Page 174 - Wind Energy Handbook
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148                        AERODYNAMICS OF HORIZONTAL-AXIS WIND TURBINES

                      800            ESBJERG measurements

                     Blade root bending moment (kNm) 750  Equilibrium wake
                                     Dynamic wake
                      700
                      650

                      600
                      550

                      500
                      450
                      400
                      350
                          0                  10                  20                 30                40                  50
                                             Time (seconds)

          Figure 3.76 Measured and Calculated Blade Root Bending Moment Responses to Blade
          Pitch Angle Changes on the Tjæreborg Turbine (from Lindenburg, 1996).


          similar to that of Equation 3.206. The comparison with the measured results clearly
          shows that the dynamic analysis predicts the initial overshoot in bending moment
          whereas the equilibrium wake method does not. Neither theory predicts the steady
          state bending moment achieved betweeen the pitch changes. Figure 3.76 is taken
          from Reference (27) which describes the PHATAS III aero-elastic code developed at
          ECN in the Netherlands. The Tjæreborg turbine is sited near Esbjerg in Denmark,
          details of which can be obtained from Snel and Schepers, 1995.
            The solution procedure requires the time varying blade element force to deter-
          mine the right-hand side of Equation (3.208), but calculating the lift and drag forces
          on a blade element in unsteady flow conditions is not a straight forward process.
          The lift force on a blade element is dependent upon the circulation around the
          element but after a change in conditions the circulation takes time to settle at a new
          level and in the interim the instantaneous lift cannot be determined via the instan-
          taneous angle of attack. In a continuously changing situation the lift is not in phase
          with the angle of attack and does not have a magnitude that can be determined
          using static, two-dimensional aerofoil lift versus angle of attack data.



          3.13.5 Quasi-steady aerofoil aerodynamics

          When the oncoming flow relative to an aerofoil is unsteady the angle of attack is
          continuously changing and so the lift also is changing with time. The simple, but
          incorrect, way of dealing with this problem is to assume that the instantaneous
          angle of attack corresponds to the same lift coefficient as if that angle of attack were
          to be constantly applied. The angle of attack is determined by the oncoming flow
          velocity and the velocity of the blade’s motion. If the blade motion includes a
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