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Question: The moment of inertia of the hollow sphere of mass \( M \) and radius \( R \) about the tangential a...

The moment of inertia of the hollow sphere of mass MM and radius RR about the tangential axis is ……….

Explanation

Solution

The parallel axis theorem is also known as the Huygens Steiner theorem that is used for finding the moment of inertia about a parallel axis. By using the theorem of parallel axis, we will find the centre of mass of the hollow sphere and add the value of centre of mass and MR2M{R^2} .
The parallel axis theorem is given by
I=ICOM+MR2\Rightarrow I = {I_{COM}} + M{R^2}
Where, II is the moment of inertia about tangential axis, ICOM{I_{COM}} is the moment of inertia at the centre of the hollow sphere, MM is the mass of the hollow sphere and RR is the radius of the sphere.

Complete step by step solution:
It is given that the
Mass of the hollow sphere is MM
Radius of the hollow sphere about tangential axis is RR
We know that the moment of inertia at the centre of the hollow sphere is given by:
ICOM\Rightarrow {I_{COM}} = 25MR2\dfrac{2}{5}M{R^2}
Now using the formula, we get
I=ICOM+MR2\Rightarrow I = {I_{COM}} + M{R^2}
Putting the value of ICOM{I_{COM}} in the above formula of the parallel axis theorem, we get
I=25MR2+MR2\Rightarrow I = \dfrac{2}{5}M{R^2} + M{R^2}
By performing the basic arithmetic operation, we get
I=73MR2\Rightarrow I = \dfrac{7}{3}M{R^2}

Hence the moment of inertia of the hollow sphere about the tangential axis is given as 73MR2\dfrac{7}{3}M{R^2}.

Note:
The parallel axis theorem is also used for the rigid body by considering its inertia at a parallel axis and the perpendicular distance from the centre of the rigid mass. Where the perpendicular axis theorem is used for calculating moment of inertia of various shapes.