When an A.C. supply is connected to a capacitor, the voltage across the capacitor is out of phase with the current. The voltage across the capacitor will be the peak voltage of the AC supply. The RMS value of the AC supply is 220 V. The peak voltage \( V_{\text{peak}} \) is related to the RMS value \( V_{\text{rms}} \) by the formula: \[ V_{\text{peak}} = V_{\text{rms}} \times \sqrt{2} \] Substituting the given value of \( V_{\text{rms}} = 220 \, \text{V} \): \[ V_{\text{peak}} = 220 \times \sqrt{2} = 220\sqrt{2} \, \text{V} \] Thus, the potential difference across the capacitor is \( 220\sqrt{2} \, \text{V} \).
The correct answer is (D) : \(220\sqrt2\ V\).
In an AC circuit, when a capacitor is connected to an alternating current (AC) supply, the potential difference across the capacitor leads the current by 90°. This is a typical property of capacitive reactance in AC circuits. Given that the supply voltage is \( V_{\text{supply}} = 220 \, \text{V} \), this is the root-mean-square (RMS) voltage of the AC supply. The peak voltage \( V_{\text{peak}} \) is related to the RMS voltage by: \[ V_{\text{peak}} = V_{\text{RMS}} \times \sqrt{2} \] Substituting the given RMS voltage \( V_{\text{RMS}} = 220 \, \text{V} \): \[ V_{\text{peak}} = 220 \times \sqrt{2} = 220\sqrt{2} \, \text{V} \] Thus, the peak potential difference across the capacitor is \( 220\sqrt{2} \, \text{V} \).
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.
You are given a dipole of charge \( +q \) and \( -q \) separated by a distance \( 2l \). A sphere 'A' of radius \( R \) passes through the centre of the dipole as shown below and another sphere 'B' of radius \( 2R \) passes through the charge \( +q \). Then the electric flux through the sphere A is