Abstract
This paper presents conversion of the volume integral of temperature gradients to a surface integral in the integral formulation of boundary value problems of uncoupled thermoelasticity. Particular classes of problems such as thermal stresses, quasi-static problems of uncoupled thermoelasticity, and stationary problems of thermoelasticity are considered. The improved formulation makes numerical computation more accurate and less formidable. The integral formulations in uncoupled thermoelasticity are given in the Laplace transform domain as well as in the time domain.
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