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Question: In the circuit shown in the figure, if both the bulbs B₁ and B₂ are identical :- ...

In the circuit shown in the figure, if both the bulbs B₁ and B₂ are identical :-

A

Their brightness will be the same

B

B₂ will be brighter than B₁

C

as frequency of supply voltage is increased, brightness of B₁ will increase & that of B₂ will decrease

D

only B₂ will glow because the capacitor has infinite impedance

Answer

B₂ will be brighter than B₁

Explanation

Solution

The circuit consists of an AC voltage source connected to two parallel branches. One branch contains a bulb B₁ in series with a capacitor C. The other branch contains a bulb B₂ in series with an inductor L. Both bulbs are identical, meaning they have the same resistance R. The brightness of a bulb is proportional to the power dissipated by it, which is given by P=Irms2RP = I_{rms}^2 R. Since R is the same for both bulbs, the brightness is proportional to the square of the RMS current flowing through the bulb.

The RMS voltage of the source is Vrms=220VV_{rms} = 220 V and the frequency is f=50Hzf = 50 Hz. The angular frequency is ω=2πf=2π(50)=100πrad/s\omega = 2\pi f = 2\pi (50) = 100\pi \, rad/s. The capacitance is C=500μF=500×106F=5×104FC = 500 \mu F = 500 \times 10^{-6} F = 5 \times 10^{-4} F. The inductance is L=10mH=10×103H=102HL = 10 mH = 10 \times 10^{-3} H = 10^{-2} H.

The impedance of the branch containing bulb B₁ and capacitor C is Z1=R+jXCZ_1 = R + jX_C, where XC=1ωCX_C = \frac{1}{\omega C} is the capacitive reactance. The magnitude of the impedance is Z1=R2+XC2|Z_1| = \sqrt{R^2 + X_C^2}. The RMS current through bulb B₁ is I1,rms=VrmsZ1=VrmsR2+XC2I_{1,rms} = \frac{V_{rms}}{|Z_1|} = \frac{V_{rms}}{\sqrt{R^2 + X_C^2}}.

The impedance of the branch containing bulb B₂ and inductor L is Z2=R+jXLZ_2 = R + jX_L, where XL=ωLX_L = \omega L is the inductive reactance. The magnitude of the impedance is Z2=R2+XL2|Z_2| = \sqrt{R^2 + X_L^2}. The RMS current through bulb B₂ is I2,rms=VrmsZ2=VrmsR2+XL2I_{2,rms} = \frac{V_{rms}}{|Z_2|} = \frac{V_{rms}}{\sqrt{R^2 + X_L^2}}.

Let's calculate the reactances at f=50Hzf = 50 Hz: XC=1ωC=1(100π)(5×104)=15π×102=1005π=20π6.366ΩX_C = \frac{1}{\omega C} = \frac{1}{(100\pi)(5 \times 10^{-4})} = \frac{1}{5\pi \times 10^{-2}} = \frac{100}{5\pi} = \frac{20}{\pi} \approx 6.366 \Omega. XL=ωL=(100π)(102)=πΩ3.142ΩX_L = \omega L = (100\pi)(10^{-2}) = \pi \Omega \approx 3.142 \Omega.

Comparing the reactances, we have XC>XLX_C > X_L. Since XC>XLX_C > X_L, we have R2+XC2>R2+XL2R^2 + X_C^2 > R^2 + X_L^2, which means Z1>Z2|Z_1| > |Z_2|. Since the voltage across both parallel branches is the same (VrmsV_{rms}), the current through the branch with lower impedance will be higher. Thus, I1,rms=VrmsZ1<VrmsZ2=I2,rmsI_{1,rms} = \frac{V_{rms}}{|Z_1|} < \frac{V_{rms}}{|Z_2|} = I_{2,rms}. Since I1,rms<I2,rmsI_{1,rms} < I_{2,rms}, the power dissipated by B₁ will be less than the power dissipated by B₂, and hence B₁ will be less bright than B₂. So, B₂ will be brighter than B₁.