A similar question has already been asked here: Derivation of Dirac-Delta with complicated argument $\delta(f(x))$
But now I want to do the following. Given the Hamiltonian $H=H(q(t),p(t),t)=E$ is a constant we can define its phase space volume as: $$\int \delta(H(q(t),p(t),t)-E)dqdp$$ How can one evaluate the rate of change of the phase space volume, considering that q and p are functions of time? $$\frac{d}{dt}\int \delta(H(q(t),p(t),t)-E)dqdp$$
If $\int ... dx(t) dy(t)$ means integrating over all possible curves (like in a path integral) then the integral makes sense but the output doesn't depend on $t$ so the derivative is 0.
– pregunton Mar 24 '17 at 16:00