Center for Ocean Renewable Energy, University of New Hampshire
Transcription
Center for Ocean Renewable Energy, University of New Hampshire
Center for Ocean Renewable Energy, University of New Hampshire Alex Johnston ajc32@unh.edu Adviser: Martin Wosnik martin.wosnik@unh.edu Tidal currents are a predictable, renewable source of energy Cross-flow axis hydrokinetic turbines ◦ Favorable turbine geometry for deployment in shallow flows (compared to horizontal, in-stream axis turbines) ◦ Can receive flow from any direction Do not have to yaw into flow or pitch blades when tidal current changes directions Reduces complexity for underwater deployment ◦ Complex and interesting fluid dynamics 2 Straight-bladed (e.g. Darrieus) ◦ Severe lift/torque pulsations Helical blades (e.g. Gorlov) ◦ Reduce lift/torque pulsations ◦ Circumferential overlap of blades ◦ With full overlap, lift/torque is circumferentially averaged (there is always some portion of a blade experiencing maximum lift) ◦ LUCID GHT uses NACA 0020 symmetrical hydrofoil Picture 1 from: http://www.energy-daily.com/reports/PacWind_To_Offer_Three_New_Proprietary_Applications_For_Wind_Energy_999.html Picture 2: Lucid Energy, Gorlov Helical Turbine 1m x 1.25m 3 Geometry and Definitions Free Stream Velocity, U Where, V = radial velocity W = relative wind U = free stream velocity L = lift force D = drag force N = normal force T = tangential force θ = angle of rotation α = angle of attack ω = 2πf http://en.wikipedia.org/wiki/File:Forces_and_velocities.png 4 Tip Speed Ratio R U Relative “wind” (velocity experienced by blade element) W U 1 2 cos 2 Angle of Attack Vector relations derived from geometry and written in terms of the tip speed ratio, λ (for a blade element) sin tan cos 1 5 Relative Velocity (constant Vinf=2m/s) Angle of Attack 8 40 Desired values TSR=1.57 TSR=1.83 TSR=2.09 TSR=2.36 TSR=2.62 TSR=2.88 30 20 alpha (rad) λ 7 6 Wrel (m/s) λ 10 TSR=1.57 TSR=1.83 TSR=2.09 TSR=2.35 TSR=2.62 TSR=2.88 theta=180 0 5 4 -10 3 -20 2 -30 -40 0 50 100 150 200 theta (deg) 250 sin cos tan 1 300 350 400 1 0 R TSR: U 50 100 150 200 theta (deg) 250 300 350 400 W U 1 2 cos 2 6 Foil data from Sandia National Laboratories CL and CD values were generated using wind tunnel data and extended using airfoil code XFOIL CL and CD functions of α for a full 360° Data for several values of Reynolds number and different airfoil shapes 7 NACA 0021 (symmetric) foil shape; Reynolds number range: 40,000-5 million Using ◦ The geometrically derived equations for α and W, ◦ CL/CD data, ◦ And equations for lift and drag forces Calculate torque and power as functions of rotation angle for a blade element 8 Breaks up blades into small individual elements Determine forces on each element Forces are integrated over the full length of the blade Performed for all 3 (or any number of) blades Determine torque and power for the entire turbine as a function of rotation angle 9 Necessary because ◦ Free stream velocity and RPM are not coupled in model ◦ no losses accounted for Scale model turbine specifications: ◦ ◦ ◦ ◦ Diameter = 1m Length = 1.1m Blade chord = 140mm Blade slope angle = 67° Data was collected during push tests of turbine (Lucid) 10 Acquire curve fits from experimental data ◦ RPM vs. Free Stream Velocity ◦ Power predicted by code (no losses) vs. Measured Power Predicted and Measured Power 14.0 12.0 Power (kW) 10.0 Measured 8.0 Power 6.0 Predicted 4.0 Power 2.0 1.5 2.5 3.5 4.5 5.5 Free Stream Velocity (m/s) 11 General Sullivan Bridge in the Great Bay Estuary, NH: good test site, strong tidal currents (up to ~ 2.5 m/s, typically >2 m/s during each tidal cycle) Data acquired by Carl Kammerer (UNH) using a bottom deployed ADCP (Acoustic Doppler Current Profiler) Tidal Energy Test Site (under bridge) Newington N Dover ocean 12 Power Output and Free Stream Velocity over Time Power Output and Free Stream Velocity over Time 1.5 1 1 0.5 0.5 0 2 4 6 8 Time (hours) 10 12 14 0 Power (kW) 1.5 2.5 2 2 Free Stream Velocity (m/s) Power (kW) 2 0 2.5 2.5 2 1.5 1.5 1 1 0.5 0 Free Stream Velocity (m/s) 2.5 0.5 0 100 200 300 400 500 Time (hours) 600 700 0 800 Prediction for 30 days (full lunar cycle) for a 1.1m2 Lucid Energy GHT (turbine diameter D=1m, height L=1.1m): Energy = 653.1 kWh Average Power: ~ 0.9 kW Note: average monthly electric energy consumption per household in New Hampshire is 616 kWh (DOE EIA, 2008) 13 Cross-flow axis turbine blades have large angle of attack variations as blades rotate Flow separates (hydrofoil stalls) for certain AoA ranges during rotation Large increase in drag on hydrofoil results in: ◦ large lift/torque variations as blades rotate ◦ decrease performance If stall avoided, hydrodynamic performance is maximized 14 ~ 0° AoA: no lift, small drag (for symmetric airfoil sections) ~ 5°-15° AoA: lift>drag ~ 15°+ AoA: lift<drag NOTE: AoA ranges are a function of Reynolds number and airfoil thickness Picture from: http://www.aviation-history.com/theory/angle_of_attack.htm 15 Lift/Drag Ratio vs. AoA 50 CL/CD 40 30 20 10 0 0 5 10 15 Angle of Attack 20 25 For low AoA lift increases with AoA, while drag does not vary much Once flow is separated, large increase in drag while large decrease in lift Separation point depends on foil shape and Reynolds number NACA0021, Re=360,000 16 NACA0021 Torque (1 blade) NACA0021 Torque (3 blades) 600 1200 TSR=1.5708 TSR=1.8326 TSR=2.0944 TSR=2.3562 TSR=2.618 TSR=2.8798 500 1000 800 300 T (Nm) T (Nm) 400 200 600 400 100 200 0 0 -100 0 50 100 150 200 theta (deg) 250 300 350 TSR=1.5708 TSR=1.8326 TSR=2.0944 TSR=2.3562 TSR=2.618 TSR=2.8798 400 -200 0 50 100 150 200 theta (deg) 250 300 350 400 Regions of stall = poor performance/large variations in torque Define “Critical Tip Speed Ratio” (λcrit) ◦ λ above which turbine torque no longer becomes negative during rotation (except at AoA = 0, 180, where there is no lift) 17 NACA0021 Torque (1 blade) NACA0021 Torque (3 blades) 700 1400 TSR=2.3562 TSR=2.618 TSR=2.8798 TSR=3.1416 TSR=3.4034 TSR=3.6652 600 500 TSR=2.3562 TSR=2.618 TSR=2.8798 TSR=3.1416 TSR=3.4034 TSR=3.6652 1200 1000 T (Nm) T (Nm) 400 300 800 600 200 400 100 200 0 -100 0 50 100 150 200 theta (deg) 250 300 350 400 0 0 50 100 150 200 theta (deg) 250 300 350 400 Stall avoided when TSR high enough Define “Optimum Tip Speed Ratio” (λopt) ◦ Where λ is sufficiently high to keep AoA below stall angle throughout turbine rotation 18 Angle of Attack (AoA) throughout rotation Angle with varying TSR of Attack (constant Vinf=2m/s) 25 Desired values TSR=2.35 TSR=2.62 TSR=2.88 TSR=3.14 TSR=3.40 TSR=3.67 theta=180 20 15 10 alpha (rad) 5 0 -5 -10 -15 -20 -25 50 100 150 200 250 theta (deg) 300 sin cos tan 1 350 400 Define range of desired values based on stall angle for a specific Reynolds number The TSR at which the derived function for angle of attack stays within the desired range is the optimal TSR (λopt) Values of λcrit and λopt are turbine-specific. For a D=1m, 67° sweep angle GHT the blade element model predicts: crit 2.24 opt 3.60 19 TSR v Vinf for No load and Peak Power TSR; Crit. and Opt. TSR 4 3.8 opt 3.60 3.6 Tip Speed Ratio 3.4 3.2 3 No Load TSR Peak Power TSR Critical TSR Optimal TSR 2.8 2.6 2.4 UNH model crit 2.24 2.2 2 0.6 Explanation for decrease in TSR: due to increase in drag on support struts? 0.7 0.8 0.9 1 1.1 1.2 Free Stream Velocity 1.3 1.4 1.5 Data from full scale LUCID turbine site testing in Amesbury, MA in the Merrimack River (MTC 2005) ◦ Diameter=1m, sweep angle = 67°, Length = 2.5m 20 The model under development uses derived equations and CL and CD data to predict torque and power curves for cross-flow turbines Model is calibrated using experimental performance data from scale testing for a specific turbine With temporally/spatially varying flow data from a deployment site, power/energy performance can be accurately predicted 21 Stall of the hydrofoil sections during rotation can lead to poor performance of the turbine Two Tip Speed Ratios of interest were defined: ◦ the “critical tip speed ratio”, λcrit , for desirable performance (torque remains positive during stall) ◦ the “optimum tip speed ratio” , λopt, for which performance is maximized (dynamic stall avoided) Working hypotheses: ◦ It appears that a turbine under no-load conditions (“freewheeling”) will try to rotate (“settle”) near λopt Hydrodynamic performance optimized Is a “range of AoA-weighted” lift/drag ratio maximized near λopt? (if turbine moves off this operating point, will weighted lift/drag decrease?) ◦ It appears that a turbine will have its maximum power output (peak performance) near λcrit If λ < λcrit, power drops due to regions of negative torque 22 Correlate data gathered from the UNH tow tank for different turbines Predict performances at the GSB test site Compare predictions with prototype deployments Further investigate/validate hypotheses that turbines will rotate at model-predicted critical and optimal tip speed ratios when under noload and at peak power, respectively 23 [1] Sheldahl, R. E. and Klimas, P. C., Aerodynamic Characteristics of Seven Airfoil Sections Through 180 Degrees Angle of Attack for Use in Aerodynamic Analysis of Vertical Axis Wind Turbines, SAND80-2114, March 1981, Sandia National Laboratories, Albuquerque, New Mexico. [2] Gorlov, A.M., Professor of Engineering, Northeastern University. [3] Fox, R.W., Pritchard, P.J., and McDonald, A.T., Introduction to Fluid Mechanics, Seventh Edition. John Wiley & Sons, Inc., 2009. [4] Verdant Power LLC, GCK Technology, Inc. Amesbury Tidal Energy Project: Integration of the Gorlov Helical Turbine into Optimized Hardware/Software System Platform, MTC Final Report. April 2005. [5] Lucid Energy Technologies, LLP, Push Test Data Acquisition for GHT, Vancouver, BC, 2007. [6] Carl Kammerer, NOAA/NOS/CO-OPS and UNH/Joint Hydrographic Center, Tidal TurbinesWith a Twist Currents in the Piscataqua River, NH: Preliminary findings from the 2007 National Current Observation Program Survey. 2008 24 New England Marine Renewable Energy Center (NE-MREC): ◦ Summer scholarship for research development U.S. Department of Transportation (DOT): ◦ Graduate Fellowship through the New England University Transportation Center (NE UTC) Lucid Energy Technologies, LLP ◦ Turbines and Data UNH Department of Mechanical Engineering 25