/*! 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 37 Use a computer algebra system to... [FREE SOLUTION] | 91Ó°ÊÓ

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Use a computer algebra system to find the exact volume of the solid. Enclosed by \(z=1-x^{2}-y^{2}\) and \(z=0\)

Short Answer

Expert verified
The exact volume is \(\frac{\pi}{2}\).

Step by step solution

01

Identify the Solid

The given equations describe a solid enclosed by the paraboloid \(z=1-x^2-y^2\) and the plane \(z=0\). The solid lies between these two surfaces.
02

Set Up the Integral

To find the volume, set up a double integral. The volume of the solid can be calculated by integrating the function \(1-x^2-y^2\) over the region \(R\) on the \(xy\)-plane, where \(z=0\) to \(z=1-x^2-y^2\).
03

Determine the Region of Integration

The region \(R\) is circular and determined by the boundary where \(z=1-x^2-y^2=0\), which simplifies to \(x^2 + y^2 = 1\). This is a circle with radius 1 centered at the origin.
04

Set Up the Polar Integral

Since the region is circular, convert to polar coordinates: \(x = r\cos(\theta), y = r\sin(\theta), \) and \(dA = r \, dr \, d\theta\). The limits for \(r\) are from 0 to 1, and for \(\theta\) from 0 to \(2\pi\).
05

Perform the Integration in Polar Coordinates

The integral becomes: \[ \int_{0}^{2\pi} \int_{0}^{1} (1 - r^2) r \, dr \, d\theta \]Integrate with respect to \(r\):\[ \int_{0}^{1} (r - r^3) \, dr = \left[ \frac{r^2}{2} - \frac{r^4}{4} \right]_{0}^{1} = \frac{1}{2} - \frac{1}{4} = \frac{1}{4} \]Then integrate with respect to \(\theta\):\[ \int_{0}^{2\pi} \frac{1}{4} \, d\theta = \frac{1}{4} [\theta]_{0}^{2\pi} = \frac{1}{4} (2\pi) = \frac{\pi}{2} \]
06

Conclude with the Volume

The volume of the solid enclosed by \(z=1-x^2-y^2\) and \(z=0\) is \(\frac{\pi}{2}\).

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Key Concepts

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

Paraboloid Volume
Calculating the volume of a paraboloid involves understanding the shape itself. A paraboloid is a three-dimensional solid, where each cross-section is a parabola. Visually, imagine an upside-down, bowl-like shape. In this exercise, the solid is defined by the paraboloid equation: \(z=1-x^2-y^2\), bounded by the plane \(z=0\).

The task is to find the volume of this solid lying above the region on the \(xy\)-plane and below the paraboloid surface. For this specific paraboloid, the peak is at \(z=1\) when both \(x\) and \(y\) are zero, and it extends downward until it meets the plane at \(z=0\). The bottom is circular, making it highly symmetrical, which aids in simplifying the calculations using polar coordinates.
Double Integral
Double integrals are a type of integral applied over two-dimensional areas. For volume calculations, they are exceptionally useful. A double integral can help find the volume underneath a surface and above a region on the plane.

In this exercise, the double integral is set up to calculate the volume of the solid paraboloid between the surface \(z=1-x^2-y^2\) and the plane \(z=0\). The function \(1-x^2-y^2\) reflects the height from the \(xy\)-plane at each point on the circular base.

To find the entire volume, you integrate this function over the circular region:
  • The inner integral computes the volume along the \(r\) axis.
  • The outer integral sums these along the \(\theta\) axis.
Converting to polar coordinates simplifies the process due to symmetry.
Polar Coordinates
Polar coordinates are a two-dimensional coordinate system where each point on a plane is determined by a distance from a reference point and an angle from a reference direction. Instead of using \(x\) and \(y\), you use \(r\) (radius) and \(\theta\) (angle).

In the context of the paraboloid, the region of integration is a circle. Using polar coordinates makes it easier to express points within this circular region. The conversions used are:
  • \(x = r\cos(\theta)\), \(y = r\sin(\theta)\)
  • The differential area element \(dA = r \, dr \, d\theta\).
The limits of integration change to reflect this: \(r\) ranges from 0 to 1 (the circle's radius), and \(\theta\) covers from 0 to \(2\pi\), a full revolution. This transformation simplifies integration for circular regions.
Region of Integration
Determining the region of integration is a crucial step in setting up a double integral. It indicates where on the plane you will apply the integral.

In this exercise, the region \(R\) is derived from the equation \(z=1-x^2-y^2=0\). This leads to the equation \(x^2 + y^2 = 1\), which is a circle with a radius of 1 centered at the origin on the \(xy\)-plane.

Recognizing this circular region enables you to utilize polar coordinates for integration. This simplifies the limits and the integration itself, due to the perfect symmetry of a circle. Understanding the region helps in setting up and visualizing the problem, ensuring accurate computation of the volume.

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Most popular questions from this chapter

(a) A lamp has two bulbs of a type with an average lifetime of 1000 hours. Assuming that we can model the probability of failure of these bulbs by an exponential density function with mean \(\mu=1000,\) find the probontity that both of the lamp's bulbs fail within 1000 hours. (b) Another lamp has just one bulb of the same type as in part (a). If one bulb burns out and is replaced by a bulb of the same type, find the probability that the two bulbs fail within a total of 1000 hours.

\(21-34\) Use spherical coordinates. (a) Find the volume of the solid that lies above the cone \(\phi=\pi / 3\) and below the sphere \(\rho=4 \cos \phi\) (b) Find the centroid of the solid in part (a).

$$\begin{array}{l}{\text { Evaluate } \iint_{D}\left(x^{2} \tan x+y^{3}+4\right) d A, \text { where }} \\ {D=\\{(x, y) | x^{2}+y^{2} \leqslant 2\\} . \text { IHint: Exploit the fact that }} \\ {D \text { is symmetric with respect to both axes. }}\end{array}$$

The latitude and longitude of a point \(P\) in the Northern Hemisphere are related to spherical coordinates \(\rho, \theta, \phi\) as follows. We take the origin to be the center of the earth and the positive \(z\) -axis to pass through the North Pole. The positive \(x\) -axis passes through the point where the prime meridian (the meridian through Greenwich, England) intersects the equator. Then the latitude of \(P\) is \(\alpha=90^{\circ}-\phi^{\circ}\) and the longitude is \(\beta=360^{\circ}-\theta^{\circ} .\) Find the great-circle distance from Los Angeles (lat. \(34.06^{\circ} \mathrm{N},\) long. \(118.25^{\circ} \mathrm{W}\) ) to Montreal (lat. \(45.50^{\circ} \mathrm{N},\) long. \(73.60^{\circ} \mathrm{W} ) .\) Take the radius of the earth to be 3960 \(\mathrm{mi} .\) (A great circle is the circle of intersection of a sphere and a plane through the center of the sphere.)

Assume that the solid has constant density \(k\) Find the moment of inertia about the \(z\) -axis of the solid cylinder \(x^{2}+y^{2} \leqslant a^{2}, 0 \leqslant z \leqslant h .\)

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