The non‐linear damping mechanisms are expressed in two general forms: velocity dependent and displacement dependent. The non‐linear damping phenomena are expressed by an array of ‘local constants’, whose value depends upon excitation frequency, excitation amplitude, and type of non‐linearity. Thus, the non‐linear system is replaced by several localized linear systems corresponding to every discrete frequency and amplitude of excitation. Each of the localized linear systems, thus formulated, characterizes the response behaviour of the original non‐linear system, quite accurately in the vicinity of the specific frequency and amplitude of excitation. An algorithm is developed, which expresses the non‐linear damping by an array of ‘local constants’. The algorithm then employs the usual linear design tools to generate the response characteristics almost identical to the response behaviour of the non‐linear system.
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1 January 1986
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Review Article|
January 01 1986
Local equivalent constant representation of non‐linear damping mechanisms
S. Rakheja;
S. Rakheja
Department of Mechanical Engineering, Concordia University, 1455 de Maisonneuve Blvd W, Montreal, Quebec, H3G 1M8, Canada
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S. Sankar
S. Sankar
Department of Mechanical Engineering, Concordia University, 1455 de Maisonneuve Blvd W, Montreal, Quebec, H3G 1M8, Canada
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Publisher: Emerald Publishing
Online ISSN: 1758-7077
Print ISSN: 0264-4401
© MCB UP Limited
1986
Engineering Computations (1986) 3 (1): 11–17.
Citation
Rakheja S, Sankar S (1986), "Local equivalent constant representation of non‐linear damping mechanisms". Engineering Computations, Vol. 3 No. 1 pp. 11–17, doi: https://doi.org/10.1108/eb023636
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