In this section, we will learn two methods for computing the volumes of solids of revolution. A solid of revolution is a solid figure obtained by revolving a region in the plane around some straight line, called the axis of revolution.

- Some examples of solids of revolution in engineering and manufacturing are pistons, axles, and funnels. Solids of revolution are also widely used in architecture (Figure 1).

Table of Contents

## Disk Method

Consider the region bounded by the curve \(y=f(x)\), the \(x\)-axis, and the vertical lines \(x=a\) and \(x=b\) (Figure 2(a)). If this region is revolved around the \(x\)-axis, it generates a three-dimensional body called a **solid of revolution** (Figure 2(b)).

(a) | (b) |

*Figure 2*

Figure 3(a) shows the region itself together with a typical infinitesimally thin rectangle of height \(f(x)\) and width \(dx\). When this rectangle is revolved, we obtain a circular disk in the form of a thin right circular cylinder with base radius \(f(x)\) and thickness is \(dx\) (Figure 3(b)). The volume of this disk, which is our element of volume \(dV\), is then \[dV=\pi[f(x)]^{2}dx.\] [Recall that the volume of a right circular cylinder of radius \(R\) and height (or thickness) \(h\) is area of the base \(\times\) thickness = \(\pi R^{2}h\).]

(a) | (b) |

*Figure 3*

The solid is composed of infinitely many infinitesimally thin disks like this. So, its total volume is obtained by adding up all the elements of volume as the typical disk sweeps through the solid from left to right. That is, \[V=\int_{a}^{b}dV=\int_{a}^{b}\pi[f(x)]^{2}dx.\] This method of finding volume is called the **disk method**.

**Volume of a Solid of Revolution: Disk Method:**

If the region bounded by the curve \(y=f(x)\), the \(x\)-axis, \(x=a\), and \(x=b\) is revolved about the \(x\)-axis, the volume of the solid generated this way is \[V=\pi\int_{a}^{b}[f(x)]^{2}dx.\]

### Revolving About the y-Axis

If the region bounded by the curve \(x=h(y)\), the \(y\)-axis, and the horizontal lines \(y=c\) and \(y=d\) (\(c<d\)) is revolved about the \(y\)-axis, we can compute the volume of the resulting solid in a similar way (Figure 4).

*Figure 4: The element of volume is \(dV=\pi[h(y)]^{2}dy\) and the total volume is \(V=\int_{a}^{b}dV=\pi\int_{c}^{d}[h(y)]^{2}dy=\pi\int_{c}^{d}x^{2}dy\).*

## Washer Method

The washer method is a generalization of the disk method. Actually, a washer is a disk with a hole. Suppose \(R\) is a region enclosed by the curves \(y=f(x)\) and \(y=g(x)\) (with \(f(x)\geq g(x)\)) on \([a,b]\) and \(R\) is revolved about the \(x\)-axis (Figure 12(a)). To compute the volume of this solid, consider an infinitely thin vertical rectangle. When this rectangle is revolved about the \(x\)-axis, it generates an infinitely thin circular hollow cylinder whose outer radius is \(f(x)\) and whose inner radius is \(g(x)\) (Figure 12(b)). The volume of this hollow cylinder, which is our element of volume, is \[dV=\pi\left([f(x)]^{2}-[g(x)]^{2}\right)dV\] [Recall that the volume of a right circular hollow cylinder of outer radius \(R\), inner radius \(r\), and height (or thickness) \(h\) is area of the base \(\times\) thickness = \(\pi(R^{2}-r^{2})h\).] and the total volume is \[V=\int_{a}^{b}dV=\pi\int_{a}^{b}\left([f(x)]^{2}-[g(x)]^{2}\right)dx.\]

(a) | (b) |

*Figure 12 *

In fact, the volume of this solid is the volume of the solid generated by revolving the region bounded by the curve \(y=f(x)\) and the \(x\)-axis minus the volume of the solid generated by revolving the region bounded by the curve \(y=g(x)\) and the \(x\)-axis (Figure 13). That is,

\[V=\pi\int_a^b[f(x)]^2\,dx-\pi\int_a^b[g(x)]^2\,dx.\]

*Figure 13*