(d) In a purely inductive circuit, current is
$i = i_{0}\sin\left( \omega t - \frac{\pi}{2} \right)$
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Which shows that the current lags behind the emf by a phase angle of $\frac{\pi}{2}$ or $90{^\circ}$ or the
emf leads the current by a phase angle of $\frac{\pi}{2}$ or $90{^\circ}$.