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Question: In an a.c. circuit an alternating voltage \(e=200 \sqrt{2} \sin 100t\) volts is connected to a capac...

In an a.c. circuit an alternating voltage e=2002sin100te=200 \sqrt{2} \sin 100t volts is connected to a capacitor of capacity 1μ\muF. The r.m.s. value of the current in the circuit is:
A. 10 mA
B. 100 mA
C. 200 mA
D. 20 mA

Explanation

Solution

The emf of the supply voltage is given in the question. Like a resistor, a capacitor also creates some voltage drop across. It has some 'impedance', which when multiplied by current gives the voltage drop across it.

Formula Used:
Capacitor's reactance (or resistance) is obtained as:
XC=1ωCX_C = \dfrac{1}{\omega C}

Complete step by step answer:
Given, the supply:
e=2002sin100te=200 \sqrt{2} \sin 100t volts
And the value of C = 1μ\mu F

We know that an alternating current source will have a supply voltage given by V0sinωtV_0 \sin \omega t type of expression. We only compare this with our given supply voltage. The direct comparison gives us:
V0=2002V_0 = 200 \sqrt{2} volts
and
ω=100\omega = 100 Hz
The reactance of the capacitor can be found by plugging in the values as:
XC=1ωC=1100×106=10000X_C = \dfrac{1}{\omega C} = \dfrac{1}{100 \times 10^{-6}} = 10000 ohms
We know, by ohm's law that the current I in the circuit with resistance R and supply voltage V is just V/R. Similarly, we can write:
I0=V0XCI_0 = \dfrac{V_0}{X_C}
Thus,
I0=200210000I_0 = \dfrac{200 \sqrt{2}}{10000}A
But, we need to find the rms value of the current, so we use the formula:
Irms=I02I_{rms} = \dfrac{I_0}{\sqrt{2}}
Therefore, we can get:
Irms=2100I_{rms} = \dfrac{2}{100}A
Or, we can say:
Irms=20I_{rms} = 20mA
Thus, the correct option (D). 20 mA. This is the value of rms ac current in the circuit consisting of 1μ\muF capacitor.

Note:
If more components are present in the circuit, the situation becomes different. If two capacitors were present in series we had to use equivalent capacitance in the reactance formula. If a resistor would have been present we would have done some vector algebra as the current in a capacitor lags behind from a resistor.