2000
DOI: 10.1006/jsvi.2000.3082
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A Hybrid Pseudo-Force/Laplace Transform Method for Non-Linear Transient Response of a Suspended Cable

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Cited by 20 publications
(6 citation statements)
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References 34 publications
(28 reference statements)
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“…To avoid some or nearly all of the aforesaid hypotheses, direct computational treatments of the approximate [7,8] or exact [10,11] PDEs of cable motion have recently been accomplished based on a space-time finite difference (FD) procedure confronting the finite-amplitude free vibration problems of sagged and arbitrarily inclined cables with/without internal resonances. In the meantime, several FD-based implementations have been used successfully to deal with a range of problems in nonlinear forced vibrations, including cables subject to random excitation [12], highly-extensible cable mechanics [13], low-tension cables with large displacements [14] or semi-active vibration control strategies [15]. Overall, the robustness, utility and versatility of FD algorithms have been evidenced.…”
Section: Introductionmentioning
confidence: 99%
“…To avoid some or nearly all of the aforesaid hypotheses, direct computational treatments of the approximate [7,8] or exact [10,11] PDEs of cable motion have recently been accomplished based on a space-time finite difference (FD) procedure confronting the finite-amplitude free vibration problems of sagged and arbitrarily inclined cables with/without internal resonances. In the meantime, several FD-based implementations have been used successfully to deal with a range of problems in nonlinear forced vibrations, including cables subject to random excitation [12], highly-extensible cable mechanics [13], low-tension cables with large displacements [14] or semi-active vibration control strategies [15]. Overall, the robustness, utility and versatility of FD algorithms have been evidenced.…”
Section: Introductionmentioning
confidence: 99%
“…e governing differential equations of the tether motion can be derived using the Hamilton principle [24]:…”
Section: Vibration Equationmentioning
confidence: 99%
“…in which δ is the symbol for variation; t 1 and t 2 are the limits of the time interval; L is the unstretched length of tether; and dt is the differential of time. Q is the kinetic energy density [24]:…”
Section: Vibration Equationmentioning
confidence: 99%
“…Since the initiating work of Skutch in 1897, much research has been done to study transverse vibrations of axially moving strings [1] . Recently, due to the increasing of the complexity of the studied problems and nonlinear characteristic of the models, semi-analytic methods and numerical methods have become important research tools, such as multiscale method [2,3] , difference method [4,5] , finite element method [6] , Laplace transformation method [7] , Galerkin method [8][9][10][11][12][13] and so on. For the real-mode Galerkin method, the basis function is essentially required to meet the boundary conditions, and the modal function of linear static strings is usually taken as the basis function in order to improve the convergence of series solution.…”
Section: Introductionmentioning
confidence: 99%