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Question Stem
In a circuit, a metal filament lamp is connected in series with a capacitor of capacitance C $$\mu F$$ across a 200 V, 50 Hz supply. The power consumed by the lamp is 500 W while the voltage drop across it is 100 V. Assume that there is no inductive load in the circuit. Take rms values of the voltages. The magnitude of the phase-angle (in degrees) between the current and the supply voltage is $$\psi$$. Assume, $$\pi \sqrt{3} \approx 5$$.
The circuit contains a pure resistor (the lamp) in series with a capacitor, connected to a 200 V, 50 Hz supply. All data are r.m.s. values.
Step 1 : Current in the circuit
For a purely resistive element, $$P = VI$$. Hence for the lamp
$$I = \frac{P}{V_{\text{lamp}}}= \frac{500\;\text{W}}{100\;\text{V}} = 5\;\text{A}$$
This 5 A is the r.m.s. current everywhere in the series circuit.
Step 2 : Voltage across the capacitor
Take the current $$I$$ as the reference phasor along the positive x-axis. The lamp voltage $$V_R$$ (100 V) is in phase with the current, while the capacitor voltage $$V_C$$ lags the current by $$90^{\circ}$$ (points along the negative y-axis). The supply voltage $$V_s$$ is the vector sum:
$$V_s^2 = V_R^2 + V_C^2$$
Substituting $$V_s = 200\;\text{V}$$ and $$V_R = 100\;\text{V}$$:
$$200^2 = 100^2 + V_C^2 \quad\Longrightarrow\quad V_C^2 = 200^2 - 100^2 = 40000 - 10000 = 30000$$
$$\Rightarrow\; V_C = 100\sqrt{3}\;\text{V} \approx 173.2\;\text{V}$$
Step 3 : Capacitive reactance
$$X_C = \frac{V_C}{I} = \frac{100\sqrt{3}}{5} = 20\sqrt{3}\;\Omega \approx 34.64\;\Omega$$
Step 4 : Resistance of the lamp
$$R = \frac{V_R}{I} = \frac{100}{5} = 20\;\Omega$$
Step 5 : Phase angle between current and supply voltage
For a series $$R$$-$$C$$ circuit the phase angle $$\psi$$ (magnitude) satisfies
$$\tan\psi = \frac{X_C}{R}$$
Hence
$$\tan\psi = \frac{20\sqrt{3}}{20} = \sqrt{3}$$
Using $$\tan60^{\circ} = \sqrt{3}$$ (and the given hint $$\pi\sqrt{3}\approx 5$$ which implies $$\sqrt{3}\approx1.732$$),
$$\psi \approx 60^{\circ}$$
Answer
The magnitude of the phase angle is approximately $$60^{\circ}$$, which lies in the range 55.00 - 62.00.
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