internal combustion engine, it can quantitively convert more fuel into mechanical effort for any given displacement. Thus, if a gasoline engine of .299 cu. in. displacement, obtains a thermal efficiency of 25%, and a steam engine of the same size has an efficiency of only 10%, this does not necessarily mean the gasoline engine is more powerful even though it is 2-1/2 times as efficient. We can burn 5 times as much fuel in the steam engine and raise its power output to twice that of its rival. The amount of fuel, which can be burned in an internal combustion engine, is strictly limited by its displacement. Therefore, for each revolution it is practical to convert to heat only as much fuel as will give the greatest expansion of gases; additional fuel will not give additional power but will simply be wasted. The maximum gas pressure over the piston for any given stroke is limited strictly to the maximum pressure it is possible to obtain by burning a given quantity of gasoline and air. This does not hold true for steam. Here, the pressure over the piston is limited only by how much heat is being applied to the bottom of the boiler. We can raise this limit by raising the burner temperature; that is, by forcing more air and fuel into the firebox. Another angle: in order to get any sort of power output from internal combustion engines they must turn over at very high speeds, speeds which it has been demonstrated are not the most efficient propeller wise. To permit high engine speeds and lower and more efficient propeller speeds, the use of some sort of reduction gearing is mandatory, bringing added weight and frictional losses. However, with the steam engine it is possible to hold the speed down with a larger propeller, of higher pitch, and let the increase in boiler pressure carry the load. What should we be able to do with props of 20" pitch, 3 to 4 times the area of today's racing toothpicks? And—just in passing, because we have done but a sketchy amount of work on the subject—what are the possibilities of using tiny impact turbines and driving the prop at a lower speed through a magnetic slip clutch? To sum it up, it is the writer's conclusion that there has never been a fair test of basic worth between the expansion engine' and gasoline power plants for model plane use. There is, today, a need for a good reliable compressed air motor for free flight which can be filled with a few strokes of a tire pump. The whole thing should not be over 24" in length and should be manufactured to tolerances comparing with those used for gasoline engines. In steam, there are boundless opportunities for both control and free flight. The application of cartridge gas (CO 2 etc.) to model prime movers has only been briefly exploited. In short, the expansion engine field is one, which has been but lightly and sketchily touched, with no real effort to extract the utmost performance from the basic idea. Now, who is going to do something about it? MODEL AIRPLANE NEWS • June 1948 I Fly a Control-Line Trainer It looks like a refugee from a Venetian-blind factory, but it flies fine—and it won't stall. By James Webb The prop is spun . . . the engine roars . . . must remember . . . pull back on stick. Then ease off . . . in the air now . . . everything's going by so fast . . . trees . . . ski . . . water . . . trees . . . a blur . . . beginning to feel dizzy . . . nose down again . . . must pull stick back . . . there's the sun . . . dazzling . . . can't see very well. . . she's stalling . . . Crash! I'd cracked up on my first solo flight. COURSE I could walk away from OFit—you always can; that's a big advantage in flying control-line models over the real thing. But the crash discouraged me from getting a model for the kids. Now, here was Roy Clough Jr., whose model I'd cracked up, with another plane, a funny-looking one. The wing was a series of slats with air spaces between. And there was a big cardboard disk in front of the prop. "What have you got there?" I asked. Roy had been mighty nice about his plane—explained that lots of beginners cracked up control-line jobs because they are so fast and so easy to stall if you freeze on the controls. Then he grinned. "This," he explained, "is a control-line model designed especially for beginners —a basic trainer. She's slow and she won't stall. Swell for kids to learn with. Why, AUGUST 1955 189 After a flight checkout ............away she goes I bet even you will be able to fly her." I was in no position to resent that. Instead, I asked for a demonstration. The little plane took off slow and easy and went around the circle with a lazy lope like a tired hound-dog. Then Roy stuck her nose up and held it there. Instead of stalling and crashing, she kept mushing around, nose in the air, even slower—walking speed. Roy wasn't kidding. This little job was as different from the model I'd flown before as a cub trainer is from a Shooting Star. "What's the secret?" I asked. He pointed to the slat wing and the prop disk. "The disk spoils the air stream from the prop so that the plane travels slowly. And she gets the lift to keep going at low speeds from this fancy wing. WING SLATS set at varying angles, ranging from negative (downward) angle at leading edge of wing to positive (upward) angle at trailing edge, give lift at low speeds. The tail surfaees are hinged with cloth tabs. Air compressed under the wing by the forward motion is squirted through the spaces and over the slats to provide the lift. "And notice the low angle of that front strip," he went on. "That's what keeps her from stalling even when the nose is way up." I took the controls, and Roy was right. Even I could fly this job, and I could turn her over to small fry with little risk of a discouraging crack-up on the first try. What was equally important, I found I could build a trainer model for the kids myself. So can you. Here's how to go about it. Fuselage. Trace the fuselage outline on a sheet of 1/4" balsa and cut it out with a razor or a modeler's knife. Cement a 1-3/8"-diameter disk of 1/4" plywood to the nose for the engine mount. Then add two half-round blocks of balsa, faired from the disk to the fuselage, to reinforce the engine mount and hold the mounting nuts and landing gear in place. Cement the cloth-hinged tail surfaces in place and brace them with two wooden toothpicks. Bend a tailskid from soft wire, press it into the fuselage, and secure it with cement. Wing. Cut the slats for the Venetianblind wing from 1/8" balsa and cement them to tip racks made from scraps of 1/4" balsa left over from the fuselage. These tip racks must be stepped or 190 POPULAR SCIENCE climbing high .......................................... into the sky notched exactly like the fuselage for good alignment. Add 1/16" tip plates to the wing and cement to the fuselage. Coat the model with fuel proof dope to protect it from the engine fuel. Controls. Cut a T-shaped bell crank from tin can stock and pivot it on a nail pressed into the fuselage. Link the control crank to the elevator horn with a length of 1/32" music wire. Support the wire at its center by a piece of plasticsoda straw cemented to the side of the fuselage. Tie and cement a 25' length of light fishing line to each leg of the bell crank and pass the lines through the wire loop on the wing tip. Trim the free ends to exactly the same length and attach them to the control handle. Engine. Almost any small half-A engine can be fitted to the mounting disk. Just be sure the engine shaft is mounted at a slight downward angle for good lowspeed behavior. Fit it with a 6" propeller and kill its efficiency by fastening a 3" disk of cardboard in front of it. Operation. As soon as the trainer was finished, the kids and I took her out to the empty lot next door. With Roy along to give us some expert advice, we quickly got the hang of it and could walk her around the circle without any trouble. Engine tune-up. After you've been flying a while, you may find your engine getting cranky and hard to start. This probably means that a gummy deposit What a show! from the fuel is clogging the tank and feed line. They can be cleaned with lacquer thinner. But a word of caution. Even a tiny half-A engine has nasty exhaust fumes; spend the evening in your shop turning her over and you'll end up with a bad headache. Have plenty of ventilation, or better still, do your tuningup outdoors. Fueling. Your fuel comes ready-mixed —a typical formula has castor oil plus methanol plus nitro-paraffins—in halfpint cans that cost about 55 cents. This may seem pretty high on a gallon basis— $8.80-but you'll find it's only slightly over a penny a flight. You can fill the tiny tank with an eyedropper, but it's a lot easier and safer to use a miniature pump that any model-supply store carries. Starting. Prime the engine first until it slops over—don't try to be neat if yon AUGUST 1955 191 want easy starting. Then hook on the batteries—a couple of 1-1/2 volt jobs wired in parallel. These supply the juice to heat the glow plug that ignites the fuel inside the cylinder. One contact goes to the glow plug, the other to the engine frame. You can make your own connecting wires, but again it's easier to use a readymade wire with a neat double tip that fits exactly and costs only 35 cents. Of course, you disconnect the batteries as soon as the engine catches. Before spinning the prop, set the fuelair-mix screw at the point recommended by the manufacturer—usually three to five turns open. If the engine catches readily but then dies, your mixture is too lean. If it does this even with a rich mixture, your fuel line is probably clogged. Once the engine catches, the engine will sputter and spit, so lean the mixture until it roars smoothly (it will really roar, too). Controls. Be careful when you unwind the reel not to cross the control lines. Operation is simple. Hold the reel vertically, with the end upward that is connected to the up action of the elevator. (Mark this end with a red dot on the reel.) Then you pull the top of the reel back to make the plane rise; the bottom to make it dip. Flying. It takes two people to handle any control-line plane: one to spin the prop, one at the controls. If there is no bare earth or pavement handy for the take-off run, the prop handler will have to hold the plane in the air and give her a little toss forward; she won't take off from grass. The take-off run should last 10 or 15 feet. Level off after a slow climb. Gentle the controls; the plane responds readily as she picks up speed. If you freeze onto the controls with the nose up, the trainer will just mush around instead of stalling. But don't get in the habit if you plan to fly conventional models. You may think the fuel supply is very small; later you can add auxiliary tanks for longer flights. Actually, however, you'll find at first you can get pretty dizzy even with a short flight. Props. You can vary the speed considerably with different combinations of props and spoiler disks. Those recommended for the plane fly her about as slowly as she'll go and still take off. You'll soon find props are expendable, so take along half a dozen spares. Beware the wind. Because the trainer flies so slowly, she develops very little centrifugal force to keep her out at the end of the control lines. Even a slight breeze may blow her toward you as she flies crosswind—and if the lines slacken, your control is lost. If necessary, keep lines taut by running downwind. - END A TIN CRANK transmits your pull on control lines to elevator. Lines are attached to a control stick hand-held in vertical position. The plane climbs when you tilt the stick back, dives when you ease it forward. Cabin windows are painted on the fuselage. 164 TOYS AND GAMES Try a Real Challenge-Build Free-Flying Powered HELICOPTER High-flying helicopter takes off vertically, and solves control problems of gyroscopic forces and torque By ROY L CLOUGH JR. Taking off vertically and flying at reduced speed forward allows you to experiment with the helicopter in reduced flying areas without it disappearing. Craft Print Project No. 202 little chance you'll lose this helicopTHERE'S ter in a free-flight, as it takes off vertically, flies forward at reduced speeds, and slowly floats down when the gas runs out. You can fly it in a limited space with less danger of cracking it up. And it will teach you about rotary-wing aircraft and their problems. With all the advantages of helicopter flyingwhy haven't we seen more of them? Controlling a model helicopter involves some complex dynamic problems. Flight stability has been a big stumbling block, as early models either crashed within seconds after take-off or rose drunkenly into the air before tipping over to one side and plummeting downward. Helicopters gained the reputation of being tricky, hard-to-control, and requiring an expert's patience to adjust all the factors that would keep it in the air for a few minutes. Actually the trouble was not with the helicopter idea, but with the approach to the problem. A rotating wing observes not only aerodynamic laws, but also the laws which govern gyroscopics. Rotors behave in much the same fashion as a toy gyro top. Applying a force at one point on the rim tilts the rotor, not at that point, but 90 degrees from that point. This is a basic law of gyroscopic action. A rotor that is rigid and stiff, as most of the early rotors were, would react at 90° to any deflection in flight. If a wind struck the front of the rotor, for example, it Counter-rotating props solve torque problem as small blade attaches to engine output shaft while main rotating wings are fastened to engine frame. TOYS AND GAMES tilted on its side. Then, if the same wind struck the side (due to the slip induced by the first displacement), the rotor would pitch fore and aft. The net result was a wild series of dips and rolls of increasing amplitude ending in a crash. These reactions happen so rapidly that it appeared the model simply 'went crazy' and crashed. Solving this stability problem calls for freeing the rotor blades so they can tilt, increasing or decreasing their pitch angle according to the aerodynamic load upon them. To obtain this motion Helicopter Adjustments Made Easy FIRST, remember that the spinning rotor is essentially a gyroscope. Since the large rotor has the most mass, it rules the system in this type of model. A gyro reacts to an adjustment or disturbance at 90 degrees from where the disturbance takes place. Thus it might be said that we adjust model helicopters "around the corner." For example, if the center of gravity is in the correct position and the model tends to nose up, we correct this by bending the rotor mast so that the rotor mechanism tilts slightly to the left. If the model tends to dive, then we tilt the mast somewhat to the right. By varying the sidewise tilt of the rotor mechanism we can make the model fly forward to right or left or rise vertically. On the other hand, suppose we load the model tail heavy. This puts a side load on the rotor, which is processed (moved 90 degrees) by the stabilizing tip weights and changes the pitch (cycles the blades) and produces FORWARD flight. If we load the model nose heavy it will tend to back up, but due to the keel surface it will swing around quickly at high speed and may dive because of sudden change in altitude. 165 automatically, small flyweights are attached to the blade tips to integrate the gyroscopic forces with the aerodynamic forces. When the rotor encounters a tilting force it reacts at 90°, causing the tip weights to bob up or down. These weights change the angle of attack of that particular blade. Since this reaction occurs at 90° from the original displacement, the control reaction, which also moves 90°, travels back to the original point of displacement to cancel out of the disturbance. The flyweight solution also provides automatic autorotation when the motor stops. Otherwise the rotor would slow down and stop, then start to spin backwards, which nine times out of 166 No. 1 1 1 2 3 4 1 5 20 2 5 1 1 1 TOYS AND GAMES MATERIALS LIST—HELICOPTER All Dimensions in Inches Size and Material 1/8 x 3 x 18 balsa 1/16x 3 x 36 balsa (spare blade allowance) 1/4 sheet balsa, approximately 1-1/2 x 3 (mast fairing) 10 x 12 stiff paper for fuselage covering small jar covers (press-on type) paper clips 3/32 hole washers length 1/16 piano wire, 36 long 5-in lengths soft iron wire, 1/16 diameter sq in tin can stock 1-diameter wheels 2/56 x % nuts and bolts 1/8 leather washer or equivalent Wasp. .049 or Atwood .049 model engine 2 or 3 pitch prop 5 to 7 diameter for engine Misc. colored fuel proof dope, cement, solder, etc. ten would tumble the model into a crash, to say nothing of presenting a very sloppy performance having little in common with full-scale machines. While our helicopter appears to be, and actually is, an extremely simple design, the design considerations behind it are based on a working knowledge of some rather complex factors, so don't alter the plans if you want the best performance. While everybody likes to make minor changes here and there, you'll find it to your advantage to build this model exactly as shown. Later on, with more experience and the understanding of gyro forces learned from this model, plus actual flying experience and observation, you can design an original. Understanding of what goes on is the keynote to success with helicopters. Our helicopter uses a 'torque reaction drive', which bypasses all problems of clutches and gearing. Two rotors supply lift—a small one attached to the engine's output shaft and a large one, which spins in the opposite direction. Along with this system's mechanical simplicity is its more dynamic complexity. The small rotor does the major lifting task while the large rotor takes care of the stability and autorotation. The fuselage is a good place to begin construction. Bulkheads slip on a simple keel and the resulting frame is covered with stiff construction paper. The rotor mast and the landing gear legs must be ruggedly attached. Cabin windows are painted on with hot fuel-proof dope in a contrasting color. The tail surfaces are fixed, as it is not necessary to adjust them (we'll explain this later). The rotor unit, the heart of the helicopter, begins with two small can covers—we used caps from baby food jars. These should be about 1-1/4 in. diameter and no larger than 2 in. diameter Clean out the seal or cardboard and accurately center a hole to fit the rotor mast in each. The blade arms are 1/16 in. diameter music wire. Bend to shape (Fig. 4) and solder in place inside one of the caps. Good balance and accurate layout are important here. Next drill holes for the engine mount, taking care to center the engine exactly. Solder the mounting nuts in place over the holes. The blade clips are bent from tin can stock. Brass or copper tubing forms the pivots on two of them (Fig. 4) while the third is soldered directly to the blade arm at a slight positive angle. A #3-48 or #2-56 nut and bolt holds the blades in place. With the rotor stems in place, take the other jar cap, butt it up against the first (which has the hardware in it) and run a bead of solder around the seam. This makes a very light and friction-free rotor bearing. Hold it to the fuselage mast with a washer soldered to the mast. Make up the rotor blades now. The woodwork is identical for all three; simply sand them to a 'glider wing' section and dope. Two of the blades are fitted with tip weights (Fig. 4). The third blade is assembled without weights and goes in the fixed holder. The only weight we put on this is whatever is required to balance the engine cylinder. Assemble the whole works and check for balance. Then make up the pivot prop and put it on the engine (Fig. 3). Use a small wood block to provide take-up for the shaft nut. You're now ready to test fly it. Check the balance of the fuselage. The center of gravity should lie about 1/8 in. behind the vertical axis of the rotor. This is why: In order for the TOYS AND GAMES helicopter to fly forward while it is rising we must have some force that makes it do so. The design of the fuselage causes it to present more resistance to the high-speed downwash of the small rotor in the direction in which we wish it to travel. This means the fuselage will tend to tilt down unless we move the CG aft to compensate for the downwash effect. In flight the fuselage will tilt forward only slightly, because the reaction to this tilting force is precessed gyroscopically to the blades, which shift position slightly and propel the model forward. Start the engine and run it up to top speed with the mixture set a bit on the rich side to compensate for the centrifugal force on the tank. Allow the main rotor to come up to its maximum speed, and then allow the model to rise under its own power from your hand. Be sure it is level and never throw it. The machine should rise up steadily and when about 10 feet up it should start to move forward, flying in a large circle to the left, and gaining altitude until the engine stops, when it will drop vertically on its spinning rotor. Bending rotor shaft to left, forward or to right controls direction of flight. This model has one fixed blade on the rotor, which is used to control forward speed and eliminate diving tendencies. The fixed pitch angle should be about the same as the normal angle of the feathering blades, otherwise the model may 'walk' a bit as it flies. If your model refuses to fly forward, decrease the pitch of the fixed blade, and at the same time bend the flyweights up on the other two blades so they rotate at the same average pitch. If, on the other hand, your model tends to dive, increase the pitch of this fixed blade by 167 bending the wire slightly and bend the flyweights on the other two blades down a bit further so that when they ride up under centrifugal force the pitch on these blades will 'seek' about the same angle as the fixed blade. Since the feathering (or pivoted) blades automatically tip up when the engine stops, the fixed pitch blade does not interfere with auto-rotation. The function of the special stabilizer arrangement, which tends to twist the fuselage to the right if the forward speed becomes high, is to lift the nose and slow the model down. This feature makes the model easier to handle, acting as a sort of built-in 'governor.' For this reason it may be flown at considerably higher forward speed than the usual run of model helicopters. Do not reduce the size of this set of surfaces, and in stubborn cases (if, for example, your model is very heavy) it may be necessary to increase the size slightly. The recommended engines for this model are the Wasp .049 or the Atwood .049. Use either STA dopes or Aerogloss finishes throughout. • Craft Print No. 202, in enlarged size for building the Powered Helicopter is available at $1. SPECIAL QUANTITY DISCOUNT! If you order two or more craft prints (this or any other print), you may deduct 25 ⊄ from the regular price of each print. Hence, for two prints, deduct 50⊄ ⊄ ; three prints, deduct 75⊄ ⊄ , etc. Order by print number. To avoid possible loss of coin or currency in the mails, we suggest you remit by check or money order (no C.O.D.'s or stamps) to Craft Print Dept. 5561, Science and Mechanics, 450 East Ohio Street, Chicago 11, Illinois. See coupon on page 192. Now available, our new illustrated catalog of "186 Do It Yourself Plans," 10⊄ ⊄ . Please allow three to four weeks for delivery Scanned in from: Toys and Games You Can Make Science and Mechanics Handbook Annual No. 6, 1958—No. 556 Autobiography of ROY L. CLOUGH, Jr. Modeler, Author, Novelist, Magazine Contributor, Designer, AMA Hall of Fame Life Member Modeler since 1931 Birth Date: November 18, 1921 AMA: 3254 Written & Submitted by RLC; Updated 7/02 Transcribed by NR (5/97) Edited by SS (2002) Career: ● Designed the Berkeley “Cloud Copters” ● Designed the first ground effect vehicle in late 1930s ● Built successful rubber powered helicopters and gas powered versions in the 1950's ● Built ducted fan delta in late 1940s ● Was an early builder of reso-jets ● Designed and built glow and diesel engines ● Built a steam-powered control liner ● Designed the original free flight version of the Martian Spaceship ● Have built and flown Flettner-type rotor planes as early as the late 1950's ● Originated the slotted flying saucer design made popular by Fran McElwee ● Built and flown several types of autogyro ● In 1948, built a liquid fuel rocket with compressed air oxidizer ● 22 years as Chief Eng. of high tech firm ● Four years as an Ind. Consultant ● Worked as reporter/writer/editor New Haven Journal-Courier, Eastern Pilot ● At present a freelance writer/designer, author of four books, including 1930s period novel: A Brief History of the Ashmont Town Team etc. ● Long time C&W musician, pedal steel, Dobro. Designer and builder of many instruments Honors: ● 1999 – AMA Hall of Fame I was about 10-years-old when I built my first flying model out of pine sticks, gray building paper and inner-tube rubber. It flew about 25 feet and I was hooked. My first kit was a Guillow 10-cent Spad, given to me by a little girl who drew my name in a school Christmas party. Spad wound up as a midwing that would not fly. Early inspiration to design my own sparked by Gordon Light's Wakefield winner. It proved a good pattern. I have built models with all sorts of power including rubber, compressed air, steam, rocket, park ignition, glow engines and electric motors. One early model, best forgotten, even had a clock spring motor. . I developed an early interest in unusual, unorthodox, new types etc., and in early 1940's built successful rubber powered helicopters and gas powered versions in the 1950's. Both types were widely copied. I got into magazine projects by accident when Popular Science's Workshop Editor, the late Harry Clough Page 2 of 3 Walton, was told by his secretary, Ria Nichol, that during a visit to my wife and I in Now Haven she had seen me repeatedly fly a model helicopter from one table top to another. When I discovered I could get paid for this stuff I published a lot of it in MAN, FM, Pop Science, Air Trails, Science & Mechanics, Popular Mechanics and Mechanix Illustrated. I also designed the Berkely “Cloud Copters.” My rotor system was widely copied, including by Cox Manufacturing who never acknowledged or paid for it. Considering the job they did on Jim Walker I figured I lacked the resources to buck them. Later involvement with Big John Elliot and Larry Renger was pleasant and productive, but they fared no better at the hands of Cox management. I had a lot of firsts including perhaps the first ground effect vehicle. It was a small gas engine powered model about three feet long. It worked great, but all the dirt, grass and twigs it threw up convinced me the idea was practically useless. Talk about blowing it!! I could have had a basic patent. Later on I built a .049 powered model for Popular Mechanics, which they reprinted in one of their workshop books. I built several early ducted fans, maybe the first to achieve worthwhile thrust. I was flying Free Flight versions when Bill Effinger and Don McGovern could not get their Control Liners off the ground, but what they told me was helpful to my later designs. Also I built two or three pressure Jets. Only one of these was published but I might get back to the idea. Jets published in Air Trails & Popular Science. I was an early builder of reso-jets; the smallest had 7/16 diameter and a tailpipe made from telescoping tubing sections from a golf club. I slid sections back and forth like a trombone to locate the proper resonant frequency. I designed and built glow and diesel engines. Little Dragon, published in Model Airplane News is the best known. I converted an OK C02 motor to run very poorly as a diesel. I also built a small steam boat and a steam race car for Popular Science. I built a steam-powered Control Liner that blew up on take-off. I designed a gas helicopter with 48" self-powered rotor that flew well on Cox .02. Pop Science. Originated the slotted flying saucer design, (Air Trails,) but it was made popular by Fran McElwee who carried the design forward. Much later I published a couple of versions in Model Builder. While I designed the original Free Flight version of the Martian Spaceship, (Air Trails,) Skip Ruff should get the lion's share of the credit for the bigger radio control versions that have made such a hit on the West Coast. I built and flew Flettner-type rotor planes as early as the late 1950's. Model Aviation News, Popular Science, latest “Rotorplane!” in MAN. (*)See bibliography Built and flown several types of autogiro. MAN. Autogyro kites for PS and S~&M. Built early but not greatly successful electric in the 50's. In 1948 I built a liquid fuel rocket with compressed air oxidizer that blew up with a very satisfactory bang. Clough Page 3 of 3 Despite early AMA membership have, until recently usually been a loner. Now, in the springtime of my senility have joined up with the Winnipesaukee Radio Controllers, and acquired a great bunch of flying buddies. I'm likely to try any construct that gets my interest. As a result of this I know more things that won't work than anybody. Background includes: 22 years as Chief Eng. of high tech firm, Four years as an Ind. Consult. Worked as reporter/writer/editor New Haven.Journal-Courier & Eastern Pilot. Co-authored a McGraw-Hill text on Industrial Psych. At present a freelance writer/designer, novelist and semi-pro C&W musician: pedal steel/ Dobro/ keyboards. Have worked with Paul Main, Hank Thompson, Dick Curless, and ran my own “Stateliners” for a few years, but enforcement of tough driving and drinking laws has wreaked havoc on the cabaret scene. Although I believe I am widely known as a designer of “weirdos,” I wonder what these same readers would think if they had seen some of the stuff I tried but did not publish. Reason? It has always been my policy to publish only those things that were easy to build, were not dangerous and would work on the first try for anybody. This ruled out my regen engine that developed so much ungovernable power it kept blowing up; my fuelless flying machine that would have to dump energy continuously to avoid melt-down, and a new system of propulsion that pilot and passengers probably could not live with. Fun stuff, but practically just curiosities. Currently I have a couple of dozen hot model projects in the works, which, now being retired, I'll finish doing whenever so will not interfere with goofing-off. Bibilography: MAN= Model Airplane News AM= American Modeler PM= Popular Mechanics AST= Astounding Science Fiction SM= Science & Mechanics MODAV= AMA'S Model Aviation Magazine CL= Car Life MI= Mechanix Illustrated PMA= PM Shop Man Date June 1945 Sept. 1945 Oct. 1945 Magazine Hunt. Fish Bas. Des. AP AT= Air Trails FM=Flying Model PS= Popular Science AZ= Amazing Stories BL= Boy's Life AP= Airports Magazine MN=Merchandising News RTV= S&M's RAD.TV.EXP. Title, Subject or Content Several Hum. Verses anent H&F Problems of Model Helis Dear Mr. Small Operator Clough Page 4 of 4 Oct. 1945 Oct. 1945 Jan. 1946 Jan. 1946 March 1946 April 1946 Summer 1946 ? Sept. 1946 Sept. 1946 Oct. 1946 March 1947 May 1947 May 1947 Sky Raiders PS PS MAN MAN PS PS PS MAN AT PS MAN PS Aug. 1947 Sept. 1947 Feb. 1948 Jan. 1948 March 1948 April 1948 June 1948 Aug. 1948 Nov. 1948 May 1949 Aug. & Sept. 1949 April 1950 Mo.? 1950 Mo.? 1950 Sept. 1950 Oct. 1950 Nov. 1950 Mo.? 1950 April 1951 June 1951 Aug. 1951 Aug. 1951 Mo.? 1951 July 1952 Aug. 1952 Sept. & Oct. 1952 Dec. 1952 Feb. 1953 AT MAN MAN MAN MAN PS MAN MAN AT MAN MAN Is German.Sec. Weapon a Rocket Plane? Skyhook Coax Helicopter Air Freighter of the Future? SOS to Model Manufacturer Unorthodox Design “Naclio” Steamboat Model Roadable Plane Model Triad (Radial Wing FF Model) Speed Made Easy Cage Drive Rubber Co-Ax Helicopter Steam Powered Model Race Car More About Model Helicopters Stressed Paper U-Control (Atom .05) Car and Plane in Home Workshop Annual for 1950 Evolution of the Model Plane Hoverbug Rubber Powered Helicopter Improving CO2 Performance – Wat. Jack. Autogiro Theory Autogiro Free Flight Rubber Job WHIZZER CO2 Racing Boat Model Experiments with Expansion Engines English Gyro to Clough Specs Beginners’ Goat (Still Flying, March 1990) Theory of Rotor Planes Reworking Old Engines MAN AZ AZ MAN MAN MAN AZ PS AST FM MAN MAN MN AT AT WhirliCO2pter Social Obligation – STF How the Saucers Fly Flying Saucer Design Little Dragon Glow Engine Part 2 Micrometer in Your Brain Why Shacks Come Apart (Foundations) Bait (Picked up for Anth. Space Police) Try a Helicopter Why Models Land in Trees (Prof. Tate) Flying Barrel – Description and pictures only Small Dealers on the Carpet Build Flying Saucer (Famous slot job) What’s the Score on Helicopters? PS FM Fly a Plane in the Living Room Sikorsky S51 TR Helicopter Clough July 1953 Aug. 1953 Sept/ 1953 Nov. 1953 Aug. 1954 June 1954 Mo. ? 1954 Not. Pub. Pub. 54-55 April 1954 July 1954 Nov. 1954 Aug. 1954 Annual 1955 Mo. ? 1954 Mo.? 1954 July 1954 July 1954 Mo.? 1954 Sept. 1954 Oct. 1954 JORA 1954 S Dec. 1954 Dec. 1954 Jan. 1955 Mo.? 1954-55 Mo.? 1954-55 Feb. 1955 March 1955 Aug. 1955 Aug. 1955 Sept.1955 Oct. 1955 Oct. 1955 Dec. 1955 Dec. 1955 Mo.? 1955 Dec. 1955 March 1956 June 1956 June 1956 Pub. 1956 March 1957 Dec. 1957 Page 5 of 5 AT AT PS AT PS SM ? PS to BERK AT AT AT AST FM AT PS PS PS AT AT AT AT BL PS PS PS PS PS PS AT AT PM AT AT AT PS AT (YM) CL SM AT MAN AT (YM) AT Ann AM AM Tubine (Duct. Fan.) Jets for Models Below Bug Pressure Jet Model Jetex Driven Turbie – FF Model Two-Part Helicopter Design Dope Hydrojet Powers Tiny Boat TR Helicopter .049 Reprinted Model Craft V3, 1954 Oil Can Reso-Jet Doggerel Verse Fillers Martian Spaceship Typhoon Expansion Engine It Didn’t Come From Mars Stunt Goat CL Model Sikorsky R-6 Helicopter TR Co-axial Autogiro Kite More Fillers per Request Fourth of July Noisemakers Channel Wing Control Line Plane Tri-Yi Rubber Model January Alouette’ .049 Duct Fan – Ukie Wind Wagon Air Drive Race Car Mille Diesel Endurance – Ukie Ceiling Repair Fillers Uses for umbrella ribs Electric Shop Heater from Oil Can Things to do with Coffee Cans Turbine Jet Race Car Model Model Submarine Bautilus Venusian Scout Saturanian Space Skimmer Slat Wing Control Line Trainer TanGiro Twin – CL Autogiro Teenie Genie Tri-Yil Aerial Tramway TEE JAY’Super Delta Ducted Fan Phantom of the Turnpike Rebec Medieval Three String Violin Sheet Metal Susie Lil’ Dragon Used as School Project Cement Drives Crazy Water Gadgets Special Case of TR Helicopters Tumblewing CL Flettner Rotor Plane Famous Firsts (Yet to be Made) Clough July 1960 Sept. 1960 Feb. 1961 June 1961 June 1961 Sept. 1961 Nov. 1961 Jan. 1962 Annual 1963 Sept. 1962 Sept. 1962 Mo.? 1961-62 Feb. 1962 March 1962 May 1962 July 1962 Aug. 1962 Sold Aug. 1962 Nov. 1962 Nov. 1962 1962 Sold Dec. 1962 Dec. 1962 Dec. 1962 Mo.? 1962 Mo.? 1962 Pub. 1962-63 Jan. – Feb. 1963 March 1963 March 1963 March 1963 April 1963 June 1963 June 1963 Aug. 1963 Fall 1963 Fall 1963 Nov. 1963 Nov. 1963 Mo.? 1963 Mo.? 1963 Page 6 of 6 PS AM SM SM PS PS SM PM PMSHOP PS PM MAN A.E. Esty Machine and Tool Employees Manual MAN PS PM AM PM SM AM Crestwood PM (Pub?) MI AM SM PM Sam Bierman AM MI PM PS PM AM PM PM SMRTVEXP SMRTVEXP SM PM PM PM Rebuild of Cecil Peoli Twin Pusher Typhoon’s Expansion Engine Two String Splinter Bass Triple Neck Steel Guitar Tethered Ducted Fan Jet Plane Boat that Flips to Go (Porp. Tail Dr) Reader Report on Guitar Projects Ground Effect Vehicle Air Car Reprint GEV Platter Plane-Non-Slot Saucer Old Mill Waterwheel Table Centerpiece Model Helicopter Dynamics Nervous Nellie .05 Stunt Job Self-Powered Rotor Helicopter Remember the Spinning Wing Autogiro? Spinning Disk Model Ven. Scout Control Line Kite Whirlybird Co-Axial Autogiro Kite Snapper .49 FF Speed Job Please Shake Carefully (Humor) Tetra Four Radial Wings Ukie (X-Wing) String Phones Deluxe Peter O’Dactyl Homemade Vernier Dials Vapor Pressure Drivers Model Boat How to Open Anything (Humor) Yankee Flea Tandem Darkroom Light Box Mystery Moving Box and Kite, p. 164 Styrofoam Model Oos on Cox .010 Hoopskirt Annular Wing FF Turkey Buzzard Flying Plank Type Water Skating Model Boat Wind Rotor Drives Boat Propeller Speaker Box Does Everything Electric Amp for Banjo Moon Scout Electric Centrifugal Cannon Harlequin Stressed Paper Glider Control Line Stunt Kite Clough Page 7 of 7 As a result of being bugged by Skip Ruff and Bill Northrop in 1990. First published was in MAN, July 1992 a review of “Modelcad.” Then “Multiwiz” in August 1992 in MAN. More articles are due in MAN, FM and MB. Date July 1992 Aug. 1992 June 1993 July 1993 Oct. 1993 Feb. 1994 May 1994 May 1994 July 1994 July 1994 Aug. 1994 Nov. 1994 May 1995 June 1995 July 1995 Aug. 1995 Oct. 1995 Nov. 1995 Dec. 1995 Dec. 1996 Dec. 1996 Dec. 1996 Dec. 1996 Magazine MAN MAN MB MAN MB MB FM MB MB FM MB MB FM MAN MAN MAN MAN MB MAN MAN FM MODAV FM Title, Subject or Content CAD for Your Model Designs Multiwiz Model 2-Channel From 1 Servo Pushcart .049 RC Pusher Rotorplane! Flettner Wing-Rotor Saucer Mania Two Slot Saucers Ment. RLC Award Winner Morles 1915 .049 FMBD RC Pix Reader Built Zoomslot Ment. Adv. For Martian SS Ment. FM Helic. Of August 1951 Mention Traysvite Ment. Page 7 and Class, Gas and Jazz Ment. Page 28 and 57 Martian Spaceship Ment. Hal DeBolt’s Col. On Early RC Stringer Wing-Warp Control 02 RC Designed 2D 6.0 Critique R.K. Hicks FF Electric Air Age RC Book Chapter “Mindset” Ringer Annular Wing .049 RC Faux Fighter FMBD ‘Pilchard’ Aileron Trainer Materia Aeronautica Modela The following list of articles are missing from my files and have incomplete information. Date Early 1960s Early 1960s Sold April 1967 Early 1960s Magazine AT or MAN PS PM Lost by AT Title, Subject or Content Flying Barrel Gyro Glider Kite Foilplane, Flying Body Aircraft Maple Seed Jetex Powered One-Bladed Helicopter Other Projects ● Constructed the steam-powered race car model made for Minimax importer ● Cloud Copters Designed for Berkley Models ● Hummingbird Helicopter Design for Hamp. Research Foundation] ● Helicopter engine design with K & B ● Helicopter blade system for Sikorsky Aircraft Patent Inter. Clough Page 8 of 8 ● Co-authored text on Ind. Psych. With Dr. Brian Kay, McGraw-Hill ● Wrote novel: “A Brief History of the Ashmont Town Team vs Equestrian Statue.” (Amazon.com Barnesandnoble.com) (signed) Roy Clough, Jr. Updated July 15, 2002 - End - BASIC DESIGN PROBLEMS OF MODEL HELICOPTERS by R. L. CLOUGH JR. A timely, interesting Article on a subject that has been stumping the experts for years EXPERIMENTERS in the model helicopter field soon discover they are working with a tricky breed in which instability is inherent and where such terms as "balance," "keel surface" and "power transmission" take on a deeper and at times maddening significance. If one approaches the holy trio—dihedral, down thrust and balance—with the proper degree of reverence in designing a fixed-wing model, it is a fairly simple task to plan a ship that will fly and fly well However, this is not so with helicopters. In the model helicopter, and we are speaking of those intended to represent the real thing and not the familiar whirligig of the "freak" contest, one soon discovers dihedral, or coning angle of the blades, does not assure stability; that balance may be a variable due to gyroscopic action when "stiff" rotor blades are used; and that "down-thrust" has no true counterpart. Unlike most scale models, the fact that a full size machine has flown does not necessarily mean a model helicopter built to the same pattern will be successful. This discrepancy is due in part to what is commonly called "scale effect," and because in a larger machine there is a pilot along to constantly correct flight aberrations as they appear. In power transmission, friction losses in a model run far higher in direct proportion than in full-scale machines. Torque effect is also more pronounced because more power is needed proportionately to fly a model. Therefore, in order to secure successful flights, the modeler must design his little ship in such a manner as to insure inherent stability—something which makers of full-scale machines have not been too successful in to date. The greatest single problem in helicopter design is: What to do with torque? Shall we concentrate on using it, nullifying it, or plot such a design wherein it may be successfully ignored? Since this article is dealing primarily with rubber powered helicopter models we shall concentrate on the first two; either to nullify torque or use it. The latter method of plotting a design wherein torque may be ignored involves self-motivated rotors, propelled by jets at their tips, and confronts the modeler with many mechanical difficulties. Perhaps we speak rather loosely of "using torque." What is meant is that torque is being "used" in a model when the method of eliminating it contributes to the overall lift. When this equalization does not contribute to the lift it is considered nullification, Gyroscopic action is another bugbear. It will always be present to a certain extent, but evidence at hand indicates it is not an insurmountable problem. 14 MODEL AIRPLANE NEWS • September, 1945 Flexible blades and articulated rotor hubs do much to alleviate this effect Proof of the power of this effect was made quite apparent to the writer in an early model design. This model was of the single-rotor and torque prop design and featured a heavy, non-flexible main rotor. It was discovered that when the model was hand launched it would maintain the position in which it took the air until the motor had wound down enough to permit the weight of the machine to overcome the gyro action and return to an even keel This effect was so pronounced that the model would fly on edge for several seconds before leveling off when launched in that position Subsequent experiments with a flexible main rotor definitely laid the blame for this condition at demon gyro's door When choosing the type of design to work with, the experimenter should make UP his mind to stick to that type until he is thoroughly familiar with its intricacies There are five basic types of helicopters and many modifications of each. There are certain disadvantages to each type and all lack the simplicity of rigid wing aircraft Probably the most familiar is the Sikorsky type which corrects for torque by means of a smaller rotor at right angles to the larger in such ratio as to amply compensate for torque at all speeds Second is the contra rotating, in which two main rotors revolve in opposite directions around a common center The De Bothezat, Hiller-copter and Bleriot machines are good representative types Third is the twin-rotored helicopter utilizing two main rotors of opposite rotation extended on booms from the side of the aircraft A variation of this principle is to put the rotors at opposite ends of the fuselage, thus doing away with the booms. The Landgraf, Platt-LePage and German Foeke-Achgelis are examples of this trend of thought. This type is probably the oldest. Fourth is a fairly recent innovation control could be effected through the and the writer has been unable to large single rotor which would secure information as to .whether the undoubtedly throw dangerous machine has actually been built or stresses onto the smaller rotors. This was merely proposed Three rotors type is definitely not recommended are employed, a large main rotor in for model experimentation. the middle and two smaller ones on The fifth type is the newest and has booms, rotating in opposition from the received quite a bit of attention. In main rotor to counterbalance its this type there is but one main rotor, torque. From casual inspection it which is activated by jets located in would seem the gearing necessary to the tips. Thus thrust is contained accomplish this would result in within the rotor and, acting directly something of a plumber's nightmare, upon it, automatically eliminates with more power being absorbed by torque effect. gear boxes than by the rotors. It is interesting to note in relation to Control, too, would offer quite a full sized ships that this idea appears problem. Either all three rotors must basically sound for two very good be controllable entailing a great deal of reasons. Tip speeds approach weight and machinery, or possibly velocities at which jet propulsion works best and with the power being applied to the tip of the rotor instead of the hub the mechanical advantage is much greater, permitting concentration of thrust where drag is heaviest and allowing rotor structures to be lighter As far as model helicopters are concerned, however, this method offers many difficulties The writer has succeeded in making a compressed air jet powered rotor lift its own weight (and no more) under 90 Ibs pressure, and a steam jet rotor lift its own boiler—but not its heat source Powder rockets will supply enough thrust and are not overly heavy, but their extremely short duration is discouraging Therefore the remainder of this article will deal with the first three types Power utilized for these experiments is rubber, chiefly because of the simplicity of hookup and the high power-to-weight ratio Helicopter gas models will probably be built, but for the present it is undoubtedly best to leave out the added complexities of internal combustion until familiarity with the stability problem is gained. A gas engine would produce a fine steady source of power, but would also mean slip-clutches and gearing. Unless one has access to a machine shop these items are rather difficult to produce The design of the model helicopter poses the question- "Straight up, or straight ahead 9" If the model is, designed to fly vertically and attain the greatest possible elevation it seldom can be adjusted for "cross country" flights of any great duration One exception to this rule is the contra rotating type with a freewheeler which may be adjusted to move forward as it climbs by adding weight to the nose It will continue to move forward during its free-wheeling descent but "glide" ratio will be small Since model helicopters are designed primarily to fly vertically, the experimenter would do well to concentrate upon arriving at a design capable of a steady climb and slow descent with good stability throughout the flight Then, and only then, should he attempt "cross country" flights. The following sketches are presented primarily to stimulate the imagination of model experimenters; however, if the general proportions are followed throughout these models will fly well, though in no case is any sketch intended to represent a completely "perfect" solution. Fig. 1 is perhaps the simplest possible form. It is a direct takeoff on the familiar contest whirligig and is the easiest to build and fly. Directional stability is only fair, but "glide" is quite good if a free-wheeler is employed. The long nose-wheel strut protects the lower prop and brings the center of gravity forward. Rubber hook-up is simple and contra-rotation is automatic. In this, as in all types of model helicopters, too much emphasis cannot be laid upon the importance of making the rotor blades flexible. For every foot of radius the blade should have a "spring" of at least 1-1/2". This enables them to bounce and helps to destroy the aforementioned gyro effect. This model is described first to point out the effect of keel surface upon the flying qualities of the helicopter. Note the very narrow rear section and pointed nose. This is because when displaced air produced by the upper rotor strikes the fuselage it has a marked tendency to rotate it in the direction of the rotors movement. Therefore, the larger the keel-surface, the greater the turning moment. A friction brake on the lower prop is, in theory, the best way to counteract this effect. In practice, however, it proves tricky to adjust. A felt washer on the lower prop will often turn the trick, but a fin hinged on a fore and aft axis works better. This same effect is why pylon gas jobs turn to the right under full power, when one might be inclined to think they should swing to the left because of the torque. One tricky phase of keel-surface, or lateral area, should be mentioned before going any further. In fixed-wing models one usually attempts to get the center of lateral area as low as possible. The reverse of this ordinarily good rule is true in model helicopters for this reason: At the top of the flight the rotors come to a stop, then reverse for a freewheeling descent. The rudder effect of the fuselage side area is very pronounced at this moment, and if the area below the center of gravity exceeds that above it the model will flip over on its back and descend inverted. Therefore, in designing a model helicopter one must work out a good compromise with sufficient area above the center of gravity to permit a rightside-up descent and sufficient area below the c. g. to permit a stable climb. About 60% above and 40% below is about right, although on some types it is advisable to have as much as 75% of the lateral area above the c. g. Fig. 2 is the contra rotating type. Two rotors of equal diameter revolve in opposed directions. Hook-up is simple but care must be exercised in building the "cage," and all bearings must be true. Balance of all moving parts is the keynote to success with this model. Directional stability is very good and this sketch points up another phase of helicopter design. In this model, forward flight may be secured by adding weight to the nose, and the mass of lateral area must be well back of the rotor axis to keep it headed right. However, this brings in another factor: top-of-fuselage area. Since with this type there is more area on top of the fuselage exposed to the downwash of the rotors, behind the rotor axis, if the model balances directly on the rotor axis the down wash will force the tail down and give the model all the symptoms of tail-heaviness. This is best counteracted by balancing the model slightly ahead of the center of lift. The upper rotor should be equipped with a freewheeling device for easy descents, and it has been found that best results are obtained if the lower rotor has a slightly greater pitch—about 2°. The climbing ability of this type apparently exceeds that of all others. This is probably due to the direct utilization of available thrust where it will do the most good with a minimum of fuselage or deflection interference. Fig. 3 illustrates the dual rotor helicopter. Principal problem here is to equalize the thrust of the two rotors. The simplest and most positive way to accomplish this is by an equalizer beam. Hook-up should be clear from the sketch. In this model it is highly important to keep the center of lateral area as high as possible and to make the two rotors as nearly identical as possible. This helicopter is the simplest to adjust for forward flight as it climbs. Simply add a bit of weight to the nose. Fig. 4 of the Platt-LePage pattern is basically the same idea as Fig. 3. Power transmission of some sort is needed for this type; therefore it requires a lot of work in building and excellent balance for good results. Pulley and belt, of the kind described in Fig. 5, seems to work better than the connecting-rod type of transmission. Bevel gearing might be the ideal solution if a set of the same, light enough for practicality, could be obtained. A horizontal stabilizer seems to be necessary on this model and a rudder often helps. The best way of winding is by a small crank in the nose section as shown on sketch. Fig. 5 is based on the Sikorsky design. This is the model shown in the accompanying photograph. Power transmission to the rear prop was a great problem in designing the original. After numerous experiments the pulley and belt system was adopted as the most simple and efficient. Ordinarily one might think such an arrangement would result in slippages so great as to obviate the possibility of any constant ratio between the main rotor and torque propeller. This problem, however, was solved very nicely by facing the pulleys with a fine grade of sandpaper. The belt is common twine, tied snugly in place and shrunk with water. A four bladed rotor is used to absorb as much thrust as possible within a small area to keep the antitorque rotor boom as short as possible. The main disadvantage of this type is the short rubber length, but due to the proportionately slow revolutions of the main rotor, longer flights than one might be inclined to think possible may be had. This model works best under power dropping quite rapidly after achieving maximum altitude. It is presented here chiefly as an experiment in power transmission. The model will fly well only if weight is kept down. This method of nullifying torque rather than "using" it does not seem to be very efficient, more rubber being required proportionately to fly this type of model than one featuring dual, or contra rotating props. One interesting fact about the antitorque propeller was discovered: It does not need to produce a thrust anywhere near equal to the torque reaction produced by the main rotor in order to hold the ship steady. This is probably due to a keel-surface effect produced by the spilling of air from the tips of the main rotor against the apparent disk of the antitorque propeller, which would of course tend to push the boom in the direction of the main rotor. Adjusting this model so that torque is evenly balanced is quite simple. With a pulley ratio of 3-1 start with the blade area of the little prop equal to % the area of the main rotor. This will cause a slight over-correction and cause the boom to swing around in the direction of the big prop. Then trim the small rotor, a little at a time until it balances. This is considered the best way, even if it amounts to cut and try, because it has been found that a difference in bearings and pulley alignment is peculiar to each builder, with a natural slight difference in results. If the blades are over-trimmed, add a small fin to the boom in the slipstream of the larger prop and trim it to fit. Once adjusted this type will stay adjusted. Varying power used will not upset the ratio between the two rotors. It is a good idea for the serious experimenter to keep a record of his experiments for future reference. Patience is the keynote to success. Do not give up any design type until you are certain you have tried everything that can be done with it. Often a very simple "bug" will prevent a model helicopter from performing well. Once this is located the model will often turn in a surprising performance. Remember that in these little jobs a somewhat different set of conditions holds sway from those of conventional models. Respect those conditions and success will be yours. VICTORY