To find the volume of this solid, we use the same strategy as for area: slice the solid into many thin pieces and sum their volumes. In this case, each slice is a thin cylindrical disk. The key insight is that each disk is formed by rotating one of the thin rectangles from a Riemann sum around the \(x\)-axis.

The volume of a single cylinder is \(\pi r^2 h\). For a disk at position \(x_i\) with a small thickness \(\Delta x\):
- The radius is the height of the function, \(r = f(x_i)\).
- The height (thickness) of the disk is \(h = \Delta x\).
The volume of one disk is \(V_i = \pi [f(x_i)]^2 \Delta x\). The total volume is approximated by summing the volumes of all the disks:$$\begin{aligned}\mathcal{V}&\approx \sum_{i=0}^{n-1}V_i\\
&\approx \sum_{i=0}^{n-1} \pi [f(x_i)]^2 \Delta x\\
\end{aligned} $$To find the volume
exactly, we take the limit as the number of disks goes to infinity and their thickness approaches zero (\(\Delta x \to 0\)). This limit is the definite integral:$$\begin{aligned}\mathcal{V}&= \lim_{n \to \infty} \sum_{i=0}^{n-1} \pi [f(x_i)]^2 \Delta x\\
&= \int_a^b \pi [f(x)]^2\, dx\\
&=\pi \int_a^b [f(x)]^2\, dx\\
\end{aligned} $$