You can also find the moment of inertia of a disk (in fact a disk is a cylinder). You can use the moment of inertia of a disk to find the moment of inertia of a solid sphere.
First consider a cylinder of height \(h\) whose inner radius is \(R_1\) and outer radius is \(R_2\) as shown in Figure 1. The cylinder rotates about an axis which passes through the centres of the cross sections of the cylinder.
![](/images/user/7/uploads/fig4.14.png)
And we consider an infinitesimally small volume element of the cylinder of mass \(dm\) and thickness \(dr\). The inner radius of the element is \(r\) and outer radius is \(r + dr\). The volume of the element of the cylinder is \(dV = 2\pi r{\kern 1pt} dr{\kern 1pt} h\) and the mass of the element is \(dm = \rho dV = 2\rho \pi r{\kern 1pt} dr{\kern 1pt} h\). Here \(\rho \) is the density of the cylinder. So the moment of inertia of the element is
\[dI = dm{\kern 1pt} {\kern 1pt} {r^2} = (2\rho \pi r{\kern 1pt} dr{\kern 1pt} h){r^2} = (2\rho \pi h){r^3}dr\]
The total moment of inertia of the whole cylinder is obtained by integrating the moment of inertia \(dI\) from \(R_1\) to \(R_2\):
\[\begin{align*} I &= 2\rho \pi h\int\limits_{{R_1}}^{{R_2}} {{r^3}dr} = 2\rho \pi h\left( {\frac{{R_2^4}}{4} - \frac{{R_1^4}}{4}} \right)\\ {\rm{or,}}\quad I &= \frac{{\rho \pi h}}{2}(R_2^4 - R{}_1^4) \end{align*}\]
The total volume of the cylinder is \(V = \pi h(R_2^2 - R_1^2)\). If \(M\) is the total mass of the cylinder, the density is \(\rho = \frac{M}{V} = \frac{M}{{\pi h(R_2^2 - R_1^2)}}\). Thus, putting the value of \(\rho\) in the above expression for the total moment of inertia \(I\) we get,
\[I = \frac{{\pi hM(R_2^4 - R{}_1^4)}}{{2\pi h(R_2^2 - R_1^2)}} = \frac{1}{2}M(R_1^2 + R_2^2)\]
Case 1: If the cylinder is solid that is, \(R_1 = 0\) the moment of inertia is \(I = \frac{1}{2}MR_2^2 = \frac{1}{2}MR_{}^2\). There is only one radius, so \(R_2\) is written as \(R\). This is also the moment of inertia of a disk.
Case 2: When \(R_1 = R_2 = R\) the moment of inertia of the cylinder becomes \(I = MR_{}^2\). This is the same as the moment of inertia of a body of mass \(M\) about an axis at a distance \(R\) from the axis of rotation. This result is the same as the moment of inertia of a thin circular ring about the axis through its centre and perpendicular to its plane.