Solids with a vertical axis of symmetry (cans, pipes, bowls, cones) are described simply in cylindrical coordinates: polar coordinates for the floor plus the height $z$. Combining the polar area element with a height step gives the volume element.
Key idea
Why it works
To set up the limits, describe the solid in three stages. First, its shadow on the $xy$-plane, in polar form: this gives the limits for $\theta$ and $r$. Second, for a point $(r, \theta)$ in the shadow, the bottom and top surfaces above it: these give the limits for $z$, written in terms of $r$ and $\theta$. Third, multiply the integrand by $r$. For example, the solid inside $x^2 + y^2 = 1$ between $z = 0$ and the plane $z = 2 + x$ has shadow ${}0 \le r \le 1$, ${}0 \le \theta \le 2\pi$, and ${}0 \le z \le 2 + r\cos\theta$. Its volume is $\int_0^{2\pi} \int_0^1 (2 + r\cos\theta)\,r\,dr\,d\theta = 2\pi$.
Worked examples
Worked example: Under a paraboloid
- In cylindrical form the top is $z = 4 - r^2$, which meets the floor at $r = 2$.
- $$V = \int_0^{2\pi}\int_0^2\int_0^{4 - r^2} r\,dz\,dr\,d\theta = \int_0^{2\pi}\int_0^2 (4r - r^3)\,dr\,d\theta.$$
- $= 2\pi\left[2r^2 - \frac{r^4}{4}\right]_0^2 = 2\pi(8 - 4) = 8\pi$.
Answer: ${}8\pi$
Worked example: A weighted cylinder
- $x^2 + y^2 = r^2$, so the integrand times $r$ is $r^3$.
- $$\int_0^{2\pi}\int_0^2\int_0^3 r^3\,dz\,dr\,d\theta = 2\pi \cdot 4 \cdot 3 = 24\pi.$$
Answer: ${}24\pi$
Worked example: Between a cone and a sphere
- Cylindrically: $r \le z \le \sqrt{2 - r^2}$. The surfaces meet where $r^2 = 2 - r^2$, at $r = 1$.
- $$V = 2\pi\int_0^1 \left(r\sqrt{2 - r^2} - r^2\right) dr = 2\pi\left[-\frac{(2 - r^2)^{3/2}}{3} - \frac{r^3}{3}\right]_0^1.$$
- $$= 2\pi\left(-\frac{1}{3} - \frac{1}{3} + \frac{2\sqrt{2}}{3}\right) = \frac{4\pi}{3}\left(\sqrt{2} - 1\right).$$
Answer: $\frac{4\pi}{3}\left(\sqrt{2} - 1\right)$
Common mistake