Does the Leibniz Integral Rule Apply to Time-Dependent Integrals?

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\frac {d} {dt} \int_{a}^{b} f(x,t) dx = \int_{a}^{b} \frac {\delta} {\delta t} f(x,t) dx

From trial and error, it seems true but I can't find it in my textbook anywhere. Am I missing something obvious?
 
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Yes, this is true provided f and \frac{\partial f}{\partial t} are continuous. This is an example of interchanging limits. Be careful about doing that because in general you can't. This borders on advanced calculus, but my regular calc textbook gives a proof in the appendix. Maybe yours does too.
 
There's a very thorough proof on page 245 of the Bartle if you have access to one of those. Also, note that as a notational thing
<br /> \frac{\delta}{\delta g}<br />
usually denotes a functional derivative, while what you want is \partial, not \delta in LaTeX, like
<br /> \frac{\partial}{\partial t}<br />
 
Ok, thanks. Just needed to confirm that the statement was true (my physics textbook used it in a proof and never justified the statement, so I wanted to make sure)
 
This is only true though when the bounds (a & b) are held constant, correct? I mean, if they were a=u(x) and b=v(x), the limits couldn't be switched.
 
If the limits themselves are also functions of t, the theorem (called Leibniz integral rule, IIRC) is:

\frac {d} {dt} \int_{a(t)}^{b(t)} f(x,t) dx = f(b(t),t)\frac{d b}{d t}-f(a(t),t)\frac{d a}{d t}+\int_{a(t)}^{b(t)} \frac {\partial} {\partial t} f(x,t) dx

I know a sufficient condition for this to hold is that f be uniformly continuous in the region of interest.
 

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