The voltage across an inductor ($V_L$) is given by:
$V_L = L \frac{dI}{dt}$
Given $I = I_0 \sin \omega t$:
$\frac{dI}{dt} = \frac{d}{dt}(I_0 \sin \omega t) = I_0 \omega \cos \omega t$
Therefore:
$V_L = L(I_0 \omega \cos \omega t) = \omega L I_0 \cos \omega t$
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 :