I'm reading a PDE book, and the authors use this often, for $u = u(x,t)$, and V an arbitrary volume on in the interior of a solid:
$${\frac{d}{dt} \int_V u \space dx}$$
$$= {\int_V u_t \space dx}$$
How is differentiating under the integral w.r.t. to time $t$ justified?
I imagine it must be so simple that I'm simply rusty with my introductory analysis coursework and don't see it right away.
My attempt:
Writing out the difference quotient and using linearity of the integral, we have that:
$$ \lim_{h \to 0} \int_V \frac { u(x,t+h) - u(x,t)} {h} \space dx $$
and assuming I can use the dominated convergence theorem, we have that:
$$ \lim_{h \to 0} \int_V \frac { u(x,t+h) - u(x,t)} {h} \space dx = \int_V \lim_{h \to 0} \frac { u(x,t+h) - u(x,t)} {h} \space dx $$
$$ = {\int_V u_t \space dx} $$
So, there seem to be some nice conditions on $u$ that the authors are assuming.
Thanks,