/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 61 Find the volume of the solid gen... [FREE SOLUTION] | 91Ó°ÊÓ

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Find the volume of the solid generated when the region bounded by \(y=\cos x\) and the \(x\) -axis on the interval \([0, \pi / 2]\) is revolved about the \(y\) -axis.

Short Answer

Expert verified
Answer: The volume of the solid is \(\frac{\pi^2}{2}\).

Step by step solution

01

Set up the integral

To set up the integral, we first need to determine the inequalities that bound the region. The region is bounded by the curve \(y=\cos x\), the x-axis, and the range \([0, \pi / 2]\). As the solid is revolved about the \(y\)-axis, the radius of each washer will be a function of \(y\). We notice that the distance from the \(y\)-axis to the curve \(y=\cos x\) is just \(x\), which on our region goes from \(0\) to \(\pi / 2\). Therefore, we have the relationship \(x = \arccos y\). Now we can set up the integral to determine the volume: $$V = \pi \int_{0}^{1} R^2(y) dy$$ where \(R(y)\) is the radius of each washer as a function of \(y\).
02

Find the radius function

To find the radius function, we observe that the radius is determined by the distance between the curve and the \(y\)-axis, and we already found the relationship \(x = \arccos y\). Therefore, the radius function is: $$R(y) = \arccos y$$ Now, we will substitute this function into the volume integral equation from Step 1.
03

Evaluate the integral

Now we will substitute our radius function into our integral and evaluate it to determine the volume: $$V = \pi \int_{0}^{1} (\arccos y)^2 dy$$ To evaluate this integral, we will use integration by parts: Let \(u = \arccos y\) and \(dv = u dy\). Then, \(du = -\frac{1}{\sqrt{1-y^2}} dy\) and \(v = y\). $$V = \pi (uv - \int v du)$$ $$V = \pi (\arccos y \cdot y - \int y(-\frac{1}{\sqrt{1-y^2}} dy))$$ The integral now becomes a bit easier to solve: $$V = \pi (\arccos y \cdot y + \int y (\frac{1}{\sqrt{1-y^2}} dy))$$ We recognize this integral as being the result of the inverse substitution (also known as the sin substitution): Let \(y = \sin t\) => \(dy = \cos t dt\). $$V = \pi (\arccos y \cdot y + \int \sin t (\frac{\cos t}{\cos t} dt))$$ So we only need to evaluate: $$V = \pi (\arccos y \cdot y + \int \sin t dt)$$ $$V = \pi (\arccos y \cdot y -\cos t|_{t=0}^{\pi -\arccos y })$$ Now we substitute \(y=\sin t\) and \(1= \sin(\pi - \arccos y)\). $$V = \pi [\arccos (\sin t) \cdot \sin t - \cos t |_{t=0}^{\pi -\arccos(\sin t )}]$$ We evaluate at the bounds and subtract: $$V = \pi [\arccos(\sin(\pi -\arccos(\sin t))) \cdot \sin(\pi -\arccos(\sin t)) - \cos(\pi -\arccos(\sin t))] - \pi [\arccos(\sin(0)) \cdot \sin(0) - \cos(0)]$$ $$V = \pi [0] - \pi [\arccos 0]$$ $$V = -\pi [0 - \pi / 2]$$ $$V = \boxed{\frac{\pi^2}{2}}$$ The volume of the solid generated when the region bounded by \(y=\cos x\) and the \(x\) -axis on the interval \([0, \pi / 2]\) is revolved about the \(y\) -axis is \(\frac{\pi^2}{2}\).

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Most popular questions from this chapter

Let \(R\) be the region between the curves \(y=e^{-c x}\) and \(y=-e^{-c x}\) on the interval \([a, \infty),\) where \(a \geq 0\) and \(c \geq 0 .\) The center of mass of \(R\) is located at \((\bar{x}, 0)\) where \(\bar{x}=\frac{\int_{a}^{\infty} x e^{-c x} d x}{\int_{a}^{\infty} e^{-c x} d x} .\) (The profile of the Eiffel Tower is modeled by the two exponential curves.) a. For \(a=0\) and \(c=2,\) sketch the curves that define \(R\) and find the center of mass of \(R\). Indicate the location of the center of mass. b. With \(a=0\) and \(c=2,\) find equations of the lines tangent to the curves at the points corresponding to \(x=0.\) c. Show that the tangent lines intersect at the center of mass. d. Show that this same property holds for any \(a \geq 0\) and any \(c>0 ;\) that is, the tangent lines to the curves \(y=\pm e^{-c x}\) at \(x=a\) intersect at the center of mass of \(R\) (Source: P. Weidman and I. Pinelis, Comptes Rendu, Mechanique \(332(2004): 571-584 .)\)

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