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A HYBRID PSEUDO-FORCE/LAPLACE TRANSFORM METHOD FOR NON-LINEAR TRANSIENT RESPONSE OF A SUSPENDED CABLE

โœ Scribed by Y.Q. NI; W.J. LOU; J.M. KO


Publisher
Elsevier Science
Year
2000
Tongue
English
Weight
512 KB
Volume
238
Category
Article
ISSN
0022-460X

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โœฆ Synopsis


A hybrid numerical scheme involving the combination of the Laplace transform technique and the pseudo-force method is proposed to analyze the non-linear transient response of a suspended cable subjected to arbitrary dynamic loading. A theoretical model of the cable with multi-degree-of-freedom is "rst obtained through discretization of the partial di!erential equations by "nite di!erence approximation. The non-linear governing equations take into account the e!ects of quadratic and cubic geometric non-linearities. The proposed method deals with the non-linear e!ects as pseudo-forces and then establishes an iterative solution scheme in the alternating Laplace/time domain by means of fast numerical Laplace transform. This method eschews a time-stepping process and therefore is computationally e$cient. It also readily deals with the viscoelastic damping with frequency-dependent model parameters and the hysteresis damping in terms of complex sti!ness models. Numerical examples are presented to evaluate the dynamic responses of suspended cables under a concentrated sinusoidal force and a distributed random excitation, and to identify the non-linear response properties by comparison with the linear vibration. The validity and accuracy of the proposed method is also veri"ed by comparing the results with those obtained by using the direct time integration. 2000 Academic Press

* *x ยน *v *x #EA dy dx # *v *x *u *x # dy dx *v *x # 1 2 *v *x #f (x, t)!c W *v *t "m *v *t . (4b)


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COMMENT ON โ€œNON-LINEAR VIBRATION ANALYSI
โœ A.Y.T. LEUNG ๐Ÿ“‚ Article ๐Ÿ“… 2000 ๐Ÿ› Elsevier Science ๐ŸŒ English โš– 53 KB

The authors of reference [1] solved the Laplace transformed equation ( 20) below by three consecutive similarity transformations to make the symmetric square matrices M, C and K diagonal for the inverse Laplace transform. The "rst transformation is