/*! 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 51 Express the volume of the solid ... [FREE SOLUTION] | 91Ó°ÊÓ

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Express the volume of the solid inside the sphere \(x^{2}+y^{2}+z^{2}=16\) and outside the cylinder \(x^{2}+y^{2}=4\) as triple integrals in cylindrical coordinates and spherical coordinates, respectively.

Short Answer

Expert verified
Set up triple integrals in cylindrical and spherical coordinates using their respective bounds defined by the sphere and cylinder equations.

Step by step solution

01

Identify Boundaries in Cartesian Coordinates

We have the sphere given by the equation \(x^2 + y^2 + z^2 = 16\) and the cylinder \(x^2 + y^2 = 4\). The sphere bounds the solid from the outside and has a radius of 4, while the cylinder acts as an internal boundary with a radius of 2. We aim to find the volume inside the sphere but outside this cylinder.
02

Convert Equations to Cylindrical Coordinates

In cylindrical coordinates, the sphere is given by \(r^2 + z^2 = 16\) and the cylinder is simply \(r = 2\). The goal is to describe the volume where \(2 \leq r \leq 4\) and the height \(z\) is bounded between \(-\sqrt{16-r^2}\) and \(\sqrt{16-r^2}\).
03

Set Up the Triple Integral in Cylindrical Coordinates

The volume element in cylindrical coordinates is \(r \, dr \, d\theta \, dz\). Therefore, the triple integral for the volume is:\[V = \int_{0}^{2\pi} \int_{2}^{4} \int_{-\sqrt{16-r^2}}^{\sqrt{16-r^2}} r \, dz \, dr \, d\theta\]
04

Convert to Spherical Coordinates

To convert to spherical coordinates, recall that \(x = \rho \sin \phi \cos \theta\), \(y = \rho \sin \phi \sin \theta\), and \(z = \rho \cos \phi\). The sphere is simply \(\rho = 4\). The cylinder \(x^2 + y^2 = 4\) converts to \( \rho^2 \sin^2 \phi = 4\), giving \(\sin \phi = \frac{2}{\rho}\).
05

Set Up the Triple Integral in Spherical Coordinates

The radial distance \(\rho\) varies from 2 to 4 (given by the cylinder and sphere), \(\theta\) varies from 0 to \(2\pi\), and \(\phi\) ranges from 0 to \(\arcsin \left( \frac{2}{\rho} \right)\). The differential in spherical coordinates is \(\rho^2 \sin \phi \, d\rho \, d\phi \, d\theta\). Thus, the integral is:\[V = \int_{0}^{2\pi} \int_{2}^{4} \int_{0}^{\arcsin \left( \frac{2}{\rho} \right) } \rho^2 \sin \phi \, d\phi \, d\rho \, d\theta\]
06

Evaluate the Integrals (Optional)

These integrals would typically be evaluated numerically or via software if necessary to get a precise volume. However, setting up the integrals correctly is often the main goal in problems like this.

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Key Concepts

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

Cylindrical Coordinates
Cylindrical coordinates are a way to describe three-dimensional regions using a combination of polar coordinates for the horizontal plane and Cartesian for the vertical dimension. They are particularly useful when dealing with regions of symmetry around a central axis, like cylinders.

This system is made up of three components:
  • \( r \): the radial distance from the origin in the horizontal \( xy \)-plane.
  • \( \theta \): the angular position measured counterclockwise from the positive \( x \)-axis.
  • \( z \): the vertical distance above the \( xy \)-plane, same as in Cartesian coordinates.
In converting the given equations to cylindrical coordinates:
  • The sphere's equation \(x^2 + y^2 + z^2 = 16\) becomes \(r^2 + z^2 = 16\).
  • The cylinder's equation \(x^2 + y^2 = 4\) becomes \(r = 2\), which is the fixed radius of the cylinder.
This conversion simplifies integration across symmetric shapes like cylinders and spheres, allowing the use of bounds: \(2 \leq r \leq 4\) and \(-\sqrt{16-r^2} \leq z \leq \sqrt{16-r^2}\).
Spherical Coordinates
Spherical coordinates represent points in three-dimensional space differently, using a radial distance, a polar angle, and an azimuthal angle. This is advantageous when working with spherical objects or boundaries.
  • \( \rho \): the distance from the origin to the point, essentially the radius in spherical terms.
  • \( \phi \): the angle between the positive \( z \)-axis and the line formed between the origin and the point.
  • \( \theta \): similar to cylindrical coordinates, this is the angle measured in the \( xy \)-plane.
To switch the existing Cartesian boundaries into spherical coordinates:
  • The sphere's equation becomes \(\rho = 4\), describing the constant radius of the sphere.
  • The cylinder \(x^2 + y^2 = 4\) gets reconceptualized into \(\sin \phi = \frac{2}{\rho}\), constraining \(\phi\) by the rotation mask of the cylinder.
This allows the bounds to be clearly defined as \(0 \leq \phi \leq \arcsin \left ( \frac{2}{\rho} \right )\) with \(2 \leq \rho \leq 4\) across the whole rotation \(0 \leq \theta \leq 2\pi\).
Volume of Solids
Computing the volume of solids using triple integrals requires setting up the correct bounds and integrating the volume elements over the specified region.

For problems like the one given, it's crucial to understand the spatial interplay between the sphere and the cylinder. The volume is inside the sphere (outer boundary) but outside the cylindrical cavity (inner boundary).

In both cylindrical and spherical coordinate solutions, the volume element needs to capture this region effectively:
  • Cylindrical coordinates use \(r \, dr \, d\theta \, dz\) as the volume element, integrating \(\theta\) from \(0\) to \(2\pi\), \(r\) from \(2\) to \(4\), and \(z\) within its bounds defined by the sphere.
  • Spherical coordinates apply \( \rho^2 \sin \phi \, d\rho \, d\phi \, d\theta\), incorporating the appropriate transformation of \(\phi\) based on the cylinder description.
Such transformations simplify the integration process and allow numerical or analytical methods to evaluate.Ensuring your bounds reflect the correct geometric constraints directly affects the accuracy of your volumetric solutions.

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Most popular questions from this chapter

If the charge density at an arbitrary point \((x, y, z)\) of a solid \(E\) is given by the function \(\rho(x, y, z)\), then the total charge inside the solid is defined as the triple integral \(\iiint_{E} \rho(x, y, z) d V .\) Assume that the charge density of the solid \(E\) enclosed by the paraboloids \(x=5-y^{2}-z^{2}\) and \(x=y^{2}+z^{2}-5\) is equal to the distance from an arbitrary point of \(E\) to the origin. Set up the integral that gives the total charge inside the solid \(E\).

The solid \(E\) bounded by the equation \(9 x^{2}+4 y^{2}+z^{2}=1\) and located in the first octant is represented in the following figure. a. Write the triple integral that gives the volume of \(E\) by integrating first with respect to \(z\), then with \(y\), and then with \(x\). b. Rewrite the integral in part a. as an equivalent integral in five other orders.

Evaluate the triple integrals over the bounded region \(E=\left\\{(x, y, z) \mid(x, y) \in D, u_{1}(x, y) x \leq z \leq u_{2}(x, y)\right\\}\), where \(D\) is the projection of \(E\) onto the \(x y\) -plane. $$ \iint_{D}\left(\int_{0}^{10-x-y}(x+2 z) d z\right) d A, \text { where } D=\\{(x, y) \mid y \geq 0, x \geq 0, x+y \leq 10\\} $$

In the following exercises, consider a lamina occupying the region \(R\) and having the density function \(\rho\) given in the first two groups of Exercises Find the moments of inertia \(I_{x}, I_{y}\), and \(I_{0}\) about the \(x\) -axis, \(y\) -axis, and origin, respectively. Find the radii of gyration with respect to the \(x\) -axis, \(y\) -axis, and origin, respectively.\(R\) is the region bounded by \(y=\frac{1}{x}, y=\frac{2}{x}, y=1\), and \(y=2 ; \rho(x, y)=4(x+y)\).

Consider the solid \(Q=\\{(x, y, z) \mid 0 \leq x \leq 1,0 \leq y \leq 2,0 \leq z \leq 3\\}\) with the density function \(\rho(x, y, z)=x+y+1\) a. Find the mass of \(Q\). b. Find the moments \(M_{x y}, M_{x z}\), and \(M_{y z}\) about the \(x y\) -plane, \(x z\) -plane, and \(y z\) -plane, respectively. c. Find the center of mass of \(Q\).

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