2015
DOI: 10.1016/j.ijnonlinmec.2015.03.011
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On the non-classical mathematical models of coupled problems of thermo-elasticity for multi-layer shallow shells with initial imperfections

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Cited by 18 publications
(11 citation statements)
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“…In particular, the multi-layer flexible Euler-Bernoulli and Timoshenko beams were investigated in reference [40], whereas multi-layer beams with a clearance have been studied in references [41,42]. Also, the non-classical mathematical models of coupled problems of thermoelasticity were derived and studied for multi-layer shells with initial imperfections in [43]. This paper extends the former investigations.…”
Section: Introductionmentioning
confidence: 76%
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“…In particular, the multi-layer flexible Euler-Bernoulli and Timoshenko beams were investigated in reference [40], whereas multi-layer beams with a clearance have been studied in references [41,42]. Also, the non-classical mathematical models of coupled problems of thermoelasticity were derived and studied for multi-layer shells with initial imperfections in [43]. This paper extends the former investigations.…”
Section: Introductionmentioning
confidence: 76%
“…where: 2 -biharmonic operator, -Laplace operator, ρ-radius of the contour ∂ curvature, ν=const > 0 [43]. By the general solution, one should understand a vector u ε = u 3ε , γ xε , γ yε , F ε ∈ H 2 satisfying the following integral identities:…”
Section: Modification Of the Timoshenko Mm2 And The ε-Regularisation Mm3mentioning
confidence: 99%
“…A generalized solution of problem A is the vector of generalized displacements a = (w1, w2, w3, 1, 2)  Wp (2) (), p  2, which satisfies the system (1) and point wise boundary conditions (2)-( 4) almost everywhere.…”
Section: Definitionmentioning
confidence: 99%
“…The representation for Sd[Φ1] + (t) is found in [22]. For the function Φ'2(z) (z  K ̅ ) from ( 9), using the representation d[g] from (6) and taking into account that ((t+z)/(t-z)) = 2t/(t-z) 2 we have the following:…”
Section: Definitionmentioning
confidence: 99%
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