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An irreversible thermodynamical theory of solids is presented where the kinematic quantities are defined in an automatically objective way. Namely, auxiliary elements like reference frame, reference time and reference configuration are avoided by formulating the motion of the continuum on spacetime directly. Solids are distinguished from fluids by possessing not only an instantaneous metric tensor but also a relaxed metric. The elastic state variable is defined through comparing these two metrics. Thermal expansion is conceived as temperature dependence of the relaxed metric and plasticity, an irreversible change in the relaxed metric, is described via a plastic change rate tensor. Thermomechanics is built around these -- finite deformation -- kinematic quantities by starting from mechanics and adding thermodynamical requirements gradually. The obtained theory is not restricted to isotropic media., Comment: 10 pages, 2 figures