Saint-Venant's principle in blow-up for higher-order quasilinear parabolic equations

Abstract

We prove localization estimates for general 2 m th-order quasilinear parabolic equations with boundary data blowing up in finite time, as t → T − . The analysis is based on energy estimates obtained from a system of functional inequalities expressing a version of Saint-Venant's principle from the theory of elasticity. We consider a special class of parabolic operators including those having fixed orders of algebraic homogenuity p > 0. This class includes the second-order heat equation and linear 2 m th-order parabolic equations ( p = 1), as well as many other higher-order quasilinear ones with p ≠ 1. Such homogeneous equations can be invariant under a group of scaling transformations, but the corresponding least-localized regional blow-up regimes are not group invariant and exhibit typical exponential singularities ~ e ( T − t )−γ → ∞ as t → T − , with the optimal constant γ = 1/[ m ( p + 1) − 1] > 0. For some particular equations, we study the asymptotic blow-up behaviour described by perturbed first-order Hamilton–Jacobi equations, which shows that general estimates of exponential type are sharp.