Page 147 - Wind Energy Handbook
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THE AERODYNAMICS OF A WIND TURBINE IN STEADY YAW                       121


             velocity is much greater than the normal velocity but it is the latter which most
             influences the variation in angle of attack at the important, outboard sections of the
             blades, shown in Figure 3.66.
               At the inboard sections of the blades it is the variation in tangential velocity
             which mostly influences the angle of attack variation and this is largely as a result
             of the changing geometry with azimuth angle rather than the effect of induced
             velocity.


             3.10.10  Blade forces for a rotor in steady yaw

             Once the flow induction factors have been determined blade forces can then be
             calculated. Although the flow expansion velocity is excluded from the determina-
             tion of the flow induction factors, on the grounds that the consequent blade forces
             do not cause any change in the momentum of the flow because flow expansion is
             not present in the developed wake, it must be included when the blade forces are
             calculated. The flow expansion velocity should be dependent on an overall average
             value of the axial flow induction factor but it is more convenient to use the annular
             average value as determined by Equations (3.137) and (3.138).
               The flow angle and the angle of attack need to be determined anew at each blade
             element position ì and at each blade azimuth position Ł because the flow expansion
             velocity must now be included, so Equation (3.131) is used in its unmodified form.
             Drag must also be included in the determination of forces even if it was not in the
             calculation of the induced velocities.
               The blade force per unit span normal to the plane of rotation is
                                           d     1    2
                                             F x ¼ rW cC x                       (3:140)
                                          dr     2
             which will vary with the azimuth position of the blade. The total force normal to
             the rotor plane can be obtained by integrating Equation (3.138) along the blade
             length for each of the blades, taking account of their azimuthal separation, and
             summing the results. The total normal force will also vary with rotor azimuth.
               Similarly, the tangential blade force per unit span is



                                   20
                                   15
                                 α
                                   10
                                          ψ
                                   5     180   270
                                      90
                                   0
                                   0
                                     0.2
                                        0.4
                                        r/R  0.6  0.8
                                                    1
                             Figure 3.66  Angle of Attack Variation at 308 of Yaw
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