Abstract

Abstract We study the comparison principle for non-negative solutions of the equation ∂ ⁡ ( | v | p - 2 ⁢ v ) ∂ ⁡ t = div ⁡ ( | ∇ ⁡ v | p - 2 ⁢ ∇ ⁡ v ) , 1 < p < ∞ . \frac{\partial(|v|^{p-2}v)}{\partial t}=\operatorname{div}(|\nabla v|^{p-2}% \nabla v),\quad 1<p<\infty. This equation is related to extremals of Poincaré inequalities in Sobolev spaces. We apply our result to obtain pointwise control of the large time behavior of solutions.

Highlights

  • Among the so-called doubly non-linear evolutionary equations, Trudinger’s equation 1 < p < ∞, (1.1)is distinguished

  • The equation was originally considered by Trudinger in [22], where a Harnack inequality was studied for a wider class of evolutionary equations

  • The equation has two special features: it is homogeneous and it is not translation invariant, except for p = 2 when it reduces to the heat equation

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Summary

Introduction

Among the so-called doubly non-linear evolutionary equations, Trudinger’s equation. is distinguished. We shall study its solutions in ΩT = Ω × (0, T), where Ω is a domain in Rn. The equation was originally considered by Trudinger in [22], where a Harnack inequality was studied for a wider class of evolutionary equations. Our result implies that for p ≥ 2, all non-negative continuous weak solutions are viscosity solutions in the sense of Crandall, Evans, and Lions in [3] Trudinger’s equation has an interesting connection to extremals of Poincaré inequalities in the Sobolev space W1,p(Ω). In [8], a comparison principle is proved for a general class of doubly non-linear equations. In the Appendix, we give a proof of the fact that the maximum of a subsolution and a constant is again a subsolution

Preliminaries
The comparison principle
Comparison in star-shaped domains
Extremals and large time behavior
Weak and viscosity solutions
A Appendix
Full Text
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