Inverse problem and heat equation

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In several books dealing with the subject of evolution equations we always find this expression: 'the equation of heat is irreversible in time' or 'the equation of the waves is reversible in time'. This expression means what? My first impression when I read this expression is: can we find the initial state of the system from the final state (inverse problem). is it true ? Thank you.

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I'm not sure if reversible is a technical term, but I'd interpret it the way you did.

Wave equation. It's clear that if $u$ is a solution of $u_{tt} = \Delta u$, then $v(t,x) = u(-t,x)$ is also a solution. Thus we can reverse the time. Given any initial conditions $f \in C^2(\mathbb{R}^n)$, $g \in C^1(\mathbb{R}^n)$, the problem $$ \begin{cases} u_{tt} = \Delta u \\ u(0,\cdot) = f \\ u_t(0,\cdot) = g \end{cases} $$ has a solution defined not only on $[0,\infty) \times \mathbb{R}^n$, but even on $\mathbb{R} \times \mathbb{R}^n$ (i.e., for all times $t \in \mathbb{R}$); the usual formula works. Then one can take $u(-1,\cdot)$ and $u_t(-1,0)$ as initial conditions and obtain $f,g$ at time $1$.

Heat equation. The same trick $t \mapsto -t$ doesn't work here. Also, one cannot solve the inverse problem in general. The formula for the solution implies that it's a smooth function for all $t>0$. Therefore you can take some function $u_0 \in C_c^2(\mathbb{R}^n) \setminus C^\infty(\mathbb{R}^n)$ to be an initial condition (which is perfectly valid even in the classical sense), but finding a solution $u \colon [0,\infty) \times \mathbb{R}^n \to \mathbb{R}$ such that $u(t,\cdot) = u_0$ for some $t>0$ is impossible.

As a side comment, I've never really understood how this irreversibility pops up when one derives the heat equation from the kinetic equations (i.e. as a limit of the model with finitely many colliding particles).