How Do You Differentiate an Integral with Variable Limits?

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To differentiate an integral with variable limits, the fundamental theorem of calculus is applied, where F is an antiderivative of f. The derivative of the integral from g(x) to h(x) of f(t) dt is given by F'(h(x))h'(x) - F'(g(x))g'(x). For the specific integral involving e^(-st), the differentiation is performed inside the integral, leading to the application of Leibniz's Integral Rule. The result shows that the derivative is not zero, as the integral can depend on the variable s. Ultimately, the correct derivative is found to be the integral of -tf(t)e^(-st) dt from 0 to infinity.
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Homework Statement


F is an antiderivative of f, so F’=f.
\begin{array}{l}<br /> \int_{g(x)}^{h(x)} {f(t)\,dt} = F\left( {h\left( x \right)} \right) - F\left( {g\left( x \right)} \right) \\ <br /> \frac{d}{{dx}}\int_{g(x)}^{h(x)} {f(t)\,dt} = F&#039;\left( {h\left( x \right)} \right)h&#039;\left( x \right) - F&#039;\left( {g\left( x \right)} \right)g&#039;\left( x \right) \\ <br /> \end{array}




Homework Equations


Can somebody show how to find the derivative of the following integral?

\frac{d}{{ds}}\int_0^\infty {f\left( t \right){e^{ - st}}dt}



The Attempt at a Solution


 
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Just reverse the order of integration and differentiation. The fundamental theorem doesn't really apply here.
 
p75213 said:
Can somebody show how to find the derivative of the following integral?

\frac{d}{{ds}}\int_0^\infty {f\left( t \right){e^{ - st}}dt}

Use integration by parts. Then d/ds every term. Then write the solution as a sum.
 
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I would think the answer is 0, since the definite integral is just a number, and the derivitive of a number if 0.
 
Villyer said:
I would think the answer is 0, since the definite integral is just a number, and the derivitive of a number if 0.

This isn't true. The definite integral for multivariable functions can be a function of a different variable, and if you actually tried the problem, you'd see that the definite integral becomes a function of s.
 
Leibniz's Integral rule as shown by Dick does the trick:

\frac{d}{{ds}}\int_0^\infty {f\left( t \right){e^{ - st}}dt} = \int_0^\infty {\frac{\delta }{{\delta s}}f\left( t \right){e^{ - st}}dt} = \int_0^\infty {f\left( t \right)\left( { - t{e^{ - st}}} \right)dt} = \int_0^\infty { - tf\left( t \right){e^{ - st}}dt}
 

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