hyperbolic-parabolic type. And this is the theory of which one problem we will solve in this encyclopedia entry. Coupled Thermoelasticity The governing equations of coupled thermoelasticity for a linear homogeneous isotro-pic material are: The equation of motion div S þ b ¼ r€ u; S ¼ S T ð1Þ The strain-displacement relation E ¼ 1 2 ðHu þ Hu T Þ ð 2Þ Hooke's law S ¼ 2mE þ lðtr EÞ1 À gT1; T ¼ y À y 0 ð3Þ The energy equation H 2 T À 1 k _ T À gy 0 k tr _ E ¼ À Q k ð4Þ Here 1 is the unit second-order tensor, y is the temperature, y 0 is the reference temperature , and T is temperature change. From the combination of the first three equations, the displacement-temperature equation of motion is obtained: mH 2 u þ ðl þ mÞHðdiv uÞ À gHT þ b ¼ r€ u ð5Þ Equations (4) and (5) represent the displacement temperature equations of coupled thermoelasticity for a solid elastic body. The full description of the problem requires the energy equation and the equation of motion complemented by appropriate initial and boundary conditions for thermal and mechanical loads.
CITATION STYLE
Hetnarski, R. B. (2014). Coupled Problem of Thermoelasticity: Solution in a Series of Functions Form. In Encyclopedia of Thermal Stresses (pp. 762–766). Springer Netherlands. https://doi.org/10.1007/978-94-007-2739-7_975
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