The problem involves understanding the concept of the radius of gyration for different axes of a uniform disc. The radius of gyration \( k \) is defined as \( k = \sqrt{\frac{I}{m}} \), where \( I \) is the moment of inertia and \( m \) is the mass of the object.
For a thin uniform disc of radius \( R \), the moment of inertia \( I \) about an axis through its center and perpendicular to its plane is \( I_c = \frac{1}{2}mR^2 \). Hence, the radius of gyration \( k_c \) about this axis is:
\( k_c = \sqrt{\frac{\frac{1}{2}mR^2}{m}} = \sqrt{\frac{1}{2}}R \)
The moment of inertia \( I_d \) about the diameter of the disc is \( I_d = \frac{1}{4}mR^2 \). Therefore, the radius of gyration \( k_d \) about the diameter is:
\( k_d = \sqrt{\frac{\frac{1}{4}mR^2}{m}} = \frac{R}{2} \)
Thus, the ratio of the radius of gyration about the center perpendicular axis to that about the diameter is given by:
\( \frac{k_c}{k_d} = \frac{\sqrt{\frac{1}{2}}R}{\frac{R}{2}} = \sqrt{2} \)
The correct ratio is therefore \( \sqrt{2}:1 \).
A string of length \( L \) is fixed at one end and carries a mass of \( M \) at the other end. The mass makes \( \frac{3}{\pi} \) rotations per second about the vertical axis passing through the end of the string as shown. The tension in the string is ________________ ML.
A sphere of radius R is cut from a larger solid sphere of radius 2R as shown in the figure. The ratio of the moment of inertia of the smaller sphere to that of the rest part of the sphere about the Y-axis is :
The current passing through the battery in the given circuit, is:
A bob of heavy mass \(m\) is suspended by a light string of length \(l\). The bob is given a horizontal velocity \(v_0\) as shown in figure. If the string gets slack at some point P making an angle \( \theta \) from the horizontal, the ratio of the speed \(v\) of the bob at point P to its initial speed \(v_0\) is :