In non-uniform circular motion, the ratio of tangential to radial acceleration is \(\textit{(r = radius, \( \alpha \) = angular acceleration, V = linear velocity)}\)
A body of mass 2 kg is acted upon by two forces, each of magnitude 1 N and inclined at \( 60^\circ \) with each other. The acceleration of the body in \( \text{m/s}^2 \) is \(\textit{(cos 60° = 0.5)}\)
A simple pendulum of length \( L \) has mass \( m \) and it oscillates freely with amplitude \( A \). At extreme position, its potential energy is \(\textit{(g = acceleration due to gravity)}\)