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Q.An alternating e.m.f. is applied across an inductor. Obtain an expression for the current (I) in the circuit and hence obtain inductive reactance of the circuit and draw a phasor diagram to show phase difference between I and V. OR

(a) A 100 Ω100\,\Omega resistor is connected to a 220 V, 50 Hz a.c. supply. What is the r.m.s. value of current and net power consumed over a full cycle? [2½]
(b) A light bulb is rated at 100 W for a 220 V supply. Find the resistance of the bulb and r.m.s. current through the bulb. [2½]
Himachal HpboseHPBOSE Plus Two Board 2025Subjective· 5mImportance★★★★★
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Figure — Stem explicitly says 'draw a phasor diagram to show phase difference between I and V' (hard draw gate) on the
Figure — Stem explicitly says 'draw a phasor diagram to show phase difference between I and V' (hard draw gate) on the

Applying Kirchhoff's voltage law to a pure inductor in an AC circuit and integrating gives a current that lags the voltage by 90°, with peak value I0=V0/ωLI_0 = V_0/\omega L.

Setup: Let an inductor of inductance LL be connected to an AC source of emf v=V0sin⁡ωtv = V_0\sin\omega t. Since the inductor has negligible resistance, at every instant the applied voltage equals the self-induced back-emf:

v=LdIdtv = L\frac{dI}{dt}

V0sin⁡ωt=LdIdtV_0\sin\omega t = L\frac{dI}{dt}

dI=V0Lsin⁡ωt  dtdI = \frac{V_0}{L}\sin\omega t\; dt

Integrating both sides:

I=V0L∫sin⁡ωt dt=−V0ωLcos⁡ωt+constantI = \frac{V_0}{L}\int \sin\omega t\, dt = -\frac{V_0}{\omega L}\cos\omega t + \text{constant}

The integration constant (any time-independent, i.e. DC, part of current) has no physical role in a purely AC circuit and is taken as zero. Using −cos⁡ωt=sin⁡(ωt−π/2)-\cos\omega t = \sin(\omega t - \pi/2):

I=V0ωLsin⁡(ωt−π2)=I0sin⁡(ωt−π2)I = \frac{V_0}{\omega L}\sin\left(\omega t - \frac{\pi}{2}\right) = I_0\sin\left(\omega t - \frac{\pi}{2}\right)

where I0=V0ωLI_0 = \dfrac{V_0}{\omega L} is the peak current.

Inductive reactance: Comparing I0=V0/(ωL)I_0 = V_0/(\omega L) with the resistive form I0=V0/RI_0 = V_0/R, the quantity ωL\omega L plays the role of an effective 'resistance' for AC in an inductor, called the inductive reactance:

XL=ωL=2πνLX_L = \omega L = 2\pi\nu L

Its SI unit is ohm (Ω\Omega). It increases with frequency — an inductor opposes fast-changing currents more strongly.

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