IV. Inverse Stefan Problem – Part 4

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# NPDE Lecture 6 Discussion

# ISP Lecture 3 Discussion

# NPDE Lecture 5 Discussion

# ISP Lecture 2 Discussion

# NPDE Lecture 4 Discussion

IV. Nonlinear Diffusion in Non-smooth Domains

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# ISP Lecture 1 Discussion

# NPDE Lecture 3 Discussion

III. Energy Estimates and Existence

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# NPDE Lecture 2 Discussion

II. Weak Solutions and Uniqueness

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### Weak Solutions

Let me remind you what I did in a previous lecture. I considered the problem

\begin{align}

u_{t}-\text{div}\big( u^{\sigma} \nabla u\big) &=0,~x \in\R^{N},~t>0; \ \sigma > 0,\label{eq:inst-pme-1}\\

\int_{\R^{N}}u(x,t)\,dx &=1,~t > 0\label{eq:inst-pme-2}\\

u(x,0) = \delta(x)\label{eq:inst-pme-3}

\end{align}

and constructed instantaneous point-source solution, also called the Zeldovich-Kompaneets-Barenblatt (ZKB) solution.

\begin{equation} u_*(x,t)=t^{-\frac{N}{2+N\sigma}}\left[\frac{\sigma}{2(2+N\sigma)} \left( \eta_{0}^{2}-\frac{|x|^{2}}{t^{\frac{2}{2+N\sigma}}}\right)_{+} \right]^{\frac{1}{\sigma}}\end{equation}

Note that the nonlinear diffusion equation is invariant under translation of time and space coordinate, and the solution to the problem

\[ \begin{cases}

u_{t}=\text{div}\big(u^{\sigma }u\big),~&(x,t) \in \R^{N}\times \R_{+}\\

u(x,0)=u_*(x,T),~&x \in \R^{N}

\end{cases}\]

is exactly $u_*(x,t+T)$, which has compact support for all $t\geq 0$.

However, several important questions are left open. First of all, ZKB solution is not a classical solution: it is not even differentiable on the boundary of the support. First important question which we need to answer is the following: In what sense is $u_*$ actually a solution of the problem? Hence, we need to define the notion of the weak solution. Second important question we need to answer is the following: May be there is a smooth solution of the same problem with different properties, and ZKB solution is just physically irrelevant mathematical example. Main goal of this lecture is to answer these important questions.

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# NPDE Localization Effect in Diffusion-Absorption Equation

Reaction-diffusion equations can exhibit a phenomenon known as space localization: not only do they exhibit finite speed of propagation, but heat can be completely contained in a compact region for all time under certain conditions. This is a physically pertinent phenomena as well, having been observed in plasmas, but not encountered in solutions to the linear heat equation.

Consider the reaction-diffusion equation

\begin{equation} u_{t}=\text{div} \big( u^{\sigma}\nabla u\big)-\gamma u,\quad u \in \R^{N},~t>0\label{eq:pme-loc-1}\end{equation}

where $\sigma >0$, $\gamma>0$. That means nonlinear diffusion is accompanied with linear absorption.

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