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Question: In the circuit shown in figure reading of voltmeter is\[{V_1}\]when only\[{S_1}\]is closed. The read...

In the circuit shown in figure reading of voltmeter isV1{V_1}when onlyS1{S_1}is closed. The reading of voltmeter isV2{V_2}when onlyS2{S_2}is closed. The reading of voltmeter isV3{V_3}when bothS1{S_1}andS2{S_2}are closed. Then,
A) V2>V1>V3{V_2} > {V_1} > {V_3}
B) V3>V2>V1{V_3} > {V_2} > {V_1}
C) V3>V1>V2{V_3} > {V_1} > {V_2}
D) V1>V2>V3{V_1} > {V_2} > {V_3}

Explanation

Solution

In case of the closed circuit, we use Kirchhoff's voltage law to find the potential flowing through the given closed circuit.
Complete step by step answer:
Kirchhoff’s law:
Kirchhoff’s voltage law states that “the algebraic sum of the product of current and resistance of the closed circuit is equal to the total EMF provided in the circuit. The symbol of the product of current and resistance depends upon the direction of the current flow in the circuit.
By applying this law we can solve the given problem

(i) The voltmeter reads the valueV1{V_1}when only the switchS1{S_1}is closed. Applying Kirchhoff’s voltage law in the given circuit in which only the switchS1{S_1}is closed. Therefore,
3IR+IR=E\Rightarrow 3IR + IR = E
4IR=E\Rightarrow 4IR = E

I=E4R\therefore I = \dfrac{E}{{4R}}
Now we can find the value of the potential through the resistance 3R3R is,

V1=IR \Rightarrow {V_1} = IR
V1=E4R×3R\Rightarrow {V_1} = \dfrac{E}{{4R}} \times 3R
V1=34E\therefore {V_1} = \dfrac{3}{4}E--------(1)

(ii) The voltmeter reads the valueV2{V_2}when only the switchS2{S_2}is closed. In this case, on applying Kirchhoff’s voltage law we get,
6IR+IR=E\Rightarrow 6IR + IR = E
7IR=E\Rightarrow 7IR = E
I=E7R\therefore I = \dfrac{E}{{7R}}

Therefore the voltage through the resistance 6R6R is,
V2=E7R×6R\Rightarrow {V_2} = \dfrac{E}{{7R}} \times 6R
V2=67E\therefore {V_2} = \dfrac{6}{7}E -------------- (2)
(iii) The voltmeter reads the value V3{V_3}when both switches are closed. Kirchhoff's law is applied in this case and the two resistances 3R3R and 6R6R are in parallel now. Hence the net resistance for the parallel loop is
13+16=36\Rightarrow \dfrac{1}{3} + \dfrac{1}{6} = \dfrac{3}{6}
2R\Rightarrow 2R
The Kirchhoff’s law is applied in this case,
IR+2IR=E\Rightarrow IR + 2IR = E
3IR=E\Rightarrow 3IR = E
I=E3R\therefore I = \dfrac{E}{{3R}}

The voltage flows when both switches are closed,
V3=E3R×2R\Rightarrow {V_3} = \dfrac{E}{{3R}} \times 2R
V3=23E\therefore {V_3} = \dfrac{2}{3}E ------------- (3)
From (1), (2) & (3), we can say that theV2>V1>V3{V_2} > {V_1} > {V_3}.

Hence option A is the correct answer.

Note:
Ohm’s law states that the potential difference across two points is directly proportional to the current flowing through the resistance RR. Using Ohm’s law, we are able to find the value of the voltage across any resistance RR. Kirchhoff's voltage law is used to find the value of the voltage in the closed circuit.