For a ring rotating about its diameter: \[ I_{\text{ring}} = \frac{MR^2}{2} \]
For a solid disc rotating about its diameter: \[ I_{\text{disc}} = \frac{MR^2}{4} \]
The problem states that the moment of inertia of the disc is 2.5 times the moment of inertia of the ring: \[ I_{\text{disc}} = 2.5 I_{\text{ring}} \]
Substituting the expressions for the moments of inertia: \[ \frac{MR^2}{4} = 2.5 \times \frac{MR^2}{2} \]
This equation verifies the stated relationship.
For a solid sphere rotating about its diameter: \[ I_{\text{sphere}} = \frac{2MR^2}{5} \]
The moment of inertia of the solid sphere is defined as \( n \) times the moment of inertia of the ring: \[ I_{\text{sphere}} = n I_{\text{ring}} \]
Substituting the expressions for the moments of inertia: \[ \frac{2MR^2}{5} = n \times \frac{MR^2}{2} \] Solving for \( n \): \[ n = \frac{2}{5} \div \frac{1}{2} = \frac{2}{5} \times \frac{2}{1} = \frac{4}{5} \]
Thus, \[ \boldsymbol{n = \frac{4}{5}} \]
The center of mass of a thin rectangular plate (fig - x) with sides of length \( a \) and \( b \), whose mass per unit area (\( \sigma \)) varies as \( \sigma = \sigma_0 \frac{x}{ab} \) (where \( \sigma_0 \) is a constant), would be 