Page 233 - Thomson, William Tyrrell-Theory of Vibration with Applications-Taylor _ Francis (2010)
P. 233

220                                      Lagrange’s Equation   Chap. 7

                                                             ----- Q 2
                                                              I
                                            0 ^ >             *2
                                                                     - y i h
                                                                           ZET            ^EI^
                                                                                           _^ q
                                                                                           *2
                                                                            io  ^3         I  ^





                                         Figure 7.3-4.  (d).  Forces  necessary  to maintain equilibrium.



                                       For ^3
                                                             0  0    0    ^0 ^

                                                                   -2 El 2
                                                     M,      0   0         0
                                                                     h    <
                                                                    AEI,
                                                     M2      0   0         ^3
                                                                   ~t t
                                                                          1 i

                                       The  stiffness  matrix  for  the  system  is  the  superposition  of these  three  results:
                                             /   \   12£/i       6£/i            (  \
                                                                             0
                                                                  /f
                                                      6EI.   i AEE   4EE    2 EE
                                              M, )  =
                                                            h r " - i T
                                                                 2 El 2    4EE
                                              M,       0                          ^3
                                                                 ~E~       ~E~
                                                                                 I  )
                                       The  mass matrix is found  from the kinetic energy:

                                                     T =  l{>^\  + "»z)«/?  +

                                                  d  d T    ,

                                                  d  d T
                                                  dt  dq.  “ ■'''^2

                                                  d  d T
                                                  dt  d q ,
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