MCQEasyJEE 2025Moment of Inertia & Radius of Gyration

JEE Physics 2025 Question with Solution

Moment of inertia of a rod of mass MM and length LL about an axis passing through its center and normal to its length is α\alpha. Now the rod is cut into two equal parts and these parts are joined symmetrically to form a cross shape. Moment of inertia of cross about an axis passing through its center and normal to the plane containing cross is:

  • A

    α\alpha

  • B

    α4\frac{\alpha}{4}

  • C

    α8\frac{\alpha}{8}

  • D

    α2\frac{\alpha}{2}

Answer

Correct answer:B

Step-by-step solution

Standard Method

Given: The moment of inertia of the original rod is

α=ML212\alpha = \frac{ML^2}{12}

where the rod has mass MM and length LL.

Find: The moment of inertia of the cross formed by joining the two equal halves, about an axis passing through its center and normal to the plane of the cross.

When the rod is cut into two equal parts, each smaller rod has mass

m=M2m = \frac{M}{2}

and length

l=L2l = \frac{L}{2}

The axis through the center of the cross and normal to its plane passes through the center of each small rod and is perpendicular to its length.

So, for one small rod,

Ismall=ml212I_{\text{small}} = \frac{ml^2}{12}

Substituting the values,

Ismall=(M2)(L2)212=ML296I_{\text{small}} = \frac{\left(\frac{M}{2}\right)\left(\frac{L}{2}\right)^2}{12} = \frac{ML^2}{96}

The cross consists of two identical small rods, so by superposition,

Icross=2Ismall=2×ML296=ML248I_{\text{cross}} = 2I_{\text{small}} = 2 \times \frac{ML^2}{96} = \frac{ML^2}{48}

Using

α=ML212\alpha = \frac{ML^2}{12}

we get

Icross=ML248=14(ML212)=α4I_{\text{cross}} = \frac{ML^2}{48} = \frac{1}{4}\left(\frac{ML^2}{12}\right) = \frac{\alpha}{4}

Therefore, the moment of inertia of the cross is α4\frac{\alpha}{4}. The correct option is B.

Using the rod formula for each half

Given: The original rod has moment of inertia

α=ML212\alpha = \frac{ML^2}{12}

Find: The moment of inertia of the new cross-shaped system.

The original rod is divided into two equal rods. For each part:

m=M2,l=L2m = \frac{M}{2}, \qquad l = \frac{L}{2}

The moment of inertia of a thin rod about an axis through its center and perpendicular to its length is

I=ml212I = \frac{ml^2}{12}

Hence for one part,

I=(M2)(L2)212I = \frac{\left(\frac{M}{2}\right)\left(\frac{L}{2}\right)^2}{12} I=(M2)(L24)12I = \frac{\left(\frac{M}{2}\right)\left(\frac{L^2}{4}\right)}{12} I=ML296I = \frac{ML^2}{96}

Since two such rods form the cross,

Icross=ML296+ML296=ML248I_{\text{cross}} = \frac{ML^2}{96} + \frac{ML^2}{96} = \frac{ML^2}{48}

Now compare with

α=ML212\alpha = \frac{ML^2}{12}

Therefore,

Icross=ML248=α4I_{\text{cross}} = \frac{ML^2}{48} = \frac{\alpha}{4}

So the correct option is B.

Common mistakes

  • Using the original rod formula directly for the cross is incorrect because after cutting, each piece has mass M2\frac{M}{2} and length L2\frac{L}{2}. First compute the moment of inertia of one smaller rod, then add the two contributions.

  • Assuming the moment of inertia doubles without accounting for the reduced length is wrong. Moment of inertia depends on both mass and the square of length, so halving the length changes the value significantly.

  • Applying the parallel axis theorem unnecessarily can lead to error here. The required axis passes through the center of each small rod in the cross arrangement, so use the center formula I=ml212I = \frac{ml^2}{12} directly for each half.

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