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THE AERODYNAMICS OF A WIND TURBINE IN STEADY YAW                        97



                                                       z


                                              y


                                                                   x




                                       γ
                                       U











                          Figure 3.46  A Wind Turbine Yawed to the Wind Direction

             which is a pressure force and so normal to the disc, is responsible for the rate of
             change of momentum of the flow then the average induced velocity must also be in
             a direction at right angles to the disc plane, i.e., in the axial direction. The wake is
             therefore deflected to one side because a component of the induced velocity is at
             right angles to the wind direction. As in the non-yawed case the average induced
             velocity at the disc is half that in the wake.
               Let the rotor axis be held at an angle of yaw ª to the steady wind direction
             (Figure 3.47) then, assuming that the rate of change of momentum in the axial

                              F= ρ  A   U  (cos(  γ – α) 2 a U
                                   p D    γ



                                          γ
                            U                 F

                                                                 γ
                                aU
                                                             2aU






                     Figure 3.47  Deflected Wake of a Yawed Turbine and Induced Velocities
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