Chapter 6: Problem 5
Let \(R\) be the region bounded by the following curves. Use the shell method to find the volume of the solid generated when \(R\) is revolved about the \(y\) -axis. $$y=x-x^{2}, y=0$$
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Chapter 6: Problem 5
Let \(R\) be the region bounded by the following curves. Use the shell method to find the volume of the solid generated when \(R\) is revolved about the \(y\) -axis. $$y=x-x^{2}, y=0$$
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Use a calculator to evaluate each expression, or state that the value does not exist. Report answers accurate to four decimal places. a. \(\operatorname{coth} 4\) b. \(\tanh ^{-1} 2\) c. \(\operatorname{csch}^{-1} 5\) d. \(\left.\operatorname{csch} x\right|_{1 / 2} ^{2}\) e. \(\ln | \tanh (x / 2) \|_{1}^{10} \quad\) f. \(\left.\tan ^{-1}(\sinh x)\right|_{-3} ^{3} \quad\) g. \(\left.\frac{1}{4} \operatorname{coth}^{-1}\left(\frac{x}{4}\right)\right|_{20} ^{\frac{36}{6}}\)
Evaluate the following integrals. $$\int \frac{\ln ^{2} x+2 \ln x-1}{x} d x$$
Zero net area Consider the function \(f(x)=\frac{1-x}{x}\) a. Are there numbers \(01\) such that \(\int_{1 / a}^{a} f(x) d x=0 ?\)
a. Confirm that the linear approximation to \(f(x)=\tanh x\) at \(a=0\) is \(L(x)=x\) b. Recall that the velocity of a surface wave on the ocean is \(v=\sqrt{\frac{g \lambda}{2 \pi} \tanh \left(\frac{2 \pi d}{\lambda}\right)} .\) In fluid dynamics, shallow water refers to water where the depth-to-wavelength ratio \(d / \lambda<0.05 .\) Use your answer to part (a) to explain why the shallow water velocity equation is \(v=\sqrt{g d}\) c. Use the shallow-water velocity equation to explain why waves tend to slow down as they approach the shore.
Two bars of length \(L\) have densities \(\rho_{1}(x)=4 e^{-x}\) and \(\rho_{2}(x)=6 e^{-2 x},\) for \(0 \leq x \leq L\) a. For what values of \(L\) is bar 1 heavier than bar \(2 ?\) b. As the lengths of the bars increase, do their masses increase without bound? Explain.
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