MCQEasyJEE 2025Theorems of M.I (Parallel & Perpendicular Axis)

JEE Physics 2025 Question with Solution

The moment of inertia of a circular ring of mass MM and diameter rr about a tangential axis lying in the plane of the ring is:

  • A

    38Mr2\frac{3}{8} M r^2

  • B

    32Mr2\frac{3}{2} M r^2

  • C

    2Mr22 M r^2

  • D

    Option unavailable in scraped data

Answer

Correct answer:A

Step-by-step solution

Standard Method

Given: A circular ring has mass MM and diameter rr.

Find: The moment of inertia about a tangential axis lying in the plane of the ring.

For a ring, if the diameter is rr, then the radius is

R=r2R = \frac{r}{2}

The moment of inertia of a ring about a diametral axis through the center and lying in its plane is

Icenter, diametral=12MR2I_{\text{center, diametral}} = \frac{1}{2}MR^2

Using the parallel axis theorem for the tangential axis at distance RR from the center,

Itangent, in-plane=Icenter, diametral+MR2I_{\text{tangent, in-plane}} = I_{\text{center, diametral}} + MR^2 Itangent, in-plane=12MR2+MR2=32MR2I_{\text{tangent, in-plane}} = \frac{1}{2}MR^2 + MR^2 = \frac{3}{2}MR^2

Now substitute R=r2R = \frac{r}{2}:

Itangent, in-plane=32M(r2)2=38Mr2I_{\text{tangent, in-plane}} = \frac{3}{2}M\left(\frac{r}{2}\right)^2 = \frac{3}{8}Mr^2

Therefore, the moment of inertia is 38Mr2\frac{3}{8}Mr^2. The correct option is A.

The solution states the correct option is B, but the listed listed options begin at (2), so the worked value 38Mr2\frac{3}{8}Mr^2 corresponds to the first available option in the recorded data.

Using the Parallel Axis Theorem

Given: Mass of ring =M= M, diameter =r= r.

Find: Moment of inertia about a tangent in the plane of the ring.

Concept used: Parallel Axis Theorem.

For a circular ring of radius RR,

Icenter, diametral=12MR2I_{\text{center, diametral}} = \frac{1}{2}MR^2

The tangential axis in the plane is parallel to this diametral axis and is displaced by distance RR. So,

I=Icenter+Md2I = I_{\text{center}} + Md^2

with

d=Rd = R

Hence,

I=12MR2+MR2I = \frac{1}{2}MR^2 + MR^2 I=32MR2I = \frac{3}{2}MR^2

Since the given diameter is rr,

R=r2R = \frac{r}{2}

Substituting,

I=32M(r2)2I = \frac{3}{2}M\left(\frac{r}{2}\right)^2 I=38Mr2I = \frac{3}{8}Mr^2

Thus, the required moment of inertia is 38Mr2\frac{3}{8}Mr^2.

Common mistakes

  • Using the moment of inertia about the axis perpendicular to the plane, I=MR2I = MR^2, instead of the diametral in-plane axis. This is wrong because the tangent axis in the plane is parallel to the diametral axis, not the perpendicular axis. Use Icenter, diametral=12MR2I_{\text{center, diametral}} = \frac{1}{2}MR^2 first.

  • Treating the given diameter rr as the radius. This is incorrect because the radius is r2\frac{r}{2}. Always convert diameter to radius before substitution.

  • Applying the parallel axis theorem with the wrong shift distance. The tangential in-plane axis is at a distance RR from the center, not r2\frac{r}{2} after separately redefining symbols incorrectly. Keep the geometry clear and use one consistent radius symbol.

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