Page 240 - Thomson, William Tyrrell-Theory of Vibration with Applications-Taylor _ Francis (2010)
P. 240

Sec. 7.5   Assumed Mode Summation                              227

                                  Generalized Stiffness (Beams)
                              Determine  the  generalized  stiffness  for  a  beam  of  cross-sectional  property  El
                              when the displacement  y{x,t) is represented by the sum

                                                                                          (7.5-9)
                                                             /-I
                                  The potential  energy of a beam  in bending is

                                                                                         (7.5-10)
                              Substituting for
                                                      d^y
                                                      dx^   / = 1
                              we obtain
                                                    u  =  jLL<li^jjEl<pW;dx


                                                        2    ^ijQiQj                     (7.5-11)
                              and the generalized stiffness is

                                                        k ,j  =   f  E i< p y ’  dx      (7.5-12)

                              Example 7.5-2 Generalized Force
                                  The frame of Fig. 7.1-3 with rigid members is acted upon by the forces and moments
                                  shown in  Fig. 7.5-2.  Determine the generalized forces.
                              Solution:  We let   be the virtual displacement of the upper left corner and  8q2  be  the
                                   translation of the right support hinge.  Due to  8q^,  the virtual work done  is

                                                2,5^1  =F|5^1  -  F2jdqj  +  (Ml  -  M2)jSq^
                                                               /

                                                 ■■■Qx  =  E >    /  |(M ,  -M ^)
   235   236   237   238   239   240   241   242   243   244   245