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Question: In a purely inductive circuit, the current: A. is in phase with the voltage B. is out of phase ...

In a purely inductive circuit, the current:
A. is in phase with the voltage
B. is out of phase with the voltage
C. leads the voltage by π2\dfrac {\pi}2
D. lags behind the voltage by π2\dfrac {\pi}2

Explanation

Solution

Hint: In a purely inductive circuit, there is no resistance or capacitance. The circuit only contains an inductor and ac voltage source. We need to know the equation of the circuit first. Then after solving it, we can find the required phase difference.

Formula used:

Ldidt=va.sinωtL\dfrac{di}{dt}={{v}_{a}}.\sin \omega t

Complete step-by-step solution:
The voltage may be assumed to be given by,

vi=va.sinωt{{v}_{i}}={{v}_{a}}.\sin \omega t

Here, vav_a is the amplitude of input voltage and ωt\omega t is called the phase angle of the voltage.

Now, the equation of the circuit can be given as,

Ldidt=va.sinωt i=vaωLcosωt+k=vaωLsin(ωtπ2)+k \begin{aligned} & L\dfrac{di}{dt}={{v}_{a}}.\sin \omega t \\\ & \Rightarrow i=-\dfrac{{{v}_{a}}}{\omega L}\cos \omega t+k=\dfrac{{{v}_{a}}}{\omega L}\sin \left( \omega t-\dfrac{\pi}{2} \right)+k \\\ \end{aligned}

Where, L is the inductance of the inductor, i is the ac current and k is a constant and can be neglected while considering phase differences.

The new phase of the current of the circuit is ωtπ2\omega t-\dfrac{\pi}{2}. Hence, clearly the phase of the current is lagging behind the voltage by π2\dfrac{\pi}{2}. So option D is the correct answer.

Additional information:
In case of purely capacitive circuits, the current of the circuit leads the voltage by π2\dfrac{\pi}{2}. And in case of purely resistive circuits, there is no phase change i.e. both the voltage and current have the same phase angle.

Note: A student may choose to assume the source voltage as va.cosωt{{v}_{a}}.\cos \omega t. Again option D will be the correct answer. In higher studies, students take the input ac voltage as va.eiωtv_a.e^{i\omega t}. Because eiωt=cosωt+i.sinωt{{e}^{i\omega t}}=\cos \omega t+i.\sin \omega t. So, there’s a combination of sine and cosine components of the voltage. In all possible methods, the answer is the same.