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On the speed rate of convergence of solutions to conservation laws with nonlinear diffusions

Raffaele Folino, Marta Strani

Abstract

In this paper we analyze the long-time behavior of solutions to conservation laws with nonlinear diffusion terms of different types: saturating dissipation (monotone and non monotone) and singular nonlinear diffusions are considered. In particular, the cases of mean curvature-type diffusions both in the Euclidean space and in Lorentz-Minkowski space enter in our framework. After dealing with existence and stability of monotone steady states in a bounded interval of the real line with Dirichlet boundary conditions, we discuss the speed rate of convergence to the asymptotic limit as $t\to+\infty$. Finally, in the particular case of a Burgers flux function, we show that the solutions exhibit the phenomenon of metastability.

On the speed rate of convergence of solutions to conservation laws with nonlinear diffusions

Abstract

In this paper we analyze the long-time behavior of solutions to conservation laws with nonlinear diffusion terms of different types: saturating dissipation (monotone and non monotone) and singular nonlinear diffusions are considered. In particular, the cases of mean curvature-type diffusions both in the Euclidean space and in Lorentz-Minkowski space enter in our framework. After dealing with existence and stability of monotone steady states in a bounded interval of the real line with Dirichlet boundary conditions, we discuss the speed rate of convergence to the asymptotic limit as . Finally, in the particular case of a Burgers flux function, we show that the solutions exhibit the phenomenon of metastability.

Paper Structure

This paper contains 19 sections, 13 theorems, 222 equations, 6 figures.

Key Result

Proposition \oldthetheorem

Let $\varepsilon>0$ and $f,Q\in C^2(\mathbb{R})$, with $Q$ satisfying eq:Qmono, and consider the boundary value problem for some $u_-<u_+$. There exists a unique (smooth) increasing solution to eq:staz-mono-BV if and only if where

Figures (6)

  • Figure 1: The dynamics of the solution to the IBVP \ref{['eq:QnonmonoNUM']}-\ref{['BIC']} with initial datum $u_0(x)=0.8\left(\frac{1}{2}x^2-x-\frac{1}{2}\right)$ and $u_*=0.8$. In the left picture $\varepsilon=0.05$, in the right one $\varepsilon=0.025$.
  • Figure 2: The dynamics of the solution to the IBVP \ref{['eq:QnonmonoNUM']}-\ref{['BIC']}. In the left picture we consider a discontinuous initial datum with $\varepsilon=0.06$ and $u_*=0.7$, in the right picture the non-monotone one $u_0(x)=0.6\left(-\frac{25}{6}x^3+\frac{3}{4}x^2+\frac{19}{6}x-\frac{3}{4}\right)$ with $\varepsilon=0.04$ and $u_*=0.6$.
  • Figure 3: The dynamics of the solution to the IBVP \ref{['eq:QunboundNUM']}-\ref{['BIC']} with $u_* = 0.75$ and initial datum $u_0(x)=\frac{1}{9}x^2-\frac{1}{2}x-\frac{1}{4}$. In the left picture $\varepsilon=0.04$, in the right one $\varepsilon=0.02$.
  • Figure 4: The dynamics of the solution to the IBVP \ref{['eq:QunboundNUM']}-\ref{['BIC']} with $\varepsilon=0.07$, $u_*=1$ and initial datum $u_0(x)=-\frac{3}{2}x^3+\frac{3}{4}x^2+\frac{1}{2}x-\frac{3}{4}$.
  • Figure 5: The dynamics of the solution to the IBVP \ref{['eq:QnonmonoNUM']}-\ref{['BIC']} with $\varepsilon=0.004$ (left), and \ref{['eq:QunboundNUM']}-\ref{['BIC']} with $\varepsilon=0.001$ (right); in both case we choose $u_*=\varepsilon/2$ and the initial datum $u_0(x)=\frac{\varepsilon}{2}\left(\frac{1}{2}x^2-x-\frac{1}{2}\right)$.
  • ...and 1 more figures

Theorems & Definitions (33)

  • Proposition \oldthetheorem
  • proof
  • Remark \oldthetheorem
  • Proposition \oldthetheorem
  • proof
  • Remark \oldthetheorem
  • Proposition \oldthetheorem
  • proof
  • Proposition \oldthetheorem
  • Remark \oldthetheorem
  • ...and 23 more