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A choke coil of resistance 5 Omega and i...

A choke coil of resistance `5 Omega` and inductance 0.6 H is in series with a capacitance of `10 (mu)F`. If a voltage of 200 V is applied and the frequency is adjusted to resonance, the current and voltage across the inductance and capacitance are `(I_0), (V_0) and (V_1)` respectively. we have

A

`(I_0)=40A`

B

`(V_0)=9.8 kV`

C

`(V_1)=9.8 kV`

D

`(V_1)=19.6 kV`

Text Solution

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The correct Answer is:
To solve the problem, we will follow these steps: ### Step 1: Determine the Current at Resonance At resonance in an RLC circuit, the inductive reactance \(X_L\) equals the capacitive reactance \(X_C\). The formula for the current \(I\) in the circuit is given by: \[ I = \frac{V}{\sqrt{R^2 + (X_C - X_L)^2}} \] Since \(X_C = X_L\) at resonance, the formula simplifies to: \[ I_0 = \frac{V}{R} \] Given: - Voltage \(V = 200 \, V\) - Resistance \(R = 5 \, \Omega\) Substituting the values: \[ I_0 = \frac{200}{5} = 40 \, A \] ### Step 2: Calculate the Inductive Reactance \(X_L\) The inductive reactance \(X_L\) is given by: \[ X_L = \omega L \] Where \(\omega = 2 \pi f\). To find \(X_L\), we first need to calculate the resonant frequency \(f\). ### Step 3: Calculate the Resonant Frequency \(f\) The resonant frequency \(f\) is given by: \[ f = \frac{1}{2 \pi \sqrt{LC}} \] Given: - Inductance \(L = 0.6 \, H\) - Capacitance \(C = 10 \, \mu F = 10 \times 10^{-6} \, F\) Substituting the values: \[ f = \frac{1}{2 \pi \sqrt{0.6 \times 10 \times 10^{-6}}} \] Calculating: \[ f \approx \frac{1}{2 \pi \sqrt{6 \times 10^{-7}}} \approx \frac{1}{2 \pi \times 0.000775} \approx 65 \, Hz \] ### Step 4: Calculate \(X_L\) Now, substituting \(f\) into the equation for \(X_L\): \[ X_L = 2 \pi f L = 2 \pi (65) (0.6) \approx 245 \, \Omega \] ### Step 5: Calculate the Voltage Across the Inductor \(V_0\) The voltage across the inductor \(V_0\) is given by: \[ V_0 = I_0 \cdot X_L \] Substituting the values: \[ V_0 = 40 \cdot 245 = 9800 \, V = 9.8 \, kV \] ### Step 6: Calculate the Voltage Across the Capacitor \(V_1\) The capacitive reactance \(X_C\) is given by: \[ X_C = \frac{1}{\omega C} \] Substituting \(\omega\) and \(C\): \[ X_C = \frac{1}{2 \pi (65) (10 \times 10^{-6})} \] Calculating \(X_C\): \[ X_C \approx \frac{1}{2 \pi (65) (10^{-5})} \approx 245 \, \Omega \] Now, the voltage across the capacitor \(V_1\) is: \[ V_1 = I_0 \cdot X_C = 40 \cdot 245 = 9800 \, V = 9.8 \, kV \] ### Final Results - \(I_0 = 40 \, A\) - \(V_0 = 9.8 \, kV\) - \(V_1 = 9.8 \, kV\)

To solve the problem, we will follow these steps: ### Step 1: Determine the Current at Resonance At resonance in an RLC circuit, the inductive reactance \(X_L\) equals the capacitive reactance \(X_C\). The formula for the current \(I\) in the circuit is given by: \[ I = \frac{V}{\sqrt{R^2 + (X_C - X_L)^2}} \] ...
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