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contributor authorD. J. McTavish
contributor authorP. C. Hughes
date accessioned2017-05-08T23:43:08Z
date available2017-05-08T23:43:08Z
date copyrightJanuary, 1993
date issued1993
identifier issn1048-9002
identifier otherJVACEK-28806#103_1.pdf
identifier urihttp://yetl.yabesh.ir/yetl/handle/yetl/112954
description abstractThe GHM Method provides viscoelastic finite elements derived from the commonly used elastic finite elements. Moreover, these GHM elements are used directly and conveniently in second-order structural models jut like their elastic counterparts. The forms of the GHM element matrices preserve the definiteness properties usually associated with finite element matrices—namely, the mass matrix is positive definite, the stiffness matrix is nonnegative definite, and the damping matrix is positive semi-definite. In the Laplace domain, material properties are modeled phenomenologically as a sum of second-order rational functions dubbed mini-oscillator terms. Developed originally as a tool for the analysis of damping in large flexible space structures, the GHM method is applicable to any structure which incorporates viscoelastic materials.
publisherThe American Society of Mechanical Engineers (ASME)
titleModeling of Linear Viscoelastic Space Structures
typeJournal Paper
journal volume115
journal issue1
journal titleJournal of Vibration and Acoustics
identifier doi10.1115/1.2930302
journal fristpage103
journal lastpage110
identifier eissn1528-8927
keywordsSpace frame structures
keywordsModeling
keywordsFinite element analysis
keywordsDamping
keywordsViscoelastic materials
keywordsMaterials properties
keywordsFunctions AND Stiffness
treeJournal of Vibration and Acoustics:;1993:;volume( 115 ):;issue: 001
contenttypeFulltext


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