<p>An analysis of the formulations and methods for solving diagnostics problems on a fixed boundary of a solid body is carried out. Based on the weak formulations of boundary value problems for a nonlinear hyperbolic equation (nonstationary wave equation with density, elasticity moodulus, and thermal stress depending on temperature) and a parabolic equation (nonstationary heat conduction equation with volumetric heat capacity and thermal conductivity depending on temperature) with mixed boundary conditions, methodologies for finding a regularized solution to the diagnostics problem of unstable boundary conditions are determined. The specified solution is found, in the space <i>L</i><sub>2</sub>, by the regularization method from the first-kind integral equation in the presence of experimental data at all points of the space–time grid in the closed region <i>G</i> + Γ and, in the space <i>W</i><sub>2</sub><sup>(1)</sup>, by the iterative regularization method from the weak formulation of the boundary value problem of thermoelasticity in the presence of experimental data only on the boundary Γ.</p>

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Diagnostics of Mathematical Models of Thermoelasticity. Part 2. Analysis of Methods for Searching and Regularizing Solutions

  • A. G. Vikulov,
  • V. E. Kuznetsov

摘要

An analysis of the formulations and methods for solving diagnostics problems on a fixed boundary of a solid body is carried out. Based on the weak formulations of boundary value problems for a nonlinear hyperbolic equation (nonstationary wave equation with density, elasticity moodulus, and thermal stress depending on temperature) and a parabolic equation (nonstationary heat conduction equation with volumetric heat capacity and thermal conductivity depending on temperature) with mixed boundary conditions, methodologies for finding a regularized solution to the diagnostics problem of unstable boundary conditions are determined. The specified solution is found, in the space L2, by the regularization method from the first-kind integral equation in the presence of experimental data at all points of the space–time grid in the closed region G + Γ and, in the space W2(1), by the iterative regularization method from the weak formulation of the boundary value problem of thermoelasticity in the presence of experimental data only on the boundary Γ.