2022
DOI: 10.1098/rsta.2021.0363
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Equilibrium problem for a thermoelastic Kirchhoff–Love plate with a delaminated flat rigid inclusion

Abstract: A new mathematical model describing an equilibrium of a thermoelastic heterogeneous Kirchhoff–Love plate is considered. A corresponding nonlinear variational problem is formulated with respect to a two-dimensional domain with a cut. This cut corresponds to an interfacial crack located on a given part of the boundary of a flat rigid inclusion. The flat inclusion is described by a cylindrical surface. Due to the presence of the flat rigid inclusion in the plate, restrictions of the functions describing displacem… Show more

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Cited by 2 publications
(3 citation statements)
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“…From a mathematical point of view, the developed non-smooth variational methods are based on the Lagrange multiplier approach and dual optimization techniques. The variational problems under consideration are subjected to gradient constraint [ 1 ] and unilateral constraints [ 2 , 3 ], they obey non-differentiable objectives and may lose the property of coercivity [ 4 ]. These features result in non-smooth optimization, quasi-variational inequalities [ 5 ] and hemi-variational inequalities [ 6 ].…”
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confidence: 99%
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“…From a mathematical point of view, the developed non-smooth variational methods are based on the Lagrange multiplier approach and dual optimization techniques. The variational problems under consideration are subjected to gradient constraint [ 1 ] and unilateral constraints [ 2 , 3 ], they obey non-differentiable objectives and may lose the property of coercivity [ 4 ]. These features result in non-smooth optimization, quasi-variational inequalities [ 5 ] and hemi-variational inequalities [ 6 ].…”
mentioning
confidence: 99%
“…From the point of view of physics, the variational approach is applied to continuum mechanics of solids as well as incompressible fluids given by the Navier–Stokes [ 9 ] and Stokes [ 6 ] models. The different types of models for solids describe elastic junctions [ 2 ], thermo-elastic composites under mechanical vibration [ 12 ], dynamic behaviour of the Euler–Bernoulli beams [ 8 ] and thermo-elastic Kirchhoff–Love plates [ 3 ]. There are considered bodies that exhibit power-law hardening like the Norton–Hoff and Ramberg–Osgood materials [ 5 ], and ideal elasto-plastic behaviour [ 1 ].…”
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confidence: 99%
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