A disc of mass $M$ and radius $R$ has a concentric hole of radius $\dfrac{R}{2}$. Its moment of inertia about an axis passing through its center and perpendicular to its plane is:
Show Hint
For an annular disc:
\[
I = \frac{1}{2}M(R_1^2 + R_2^2)
\]
Always check whether the given mass belongs to the original disc or the remaining annular disc.
Concept:
The given body is an annular disc (ring-shaped disc).
Moment of inertia is calculated by subtracting the inner removed disc from the full disc.
For a solid disc:
\[
I = \frac{1}{2}MR^2
\]
For an annular disc:
\[
I = \frac{1}{2}M(R_1^2 + R_2^2)
\]
where:
• $R_1$ = outer radius
• $R_2$ = inner radius
Step 1: Identify radii.
Outer radius:
\[
R_1 = R
\]
Inner radius:
\[
R_2 = \frac{R}{2}
\]
Step 2: Substitute into annular disc formula.
\[
I
=
\frac{1}{2}M
\left(
R^2 + \left(\frac{R}{2}\right)^2
\right)
\]
\[
I
=
\frac{1}{2}M
\left(
R^2 + \frac{R^2}{4}
\right)
\]
\[
I
=
\frac{1}{2}M
\left(
\frac{5R^2}{4}
\right)
\]
\[
I
=
\frac{5}{8}MR^2
\]
This expression corresponds to mass of the annular disc itself.
But in the question, $M$ denotes the mass of the original full disc before removal.
Step 3: Relate remaining mass with original mass.
Area ratio:
\[
\text{Remaining area}
=
\pi R^2 - \pi \left(\frac{R}{2}\right)^2
\]
\[
=
\pi R^2 - \frac{\pi R^2}{4}
=
\frac{3\pi R^2}{4}
\]
Thus remaining mass:
\[
M' = \frac{3M}{4}
\]
Now substitute:
\[
I
=
\frac{5}{8}
\left(
\frac{3M}{4}
\right)
R^2
\]
\[
I
=
\frac{15}{32}MR^2
\]
Step 4: Conclusion.
Hence, the correct answer is:
\[
\boxed{\frac{15}{32}MR^2}
\]