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Question: The value of current through \(2\Omega \) resistor in the circuit is ![](https://www.vedantu.co...

The value of current through 2Ω2\Omega resistor in the circuit is

A) 10A10A
B) 2.1A2.1A
C) 20A20A
D) 25A25A

Explanation

Solution

To proceed, we have to apply Kirchhoff’s rules. Kirchhoff’s first rule says that the algebraic sum of the currents meeting at a junction in a closed electric circuit is zero. Kirchhoff’s second rule says that the algebraic sum of change in potential around any closed path of an electric circuit (or closed loop) involving resistors and cells in the loop is zero.

Complete answer:
Firstly, let us redraw the circuit by naming the components according to our comfortability.

Let us name the resistors as
R1=2Ω{{R}_{_{1}}}=2\Omega , R2=4Ω{{R}_{2}}=4\Omega , and R3=1Ω{{R}_{3}}=1\Omega
Let the currents flowing through resistors R1,R2,{{R}_{1}},{{R}_{2}}, and R3{{R}_{3}} be I1,I2,{{I}_{1}},{{I}_{2}}, and I3{{I}_{3}}, respectively.
We are also provided with two electromotive forces. Let us call them emf1=10Vem{{f}_{1}}=10V and emf2=20Vem{{f}_{2}}=20V, respectively.
Kirchhoff’s first rule or current rule (KCL) says that the algebraic sum of the currents meeting at a junction in a closed electric circuit is zero. It says that
I=0\sum I=0

Applying this rule in our circuit, we have
I3=I1+I2{{I}_{3}}={{I}_{1}}+{{I}_{2}}, at node B as well as node C. Let this be equation 1.
Kirchhoff’s second rule or voltage rule (KVL) says that the algebraic sum of change in potential around any closed path of an electric circuit (or closed loop) involving resistors and cells in the loop is zero. It says that emf+IR=0\sum emf+\sum IR=0

Applying this rule in closed loop ABCDA, we have
emf1+I3R3+I1R1=010+(I1+I2)1+I1(2)=0(I1+I2)+2I1=103I1+I2=10-em{{f}_{1}}+{{I}_{3}}{{R}_{3}}+{{I}_{1}}{{R}_{1}}=0\Rightarrow -10+({{I}_{1}}+{{I}_{2}})1+{{I}_{1}}(2)=0\Rightarrow ({{I}_{1}}+{{I}_{2}})+2{{I}_{1}}=10\Rightarrow 3{{I}_{1}}+{{I}_{2}}=10...Let this be equation 2.

Applying the same rule to the loop EBCFE, we have
emf2+I3R3+I2R2=020+(I1+I2)1+I2(4)=0(I1+I2)+4I2=20I1+5I2=20-em{{f}_{2}}+{{I}_{3}}{{R}_{3}}+{{I}_{2}}{{R}_{2}}=0\Rightarrow -20+({{I}_{1}}+{{I}_{2}})1+{{I}_{2}}(4)=0\Rightarrow ({{I}_{1}}+{{I}_{2}})+4{{I}_{2}}=20\Rightarrow {{I}_{1}}+5{{I}_{2}}=20.....Let this be equation 3.

Solving equation 2 and equation 3, we have
I2=257A{{I}_{2}}=\dfrac{25}{7}A and I1=157=2.1A{{I}_{1}}=\dfrac{15}{7}=2.1A
Therefore, the current flowing through the resistor,R1=2Ω{{R}_{1}}=2\Omega is given by I1=2.1A{{I}_{1}}=2.1A.

So, the correct answer is “Option B”.

Note:
Kirchhoff’s rules follow sign convention. To make it easy, in KCL, the current flowing towards a node is taken as positive and the current flowing away from the node is taken as negative. In KVL, while traversing a loop, if a negative pole of the cell is encountered first, then its emf is negative, otherwise positive.