MCQMediumJEE 2026Moment of Inertia & Radius of Gyration

JEE Physics 2026 Question with Solution

The pulley shown in figure is made using a thin rim and two rods of length equal to diameter of the rim. The rim and each rod have a mass of MM. Two blocks of mass of MM and mm are attached to two ends of a light string passing over the pulley, which is hinged to rotate freely in vertical plane about its center. The magnitudes of the acceleration experienced by the blocks is _____ (assume no slipping of string on pulley).

A pulley with a circular rim and two crossed diametrical rods, with a light string over it carrying blocks m and M on opposite sides.
  • A

    (Mm)g(136)M+m\frac{(M-m)g}{\left(\frac{13}{6}\right)M + m}

  • B

    (Mm)g(83)M+m\frac{(M-m)g}{\left(\frac{8}{3}\right)M + m}

  • C

    (Mm)g2M+m\frac{(M-m)g}{2M + m}

  • D

    (Mm)gM+m\frac{(M-m)g}{M + m}

Answer

Correct answer:B

Step-by-step solution

Standard Method

Given: Masses of the two blocks are MM and mm. The pulley consists of a thin rim of mass MM and two rods, each of mass MM and length equal to the diameter 2R2R.

Find: The magnitude of acceleration of the blocks.

For an Atwood machine with a massive pulley,

a=(Mm)gM+m+IR2a = \frac{(M-m)g}{M + m + \frac{I}{R^2}}

So we first calculate the moment of inertia of the pulley.

For the thin rim,

Irim=MR2I_{\text{rim}} = MR^2

For each rod of length 2R2R rotating about its midpoint,

Irod=112M(2R)2=13MR2I_{\text{rod}} = \frac{1}{12}M(2R)^2 = \frac{1}{3}MR^2

Since there are two rods,

I=Irim+2Irod=MR2+2(13MR2)=53MR2I = I_{\text{rim}} + 2I_{\text{rod}} = MR^2 + 2\left(\frac{1}{3}MR^2\right) = \frac{5}{3}MR^2

Now,

IR2=53M\frac{I}{R^2} = \frac{5}{3}M

Substituting in the acceleration formula,

a=(Mm)g83M+ma = \frac{(M-m)g}{\frac{8}{3}M + m}

Therefore, the correct option is B.

Effective Mass Idea

Given: The pulley has rotational inertia, so it contributes an effective translational mass of IR2\frac{I}{R^2}.

Find: The acceleration using the effective-mass approach.

The total effective mass resisting motion is

M+m+IR2M + m + \frac{I}{R^2}

The pulley has

  • rim contribution: MR2MR^2
  • two rod contributions: 2×13MR22 \times \frac{1}{3}MR^2

So,

I=MR2+23MR2=53MR2I = MR^2 + \frac{2}{3}MR^2 = \frac{5}{3}MR^2

Hence,

IR2=53M\frac{I}{R^2} = \frac{5}{3}M

Thus,

a=(Mm)gM+m+53M=(Mm)g83M+ma = \frac{(M-m)g}{M + m + \frac{5}{3}M} = \frac{(M-m)g}{\frac{8}{3}M + m}

This works because the pulley's rotational inertia appears as an additional inertia term in the denominator. Therefore, the correct option is B.

Common mistakes

  • Using only the masses of the blocks in the denominator and ignoring the pulley inertia is incorrect. The pulley is massive and rotating, so add IR2\frac{I}{R^2} to the effective mass.

  • Taking the moment of inertia of each rod as MR2MR^2 is wrong. Each rod is a slender rod of length 2R2R about its midpoint, so use Irod=112M(2R)2=13MR2I_{\text{rod}} = \frac{1}{12}M(2R)^2 = \frac{1}{3}MR^2.

  • Forgetting that there are two rods leads to an underestimated pulley inertia. After finding inertia of one rod, multiply by 22 before adding the rim contribution.

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