The power rating of the electric bulb is \( P = 100 \, \text{W} \) at an rms voltage \( V_{rms} = 220 \, \text{V} \).
When the bulb is connected to an ac source of rms voltage 220 V, it will operate at its rated power.
The relationship between power, rms voltage, and rms current \( I_{rms} \) is: \[ P = V_{rms} I_{rms} \] We can find the rms current through the bulb: \[ I_{rms} = \frac{P}{V_{rms}} = \frac{100 \, \text{W}}{220 \, \text{V}} = \frac{10}{22} \, \text{A} = \frac{5}{11} \, \text{A} \] The peak value of the current \( I_0 \) in an ac circuit is related to the rms current by: \[ I_0 = \sqrt{2} I_{rms} \] Substituting the value of \( I_{rms} \): \[ I_0 = \sqrt{2} \times \frac{5}{11} \, \text{A} \] We know that \( \sqrt{2} \approx 1.414 \). \[ I_0 \approx 1.414 \times \frac{5}{11} = \frac{7.07}{11} \approx 0.6427 \, \text{A} \] Rounding to two decimal places, the peak value of the current through the bulb is approximately 0.64 A.
For the AC circuit shown in the figure, $ R = 100 \, \text{k}\Omega $ and $ C = 100 \, \text{pF} $, and the phase difference between $ V_{\text{in}} $ and $ (V_B - V_A) $ is 90°. The input signal frequency is $ 10^x $ rad/sec, where $ x $ is:
Match List - I with List - II.