A disc of mass \(M\) and radius \(R\) has a concentric hole of radius \(R/2\). Its moment of inertia about an axis passing through its center and perpendicular to its plane is:
Show Hint
For an annular disc:
\[
I=\frac12 M(R_1^2+R_2^2)
\]
where:
\[
R_1=\text{inner radius}
\]
\[
R_2=\text{outer radius}
\]
This formula is extremely important for rotational motion problems.
Concept:
The given body is an annular disc (ring-shaped disc).
Moment of inertia of a disc about its center:
\[
I=\frac12 MR^2
\]
For an annular disc with inner radius \(R_1\) and outer radius \(R_2\):
\[
I=\frac12 M(R_1^2+R_2^2)
\]
Step 1: Identifying inner and outer radii.
Outer radius:
\[
R_2=R
\]
Inner radius:
\[
R_1=\frac{R}{2}
\]
Step 2: Substituting into the annular disc formula.
\[
I
=
\frac12 M
\left[
\left(\frac{R}{2}\right)^2+R^2
\right]
\]
\[
=
\frac12 M
\left[
\frac{R^2}{4}+R^2
\right]
\]
\[
=
\frac12 M
\left[
\frac{5R^2}{4}
\right]
\]
\[
I
=
\frac{5}{8}MR^2
\]
Thus, the moment of inertia is:
\[
\boxed{\frac{5}{8}MR^2}
\]