JEE Challenger
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Effect of Angular Frequency on Bulb Brightness in RC Circuit

An AC voltage source of variable angular frequency ω\omega and fixed amplitude V0\text{V}_0 is connected in series with a capacitance C\text{C} and an electric bulb of resistance R\text{R} (inductance zero). When ω\omega is increased

Options

A

the bulb glows dimmer

B

the bulb glows brighter

Correct
C

total impedance of the circuit is unchanged

D

total impedance of the circuit increases

Step-by-Step Solution

To determine the effect of increasing the angular frequency ω\omega on the brightness of the bulb, let us analyze the circuit parameters.

  1. Impedance of the Circuit:
    The circuit is a series RCRC circuit connected to an AC voltage source of fixed amplitude V0V_0 and angular frequency ω\omega.
    The capacitive reactance XCX_C is given by:
    XC=1ωCX_C = \frac{1}{\omega C}
    The total impedance ZZ of the series circuit is:
    Z=R2+XC2=R2+(1ωC)2Z = \sqrt{R^2 + X_C^2} = \sqrt{R^2 + \left(\frac{1}{\omega C}\right)^2}

  2. Effect of Increasing ω\omega:
    When the angular frequency ω\omega increases:

    • The capacitive reactance XC=1ωCX_C = \frac{1}{\omega C} decreases.
    • Consequently, the total impedance Z=R2+XC2Z = \sqrt{R^2 + X_C^2} decreases.
  3. Current and Power Dissipated in the Bulb:
    The root-mean-square (rms) current in the circuit is:
    Irms=VrmsZI_{\text{rms}} = \frac{V_{\text{rms}}}{Z}
    Since the source amplitude V0V_0 is fixed, Vrms=V02V_{\text{rms}} = \frac{V_0}{\sqrt{2}} is also constant.
    As ZZ decreases, the current IrmsI_{\text{rms}} flowing through the circuit increases.

    The brightness of the bulb depends on the average electrical power dissipated as heat and light across its resistance RR:
    P=Irms2RP = I_{\text{rms}}^2 R
    Since IrmsI_{\text{rms}} increases and the resistance RR remains constant, the power dissipated PP increases.

Therefore, when ω\omega is increased, the bulb glows brighter.

Correct Option: B