NVAMediumJEE 2025Moment of Inertia & Radius of Gyration

JEE Physics 2025 Question with Solution

M and R be the mass and radius of a disc. A small disc of radius R3\frac{R}{3} is removed from the bigger disc as shown in figure. The moment of inertia of remaining part of bigger disc about an axis AB passing through the centre O and perpendicular to the plane of disc is 4xMR2\frac{4}{x} MR^2. The value of x is _____.

Answer

Correct answer:9

Step-by-step solution

Standard Method

Given: Mass of the original disc is MM, radius is RR, and a small disc of radius R3\frac{R}{3} is removed. The required moment of inertia of the remaining part about the axis through OO and perpendicular to the plane is 4xMR2\frac{4}{x}MR^2.

Find: The value of xx.

Since the question says as shown in figure and the extracted figure is not available, the solution indicates the intended case is non-concentric (tangential) removal. Therefore the removed small disc has its centre at a distance 2R3\frac{2R}{3} from OO.

For the original disc,

Ioriginal=12MR2I_{\text{original}} = \frac{1}{2}MR^2

Because the disc is uniform, the mass of the removed small disc is proportional to area:

m=M(π(R/3)2πR2)=M9m = M\left(\frac{\pi (R/3)^2}{\pi R^2}\right) = \frac{M}{9}

Moment of inertia of the removed disc about its own centre is

Icm=12m(R3)2=12M9R29=MR2162I_{\text{cm}} = \frac{1}{2}m\left(\frac{R}{3}\right)^2 = \frac{1}{2}\cdot \frac{M}{9} \cdot \frac{R^2}{9} = \frac{MR^2}{162}

Using the parallel axis theorem for distance 2R3\frac{2R}{3},

Iremoved=Icm+m(2R3)2I_{\text{removed}} = I_{\text{cm}} + m\left(\frac{2R}{3}\right)^2 Iremoved=MR2162+M94R29I_{\text{removed}} = \frac{MR^2}{162} + \frac{M}{9}\cdot \frac{4R^2}{9} Iremoved=MR2162+4MR281=MR218I_{\text{removed}} = \frac{MR^2}{162} + \frac{4MR^2}{81} = \frac{MR^2}{18}

Hence the moment of inertia of the remaining part is

Iremaining=IoriginalIremoved=12MR2MR218I_{\text{remaining}} = I_{\text{original}} - I_{\text{removed}} = \frac{1}{2}MR^2 - \frac{MR^2}{18} Iremaining=49MR2I_{\text{remaining}} = \frac{4}{9}MR^2

Now compare with the given form:

4xMR2=49MR2\frac{4}{x}MR^2 = \frac{4}{9}MR^2

So,

4x=49\frac{4}{x} = \frac{4}{9} x=9x = 9

Therefore, the value of xx is 99.

Why the concentric answer is not used

Given: the solution discusses both concentric and non-concentric removal.

If the removed disc were concentric, then

Iremoved=MR2162I_{\text{removed}} = \frac{MR^2}{162}

and

Iremaining=12MR2MR2162=4081MR2I_{\text{remaining}} = \frac{1}{2}MR^2 - \frac{MR^2}{162} = \frac{40}{81}MR^2

This would give

4x=4081\frac{4}{x} = \frac{40}{81} x=8110x = \frac{81}{10}

which does not match the intended numerical answer.

The second approach in the solution explicitly notes that because the question refers to a figure, the intended geometry is the tangentially removed disc, for which the parallel axis theorem must be used. That produces

Iremaining=49MR2I_{\text{remaining}} = \frac{4}{9}MR^2

and hence x=9x = 9.

So the correct extracted answer is 99, and the first approach is incomplete because it ignores the offset shown in the missing figure.

Common mistakes

  • A common mistake is to subtract only the moment of inertia of the small disc about its own centre. That is wrong because the removed disc is not concentric with the big disc. Use the parallel axis theorem to calculate the removed part's moment of inertia about the axis through OO.

  • Another mistake is to take the mass of the removed disc as proportional to radius instead of area. For a uniform disc, mass is proportional to area, so the removed mass is m=M9m = \frac{M}{9}, not M3\frac{M}{3}.

  • Students may use the distance R3\frac{R}{3} in the parallel axis term. That is incorrect. The centre of the removed tangential disc is at distance 2R3\frac{2R}{3} from OO, so the shift term is m(2R3)2m\left(\frac{2R}{3}\right)^2.

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