2007
DOI: 10.1007/s10492-007-0030-5
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Unilateral dynamic contact of von Kármán plates with singular memory

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Cited by 11 publications
(26 citation statements)
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“…(cf. [1]) hence it satisfies the corresponding requirements and the quadratic forms generated by such defined A , B, E ·, · Q are weakly lower semicontinuous and we are done. We remark that M(u) = b(e 1 m(u) + e 0 m(u)), where m(u) = △u + (1 − ν) 2n 1 n 2 ∂ 12 u − n 2 1 ∂ 22 u − n 2 2 ∂ 11 u .…”
Section: Introduction and Notationmentioning
confidence: 99%
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“…(cf. [1]) hence it satisfies the corresponding requirements and the quadratic forms generated by such defined A , B, E ·, · Q are weakly lower semicontinuous and we are done. We remark that M(u) = b(e 1 m(u) + e 0 m(u)), where m(u) = △u + (1 − ν) 2n 1 n 2 ∂ 12 u − n 2 1 ∂ 22 u − n 2 2 ∂ 11 u .…”
Section: Introduction and Notationmentioning
confidence: 99%
“…And, as well, it is realistic to assume that such a bound cannot be reached. u = Au + Bu − Eu + p(u + g) + f in X on I, D(u) = 0 ∈ Y, u(0) = u 0 ,u(0) = u 1 (1) Here D is a general differential operator of a Dirichlet or somewhat combined type. If X = H 2 (Ω), the space of square integrable functions having the (possibly generalized) first and the second derivatives square integrable as well and A, B are differential operators of the fourth order then D(u) ≡ {D 1 (u), D 2 (u)}, D 1 (u) = u−u 0 for both cases, D 2 (u) = ∂ñ(u−u 0 ) (the outer co-)normal derivative) or D 2 (u) = M(u) a Neumann-type operator, which ensures that after the integration by parts in the space variable in the variational formulation of the problem no additional boundary term occurs.…”
Section: Introduction and Notationmentioning
confidence: 99%
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“…The inner dynamic obstacle problem for a viscoelastic plate with moderately large deflections has been solved in [2]. We deal here with an optimal design problem for a viscoelastic cantilever beam in a dynamic contact on one part of the boundary.…”
Section: Introductionmentioning
confidence: 99%
“…[5], for bodies [7], and for the linear models of plates [6]. The inner obstacle problems for viscoelastic von Kármán plates with a short and a singular long memory have been solved in [1] and [2], respectively. The aim of the present paper is to extend these results to the dynamic full von Kármán system for short memory plates with Signorini conditions for plane displacements on the boundary.…”
Section: Introduction and Notationmentioning
confidence: 99%