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If the M.I. about diameter, for ring, di...

If the M.I. about diameter, for ring, disc, solid sphere and spherical shell of same radius and mass respectively be `I_(1), I_(2), I_(3) and I_(4)`, then:

A

`I_(1) gt I_(2) gt I_(3) gt I_(4)`

B

`I_(1) lt I_(2) lt I_(3) lt I_(4)`

C

`I_(4) gt I_(1) gt I_(3) gt I_(2)`

D

`I_(1) lt I_(4) lt I_(3) lt I_(2)`

Text Solution

AI Generated Solution

The correct Answer is:
To solve the problem of comparing the moment of inertia (M.I.) about the diameter for a ring, disc, solid sphere, and spherical shell of the same radius and mass, we will derive the expressions for each and then compare them step by step. ### Step-by-Step Solution: 1. **Moment of Inertia of a Ring (I1)**: - For a ring of mass \( m \) and radius \( R \), the moment of inertia about an axis perpendicular to the plane of the ring (through its center) is given by: \[ I_{z} = mR^2 \] - Using the perpendicular axis theorem, the moment of inertia about the diameter (which lies in the plane of the ring) is: \[ I_{D} = \frac{I_{z}}{2} = \frac{mR^2}{2} \] - Thus, we have: \[ I_{1} = \frac{mR^2}{2} \] 2. **Moment of Inertia of a Disc (I2)**: - For a disc of mass \( m \) and radius \( R \), the moment of inertia about an axis perpendicular to the plane of the disc (through its center) is: \[ I_{z} = \frac{1}{2} mR^2 \] - Again, using the perpendicular axis theorem, the moment of inertia about the diameter is: \[ I_{D} = \frac{I_{z}}{2} = \frac{1}{2} \left(\frac{1}{2} mR^2\right) = \frac{mR^2}{4} \] - Thus, we have: \[ I_{2} = \frac{mR^2}{4} \] 3. **Moment of Inertia of a Solid Sphere (I3)**: - For a solid sphere of mass \( m \) and radius \( R \), the moment of inertia about any axis through its center is given by: \[ I = \frac{2}{5} mR^2 \] - Since the sphere is symmetric, this is also the moment of inertia about the diameter: \[ I_{3} = \frac{2}{5} mR^2 \] 4. **Moment of Inertia of a Spherical Shell (I4)**: - For a spherical shell of mass \( m \) and radius \( R \), the moment of inertia about any axis through its center is given by: \[ I = \frac{2}{3} mR^2 \] - Thus, the moment of inertia about the diameter is: \[ I_{4} = \frac{2}{3} mR^2 \] 5. **Comparison of Moments of Inertia**: - Now we have: - \( I_{1} = \frac{mR^2}{2} \) - \( I_{2} = \frac{mR^2}{4} \) - \( I_{3} = \frac{2}{5} mR^2 \) - \( I_{4} = \frac{2}{3} mR^2 \) - To compare these values, we convert them to decimal forms: - \( I_{1} = 0.5 mR^2 \) - \( I_{2} = 0.25 mR^2 \) - \( I_{3} = 0.4 mR^2 \) - \( I_{4} = 0.6667 mR^2 \) - Ordering them from largest to smallest: \[ I_{4} > I_{1} > I_{3} > I_{2} \] ### Final Result: Thus, the order of the moment of inertia about the diameter for the ring, disc, solid sphere, and spherical shell is: \[ I_{4} > I_{1} > I_{3} > I_{2} \]
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