Dynamically Variable Blade Geometry for Wind Energy Greg Meess, Michael Ross Dr. Ephrahim Garcia Laboratory for Intelligent Machine Systems AIAA Regional Student Conference Boston University April 23-24, 2010
Goal: Increase wind turbine energy output by morphing blade shape to match changing wind speeds. Pitch Chord Twist
Outline Motivation Experimental Design Airfoil Generation Simulation Optimization Results Geometry Power output
Motivation Wind turbines are constantly increasing in size Power output is proportional to rotor swept area The largest turbines cannot be built on land Blades are designed for higher wind speeds Maximize rated power Turbine spends little time operating at rated power Little focus on low wind speeds Variable Pitch http://www.terramagnetica.com/2009/08/01/why-are-wind-turbines-getting-bigger/
Problem Parameterization Blade Element Momentum (BEM) Theory is used Turbine has operating regime between 4 m/s and 20 m/s 4 m/s is lower limit of current turbines Fixed speed generator of 60 rpm Rotations vary from 30 to 120 rpm. Rayleigh Distribution is used to assess annual power output Chord, twist, and camber are examined Vestas V90 power output vs. wind speed Sample wind speed Rayleigh distribution
Airfoil Generation NACA XX12 Series XFOIL Simulation Leading edge, trailing edge follow NACA equations Flexible panels connect to leading edge, rest on trailing edge As chord extends/retracts, panels keep airfoil profile XFOIL Simulation CL, CD data collected for angles of attack between -10° and 45° NACA 2412 original, fully extended, and fully retracted shapes Sample data from XFOIL for modified shapes
Turbine Performance Analysis Equations based on basic BEM theory1, WT_Perf source code2, and Aerodyn Theory Manual3. Blade divided into a number of elements Power of each element is P= 1/2ρAU34a(1-a) Power Coefficient Cp = 4a(1-a) Axial induction factor defined as a = (U1-U2)/U1 Need initial guess for axial induction factor Axial induction factor calculated using relative wind angle, coefficients of lift and drag, tip loss factor Initial axial induction factor updated Iterate for convergence Calculate power Polyamide Streamtube around wind turbine rotor, used as basis for BEM theory (Manwell 85). Nylon “Kite Wing” 1 Manwell, J.F., et al., Wind Energy Explained, John Wiley & Sons Ltd., 2002. 2 Buhl, Marshall, National Renewable Energy Laboratory, 2004. 3 Laino, David and A. Hansen, User’s Guide to Wind Turbine Aerodynamics Software AeroDyn, Windward Engineering, 2002. Blade geometry for analysis of horizontal axis wind turbine (Manwell 108).
Parametric Study Performance of morphing blades compared to that of a fixed blade Sample blade from WT_Perf optimized across all parameters at wind speed of 10 m/s All morphing blades begin with this shape Each morphing blade changes one parameter Three chord scenarios are examined Extension only Extension and retraction Retraction only Add arrows
Optimization
Variable Pitch Low Speed Shape Morphology Plot 15° High Speed Shape
Variable Camber Add picture Morphology Plot
Annual Output Power Curve Highlight new lines
Variable Chord Low Speed Shape Define retraction factor High Speed Shape Emphasize retraction over others Morphology Surface
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Variable Twist Low Speed Shape Morphology Surface High Speed Shape
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Conclusion Cite “Fair”, “Good”,etc. Percent Improvement over Static Blade wind speed (m/s) retracting chord variable pitch variable twist variable camber Fair (6.7) 18.64% 23.54% 29.26% 21.77% Good (7.25) 15.51% 18.45% 23.71% 17.09% Excellent (7.75) 13.44% 14.98% 20.14% 13.79% Outstanding (8.4) 11.56% 11.60% 16.99% 10.47% Superb (10.45) 9.67% 7.51% 14.22% 6.16% Emphasize improvement over pitch Variable Twist has the most influence on the performance Consistent 5% improvement over current pitch control scheme Achievable using torque tube mechanism Shape distribution close to linear Find V-22 paper or illustration
Future Work
Acknowledgements Find official titles
Questions & Comments? Laboratory for Intelligent Machine Systems Acknowledgements: Professor Sidney Leibovich, Donald Barry