Overview
The system of classical thermoelasticity is a hyperbolic-parabolic coupled system describing the elastic and the thermal behavior of an elastic medium ([1–3]). It is well known that with respect to the decay of solutions as time tends to infinity and also with respect to the existence of global smooth solutions for small data in one space variable or of the potential part of displacement and temperature in multidimensional thermoelasticity, the system behaves like a purely parabolic one (see, e.g., [2–5] and references cited there). As in nonlinear wave equations, the smooth solutions to the nonlinear thermoelasticity shall blowup in a finite time in general (cf. [6–8]). In [9], it was observed that solutions to the linear problem do not have a smoothing effect, like in a parabolic problem. Moreover, in [10], the author proved that for the linear equations of thermoelasticity, even when the initial displacement and velocity are smooth, the nonsmooth initial temperature shall...
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This research was supported in part by the National Science Foundation of China under grants 10971134, 11031001 and 91230102.
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Wang, YG. (2014). Propagation of Singularities. In: Hetnarski, R.B. (eds) Encyclopedia of Thermal Stresses. Springer, Dordrecht. https://doi.org/10.1007/978-94-007-2739-7_257
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DOI: https://doi.org/10.1007/978-94-007-2739-7_257
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