Page 273 - Wind Energy Handbook
P. 273

BLADE LOADS DURING OPERATION                                           247


                  10        Integral length scale, L = 73.5 m
               Rotationally sampled power spectral density function, R(r,n)  (logarithmic scale)  0.1 1  r = 0 m

                             Mean wind speed = 8 m/s
                            Speed of rotation = 30 r.p.m.









                                                       r = 10 m


                 0.01                                  r = 20 m
                  0.001            0.01             0.1             1               10
                                            Frequency, n (Hz, logarithmic scale)
             Figure 5.20  Rotationally Sampled Power Spectra of Longitudinal Wind Speed Fluctuations
             at Different Radii: log–log Plot



             roughly in proportion to the tip speed ratio, Ùr=U, and will thus be most significant
             for fixed-speed two-bladed machines (which generally rotate faster than three-
             bladed ones) in low wind speeds.



             Rotationally sampled cross spectra

             The expressions for the spectra of blade bending moments and shears are normally
             functions of entities known as rotationally sampled cross spectra for pairs of points
             along the blade, which are analogous to the rotationally sampled ordinary spectra
             for single points described above. The cross spectrum for a pair of points at radii r 1
             and r 2 on a rotating blade is thus related to the corresponding cross correlation
             function by the Fourier transform pair
                                              ð
                                               1
                                 o
                                                 o
                                S (r 1 , r 2 , n) ¼ 4  k (r 1 , r 2 , ô) cos 2ðnô dô  (5:46a)
                                 u               u
                                               0
                                             ð
                                              1
                                                o
                                 o
                                k (r 1 , r 2 , ô) ¼  S (r 1 , r 2 , n)cos 2ðnô dn  (5:46b)
                                 u
                                                u
                                             0
             Setting ô ¼ 0 in Equation (5.46b) gives
                                                ð 1
                                                    o
                                     o
                                    k (r 1 , r 2 ,0) ¼  S (r 1 , r 2 , n)dn       (5:47)
                                                    u
                                     u
                                                 0
             which, when substituted into the expression for the standard deviation of the blade
             root bending moment in Equation (5.27) gives
   268   269   270   271   272   273   274   275   276   277   278