/*! 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 40 \(D\) is the solid right cylinde... [FREE SOLUTION] | 91Ó°ÊÓ

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\(D\) is the solid right cylinder whose base is the region between the circles \(r=\cos \theta\) and \(r=2 \cos \theta\) and whose top lies in the plane \(z=3-y .\)

Short Answer

Expert verified
Integrate height 3-y over the defined polar base region to find volume.

Step by step solution

01

Understand the Problem

We have a solid right cylinder with a base defined by two curves, \( r = \cos \theta \) and \( r = 2\cos \theta \), which means the base is the region between these circles in polar coordinates. The cylinder extends up to a height defined by \( z = 3 - y \).
02

Set Up the Base Region in Polar Coordinates

In polar coordinates, the area between the circles \( r = \cos \theta \) and \( r = 2\cos \theta \) involves radius \( r \) ranging from \( \cos \theta \) to \( 2\cos \theta \). \( \theta \) varies from \(-\pi/2\) to \(\pi/2\) because \( \cos \theta \) is non-negative and these are the limits where \(r\) remains positive.
03

Determine the Cylinder's Height

The height of the cylinder is determined by the plane \( z = 3 - y \). In terms of polar coordinates, \( y = r \sin \theta \), hence the height becomes \( z = 3 - r \sin \theta \).
04

Integrate Over the Base Region

The volume of the cylinder can be determined by integrating the height over the base region. The double integral in polar coordinates is:\[ \int_{-\pi/2}^{\pi/2} \int_{\cos \theta}^{2\cos \theta} (3 - r \sin \theta) \cdot r \, dr \, d\theta \]
05

Perform the Integration

First, integrate with respect to \( r \):\[ \int (3r - r^2 \sin \theta) \, dr = \left[ \frac{3}{2}r^2 - \frac{r^3}{3} \sin \theta \right] \Bigg|_{\cos \theta}^{2\cos \theta} \]Evaluate from \( r = \cos \theta \) to \( r = 2\cos \theta \).
06

Simplify and Calculate

After substituting the limits of \( r \) and simplifying, integrate the result with respect to \( \theta \) over \(-\pi/2 \) to \( \pi/2 \). This involves solving for the definite integrals and summing the results.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Polar Coordinates
Polar coordinates offer a unique and useful way to represent points in a plane. Unlike the Cartesian coordinate system, which uses x and y to define a point, polar coordinates use \(r, \theta\). Here, \(r\) is the radius or distance from the origin to the point, and \(\theta\) is the angle between the radius and the positive x-axis.
Polar coordinates are especially helpful when dealing with circular or spiral shapes, as they naturally align with round structures.
  • The radius \(r\) tells us how far from the origin we are.
  • The angle \(\theta\) provides direction, measured in radians or degrees.
In the context of this exercise, we're looking at two circles defined by \(r = \cos \theta\) and \(r = 2\cos \theta\). This means that instead of being circles centered at the origin, these circles are offset along the x-axis, which is a typical feature when using \(\cos \theta\) for \(r\) values.
This offset is crucial for defining the region over which we calculate the volume of the solid.
Double Integration
Double integration is a technique used to calculate the volume under a surface or the area in a plane. When integrating over a two-dimensional region, we perform an inner and an outer integral. In polar coordinates, this requires integrating with respect to \(r\) first, and then \(\theta\).
The general form of a double integral in polar coordinates is \[ \int_{\theta_1}^{\theta_2} \int_{r_1(\theta)}^{r_2(\theta)} f(r, \theta) \cdot r \, dr \, d\theta \]The extra \(r\) in the integral accounts for the change in area element that happens when converting from Cartesian to polar coordinates.
This method is particularly useful for calculating areas and volumes where the limits are better expressed in terms of angles and radii.
In our exercise, double integration is applied to find the volume of the region defined by two concentric circular segments and a height function. The inner integral computes areas for each small segment of \(r\), while the outer integral accumulates these areas across all \(\theta\) values.
Volume of Solid
Calculating the volume of a solid using integration involves summing up infinitely small elemental volumes (slices) through the structure. For solids based on circular or cylindrical shapes, polar coordinates make this calculation more intuitive.
In our exercise, the solid is a right circular cylinder with its height defined by a plane. This height difference across the cylinder is represented by \(z = 3 - y\), where \(y = r \sin \theta\) in polar form.
The double integral calculates the volume by evaluating each infinitesimal slice of the solid's height \(3 - r \sin \theta\). By integrating over the specified range of radius \(r\) and angle \(\theta\), we get the total volume of the cylinder between the two circular segments.
This method is a powerful application of calculus in determining exact volumes in physics and engineering.
Integral Calculus
Integral calculus is a fundamental part of mathematics that deals with the concepts of integration, which is essentially the reverse process of differentiation. It is used to determine areas, volumes, central points, and many other useful things.
In more practical terms, while differential calculus breaks things into small parts and finds the rate of change, integral calculus reverses this by summing up parts to find the whole.
  • Definite integrals compute the accumulated value between two limits.
  • Indefinite integrals provide general antiderivatives without specific limits.
In this exercise, integral calculus is used to find the volume of the solid between curves and under a surface. By translating the problem into polar coordinates, integrating with respect to \(r\) and \(\theta\) simplifies the calculation.
Integral calculus not only allows for solving straightforward volume problems but also provides insights into the behavior of functions over certain regions or intervals.

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Most popular questions from this chapter

Sketch the region of integration and write an equivalent double integral with the order of integration reversed. \begin{equation} \int_{0}^{1} \int_{-\sqrt{1-y^{2}}}^{\sqrt{1-y^{2}}} 3 y d x d y \end{equation}

The Parallel Axis Theorem Let \(L_{\mathrm{cm}}\) be a line through the center of mass of a body of mass \(m\) and let \(L\) be a parallel line \(h\) units away from \(L_{c . m .}\) The Parallel Axis Theorem says the moments of inertia \(I_{\mathrm{cm}}\) and \(I_{L}\) of the body about \(L_{\mathrm{cm}}\) and \(L\) satisfy the equation $$ I_{L}=I_{\mathrm{c.m.}}+m h^{2} $$ As in the two-dimensional case, the theorem gives a quick way to calculate one moment when the other moment and the mass are known. Proof of the Parallel Axis Theorem a. Show that the first moment of a body in space about any plane through the body's center of mass is zero. (Hint: Place the body's center of mass at the origin and let the plane be the \(y z\) -plane. What does the formula \(\overline{x}=M_{y z} / M\) then tell you?) b. To prove the Parallel Axis Theorem, place the body with its center of mass at the origin, with the line \(L_{c . m . \text { along the }}\) \(z\) z-axis and the line \(L\) perpendicular to the \(x y\) -plane at the point \((h, 0,0) .\) Let \(D\) be the region of space occupied by the body. Then, in the notation of the figure, $$ I_{L}=\iiint_{D}|\mathbf{v}-h \mathbf{i}|^{2} d m $$ Expand the integrand in this integral and complete the proof.

Find the volume of the solid in the first octant bounded by the coordinate planes, the cylinder \(x^{2}+y^{2}=4,\) and the plane \(z+y=3 .\)

\(\begin{aligned} \text { Converting to } & \text { a polar integral Evaluate the integral } \\ & \int_{0}^{\infty} \int_{0}^{\infty} \frac{1}{\left(1+x^{2}+y^{2}\right)^{2}} d x d y \end{aligned}\)

Verify that \(f\) gives a joint probability density function. Then find the expected values \(\mu_{X}\) and \(\mu_{Y}\) . $$ f(x, y)=\left\\{\begin{array}{ll}{x+y,} & {\text { if } 0 \leq x \leq 1 \text { and } 0 \leq y \leq 1} \\ {0,} & {\text { otherwise }}\end{array}\right. $$

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