Vertical Axis Wind Turbine Noise

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Presentation transcript:

Vertical Axis Wind Turbine Noise Charlie Pearson Dr. Will Graham Dr. Tamás Bertényi Charlie Pearson 1st year PhD

What is a VAWT? Drag Type Lift Type

Why VAWTs? Ideal for built environment…

Built Environment Application Issues: Turbines are in close proximity to people. Noise is a potentially significant problem Objectives: Identify dominant mechanisms of noise generation. Investigate possible methods for reducing radiated sound. Turbine on your house or your office  noise will be a problem What is the dominant source of noise on a VAWT At the moment the noise mechanisms are very poorly understood No detailed experimental measurements have been made. How might we reduce that noise?

How does a lift-type VAWT work? VBlade VRel FLift FTang. V∞ VBlade VRel FLift FTang. Angle of attack, α V∞ VBlade VRel FLift FTang. In order to understand the noise generation we need to first understand how a VAWT produces torque… 1 Angle of attack generated by combination of wind speed and blade speed Produces a tangential force and therefore torque 2 Varies as a function of blade position 3 The magnitude of the variation is dependent on the TSR 4 5 The variation is greater at lower TSR Even at higher TSR the blades are likely to go into stall Key conclusion is that the blade loading is fundamentally unsteady. Key Parameter: Tip Speed Ratio TSR= Blade speed / Wind Speed

Where does noise come from? Kinetic energy is converted into acoustic energy by three mechanisms: By forcing the mass in a fixed region of space to fluctuate, e.g. a loudspeaker in a large baffle. By forcing the momentum in a fixed region of space to fluctuate, e.g. a solid object vibrating after being struck. By forcing the rates of momentum flux across fixed surfaces to vary, e.g. turbulent jet. In order to understand why unsteady loads are important we need to look at how noise is generated… Forcing the mass to fluctuate: Loudspeaker in baffle, pulsating sphere Momentum fluctuation: Vibrating solid object, oscillating sphere Momentum flux fluctuation: turbulent fluctuations These are in order of strength (high to low) for low Mach number flows. VAWTs operate at low Mach Definitions from MJ Lighthill, 1952, On Sound Generated Aerodynamically, Proc. R. Soc. Lond. A, Vol.267, 147-182 Jet noise image from: http://cms.tacc.utexas.edu/news/feature-stories/2011/reducing-jet-noise-by-controlling-turbulence/

Where does VAWT noise come from? Dipole noise due to fluctuating blade loads dominates at low Mach number. Need to know the blade loads in order to determine the noise analytically. This presents some significant problems… Now the situation is becoming clearer… Unsteady loads drive the sound field If we know the blade loads then we can determine the sound field How do we go about calculating the sound field? It is pretty tricky

CFD Modeling? Flow is fundamentally unsteady Flow is 3D Flow is turbulent and has a wide range of length and time scales Flow is VERY complicated! Difficult to determine the most significant noise sources. First attempt might be to try CFD… As we have seen the flow is: Unsteady Effect of blade tips make the flow very 3D in nature To resolve all acoustic wavelengths we need to have high resolution on the blades – TIME AND SPACE Flow is complex! Unless we can perform very high fidelity simulations we are not likely to get an accurate picture of the sound field. Image from Scheurich, Fletcher and Brown, (2010), The influence of Blade Curvature and Helical Blade Twist on the Performance of a Vertical Axis Wind Turbine, 48th AIAA Aerospace Sciences Meeting, Orlando, USA

An alternative approach... Use analytic acoustic model for moving point source. Guess the blade loads Sinusoidal variation with azimuth? Blade/wake interactions? Dynamic Stall? Predict the resulting sound field Far field: Near field: MV Lowson, (1965), The Sound Field for Singularities in Motion, Proc. R. Soc. A, Vol.286, 559-572 Use moving singularity model developed by Lowson. Keeps the key components while avoiding unnecessary complication Key component is the fluctuating force component in the far field term Set up the rotor geometry and the observer location Guess the blade loads 4. Identify key characteristics of sound field for comparison with experimental data.

Loading Profiles Tested Define normal and tangential blade loads as a function of azimuth: Constant Load Sine Wave Blade Vortex Interaction Zero wind load Constant drag load Loads you would get if there were no blade/wake effects. Load due to the blade passing close to a coherent vortex. Constant load: Good for calibration Sinusoidal load: Sort of loading you would get if there were no wake interactions Good representation of the upstream half of the rotor BVI load: Loading profile is dependent on the strength of the vortex and the blade/vortex separation Strongly directional sound field

Experiments Use acoustic array in Markham wind tunnel to locate dominant noise sources. Investigate parameters for noise reduction Blade tip shape Spoke geometry Variable radius Blade sweep / helical blades Measure the sound field using the acoustic array in the Markham tunnel. Based on results of initial measurements, investigate some design parameters to see if the noise can be reduced. Blade tips: change structure of the rotor wake Spoke geometry: cylindrical / aerofoil Radius: Impact on tip vortices Helix: Twist spreads load around rotor, smoother loading?

3 Straight blades Motor driven so we can control the speed more accurately Measure the unsteady torque on the shaft. Measure the sound field using the acoustic array

Array Measurements Sijtsma, P (2004), Experimental techniques for identification and characterisation of noise sources, National Aerospace Laboratory NLR Report, NLR-TP-2004-165 Use phase relationship between signal received at multiple microphones. Acoustic array consists of multiple microphones which simultaneously record the sound from an object. By comparing the signals at each microphone it is possible to estimate the source location. We want to attempt to do for VAWTs what Peter Sijtsma has done for HAWTs. Sijtsma, P, Oerlermans, S and Holthusen, H (2001), Location of Rotating Sources by Phased Array Measurements, NLR-TP-2001-135

Plan of action Measure sound field in the wind tunnel using acoustic array. Compare results with computer model predictions. Investigate dominant noise sources in detail. Inform the design of quieter VAWTs Questions?