If \(I_1\) is the moment of inertia of a thin rod about an axis perpendicular to its length and passing through its centre of mass and \(I_2\) is the moment of inertia of the ring about an axis perpendicular to the plane of the ring and passing through its centre, formed by bending the rod, then:
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Key formulas to remember:
Rod (about centre, perpendicular): \(I = \dfrac{1}{12}ML^2\)
Ring (about centre, perpendicular): \(I = MR^2\)
When a rod is bent into a ring: \(L = 2\pi R\)
Always convert geometry correctly before comparing moments of inertia.
Step 1: Moment of inertia of the thin rod.
Let the mass of the rod be \(M\) and its length be \(L\).
The moment of inertia of a thin rod about an axis perpendicular to its length and passing through its centre of mass is:
\[
I_1 = \frac{1}{12} M L^2
\]
Step 2: Geometry of the ring formed by bending the rod.
When the rod is bent into a ring:
\[
\text{Circumference of ring} = L = 2\pi R
\]
\[
\Rightarrow R = \frac{L}{2\pi}
\]
Step 3: Moment of inertia of the ring.
The moment of inertia of a ring about an axis perpendicular to its plane and passing through its centre is:
\[
I_2 = M R^2
\]
Substitute \(R = \dfrac{L}{2\pi}\):
\[
I_2 = M \left(\frac{L}{2\pi}\right)^2
= \frac{M L^2}{4\pi^2}
\]
Step 4: Find the ratio \( \dfrac{I_1}{I_2} \).
\[
\frac{I_1}{I_2}
=
\frac{\dfrac{1}{12} M L^2}{\dfrac{M L^2}{4\pi^2}}
\]
Cancel \(M L^2\):
\[
\frac{I_1}{I_2}
=
\frac{1}{12} \times 4\pi^2
=
\frac{\pi^2}{3}
\]
Final Answer:
\[
\boxed{\dfrac{I_1}{I_2} = \dfrac{\pi^2}{3}}
\]