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0593_C13_fm  Page 453  Monday, May 6, 2002  3:21 PM





                       Introduction to Vibrations                                                  453


                       or

                                 [ −ω 2  + ( 2 km )] [ {  −ω  2  + ( 2 km )] (km ) 2 } −(km ) −ω  2  + ( 2 km )]  = 0  (13.7.17)
                                                                          [
                                                          2
                                                                          2
                                                           −
                        Solving for ω  we obtain:
                                    2
                                       ω = (          )  ω =       )  ω = (          )
                                        2
                                                                        2
                                                           2
                                                2
                                                                               2
                                        1   2 − )(km ,     2  2(km ,    3  2 + )(km           (13.7.18)
                        Observe that instead of obtaining one solution we have three solutions. That is, there
                       are three positive frequencies (three natural frequencies) that make the determinant of Eq.
                       (13.7.16) equal to zero and thus allow a nonzero solution of Eqs. (13.7.13), (13.7.14), and
                       (13.7.15) to occur. This in turn means that we can expect to find three sets of amplitudes
                       solving Eqs. (13.7.13), (13.7.14), and (13.7.15), one set for each frequency ω  (i = 1, 2, 3).
                                                                                         i
                        To find these amplitude solutions, we can select one of the ω  (say, the smallest of the
                                                                                i
                       ω ), substitute it into Eqs. (13.7.13) to (13.7.15), and thus solve for the amplitudes A  (i =
                                                                                                  i
                        i
                       1, 2, 3). We can then repeat the process for the other two values of ω . Notice, however,
                                                                                     i
                       that although there are three equations for the three amplitudes, the equations are not
                       independent in view of Eq. (13.7.16). That is, there are at most two independent equations,
                       thus we need another equation to obtain a unique solution for the amplitudes. Such an
                       equation can be obtained by arbitrarily specifying the magnitude of one or more of the
                       amplitudes. For example, we could “normalize” the amplitudes such that
                                                       A + A + A =  1                         (13.7.19)
                                                        2
                                                                 2
                                                            2
                                                        1   2   3
                       Then, Eqs. (13.7.13), (13.7.14), (13.7.15), and (13.7.19) are equivalent to an independent set
                       of three equations, enabling us to determine unique values of the amplitudes.
                        To this end, let us select the smallest of the ω  (ω ) and substitute it (that is, {(2 –  ) 2
                                                                     1
                                                                  i
                       (k/m)} 1/2 ) into Eqs. (13.7.13), (13.7.14), and (13.7.15). This produces the equations:
                                                          2 A − A =  0                        (13.7.20)
                                                            1   2

                                                      −A  + 2  A  − A  = 0                    (13.7.21)
                                                        1      2   3

                                                        −A  + 2  A  = 0                       (13.7.22)
                                                          2      3
                       Observe that these equations are dependent. (If we multiply the first and third equations
                       by  2  and add them we obtain a multiple of the second equation.) Thus, by selecting two
                       (say, the first two) of these equations and by combining them with Eq. (13.7.19), we obtain
                       upon solving the expressions:

                                                 A =  12 ,  A =  2 2 ,  A =  12               (13.7.23)
                                                  1        2           3
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