English

A simple model for one-dimensional nonlinear thermoelasticity: Well-posedness in rough-data frameworks

Analysis of PDEs 2026-02-06 v1

Abstract

In an open bounded interval Ω\Omega, the problem utt=uxx(f(Θ))x,Θt=Θxxf(Θ)uxt, u_{tt} = u_{xx} - \big(f(\Theta)\big)_x, \Theta_t = \Theta_{xx} - f(\Theta) u_{xt}, is considered under the boundary conditions uΩ=ΘxΩ=0u|_{\partial\Omega}=\Theta_x|_{\partial\Omega}=0, and for fC2([0,))f\in C^2([0,\infty)) satisfying f(0)=0f(0)=0, f>0f'>0 on [0,)[0,\infty) and fW1,((0,))f'\in W^{1,\infty}((0,\infty)). In the sense of unconditional global existence, uniqueness and continuous dependence, this problem is shown to be well-posed within ranges of initial data merely satisfying u_0\in W_0^{1,2}(\Omega), \quad u_{0t} \in L^2(\Omega) \quad \mbox{and} \quad \Theta_0 \in L^2(\Omega) \mbox{ with $\Theta\ge 0$ a.e.~in $\Omega$,} and in classes of solutions fulfilling uC0([0,);W01,2(Ω)),utC0([0,);L2(Ω))\mboxandΘC0([0,);L2(Ω))Lloc2([0,);W1,2(Ω)). u\in C^0([0,\infty);W_0^{1,2}(\Omega)), \qquad u_t \in C^0([0,\infty);L^2(\Omega)) \qquad \mbox{and} \qquad \Theta\in C^0([0,\infty);L^2(\Omega)) \cap L^2_{loc}([0,\infty);W^{1,2}(\Omega)).

Keywords

Cite

@article{arxiv.2602.05963,
  title  = {A simple model for one-dimensional nonlinear thermoelasticity: Well-posedness in rough-data frameworks},
  author = {Michael Winkler},
  journal= {arXiv preprint arXiv:2602.05963},
  year   = {2026}
}
R2 v1 2026-07-01T10:23:00.847Z