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Question

Question: What is the steady current in the \( 2\Omega \) resistor shown in the figure? The internal resistanc...

What is the steady current in the 2Ω2\Omega resistor shown in the figure? The internal resistance of the battery is negligible and the capacitance C=0.5μFC = 0.5\mu F

(A) 0.3A0.3{\text{A}}
(B) 0.6A0.6{\text{A}}
(C) 0.9A0.9{\text{A}}
(D) 1.2A1.2{\text{A}}

Explanation

Solution

A capacitor does not allow steady current (direct current) to flow through it and hence acts as an open circuit. The 2 ohms and 3 ohms are resistors connected in parallel. So we need to calculate the equivalent resistance from the rest of the arms and then using Kirchhoff’s law we can calculate the current.

Formula used: In this solution we will be using the following formula;
V=IRV = IR where VV is the potential difference across a resistor, II is the current flowing through it and RR is the resistance of the resistor
1Rp=1R1+1R2+...+1Rn\dfrac{1}{{{R_p}}} = \dfrac{1}{{{R_1}}} + \dfrac{1}{{{R_2}}} +... + \dfrac{1}{{{R_n}}} where Rp{R_p} is the equivalent resistance of a parallel arrangement of resistors and R1...Rn{R_1}...{R_n} are the individual resistors in the parallel arrangement.

Complete step by step answer
To calculate the current flowing through the 2 ohms resistor, we have to calculate the potential difference across it. Now, the 2 ohms and 3 ohms resistors are in parallel, hence the same potential is across them. The equivalent resistance can be given as
1R2,3=1R2+1R3\dfrac{1}{{{R_{2,3}}}} = \dfrac{1}{{{R_2}}} + \dfrac{1}{{{R_3}}} where R2,3{R_{2,3}} is the equivalent resistance of the 2 and 3 ohms resistor. R2{R_2} and R3{R_3} are the 2 ohms and 3 ohms resistance respectively. Hence
1R2,3=12+13=3+26=56\dfrac{1}{{{R_{2,3}}}} = \dfrac{1}{2} + \dfrac{1}{3} = \dfrac{{3 + 2}}{6} = \dfrac{5}{6}
Hence, by inversion, we get
R2,3=65=1.2Ω{R_{2,3}} = \dfrac{6}{5} = 1.2\Omega
Since there is a capacitor in the middle branch, the middle branch can be eliminated since a capacitor will act as an open circuit. Current will not flow through the branch.
Then, the 1.2Ω1.2\Omega is in series with the 2.8Ω2.8\Omega
We can apply Kirchhoff’s voltage rule across the loop as in
VIR2,3IR2.8=0V - I{R_{2,3}} - I{R_{2.8}} = 0 where VV is the voltage of the battery, and R2.8{R_{2.8}} is the resistance of the 2.8Ω2.8\Omega resistor, and II is the current flowing through the equivalent circuit.
Hence, by inserting the known values
6I(1.2)I(2.8)=06 - I\left( {1.2} \right) - I(2.8) = 0
6=I(1.2+2.8)=4.0I\Rightarrow 6 = I\left( {1.2 + 2.8} \right) = 4.0I
Then, the current
I=64.0=1.5AI = \dfrac{6}{{4.0}} = 1.5A
Then the voltage across AB is
VAB=IR2,3=1.5(1.2)=1.8V{V_{AB}} = I{R_{2,3}} = 1.5(1.2) = 1.8{\text{V}}
Then the current through 2 ohms resistor will be
I2=VABR2=1.82=0.9A{I_2} = \dfrac{{{V_{AB}}}}{{{R_2}}} = \dfrac{{1.8}}{2} = 0.9A
Hence, the correct answer is C.

Note
For clarity, the capacitor does not allow direct current to pass through it because, really, the capacitor is just two conductors placed in proximity to one another, without actually touching. Hence, this causes a break in the circuit.