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:
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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.