Abstract

We consider semilinear evolution equations of the form $a(t)\partial_{tt}u + b(t) \partial_t u + Lu = f(x,u)$ and $b(t) \partial_t u + Lu = f(x,u),$ with possibly unbounded $a(t)$ and possibly sign-changing damping coefficient $b(t)$, and determine precise conditions for which linear instability of the steady state solutions implies nonlinear instability. More specifically, we prove that linear instability with an eigenfunction of fixed sign gives rise to nonlinear instability by either exponential growth or finite-time blow-up. We then discuss a few examples to which our main theorem is immediately applicable, including evolution equations with supercritical and exponential nonlinearities.

Highlights

  • We consider the second order evolution equation a(t)∂ttu + b(t)∂tu + Lu = f (x, u), x ∈ Ω, t > 0 (1.1)and its first-order counterpart b(t)∂tu + Lu = f (x, u), x ∈ Ω, t > 0 (1.2)where L is a linear differential operator with smooth, bounded coefficients, f is a nonlinear source, b(t) is a damping term, and a(t) is a time dependent coefficient related to the relaxation time of the system (1.1)

  • We present results concerning the instability of steady solutions to evolution equations that involve very general conditions on the spatial operator L, the associated variable coefficients a(t) and b(t), the nonlinearity f, and the spatial domain Ω

  • To prove theorems regarding the instability of steady states for a family of nonlinear parabolic and hyperbolic equations

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Summary

Introduction

To prove theorems regarding the instability of steady states for a family of nonlinear parabolic and hyperbolic equations. With the addition of the time-dependent coefficients in the nonlinear problem, the question arises as to whether steady states become unstable under smooth perturbations for more general evolution equations, and the present study is devoted to addressing this open question.

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