A coil of inductive reactance frac{1}{sqrt{3 | vedclass

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(B) Given: Inductive reactance $ X_L = \omega L = \frac{1}{\sqrt{3}} \ \Omega $,Resistance $ R = 1 \ \Omega $,Frequency $ f = 50 \ Hz $.In an $ RL $ c

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$ \frac{1}{600} \ s $

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(B) Given: Inductive reactance $ X_L = \omega L = \frac{1}{\sqrt{3}} \ \Omega $,Resistance $ R = 1 \ \Omega $,Frequency $ f = 50 \ Hz $.In an $ RL $ circuit,the phase difference $ \phi $ between voltage and current is given by $ 	an \phi = \frac{X_L}{R} $.Substituting the values,$ 	an \phi = \frac{1/\sqrt{3}}{1} = \frac{1}{\sqrt{3}} $.Thus,$ \phi = 30^{\circ} = \frac{\pi}{6} 	ext{ radians} $.The phase difference $ \phi $ is related to time lag $ t $ by the relation $ \phi = \omega t $.Since $ \omega = 2\pi f = 2\pi 	imes 50 = 100\pi \ rad/s $.Therefore,$ t = \frac{\phi}{\omega} = \frac{\pi/6}{100\pi} = \frac{1}{600} \ s $.The time lag between maximum voltage and current is $ \frac{1}{600} \ s $.

$A$ coil of inductive reactance $ \frac{1}{\sqrt{3}} \Omega $ and resistance $ 1 \Omega $ is connected to a $ 200 \ V, 50 \ Hz $ $AC$ supply. The time lag between maximum voltage and current is

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