We're going to keep moving, into section
15.8: Cylindrical coordinates represents one generalization of polar
coordinates:
\[
x=r\cos{\theta} \hspace{1in}
y=r\sin{\theta} \hspace{1in}
r^2=x^2+y^2 \hspace{1in}
z=z
\]
So it represents a polar coordinate transformation for two coordinates, and leaves $z$ untransformed.
The volume element ($dV$) is given by $rdrd{\theta}dz$, as one can see in Figure 7, p. 1054:
This is a simple
generalization of the polar formula of the area element $dA$.
Examples:
- #1, p. 1055
- #3
- #13
- let's revisit the problem, #20, p. 1049.
- #26
- Then we'll try #31 -- Mt. Fuji!