Page 48 - Thomson, William Tyrrell-Theory of Vibration with Applications-Taylor _ Francis (2010)
P. 48

Sec. 2.8   Coulomb Damping                                      35


                              Solution:  The  amplitude ratio for any two consecutive  amplitudes is
                                                   Xi   X2   ^3
                                  The  ratio   can be written  as
                                               Í! -(Í7)(S)(Íí)
                                  from which the  required  equation  is obtained as
                                                            8 - i l n S
                                                                n   x^
                                      To  determine  the  number  of  cycles  elapsed  for  a  50-percent  reduction  in
                                  amplitude, we obtain the following relation from the preceding equation:

                                                       _
                                                                       0.693
                                                          .  ^
                                                                1  ,  .
                                                       b =  l i r i  =  — In 2 =  --------
                                                             ^   n      n
                                                         =  0 ^   = 0.110
                                                            277
                                  The last equation  is that of a rectangular hyperbola and is plotted in  Fig. 2.7-3.





















                                                                     Figure 2.7-3.
                       2.8  COULOMB DAMPING

                              Coulomb damping results from the sliding of two dry surfaces. The damping force
                              is equal to the product of the normal force and the coefficient of friction  fx  and is
                              assumed  to  be  independent  of the velocity,  once  the  motion  is  initiated.  Because
                              the  sign  of  the  damping  force  is  always  opposite  to  that  of  the  velocity,  the
                              differential  equation  of motion  for  each  sign  is valid  only  for  half-cycle  intervals.
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