Step 1: Identify the given parameters.
Inductive reactance, \( X_L = 100 \, \Omega \)
Capacitive reactance, \( X_C = 50 \, \Omega \)
Resistance, \( R = 50 \, \Omega \)
RMS voltage of the AC source, \( V_{rms} = 10 \, V \)
Frequency of the AC source, \( f = 50 \, Hz \)
Step 2: Calculate the impedance \( Z \) of the series LCR circuit.
The impedance of a series LCR circuit is given by: \[ Z = \sqrt{R^2 + (X_L - X_C)^2} \] Substitute the given values: \[ Z = \sqrt{(50 \, \Omega)^2 + (100 \, \Omega - 50 \, \Omega)^2} \] \[ Z = \sqrt{(50)^2 + (50)^2} = \sqrt{2500 + 2500} = \sqrt{5000} \, \Omega \] \[ Z = 50\sqrt{2} \, \Omega \]
Step 3: Calculate the RMS current \( I_{rms} \) in the circuit.
Using Ohm's law for AC circuits: \[ I_{rms} = \frac{V_{rms}}{Z} \] Substitute the values of \( V_{rms} \) and \( Z \): \[ I_{rms} = \frac{10 \, V}{50\sqrt{2} \, \Omega} = \frac{1}{5\sqrt{2}} \, A = \frac{\sqrt{2}}{10} \, A \]
Step 4: Calculate the average power \( P_{avg} \) dissipated by the circuit.
The average power dissipated in an AC circuit is only through the resistor and is given by: \[ P_{avg} = I_{rms}^2 R \] Substitute the values of \( I_{rms} \) and \( R \): \[ P_{avg} = \left(\frac{\sqrt{2}}{10} \, A\right)^2 \times 50 \, \Omega \] \[ P_{avg} = \left(\frac{2}{100}\right) \times 50 \, W \] \[ P_{avg} = \frac{1}{50} \times 50 \, W \] \[ P_{avg} = 1 \, W \] The average power dissipated by the circuit is 1 W.
Draw the plots showing the variation of magnetic flux φ linked with the loop with time t and variation of induced emf E with time t. Mark the relevant values of E, φ and t on the graphs.
The motion of an airplane is represented by the velocity-time graph as shown below. The distance covered by the airplane in the first 30.5 seconds is km.