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A capacitor of 1muF is connected to sour...

A capacitor of `1muF` is connected to source of ac having emf given by equation `E = 200 sin(120pit)`. Find the value of rms current through the capacitor.

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To find the value of the RMS current through a capacitor connected to an AC source, we can follow these steps: ### Step 1: Identify the given values - Capacitance \( C = 1 \, \mu F = 1 \times 10^{-6} \, F \) - The EMF of the AC source is given by \( E(t) = 200 \sin(120 \pi t) \). ### Step 2: Determine the angular frequency \( \omega \) From the equation of the EMF, we can identify the angular frequency \( \omega \): \[ \omega = 120 \pi \, \text{rad/s} \] ### Step 3: Calculate the peak voltage \( E_0 \) The peak voltage \( E_0 \) is given as: \[ E_0 = 200 \, V \] ### Step 4: Calculate the RMS voltage \( E_{rms} \) The RMS voltage is related to the peak voltage by the formula: \[ E_{rms} = \frac{E_0}{\sqrt{2}} = \frac{200}{\sqrt{2}} \approx 141.4 \, V \] ### Step 5: Calculate the capacitive reactance \( X_C \) The capacitive reactance \( X_C \) is given by the formula: \[ X_C = \frac{1}{\omega C} \] Substituting the values: \[ X_C = \frac{1}{120 \pi \times 1 \times 10^{-6}} \approx \frac{1}{0.00037699} \approx 2654.9 \, \Omega \] ### Step 6: Calculate the RMS current \( I_{rms} \) The RMS current through the capacitor can be calculated using Ohm's law: \[ I_{rms} = \frac{E_{rms}}{X_C} \] Substituting the values: \[ I_{rms} = \frac{141.4}{2654.9} \approx 0.0533 \, A \approx 0.05 \, A \] ### Final Answer The value of the RMS current through the capacitor is approximately: \[ I_{rms} \approx 0.05 \, A \] ---

To find the value of the RMS current through a capacitor connected to an AC source, we can follow these steps: ### Step 1: Identify the given values - Capacitance \( C = 1 \, \mu F = 1 \times 10^{-6} \, F \) - The EMF of the AC source is given by \( E(t) = 200 \sin(120 \pi t) \). ### Step 2: Determine the angular frequency \( \omega \) From the equation of the EMF, we can identify the angular frequency \( \omega \): ...
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