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Rotational Motion question

2015 · Shift 0 · Q66
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Rotational Motion question

2015 · Shift 0 · Q66

JEE MainPhysicsRotational MotionMCQ+4 / −1
From a solid sphere of mass MMM and radius RRR a cube of maximum possible volume is cut. Moment of inertia of cube about an axis passing through its center and perpendicular to one of its face is:
  1. A
    4MR293π{{4M{R^2}} \over {9\sqrt {3\pi } }}93π​4MR2​
  2. B
    4MR233π{{4M{R^2}} \over {3\sqrt {3\pi } }}33π​4MR2​
  3. C
    MR2322π{{M{R^2}} \over {32\sqrt {2\pi } }}322π​MR2​
  4. D
    MR2162π{{M{R^2}} \over {16\sqrt {2\pi } }}162π​MR2​
View written solutionFree

Correct answer: A

  1. Find the side of the largest cube that can be cut from the sphere

For a cube of side aaa inscribed in a sphere of radius RRR, the space diagonal of the cube equals the diameter of the sphere.

a3=2Ra\sqrt{3} = 2Ra3​=2R

So,

a=2R3a = \frac{2R}{\sqrt{3}}a=3​2R​


  1. Find the mass of the cube

Since the cube is cut from a uniform solid sphere, density remains same.

Let density be ρ\rhoρ.

Mass of sphere:

M=ρ⋅43πR3M = \rho \cdot \frac{4}{3}\pi R^3M=ρ⋅34​πR3

Hence,

ρ=M43πR3=3M4πR3\rho = \frac{M}{\frac{4}{3}\pi R^3} = \frac{3M}{4\pi R^3}ρ=34​πR3M​=4πR33M​

Volume of cube:

Vcube=a3=(2R3)3=8R333V_{\text{cube}} = a^3 = \left(\frac{2R}{\sqrt{3}}\right)^3 = \frac{8R^3}{3\sqrt{3}}Vcube​=a3=(3​2R​)3=33​8R3​

Therefore mass of cube is

m=ρa3=3M4πR3⋅8R333m = \rho a^3 = \frac{3M}{4\pi R^3} \cdot \frac{8R^3}{3\sqrt{3}}m=ρa3=4πR33M​⋅33​8R3​

m=2Mπ3m = \frac{2M}{\pi\sqrt{3}}m=π3​2M​


  1. Moment of inertia of the cube about an axis through its center and perpendicular to a face

For a cube (or cuboid) of mass mmm and side aaa, about an axis through center and perpendicular to one face:

I=112m(a2+a2)=16ma2I = \frac{1}{12}m(a^2+a^2) = \frac{1}{6}ma^2I=121​m(a2+a2)=61​ma2

Now substitute m=2Mπ3m = \frac{2M}{\pi\sqrt{3}}m=π3​2M​ and a=2R3a = \frac{2R}{\sqrt{3}}a=3​2R​.

First,

a2=4R23a^2 = \frac{4R^2}{3}a2=34R2​

So,

I=16⋅2Mπ3⋅4R23I = \frac{1}{6}\cdot \frac{2M}{\pi\sqrt{3}} \cdot \frac{4R^2}{3}I=61​⋅π3​2M​⋅34R2​

I=8MR218π3I = \frac{8MR^2}{18\pi\sqrt{3}}I=18π3​8MR2​

I=4MR29π3I = \frac{4MR^2}{9\pi\sqrt{3}}I=9π3​4MR2​

Now rewrite the denominator:

π3=3π2\pi\sqrt{3} = \sqrt{3\pi^2}π3​=3π2​

So the simplified standard form is

I=4MR29π3I = \frac{4MR^2}{9\pi\sqrt{3}}I=9π3​4MR2​

This does not match any option exactly as written. But option A is likely intended as

4MR293 π\frac{4MR^2}{9\sqrt{3}\,\pi}93​π4MR2​

which is algebraically the same as our result.

Thus the correct option is A.


  1. Option check
  • A: 4MR293 π\displaystyle \frac{4MR^2}{9\sqrt{3}\,\pi}93​π4MR2​ if interpreted properly, matches.
  • B: four times larger than correct value.
  • C, D: clearly inconsistent in dimensionless coefficient.

Hence, Option A is correct.

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