Encdurance Capacity for Continuous Eflon in Terms of Aerobic and
Transcription
Encdurance Capacity for Continuous Eflon in Terms of Aerobic and
ENDURANCE CAPACITY FDR CONTINUOUS EFFORT IN TERMS OF AEROBIC AND ANAEROBIC FRACTION OF OXYGEN SUPPLY J. SEN GUPTA. S.S. VERMA AND N.C. MAJUMDAR Defen::e Institute of Physiology and Allied Sciences. Delhi Cantt - 170010 Bnd Defence Science Laborarory, Delhi-llD U06 Summ.ry: Studies hIve been conducted on 13 young healthy adulla 01 average fitness on endurance work of varying dUfatlons lasting for 2·31 minutes using bicycle e<gometer. Aerobic-anal:!fOblc o fractions of oxygen supp1v during each effort was determined. The data from Astrand and Aodahl on aerobic O~ - supply and duration in ffiallimlll eltolls flom 1-120 minutes on a highly trained subjoct havo also been considered. Tho plol of log endurance lime against log (all/obic/anaerobic ralio) exhiblls a slIght deparlUllI Irom IiOElI/itl', ;ndiclIling Independent contributions from aerobIC and anaerobic fractiofls of oxygen supply. An equallon was derived of the form : T _ Au. k1 uz- k2 where UI end U2 are the aerobIC and anaerobic fractions respeclivelywhich has been found to yield highly signO/jcanl correlation cooffident botween log-eslimated and 10g-obselVed enduraflce time (09996 for Astralld and Rodahl's dala on a sillgle sublect and 0.9640 for lhe present data on 13 subJocls). This index IS. therefore. Quite suitable for the llssessmenl of elldurence capacity in terms of a single physiological parameter. and Is likely to be superior 10 illdices in current use. Key words: endurar!ce work aerobic and anaerobic fraction of oxygen supply INTRODUCTION Assessment of endurance work capacity of individuals is a problem of considerable imparlance in industrial and military situations. and also in sports. Light work can be sustained for an indefinite period because the energy requirement is met exclusively by aerobic process. While anaerobic energy yielding processes assume significant importance with increasing work load (19.20.21). It has also been fairl~' well established that the use of work load relative to the individual's aerobic capacity ('JO: max) eliminates most of the differences in endurance capacity among ind~viduals (12). However, a trained athlete can work at a relatively higher oxygen uptake relative to hj,;; maximum (70-75 per cent) without any significant increase in oxygen deficiency and b:ood lactate concentration (9.10,28). Untrained subjects. on the other hand. show a r,se in O2 debt and lactate accumu alion at only about 45-55% of their aerobic capacity (3 16.28). Experiments with animals and may have revealed that this adaptation in trained individuals is primar 110 Sen GUptll ~r July-September 1 9~9 Imt J. Ph".~iol. Phllfmitc. al due to a change in the capacity of aerobic metabolism brought about by an increase in the e:lzymatic capacity for oxidati'Je phosphorylation (17) and also due to higher perC!lntage of 5T fibers (10.13,14). Prolonged work at a high intensity reduces the available energy stores and thereby limits the supply processes (1.5.18.23). Other associated factors limiting endurance effort are hypertharmia and dehydration (10.24,29.30). It w'll thus be clear from the foregoing that assessments of individual er:dJrance capacity from physiological mea~urements is a complex problem and that any simple index for the purpose b :sed on a single parameter like aerobic capacity cannot have general applicability. Recently we observed a high degree of correlation between endurance work and combined cardiorespiratory stresses (26). In one of our earlier study (25). it was observed that endurance time for heavy work was highly related to the aerobic-anaerobic ratio of oxygen supply (27). The present study was undertaken with a view to examining the merits of this alternative approach. MATERIALS AND METHODS Thirteen young healthy subjects of average fitness status were selected for the Mean age. height and weight of the subjects were 23.8 years. 166.6 cm. and 56.3 kg respectively their mean VO, max was 2.36 1/min (42.5 mt/kg/min) and mean maximum heart rate, 187.5 beats/min. study. The subjects reported in the laboratory in the morning after a light breakfast and after one hour rest. the resting 02 consumption, pulmonary ventilation and heart rales were noted. The subject was then asked to perform a fixed rate of 800.1000 or 1200 kg/ min work on bicycle ergometer till exhaUSTion which was taken to be the moment when the subject failed to maintain the fixed speed of 60 rpm. Endurance time was noted when the speed dropped to 50 rpm inspite of his besl effort. Different work rates of 800·1200 kg/min were given to the same subject at intervals of 4-5 days to m'lnimize any training effect. During exercise. the subjects were breathing through a Collin's Triple 'J' low - resistance breathing valve. The expired air volumes were collected continuously in large meteorological rubber baloons over a period of 5 minutes through a three-way stopcock. The volume of expired air from each baloon wa!> measured by passing through Koffranyi Michaelis Respirometer and an aliquot sample collected during the process. Expired air samples were analysed for CO: and '0 1 in Scholander Microgas Analyser. Thus the total O~ consumed during the effort was determined (Exercise V01 ). After cessation Vo!-Jmo r-.umbcr n [nflUfarlCe J Caparilll fOf Cominuous Hfofl 171 of exercise, recovery oxygen consumption over the resting level was also estimated for 30 min (recovery VOl). Thus the total aerobic and "anaerobic" 0 1 utilised during the effort were calculated. The studies were conducted indoors with room temperature and relative humidity v':>rying from 20 - 22°C and 50-55 per cent respectively. Motivation of the subject was achieved by creating competitive spirit and seeking their best cooperation. RESULTS In Table I. experimental data on the 13 subjects have been presented which inc'ude end!.Jrance time (T) in minutes. 0 1 consumed (above resting level). during work (Ex V02) and during recovery (Rec V02). total O2 requirement of the work. all expressed in litres at STPD. aerobic (lla) and anaerobic (uz) fraction as well as aerobic/anaerobic ratio ( l!u,) 0) supply. In Fig. 1, log T has been plotted against log (U 1/U2) for all the 31 observations on the 13 subjects (solid circles). The correlation appears to be reasonably linear. but to close inspection of the points indicates a slight departure from linearity. o However, Astrand and Rodahl (4) have reported similar observations on a single subject of athletic type (V02 max 5.01/min) with endurance time varying from 1 to 120 min. These data are represented in Table II and the 7 corresponding points (open circles) plDlted in Fig. 1 which lie Dn a smDoth curve (hand fitted). The curve clearly shDws a slight departure fr)m linearitY. and the 31 pDints from the present study exhibit a very similar trend but mostly lie above the curve. A simple mathematical appro3ch : It is well known that from moderately heavy to very heavy work. the endurance time decreases primarily due tD a decrease in the aerobic fraction (u.) of Oz supply. The anaerobic fractiDn (u\-,-l-uJl increase at the same time. and is likely tD reduce the endurance time independently. If that be the case, the slight nDn-linearity of the curve in Fig. 1 can be easily explained Dn the basis of the folloWing assumptions:(i) Endurance time (T) is determined nDt by the ratiD tions U 1 and ul respectively. (ii) Relative changes in u. and U2 cause thDUgh (n opposite directions. proportional (ul/uz) but by the frac· relAtive changes in T. 172 Ju!v-Sepl~mt>er Sen GUptll et .". 197~ Ind. J. PhyslOI. PharmJc. TABLE I : Aerobic. Anaerobic fraction of O2 utilization 0113 subjects in different endurance tasks. Ex. V0 2 Endu- ranee S"b S. No. R",. V02 (1m" (T) MSS SA 12.0 2 3 80 2.0 DN RD AnaerObic frection 26.08 17 .85 3.60 4.25 5 33 3 71 Aerobicl anaerobic rallO -", (Ul) 1 (ud u,) (ul) 30 33 23.18 7.31 f.86 0 0.77 0.49 0.23 0.51 51 20 066 0.14 6 34.07 80' 0.83 0.17 0.58 4.88 0.72 0.23 0.25 0.48 3.35 " 6 14 3.35 0.96 , 19.0 5 12.0 6 2.0 7 8 11.0 23.17 6.92 6.0 2.0 12.97 , 32 3.84 3.54 10 11 23.0 11.0 44.28 3.84 3.29 48.12 0.92 0.89 0.08 29.91 0.11 '1.50 8.09 12 13 13.0 29.09 5 14 34.23 0.85 0.15 5.67 2.0 4.13 5.26 .39 0.44 0.56 079 14 15 16 23.0 51.36 18.98 3.80 508 56.44 27.51 9.51 0.91 0.69 0.40 o O. 10.11 8.53 5.71 0.31 0.60 223 067 19.61 3.30 5.21 7.70 24 82 11 00 0.79 021 o 70 3.76 o 3D 5" D67 • AS Aerobic frection flJqulfe· min AKG Tote/ 0, 8.0 2.0 44.04 28.27 3.40 25.62 7.16 5.80 4.69 30.09 17.29 7.38 0.42 077 0.75 0.52 14 3.00 , .08 17 10.0 18 2.D 19 8.0 2.D 15.70 299 5 37 18 69 D84 016 358 895 0.40 0.60 42.78 13.10 3.89 3.72 4.13 3.74 46 50 17.73 7.63 D92 0.76 0.51 D 08 D24 23 21 D 6.D 20 24 16.0 31 22 " 8.0 2 0 16.14 3.79 3 47 6 28 394 34.69 22.42 27 120 2.0 29.66 367 33.33 28 , D' 3.44 748 089 064 0.46 809 1 17 DB 29 31 D 59.61 313 62 74 D95 D 05 1900 BB 30 31 19 0 10 S 35 15 24.09 306 3.92 38 21 28.01 092 0.08 0.86 o 11 50 6.14 NR PC 2D VP 21 22 JS 26 8R 773 0.90 0.72 0.49 0.49 0.10 D28 DOl D 11 14 D43 11.50 3.17 1.04 '00 257 0.96 Volume 2J N'JIT:b"r 3 Enduflnre Cftpaclty IOf Continuous EHoH 173 Assumption (ii) may be mathematical.y put in the form : - aT = T ~ kl k ~ _ LI • .... (1) u. where k l and k! are positive constrtnts. Integration of eqn (1) finally leads to T = A (ulkl/Ulk2) (2) It may be noted that in the special case when k, = kz = k. eqn (2) reduces to T = A (UdU2)k (3) in which case alone. fog T will be linearly related to log (aerobic/anaerobic ratio). It may be concluded. therfore, that the non-linearitY of the curve in Fig. 1 is because k1 /k.:;t.1. Statistical analysis From eqn (2) we have .... (4) log T = Log A+k j log Ut-"2 log U1 which is of the form : + b, Xl where Y=log T. XI = Y= a ..J,.. b. Xl log v" ••.. X2 = log uz. a = log A. (5) b I = k 1 b. =-kl . Eqn (5) was fitted to the data of Table 11 by the method of least squares and the values obtained for the constants were : a = 0.3971. b, = 1.1087 and b 1 =-0.7631 .... (6) which were found to be highly significant (P <0.001). The standard error of the estimate was 0.0268. The coefficient of correlation (r) between observed and estimated log T was 0,9996 indicating almost a perfect linear relationship. Similar analysis was performed with the present data on Indian subjects (Table I). It was found that the constant b. and b2 do not change significantly while the constant 'a' differs significantly (P<O.05) from that in (6) being equal to 0.5184. The coefficient of correlation (r) between observed and estimated log T for this set of data was 0.9640. The equations fitting the two sets of data noted above are : - T =- 3.3C (U I 1.1087 07631 /Vz (Table; I and 11) with the constants .... (7) 174 Ju :y-SeptlJmber 1979 Ind. J. Physio!. Pharmac. Sen Gupta et al. (Present data on 13 Indian Subjects) and T = 2.50 (u 1 ...... (8) !.!OS7/U2 °'7 631 ) (Data of Astrand and Rodahl (4) on one subject) 2·2 2·0 z- ~ r 1· 8 .: 1· 6 w 1." ~ 1· 2 • ~ •• 1·0 UJ U Z LEGEND 0·8 <[ - cr -' 0·6 C1 Z UJ • DATA FROM ASTRAND to ROOtlHAL 0 I 0·' en 0 1970 J 0·2 ~ o.0_ ~....L.....---L._.l.....----L...----L_..L.---'-----JL-...L.....-..L._.l.....--'----L.--L 1·6 Fig PRESENT DATA ,~ 0·0 0·2 0·1. 0·6 0·8 1·0 1·2 H. 1·6 1·8 2·C 2·2 2·/. L09 (AEROBIC/ ANAEROelC ) RATIO Relationship between p.nduranrc time <>n:l 3crobir.-anaJrobi:: ril';O of oxygen 1 • ~uppl'l. TABLE II : Aerobic. anaerobiC fraclIon of 02 utilization of one subject in different endurance tasks (Data from Astrand and Rodahl. 1970) S. IVa. Endurance time (T) Rec. V0 2 Total O2 requiremcnt Aerobic fraction min 2 3 4 120 60 30 10 5 4 6 7 2 1 1 (L I) 480 260 140 50 20 3 4 6 7 9 4 9 !) 8 483 264 146 57 29 18 12 ° 994 0.985 o 959 0877 o 690 0.500 o 333 Anaerobic fraction (L1 2 ) 0.006 0.015 0.041 0.123 0.310 0.500 0.667 Aerobic I anaerobic ratio (u l /Ll2) 166 65.7 23.4 713 2 23 1.00 0.50 EndLl:.~1CC '.o!umll 21 Num!:'er :3 CJpll~iW for Conlinuo~s rf:mt 1711 Observed and estimated endurance time for both sets of data have been compared in Fig. 2 using respective constants as given in eqns (7) and (8). l~G("O o 6 100 '0 10 PA[~('d 0 ... '7.\ o.. t. 'laO'" '\S'IIAHO AI,!. ROOAHl f I ''0 I , . .. U 50 w ::> z .... lI.NE OF PUFEel CO"RElAIl!lN '0 i ! 10 . , .'" • ~ o ! 10 ~ ;> ,~ 1 I .'" w ~ ~ :l \ '-I 0 , ' I 1 I ... ~If.wt~ (IOU-' rrr'J '>. "lal;6n~hiD. el.-.e n obsprv'!d W", II 'I~!' enc'l;r~nce '0 co II "" .. , . , . 101 IN MI!IIu1£5 limo; ·.il" estim. lEd enduran-:e time. DISCUSSION Limited information is available in the literature on estimation of endurance time for continuous heavy physical effort in terms of work load relative to individual V0 2 max (2.22). Bink (6) and Bon1er(7.8) proposed an expon2ntial equation connecting endurance time and work load which reduces to a linear relationship between log T and work lood. Recently. GIeser and Vogel (12) also derived a similar equation on the basis of data obtained with eight sub/ects of a average fitness both before and after 4 weeks of physical traming. Training has been shown to effect the constants of the equation significantly, despite the fact that work load was expressed re[ati'le to the individual V0 2 m<.Jx which is. by itself. a measure of the degree of training. Sen G\:pt~ et a/. i 76 July·Se!>tember 1919. Ind. J. Phy:.101. f'harmac. Gross-Lordemann and Muller (15) on the other hand. have used the general hyperbolic equation which is equivalent to a linear relationship between log T and log (w rk load). Tornvall (27) also used a similar relationship in his studies on capacity for short and prolonged work. However. he related his results with the maximum work rate that could be sustained for 6 min (Wmax/min) instead of aerobic capacity ('J0 2 max). None of the above two types of relationship have been found to be valid over the entire range of endurance time (1-120 min) covered by the data (Table II) of Astrand an \ Rodahl (4). as may be evident from Fig. 3 (a and b). in which log T has been plotted DATA ON ONE SUIJECT (YO,,.. I "01/"',,, ,AST"ANO&' ROO .... l •••• '1 6 " 2 0·' 0·2 0·) l09f Vol/V02 MAX ) o.() rig. 3: RelalJCnship between log endurance time witll relau'/'l work load llnd log rel:ltivg \/\,or\' 1')3d. against relative work load (V02/V02 max) and its logarithm respectively. Both the curves are resonably linear down to about 6-8 min, corresponding to a relative work load of about 1.2. The graph with respect to log (VO,.IVOl max) actually consists of two linear portions with different slopes. meeting at a point where T is about 6 min. This suggests the existence of two distinct ranges (viz., submaximal and supermaximal) of work load which are satisfied by general hyperbolic equations (15) with different constants. In the lower range (T < 6 min), endurance is primarily limited by anaerobic power which is not adequately reflected in either of the two relationships mentioned above Vclurrc Numtx.r n Fnl'!u'~nce C~pa':l!y for Conllf\1I0'1~ ffinrl 177 3 That aerobic capacity alone is not a reliable index of endurance performance has been well demonstrated by observations all long-distance. and marathon runners (9.10.11). The present approach based on a:robic and anaerobic fractions of O2 supply. has been found to be quite satisfactory in so far as a single equation (No.8) fits the data of • Astrand and Aodahl (4) almJst perfectly over the entire range of T (1-120 min). An equation of th3 same type (No.7) fits the present data reasonably well «(=0.9640). the observed scatter (Fig 2) being mainly due to individual difference among the 13 subjects ard possible errors in 0 1 estimations. particularly for UI > 0.9. The values of Tare, on the average. 32% higher than those reported by Astrand and Rodahl (Fig.1). The I tter data pertain to an athletic subject (Val max= 5.0 1/min). whereas the Indian subjects of the present study are of average fitness (mean VOl max = 2.38 l/min). Any rossible effect of training on the proposed equation can. therefore. be safely ruled out. The unexpected difference in T for the same aerobic fraction of 0 1 supply for the two sets of data (Tables I and II) may be possibly due to superior thermoregulatory mechanism of the heat-acclimatised Indian subjects. However. no definite conclusion in this regard. can be drawn from the • present study. particularly because the data of Astrand and Rodahl pertain to a single individual. In view of the high degree of correlation between observed and estimated log T on the basis of aerobic and anaerobic fraction of O2 supply (r=0.9996 and 0.9640 for the two sets of data). it appears that this index in terms of a single physiological parameter is quite suitable for the assessment of endurance capacity. However. it will be interesting to study the effect of various other factors limiting endurance of this index. Some of these are. initial glycogen level in muscles (1) hyperthermia and dehydration (24,29) and relative distribution of ST fibers (11.13.14). ACKNQI.'VLEDGEMENTS Thanks are due to Sarvashri T. Sampathkumar. N. Srinivasulu, P.B.S. Pillai and B.S. Arora for technical assistance and to the soldiers for their whole hearted cooperation. REFERENCES 1. Ahlbo'g. B., J. BergSlfom. L G. Ekelund. LG_E. Hullman. Muscle glycogen and muscle cleclrolytes during prolonged physical exe.cise. AC/II Physlo/. Scand., 70:129·142. 1967. 2. Ast'and. I. Degree of Slrain ouring building work as /elated to ind,vidual aerobic capacity. Ergonomics. 10 : 293-303.1967. . 3. Astrand. P.O. Expe.imental sludles 01 physical working capacily In retation 10 sex and age. flnDr Munksg:r.ard. Copenh8(JlJn, 1952. 4. ~ASlrand. P.O. and K. Rodlh1. Text Book of Work Physiology. Chap. 9. pp. 303. McGraw Hill Company. New YO'k,1970. 5. BergSI.om. J .. L Hermar'lsen. E. Hultman and B. Sail"'. Diel. musc.le glycogen end physical performance. Acta Physwl. Scand., 71 : 140-150, 1967. 176 Sen r.>UOI~ ": III Ind 6 7. 8. t. 10. 11. 12 13 14. 15 ut 17. 18. 19. 20. 21. 22 23 24. 25. 26. 27. 28. 29. 30. July c;':'l'moo' ~979 J. Ph'l~OI Phll,mlll". 8mk.8 TM phYSIcal WOfkJng C'oiloty in relation to working tIme and age EfJIO'Ionua.': 25·28. 1962 BonjCf. r H AclIJ,t enfNgy elilpendulJfe In 'elation 10 the phVS/c,1 working c:a~rty. E,gotIonIIt:J.. I : 23 31. 1962 8on,et. F H R~lalionlhJO bet_n phy$lc,. WOfk'ng capaciW ,nd ,llowable calorie 'lIpendl!l.I'e. In. Inlel· national ColloqUlfOl Otl MuCIJ'-r Uelci$• •nd T';afniflg Oarmft¥Jt. Germany. t968 CGlul. 0, L Ptl'(1)O'ogy of m.I.lhon rUI'IIMg_J.A.M.A. 22 ; 1024·1028 1972 COltlll.O l. G Ell,nam. G EOdy. Delelmonanls of mar.lhon nJRfIlng success /m z.~, Pfly$IOI.• IS : 249. 254. 1971 COIIIll.O l. H Thomason .nd E Robetls. fradiol'lal utibtlOn of IhtI aerob«; e-OKlly (!wIng dlstanU rut\f'llng M«I SCI Spons.. If : 248 252. 1913. G__• M A and JA Vooet Endurance capaCll)' for prolonotd oaro.. on the ~ ... gomclar J AppI f¥ry1JoL. Jot : 438·442. 1973. Goliruck. P 0 R 8. NmlUong_ C W. fV Sauberg. K.. Piehl and 8 $alUti. [t\lVf'le KIMI)' .nd f.c. compClSIllOrl ,n .uletal ""u~ of UtlUalned.nd trained man. J. AppI, Ph'P6Ol_ U : 312·319. 1972. GoInock. PO. R 8 Armstr(lt'lg.8 SaJIlIl_ CWfV SaubM_ W. L SeI'\'lblOWlctl .nd R J Shephard Effec'lol ual""'G on eRlY""t KtMty.nd t,bet composotlon of human sblotuol mu$de. J. AppI Ph'fJlOl. J4 : 101-111. 1i73 Gloue·lof~. H, .nd E. A. Muhr Ofl EinAwis der lalStung under IfbeItsgeKhwIl'Oogq.t .uf do IfbejlSmamnum ~ den _kangsgrad Mlm tIldtM. .n.. ~.: 454·415. 1131. H__ nsatt. L and 8, Sa/lIn Blood t1ctala concenValJOtl durIng ~. II acu.. e!lPC*"e 10 a1UIua. In: barase.l.ltrtuOa- Ed ROo MaI"gena. pp_ 48-53. E>teerpg Medlet Founda1JOfl. Amttarciam• . . - Yort. london. '96' Holouv. J 0 8fochltmKa1 adaptauon In musda: Effects of exarCtSe on InllOChoIldnal oxyvetl upu,t.e .f'ld 'esp!' ..lory enzyme a<:tr\llty III skrHe"l "",sdt. J. BIOi.. ChenL. Z4.Z : 2218_2282. 1961 Hul1tNon. E PhysIoIoOf<:al teM mulde ~ ,tI man _th sptClalre:lerenct 10 o.ase· Itl Ptl~ of muscu~ lVl.au Amtw. HeMt Anoc:. Monogaph No. 15. 1967 Margana. R atld H T. E~dl. The sourc. of energy ,n 1TlUSC\l1.. work performed III _oble WRO,uons. ~ J Phys«JI.1M : :J41-348.1934 M"g.na. R.• P Chttfltl~.nd F Matlglll. 8alance and b~bC:S of .naeroboe eMfgy I ' " dur.f'g Sllenuous UelON In man J, AppI, PhysKJI. 11 : 623-628_ 1964. MaI"gana. R ~oblc and 'fIMl'ot»c IMfgy SOUtce In mU1aJ1at exerCIse. In barClN.t .lllluM. Ed. R. Mal"o. gatll Exc""l~ M«JIU FauncMlJOII. ~tenJarn. 1961. Michael. E.D.. " E. Hulton.•nd S M. Horvalh. tardio·resplratory ruporlHS dUl'If'g plolOt'lgtd IlIill'Ose. J. AppI. PhI'SKJ/.. 11 : 997-1000.1961. Ptuell. ED R FFA moOlllution durif'g .nd alter prolo~ severe muscular work in m.n. J. Appi. Phys,ol. It : 809-815. 1910. Pugh. l.G C.E.. J.L Corbell and RH. Johnson. Rectal temperatures. weight losses and Swell r.tet In matathon running. J. AIJpI. Phys,oI•• U : 341-352. 1961. R.maswlmy. S S. G l. Oua. J Sen Gupla and G_P. Olm,i. ASSessmenl 01 physical work c.paCtl)' of human belnllS. Proc. 2nd Intflfna/lOlW E,gono'llIc:r Congress. pp. 541-547. 1964. Sen Gupt•. J .. S S. Velm,. N.T. Joseph .nd N.C. Majumdar. A new app.oach lor lhl asSlssment of endurance work Eu,op. J. Appf. Physiol.• U : 83-94. 1914. Tortwall. G. Auusm,nt of phytical capacities. Acta Physiol. SCIlOO.• II Suppl•• 201. 1963. Wyndham. C.H .. C.G. Williams and M. Vonrahden. A physiologiclIl buis of Ihe optimum htvel of the ,nlrgy Iltpendnure. N'(u", 111 : 1210·1212.1962. Wyndham. C.H. and N.B. Strydom. The danger 01 an inadequate wale, intake durlflog maralhon running. S. A/r. Mild. J" . . : 893·896. 1969· Wenlel. H G. Uber die ufllchen der begrenlung der koperlichen daufeltSlUngl'helgkeil du menlchen sond'forack aus setmftenrelcne. AJbeifsm«Jizm-soliel-modlZln--iJrbeits hyg/M. Od. 29. 1969.