Let $u:\Omega\subset \mathbb R^N \to \mathbb R$ be bounded function that solves (in the sense of distributions) an evolution PDE $\partial_t u(t,x)= L(u(t,\cdot))(x)$, where $L$ is some elliptic operator in divergence form.
In a post on MathOverflow, a calculation was made regarding the time derivative $$\partial_t\int_{\{u(t,\cdot) >0\} } 1\, dx$$ in the following way:
$$\partial_t\int_{\{u(t,\cdot) >0\} } 1\, dx= ∫_\Omega \delta[u(t,x)]\partial_t u(t,x)\,dx=\int_{S(t)}\frac{\partial_t u(t,x)}{|\nabla_x u(t,x)|}d\sigma(x).$$
How can one rewrite this calculation emphasizing the fact that we are doing a derivative in the sense of distributions, i.e. $$\langle \partial_t T, \phi\rangle = -\langle T, \partial_t\phi \rangle $$ where $T$ is the distribution associated with $\int_{\{u(t,\cdot) >0\} } 1\, dx$?
And how can we use the fact that $u$ solves the PDE above in the final formula?
Let $S = { x, v(x)=0}$. If $v$ is smooth and $\nabla v(x_0)$ never vanishes for $x_0\in S$ then $S$ is a hypersurface, locally it is an hyperplane and $\nabla v(x)$ is constant, so it suffices to check the case $v(x) = \nabla v(x_0) . (x-x_0)$ for which $\int_{\Bbb{R}^N} \delta(v(x)) \phi(x)d^N x = \int_S\frac{\phi(x)}{|\nabla v(x)|_2}d\sigma_S(x)$ where $\sigma_S$ is the Minkowski content measure of $S$. From there it suffices to extend from test functions $\phi$ to distributions.
– reuns May 17 '19 at 22:06