The time period of a simple pendulum at a height h = R above the earth’s surface is given by:
\[ T_1 = 2\pi \sqrt{\frac{\ell}{g_{\text{eff}}}} \]
where the effective acceleration due to gravity at a height \(h = R\) is: \[ g_{\text{eff}} = \frac{GM}{(2R)^2} = \frac{g}{4} \]
Thus, the time period at height \(R\) is: \[ T_1 = 2\pi \sqrt{\frac{\ell}{g/4}} = 2\pi \sqrt{\frac{4\ell}{g}} \]
Similarly, at height \(h = 2R\), the effective acceleration due to gravity is: \[ g_{\text{eff}} = \frac{GM}{(3R)^2} = \frac{g}{9} \]
Hence, the time period \(T_2\) is: \[ T_2 = 2\pi \sqrt{\frac{\ell}{g/9}} = 2\pi \sqrt{\frac{9\ell}{g}} \]
The ratio of the time periods is: \[ \frac{T_1}{T_2} = \sqrt{\frac{4}{9}} = \frac{2}{3} \]
This implies: \[ 3T_1 = 2T_2 \]
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 : 

In the first configuration (1) as shown in the figure, four identical charges \( q_0 \) are kept at the corners A, B, C and D of square of side length \( a \). In the second configuration (2), the same charges are shifted to mid points C, E, H, and F of the square. If \( K = \frac{1}{4\pi \epsilon_0} \), the difference between the potential energies of configuration (2) and (1) is given by: