Page 238 - Thomson, William Tyrrell-Theory of Vibration with Applications-Taylor _ Francis (2010)
P. 238

Sec. 7.5   Assumed Mode Summation                             225

                               where the generalized stiffness is

                                                           =  ¡AE<pWjdx                    (7.5-8)

                               Example 7.5-1
                                   Determine  the  equation of motion  and the natural  frequencies and  normal  modes of
                                   a fixed-free uniform rod of Fig. 7.5-1 using assumed modes (p^ix) = x/l and  iP2ix)  =
                                   {x/lY.
                                       The equation for the  displacement of the  rod  is

                                                    u{x,t)  = <p,(Ar)i7,(0  + <P2(-i)i2(0

                                                                       Qi
                                   Note that the assumed modes chosen satisfy the only geometric boundary condition of
                                   the  problem,  which  is  w(0, t) = 0.  Thus,  the  generalized  mass  and  the  generalized
                                   stiffness  are evaluated from

                                                        "î/y = j^<Pi(x)<Pj(x)mdx


                                                         kij = jEA(p'i(x)<Pj(x) dx
                                                                                    EA
                                                                     = EAÇ j   •  j  dx
                                                                                  ~  1
                                                                                   2x  ,   EA
                                             2,  = m /J (y )  dx =  jml  ^12 ~ ^21  ^   /  T ^ d x =   —
                                              rl( X     1  ,       ,   ^  riAx^  ,  AEA
                                             /o ( l )   ^ ^ = 5 ^ ^  ki2 = EAl  '    dx =   31
                                                                          •0 1
                                   which can be assembled into the following matrices:
                                                           1  1  ■
                                                           3  4            1   1  '
                                                    M = ml  1  1
                                                           4  5
                                   The equation of motion for the normal mode vibration  then becomes
                                                        1  j_      1   1
                                                   o^ml  3  I   4 I  EA
                                                        4   5





                                                                      Figure 7.5-1.
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