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Finite strains: Objective rates, conjugate stress tensors, constitutive equations for composite materials that determine material (Lagrangian) and spatial (Eulerian) tensors are taken as a basis. Such an approach allows
Finite strains: Objective rates, conjugate stress tensors, constitutive equations for composite materials that determine material (Lagrangian) and spatial (Eulerian) tensors are taken as a basis. Such an approach allows
Kinematics of finite elastoplastic deformations and nonelastic (plastic) components in the multiplicative representation of the deformation gradient tensor. We
Kinematics of finite elastoplastic deformations and nonelastic (plastic) components in the multiplicative representation of the deformation gradient tensor. We
Statement of the problem of numerical modelling of finite deformations are stated. The first section is devoted kinematics of finite strains in the Lagrangian frame, tensors
Statement of the problem of numerical modelling of finite deformations are stated. The first section is devoted kinematics of finite strains in the Lagrangian frame, tensors
Nonlinear problem on hyperelastic deformation of the shell of average thickness FEM-Euler as linear function from tensor of a spatial gradient of speed are deduced. In the second section within
ANOMALOUS WAVE PROPERTIES OF GRADIENT CHIRAL METAMATERIALS WITH ANISOTROPY OF THE MAGNETOELECTRIC COUPLING AND SPATIAL DISPERSIONWe obtained the material equations of the meta-environment and determined the dispersion equations
Thermal Casimir and Casimir-Polder interactions in N parallel 2D Dirac materials using gauge invariant components of the polarization tensor extended to the whole complex frequency
Nonlinear problem on hyperelastic deformation of the shell of average thickness FEM-Euler as linear function from tensor of a spatial gradient of speed are deduced. In the second section within
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