
For pure rolling motion, mechanical energy is conserved. At the initial position (\( A \)), the ball has kinetic energy due to both translational and rotational motion, and at the maximum height (\( B \)), all the kinetic energy is converted into potential energy.
Step 1: Write the conservation of energy equation. The total mechanical energy at \( A \) is: \[ \text{(M.E.)}_A = \frac{1}{2} m v_0^2 + \frac{1}{2} I \omega^2, \] where \( m \) is the mass of the ball, \( v_0 = 3 \, \text{m/s} \) is the initial velocity, \( I \) is the moment of inertia of the hollow sphere (\( I = \frac{2}{3} m R^2 \)), and \( \omega = \frac{v_0}{R} \) is the angular velocity. At the maximum height (\( B \)), all kinetic energy is converted into potential energy: \[ \text{(M.E.)}_B = m g h_{\text{max}}, \] where \( h_{\text{max}} \) is the maximum height. Using energy conservation: \[ \text{(M.E.)}_A = \text{(M.E.)}_B. \]
Step 2: Substitute the expressions. \[ \frac{1}{2} m v_0^2 + \frac{1}{2} \left(\frac{2}{3} m R^2\right) \left(\frac{v_0}{R}\right)^2 = m g h_{\text{max}}. \] Simplify: \[ \frac{1}{2} m v_0^2 + \frac{1}{3} m v_0^2 = m g h_{\text{max}}. \] Combine terms: \[ \frac{1}{2} + \frac{1}{3} = \frac{3}{6} + \frac{2}{6} = \frac{5}{6}. \] \[ \frac{5}{6} m v_0^2 = m g h_{\text{max}}. \] Cancel \( m \) on both sides: \[ h_{\text{max}} = \frac{\frac{5}{6} v_0^2}{g}. \]
Step 3: Substitute values. Substitute \( v_0 = 3 \, \text{m/s} \) and \( g = 10 \, \text{m/s}^2 \): \[ h_{\text{max}} = \frac{\frac{5}{6} \cdot (3)^2}{10}. \] Simplify: \[ h_{\text{max}} = \frac{\frac{5}{6} \cdot 9}{10} = \frac{45}{60} = 0.75 \, \text{m}. \] Convert to centimeters: \[ h_{\text{max}} = 0.75 \times 100 = 75 \, \text{cm}. \]
Final Answer: The maximum height covered is: \[ \boxed{75 \, \text{cm}}. \]
Net gravitational force at the center of a square is found to be \( F_1 \) when four particles having masses \( M, 2M, 3M \) and \( 4M \) are placed at the four corners of the square as shown in figure, and it is \( F_2 \) when the positions of \( 3M \) and \( 4M \) are interchanged. The ratio \( \dfrac{F_1}{F_2} = \dfrac{\alpha}{\sqrt{5}} \). The value of \( \alpha \) is 


Two circular discs of radius \(10\) cm each are joined at their centres by a rod, as shown in the figure. The length of the rod is \(30\) cm and its mass is \(600\) g. The mass of each disc is also \(600\) g. If the applied torque between the two discs is \(43\times10^{-7}\) dyne·cm, then the angular acceleration of the system about the given axis \(AB\) is ________ rad s\(^{-2}\).
