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Given :-
Radius of small disc = R
Radius of large disc = 2R
As the density of disc is constant.
Mass of larger disc = M = σ π(2R)²
M = 4σπR²
Similarly,
Mass of smaller disc = m = σ πR²
m = σ πR²
Now,
Moment of Inertia of Larger disc = I = MR²/2
I = 4σπR²(2R)²/2
I = 16σπR⁴/2
I = 8σπR⁴
Again,
Moment of Inertia of smaller disc about Perpendicular to the plane = I' = σπR²(R)²
I' = σπR⁴
Using Parallel axes theorem we will find the Centre of Mass of smaller disc along the tangential.
I* = I + mR²
I* = mR² + mR²/2
I* = 3mR²/2
I* = 3(σπR²)(R²)/2
I* = 3σπR⁴/2
Now,
For Moment of Inertia of Remaining disc.
Let the Moment of Inertia of Remaining disc = M
M = I - I*
M = 8σπR⁴ - 3σπR⁴/2
M = (16σπR⁴ - 3σπR⁴)/2
M = 13σπR⁴/2
Hence,
Option (B) is correct.
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