Find the mass of the solid bounded by the paraboloid z=x^{2}+y^{2} and the plane z=4 if the density at any point is proportional to the distance from the point to the z-axis.
Find the mass of the solid bounded by the paraboloid z=x^{2}+y^{2} and the plane z=4 if the density at any point is proportional to the distance from the point to the z-axis.
The solid is sketched in Figure 2. The density is given by \rho(x, y, z)= \alpha \sqrt{x^{2}+y^{2}}, where \alpha is a constant of proportionality. Thus since the solid may be written as S=\left\{(x, y, z):-2 \leq x \leq 2,-\sqrt{4-x^{2}} \leq y \leq \sqrt{4-x^{2}}, x^{2}+y^{2} \leq z \leq 4\right\}
we have
\mu=\iiint_{S} \alpha \sqrt{x^{2}+y^{2}} d V=\int_{-2}^{2} \int_{-\sqrt{4-x^{2}}}^{\sqrt{4-x^{2}}} \int_{x^{2}+y^{2}}^{4} \alpha \sqrt{x^{2}+y^{2}} d z d y d xWe write this expression in cylindrical coordinates, using the fact that \alpha \sqrt{x^{2}+y^{2}}= \alpha r. We note that the largest value of r is 2, since at the “top” of the solid, r^{2}=x^{2}+y^{2}=4. Then
\begin{aligned}\mu &=\int_{0}^{2 \pi} \int_{0}^{2} \int_{r^{2}}^{4}(\alpha r) r d z d r d \theta=\int_{0}^{2 \pi} \int_{0}^{2} \alpha r^{2}\left(4-r^{2}\right) d r d \theta \\&=\alpha \int_{0}^{2 \pi}\left\{\left.\left(\frac{4 r^{3}}{3}-\frac{r^{5}}{5}\right)\right|_{0} ^{2}\right\} d \theta=\frac{64 \alpha}{15} \int_{0}^{2 \pi} d \theta=\frac{128}{15} \pi \alpha.\end{aligned}