Page 289 - Wind Energy Handbook
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BLADE DYNAMIC RESPONSE                                                 263


             of strain, i.e., as an additional moment which results in an additional lateral load.
             Equation (5.62) can thus be written

                                                 2
                                                                  2
                                  @ 2       @   @ x     @ 2      @ x
                              x
                          c
                   m(r)€ x þ ^ c a (r) _ x þ  a 1 EI(r)  þ  EI(r)    ¼ q(r, t)    (5:79)
                      x
                                 @r 2       @t @r 2     @r 2     @r 2
                    c
             where ^ c a (r) is the aerodynamic damping per unit length, and a 1 is a constant
                                                                           P
             defining the magnitude of the structural damping. Inserting x(t, r) ¼  1  f
                                                                             j¼1 j (t)ì j (r)
             as before, and using Equation (5.65), the structural damping term becomes
             P
               1         2    _
                              f
                  a
               J¼1 1 m(r)ø ì j (r) f j (t). Thus the structural damping per unit length for the jth
                         j
                            2
             mode is a 1 m(r)ø ì j (r), and therefore varies as the mass per unit length as assumed
                            j
             in the Section 5.8.1. Continuing with the same procedure as in the Section 5.8.1, a
             modified modal response equation is obtained as follows
                                                              ð
                                                               R
                          €
                                           2 _
                                                       2
                                             f
                          f
                        m i f i (t) þfc ai þ a 1 m i ø gf i (t) þ m i ø f i (t) ¼  ì i (r) p(r, t)dr  (5:80)
                                           i
                                                       i
                                                               0
             Thus the structural damping ratio for the ith mode, defined as î si ¼
                             2
             c si =2m i ø i ¼ a 1 m i ø =2m i ø i , becomes î si ¼ a 1 ø i =2, i.e., it increases in proportion to
                             i
             the modal frequency. Values for the structural damping logarithmic decrement,
             ä s ¼ 2ðî s at the fundamental natural (i.e., first mode) frequency are given in DS 472
             for several different materials, and these are reproduced in Table 5.4 below. Similar
             values are given in Eurocode 1 for welded steel and concrete. Note that the first
             mode structural damping ratio for a fibreglass blade is much smaller than the
             aerodynamic damping ratio for Blade TR derived above.
               It is instructive to evaluate the combined damping ratio for the first and second
             flapwise modes of Blade TR. These are presented in Table 5.5.
                       Table 5.4  Values of First Mode Structural Damping Logarithmic
                       Decrements for Different Materials
                       Material      Logarithmic decrement,  Structural damping
                                              ä s               ratio, î s
                       Concrete              0.05                0.008
                       Steel – welded        0.02                0.003
                       Steel – bolted        0.05                0.008
                       GRP                   0.05                0.008
                       Timber                0.05                0.008
                     Table 5.5  Comparison of Blade TR Damping Ratios for First Two Modes
                                                                  First mode  Second mode
             Natural frequency including effect of centrifugal stiffening  1.78 Hz  5.88 Hz
             Aerodynamic damping ratio                              0.16      0.04
             Structural damping ratio (proportional to frequency)  0.008      0.03
             Combined damping ratio                                 0.17      0.07
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