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In a series LCR circuit with an AC so (E...

In a series LCR circuit with an AC so `(E_(rms)=50V)` and `f=50//pi` Hz, R=300 ohm, C=0.02mF, L=1.0H, which of the follwing is correct

A

the rms current in the circuit is 0.1 A

B

the rms potential difference acrosss the capacitor is 50V

C

the rms potential difference across the inductor is 10V

D

the rms current in the circuit is 0.14A

Text Solution

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The correct Answer is:
To solve the problem, we need to analyze the series LCR circuit with the given parameters. Let's break it down step by step. ### Step 1: Identify Given Values - \( E_{\text{rms}} = 50 \, \text{V} \) - Frequency \( f = \frac{50}{\pi} \, \text{Hz} \) - Resistance \( R = 300 \, \Omega \) - Capacitance \( C = 0.02 \, \text{mF} = 0.02 \times 10^{-3} \, \text{F} = 2 \times 10^{-5} \, \text{F} \) - Inductance \( L = 1.0 \, \text{H} \) ### Step 2: Calculate Angular Frequency The angular frequency \( \omega \) is given by: \[ \omega = 2\pi f \] Substituting the value of \( f \): \[ \omega = 2\pi \left(\frac{50}{\pi}\right) = 100 \, \text{rad/s} \] ### Step 3: Calculate Inductive Reactance \( X_L \) The inductive reactance \( X_L \) is calculated using the formula: \[ X_L = \omega L \] Substituting the values: \[ X_L = 100 \times 1.0 = 100 \, \Omega \] ### Step 4: Calculate Capacitive Reactance \( X_C \) The capacitive reactance \( X_C \) is calculated using the formula: \[ X_C = \frac{1}{\omega C} \] Substituting the values: \[ X_C = \frac{1}{100 \times 2 \times 10^{-5}} = \frac{1}{0.002} = 500 \, \Omega \] ### Step 5: Calculate Impedance \( Z \) The total impedance \( Z \) in the circuit is given by: \[ Z = \sqrt{R^2 + (X_L - X_C)^2} \] Substituting the values: \[ Z = \sqrt{300^2 + (100 - 500)^2} = \sqrt{300^2 + (-400)^2} \] Calculating: \[ Z = \sqrt{90000 + 160000} = \sqrt{250000} = 500 \, \Omega \] ### Step 6: Calculate RMS Current \( I_{\text{rms}} \) The RMS current can be calculated using Ohm's law: \[ I_{\text{rms}} = \frac{E_{\text{rms}}}{Z} \] Substituting the values: \[ I_{\text{rms}} = \frac{50}{500} = 0.1 \, \text{A} \] ### Step 7: Calculate Potential Difference Across Capacitor \( V_C \) The potential difference across the capacitor can be calculated as: \[ V_C = I_{\text{rms}} \times X_C \] Substituting the values: \[ V_C = 0.1 \times 500 = 50 \, \text{V} \] ### Step 8: Calculate Potential Difference Across Inductor \( V_L \) The potential difference across the inductor can be calculated as: \[ V_L = I_{\text{rms}} \times X_L \] Substituting the values: \[ V_L = 0.1 \times 100 = 10 \, \text{V} \] ### Summary of Results - \( I_{\text{rms}} = 0.1 \, \text{A} \) - \( V_C = 50 \, \text{V} \) - \( V_L = 10 \, \text{V} \) ### Conclusion Based on the calculations: - Option A is correct (RMS current is 0.1 A). - Option B is correct (Potential difference across capacitor is 50 V). - Option C is correct (Potential difference across inductor is 10 V). - Option D is incorrect (RMS current is not 0.14 A).
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