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A resistor of resistance '$R$' draws power '$P$' when connected to an AC source. If an inductance is now placed in series with $R$, such that the impedance of the circuit becomes '$Z$', the power drawn will be

This question was previously asked in
WBJEE 2026 Physics and Chemistry Question Paper (24-May-2026)
The correct answer is
$P \left( \frac{R}{Z} \right)^2$

AC Power Calculation with Impedance

The initial power P drawn by a resistor R connected to a constant AC voltage source ($V_{rms}$) is:

$P = \frac{V_{rms}^2}{R}$

When an inductance is added in series with the resistor, the total impedance of the circuit becomes Z. The source voltage $V_{rms}$ remains unchanged.

The new RMS current $I'_{rms}$ in this series R-L circuit is calculated using Ohm's law for AC circuits:

$I'_{rms} = \frac{V_{ سےms}}{Z}$

The power dissipated by the resistor in the new circuit is the new power $P'$. Since only the resistor dissipates average power in an AC circuit:

$P' = (I'_{rms})^2 R$

Substitute the expression for $I'_{rms}$:

$P' = \left(\frac{V_{rms}}{Z}\right)^2 R = \frac{V_{rms}^2}{Z^2} R$

From the initial power equation ($P = \frac{V_{rms}^2}{R}$), we can rearrange to find $V_{rms}^2$:

$V_{rms}^2 = P \times R$

Now, substitute this expression for $V_{rms}^2$ into the equation for $P'$:

$P' = \frac{(P \times R)}{Z^2} R$

Simplify the expression:

$P' = P \frac{R^2}{Z^2}$

$P' = P \left(\frac{R}{Z}\right)^2$

Thus, the power drawn by the circuit in the presence of the inductor will be $P \left( \frac{R}{Z} \right)^2$.

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  4. The electrostatic potential on the surface of uniformly charged spherical shell of radius $R = 10 \ cm$ is $120 \ V$. The potential at the centre of shell, at a distance $r = 5 \ cm$ from centre, and at a distance $r = 15 \ cm$ from the centre of the shell respectively, are:

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