
In this chapter, we consider the equilibrium theory of classical thermoelasticity. In the absence of time dependence, the basic equations from Section 3.1 reduce to the equations of equilibrium (4.1.1) the equilibrium energy equation (4.1.2) the constitutive equations (4.1.3) (4.1.4) and the geometrical equations (4.1.5) on B. The constitutive coefficients satisfy the properties (3.1.4).
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