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As needed, use a computer to plot graphs and to check values of integrals. Find the volume inside the cone \(z^{2}=x^{2}+y^{2},\) above the \((x, y)\) plane, and between the spheres \(x^{2}+y^{2}+z^{2}=1\) and \(x^{2}+y^{2}+z^{2}=4 .\) Hint: Use spherical coordinates.

Short Answer

Expert verified
The volume inside the cone and between the spheres is \(\frac{14\pi}{3} (1 - \frac{1}{\sqrt{2}})\).

Step by step solution

01

- Convert to spherical coordinates

Use spherical coordinates where \(x = \rho \, \text{sin} \theta \, \text{cos} \phi \), \(\, y = \rho \, \text{sin} \theta \, \text{sin} \phi \, \), and \(\, z = \rho \, \text{cos} \theta \). The volume element in spherical coordinates is \(dV = \rho^2 \, \text{sin} \theta \, d\rho \, d\theta \, d\phi\).
02

- Determine the bounds for \(\rho\)

The volume is bounded by the spheres \(x^2 + y^2 + z^2 = 1\) and \(x^2 + y^2 + z^2 = 4\). Thus, \(\rho\) ranges from 1 to 2.
03

- Determine the bounds for \(\theta\)

The cone \(z^2 = x^2 + y^2\) translates to \(\text{cos}^2 \theta = \text{sin}^2 \theta \), meaning \(\theta\) ranges from 0 to \(\pi/4\).
04

- Determine the bounds for \(\phi\)

\(\phi\) represents the azimuthal angle, which ranges from 0 to \(2\pi\).
05

- Setup the integral

The integral to find the volume is \[V = \int_{0}^{2\pi} \int_{0}^{\pi/4} \int_{1}^{2} \rho^2 \, \text{sin} \theta \, d\rho \, d\theta \, d\phi \]
06

- Integrate with respect to \(\rho\)

Evaluate the inner integral: \[\int_{1}^{2} \rho^2 \, d\rho = \left[ \frac{\rho^3}{3} \right]_{1}^{2} = \frac{2^3}{3} - \frac{1^3}{3} = \frac{8}{3} - \frac{1}{3} = \frac{7}{3} \]
07

- Integrate with respect to \( \theta \)

Evaluate the next integral: \[ \int_{0}^{\pi/4} \frac{7}{3} \, \text{sin} \theta \, d\theta = \frac{7}{3} \left[- \text{cos} \theta \right]_{0}^{\pi/4} = \frac{7}{3} (1 - \frac{1}{\sqrt{2}}) \]
08

- Integrate with respect to \(\phi\)

Evaluate the outer integral: \[ \int_{0}^{2\pi} \frac{7}{3} (1 - \frac{1}{\sqrt{2}}) \, d\phi = \frac{7}{3} (1 - \frac{1}{\sqrt{2}}) \cdot 2\pi = \frac{14\pi}{3} (1 - \frac{1}{\sqrt{2}}) \]

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Key Concepts

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

spherical coordinates
Spherical coordinates are a three-dimensional coordinate system. They are used to define a point in space with three values: radial distance (\(\rho\)), polar angle (\(\theta\)), and azimuthal angle (\(\phi\)). These are helpful for problems involving symmetry such as spheres and cones. The relationship between rectangular coordinates \((x, y, z)\) and spherical coordinates is:
  • x = \(\rho \, \text{sin} \theta \, \text{cos} \phi \)
  • y = \(\rho \, \text{sin} \theta \, \text{sin} \phi \)
  • z = \(\rho \, \text{cos} \theta \)

Understanding these relationships allows you to transform a complex integral into a simpler form. For volume calculations in spherical coordinates, the volume element is \(dV = \rho^2 \, \text{sin} \theta \, d\rho \, d\theta \, d\phi \). This change of variables often simplifies the evaluation.
volume integral
A volume integral helps to find the volume of a three-dimensional region. When using spherical coordinates, the volume integral is written as:
  • \[V = \int_{volume} dV = \int_{0}^{2\pi} \int_{0}^{\pi/4} \int_{1}^{2} \rho^2 \, \text{sin} \theta \, d\rho \, d\theta \, d\phi \]

This integral sums up tiny volume elements across the given bounds. The bounds will typically derive from the geometric constraints of the problem, such as the sphere and cone in our example. Each integral is computed step-by-step, respecting the inner integral's bounds while moving outward.
multivariable calculus
Multivariable calculus extends the concepts of single-variable calculus to higher dimensions. It involves several variables and functions that depend on more than one variable. This field covers differentiation and integration in higher dimensions.
In our context, we use triple integrals to compute volume. It involves stepping through each variable in sequence, starting with the innermost until the complete integral is computed. This approach allows tackling complex regions and functions efficiently.
bounds determination
Determining the bounds for the variables is a crucial step in setting up a volume integral. Each variable will have its range dictated by the problem constraints.
In our exercise:
  • The radial distance \(\rho\) ranges from 1 to 2, given by the spheres \(x^2 + y^2 + z^2 = 1\) and \(x^2 + y^2 + z^2 = 4\).
  • The polar angle \(\theta\) ranges from 0 to \(\pi/4\), derived from the cone's equation \(z^2 = x^2 + y^2\).
  • The azimuthal angle \(\phi\) covers a full rotation around the z-axis, thus ranging from 0 to \(2\pi\).

Accurately determining these bounds is essential for setting up and solving the integral correctly.
integral evaluation
Evaluating the integral involves computing each part step-by-step while respecting the determined bounds. Here's how we do it in our example:
  • First, integrate with respect to \(\rho\): \[\int_{1}^{2} \rho^2 \, d\rho = \left[ \frac{\rho^3}{3} \right]_{1}^{2} = \frac{2^3}{3} - \frac{1^3}{3} = \frac{8}{3} - \frac{1}{3} = \frac{7}{3}\]
  • Next, integrate with respect to \(\theta\): \[\int_{0}^{\pi/4} \frac{7}{3} \, \text{sin} \theta \, d\theta = \frac{7}{3} \left[- \text{cos} \theta \right]_{0}^{\pi/4} = \frac{7}{3} (1 - \frac{1}{\sqrt{2}})\]
  • Finally, integrate with respect to \(\phi\): \[\int_{0}^{2\pi} \frac{7}{3} (1 - \frac{1}{\sqrt{2}}) \, d\phi = \frac{7}{3} (1 - \frac{1}{\sqrt{2}}) \cdot 2\pi = \frac{14\pi}{3} (1 - \frac{1}{\sqrt{2}})\]

Each integration step simplifies the expression further until we get the final volume solution.

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Most popular questions from this chapter

The following notation is used in the problems: \(M=\) mass, \(\bar{x}, \bar{y}, \bar{z}=\) coordinates of center of mass (or centroid if the density is constant), \(I=\) moment of inertia (about axis stated), \(I_{x}, I_{y}, I_{z}=\) moments of inertia about \(x, y, z\) axes, \(I_{m}=\) moment of inertia (about axis stated) through the center of mass. Note: It is customary to give answers for \(I, I_{m}, I_{x},\) etc., as multiples of \(M\) (for example, \(I=\frac{1}{3} M l^{2}\) ). A thin rod \(10 \mathrm{ft}\) long has a density which varies uniformly from 4 to \(24 \mathrm{lb} / \mathrm{ft}\). Find (a) \(M\), (b) \(\bar{x}\), (c) \(I_{m}\) about an axis perpendicular to the rod, (d) \(I\) about an axis perpendicular to the rod passing through the heavy end.

A triangular lamina is bounded by the coordinate axes and the line \(x+y=6\). Find its mass if its density at each point \(P\) is proportional to the square of the distance from the origin to \(P\).

The following notation is used in the problems: \(M=\) mass, \(\bar{x}, \bar{y}, \bar{z}=\) coordinates of center of mass (or centroid if the density is constant), \(I=\) moment of inertia (about axis stated), \(I_{x}, I_{y}, I_{z}=\) moments of inertia about \(x, y, z\) axes, \(I_{m}=\) moment of inertia (about axis stated) through the center of mass. Note: It is customary to give answers for \(I, I_{m}, I_{x},\) etc., as multiples of \(M\) (for example, \(I=\frac{1}{3} M l^{2}\) ). For a square lamina of uniform density, find \(I\) about (a) a side, (b) a diagonal, (c) an axis through a corner and perpendicular to the plane of the lamina. Hint: See the perpendicular axis theorem, Example 1f.

(a) Write a triple integral in spherical coordinates for the volume inside the cone \(z^{2}=x^{2}+y^{2}\) and between the planes \(z=1\) and \(z=2 .\) Evaluate the integral. (b) Do (a) in cylindrical coordinates.

(a) Using spherical coordinates, find the volume cut from the ball \(r \leq a\) by the cone \(\theta=\alpha<\pi / 2\). (b) Show that the \(z\) coordinate of the centroid of the volume in (a) is given by the formula \(\bar{z}=3 a(1+\cos \alpha) / 8\).

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