
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:
$V_L = L(I_0 \omega \cos \omega t) = \omega L I_0 \cos \omega t$