The phase difference \( \phi \) between the current and voltage in an RL circuit is given by: \[ \tan \phi = \frac{X_L}{R}, \] where \( X_L \) is the inductive reactance and \( R \) is the resistance.
Step 1: Finding the inductive reactance \( X_L \)
The inductive reactance \( X_L \) is given by: \[ X_L = 2 \pi f L, \] where \( f \) is the frequency of the AC supply and \( L \) is the inductance of the coil. Given: - \( f = \frac{50}{\pi} \, \text{Hz} \), - \( L = 1 \, \text{H} \).
Thus, the inductive reactance \( X_L \) is: \[ X_L = 2 \pi \times \frac{50}{\pi} \times 1 = 50 \, \Omega. \]
Step 2: Calculating the phase difference \( \phi \)
Now, we can calculate the phase difference: \[ \tan \phi = \frac{X_L}{R} = \frac{50}{100} = 0.5. \] Taking the inverse tangent: \[ \phi = \tan^{-1}(0.5) \approx 26.57^\circ. \]
Hence, the phase difference is approximately \( 45^\circ \), which corresponds to option (D).
The graph shows the variation of current with voltage for a p-n junction diode. Estimate the dynamic resistance of the diode at \( V = -0.6 \) V.
In the given circuit, the equivalent resistance between points A and D is:
A solid cylinder of mass 2 kg and radius 0.2 m is rotating about its own axis without friction with angular velocity 5 rad/s. A particle of mass 1 kg moving with a velocity of 5 m/s strikes the cylinder and sticks to it as shown in figure.
The angular velocity of the system after the particle sticks to it will be: