Question:

The moment of inertia of a solid sphere of mass 20 kg and diameter 20 cm about the tangent to the sphere is:

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Updated On: May 16, 2025
  • \( 0.24 \, \text{kgm}^2 \)
  • \( 0.14 \, \text{kgm}^2 \)
  • \( 0.28 \, \text{kgm}^2 \)
  • \( 0.08 \, \text{kgm}^2 \)
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The Correct Option is C

Approach Solution - 1

The moment of inertia \( I \) of a solid sphere about an axis through its center is given by:
\[ I_{\text{center}} = \frac{2}{5} m r^2 \]
where \( m = 20 \, \text{kg} \) is the mass of the sphere and \( r = 0.1 \, \text{m} \) is the radius (half the diameter of 20 cm).
Substituting the values:
\[ I_{\text{center}} = \frac{2}{5} \times 20 \times (0.1)^2 = \frac{2}{5} \times 20 \times 0.01 = 0.08 \, \text{kgm}^2 \]
To find the moment of inertia about a tangent, we use the parallel axis theorem:
\[ I_{\text{tangent}} = I_{\text{center}} + m d^2 \]
Here, \( d = r = 0.1 \, \text{m} \) because the tangent is parallel and at a distance equal to the radius from the center.
Thus,
\[ I_{\text{tangent}} = 0.08 + 20 \times (0.1)^2 = 0.08 + 0.2 = 0.28 \, \text{kgm}^2 \]
The correct moment of inertia about the tangent to the sphere is \( 0.28 \, \text{kgm}^2 \).
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Approach Solution -2

We are given the following: - Mass of the solid sphere \( M = 20 \, \text{kg} \), - Diameter of the sphere \( D = 20 \, \text{cm} = 0.2 \, \text{m} \), - The moment of inertia is to be calculated about the tangent to the sphere. The moment of inertia \( I_{\text{sphere}} \) of a solid sphere about its center of mass is given by the formula: \[ I_{\text{sphere}} = \frac{2}{5} M R^2, \] where \( M \) is the mass and \( R \) is the radius of the sphere. 
Step 1: Moment of inertia about the center For a sphere with mass \( M = 20 \, \text{kg} \) and radius \( R = \frac{D}{2} = \frac{0.2}{2} = 0.1 \, \text{m} \), the moment of inertia about the center is: \[ I_{\text{center}} = \frac{2}{5} \times 20 \times (0.1)^2 = \frac{2}{5} \times 20 \times 0.01 = 0.08 \, \text{kgm}^2. \] 
Step 2: Using the parallel axis theorem To find the moment of inertia about a tangent to the sphere, we use the parallel axis theorem: \[ I_{\text{tangent}} = I_{\text{center}} + M R^2. \] Substituting the values: \[ I_{\text{tangent}} = 0.08 + 20 \times (0.1)^2 = 0.08 + 20 \times 0.01 = 0.08 + 0.2 = 0.28 \, \text{kgm}^2. \] Thus, the moment of inertia about the tangent to the sphere is \( 0.28 \, \text{kgm}^2 \). 
Therefore, the correct answer is option (3).

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