2020
DOI: 10.1080/01495739.2020.1722771
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Thermoelastic damping in strain gradient microplates according to a generalized theory of thermoelasticity

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Cited by 50 publications
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“…In this case, a specific temperature field and quite specific deformations for the second phase, which are determined by relations ( 22) and ( 16), (18)(19) are realized for the equilibrium structure. Note that, if the coupled parameters tend to zero, then the problems of thermoelasticity and stationary thermal conductivity are completely separated, and their solutions correspond to the gradient equilibrium case or the classical representation if the gradient parameters are equal to zero.…”
Section: Resultsmentioning
confidence: 99%
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“…In this case, a specific temperature field and quite specific deformations for the second phase, which are determined by relations ( 22) and ( 16), (18)(19) are realized for the equilibrium structure. Note that, if the coupled parameters tend to zero, then the problems of thermoelasticity and stationary thermal conductivity are completely separated, and their solutions correspond to the gradient equilibrium case or the classical representation if the gradient parameters are equal to zero.…”
Section: Resultsmentioning
confidence: 99%
“…It should be noted that the one-dimensional analogue of the Eshelby problem [31][32][33], implemented for coupled gradient thermoelasticity, also leads to the algebraic Equation (22), in which the transition matrix connects the stress-strain state of a homogeneous deformation at infinity with the stress state of a composite two-phase rod. Condition (22) allows us to reduce formally the problem of constructing a contact problem to an algebraic problem using the general representation (18), (19) for the temperature and displacement potentials:…”
Section: Transition Matrixmentioning
confidence: 99%
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