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, \[ \boldsymbol{n = \frac{4}{5}} \]
A cylindrical tube \(AB\) of length \(l\), closed at both ends, contains an ideal gas of \(1\) mol having molecular weight \(M\). The tube is rotated in a horizontal plane with constant angular velocity \(\omega\) about an axis perpendicular to \(AB\) and passing through the edge at end \(A\), as shown in the figure. If \(P_A\) and \(P_B\) are the pressures at \(A\) and \(B\) respectively, then (consider the temperature to be same at all points in the tube) 
As shown in the figure, radius of gyration about the axis shown in \(\sqrt{n}\) cm for a solid sphere. Find 'n'. 
When rod becomes horizontal find its angular velocity. It is pivoted at point A as shown. 