Chapter 6: Problem 19
Find the integral. (Note: Solve by the simplest method-not all require integration by parts.) $$ \int x \cos x d x $$
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Chapter 6: Problem 19
Find the integral. (Note: Solve by the simplest method-not all require integration by parts.) $$ \int x \cos x d x $$
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Laplace Transforms Let \(f(t)\) be a function defined for all positive values of \(t\). The Laplace Transform of \(f(t)\) is defined by \(F(s)=\int_{0}^{\infty} e^{-s t} f(t) d t\) if the improper integral exists. Laplace Transforms are used to solve differential equations. Find the Laplace Transform of the function. $$ f(t)=\sin a t $$
Graphical Analysis In Exercises 61 and 62, graph \(f(x) / g(x)\) and \(f^{\prime}(x) / g^{\prime}(x)\) near \(x=0 .\) What do you notice about these ratios as \(x \rightarrow 0\) ? How does this illustrate L'Hôpital's Rule? \(f(x)=e^{3 x}-1, \quad g(x)=x\)
Evaluate the definite integral. $$ \int_{0}^{\pi / 4} \tan ^{3} x d x $$
In Exercises 59 and \(60,\) (a) explain why L'Hôpital's Rule cannot be used to find the limit, (b) find the limit analytically, and (c) use a graphing utility to graph the function and approximate the limit from the graph. Compare the result with that in part (b). \(\lim _{x \rightarrow \infty} \frac{x}{\sqrt{x^{2}+1}}\)
A "semi-infinite" uniform rod occupies the nonnegative \(x\) -axis. The rod has a linear density \(\delta\) which means that a segment of length \(d x\) has a mass of \(\delta d x .\) A particle of mass \(m\) is located at the point \((-a, 0)\). The gravitational force \(F\) that the rod exerts on the mass is given by \(F=\int_{0}^{\infty} \frac{G M \delta}{(a+x)^{2}} d x\) where \(G\) is the gravitational constant. Find \(F\).
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