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0593_C13_fm  Page 466  Monday, May 6, 2002  3:21 PM





                       466                                                 Dynamics of Mechanical Systems


                       where as before T is the period. Solving Eq. (13.11.20) for T we obtain:


                                                   T = 2π l  g 1 −  A ( [  2  16 )]          (13.10.21)
                                                                    0
                       For a measure of the accuracy of the approximation, consider again the example of the
                       foregoing section where the pendulum is displaced through 60° and released from rest.
                       Then, A  is π/3, and T becomes:
                              0
                                                           [ {  2  ]}
                                                            π
                                            T = 2π l  g  1 − ( ) 3  16  = 6 7455 l  g        (13.10.22)
                                                                        .
                       Recall that for the linearized equation we obtained (see Eq. (13.3.18)):


                                                   T = 2π l  g = 6 2832 l  g                 (13.10.23)
                                                                .
                       Recall also that the “exact” solution, obtained with elliptic integrals, is (see Eq. (13.9.24)):


                                                        T = 6 7432 l  g                      (13.10.24)
                                                            .






                       13.11 Closure
                       Vibration analysis is based primarily upon the solution of differential equations; therefore,
                       vibration analyses are largely dependent upon available methods for solving differential
                       equations. This means that most analyses are confined to systems that can be modeled by
                       linear equations. Linear models, however, may fail to adequately represent a mechanical
                       system if displacements are large or if damping is not proportional to the velocity. Thus,
                       most vibration analyses ultimately involve approximate numerical and experimental pro-
                       cedures. Research in vibration is ongoing, with an emphasis upon experimental techniques
                       for determining natural frequencies, mode shapes, and damping characteristics. In the
                       following chapter, we will use some of our fundamental results in examining stability of
                       mechanical systems.




                       References

                       13.1. Meirovitch, L., Elements of Vibration Analysis, McGraw-Hill, New York, 1975.
                       13.2. Newland, D. E., Mechanical Vibration Analysis and Computation, Wiley, New York, 1989.
                       13.3. Thompson, W. T., Theory of Vibration with Application, Prentice Hall, Englewood Cliffs, NJ, 1988.
                       13.4. Tse, F. S., Morse, I. E., and Hinkle, R. T., Mechanical Vibration Theory and Applications, Allyn &
                           Bacon, Boston, MA, 1978.
                       13.5. Steidel, R. F., An Introduction to Mechanical Vibration, Wiley, New York, 1989.
                       13.6. Weaver, W., Timoshenko, S. P., and Young, D. H., Vibration Problems in Engineering, John Wiley
                           & Sons, New York, 1990.
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