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Question: In the circuit shown in figure, \({{E}_{1}}\) and \({{E}_{2}}\) are two ideal sources of unknown emf...

In the circuit shown in figure, E1{{E}_{1}} and E2{{E}_{2}} are two ideal sources of unknown emfs. Some currents are shown. Potential difference appearing across 6Ω6\Omega resistance is VAVB=10V{{V}_{A}}-{{V}_{B}}=10V.

(This questions has multiple correct options)
A. The current in the 4Ω resistance between C and B is 5A.\text{A}\text{. The current in the 4}\Omega \text{ resistance between C and B is 5A}\text{.}
B. The unknown emf E1 is 36V.\text{B}\text{. The unknown emf }{{\text{E}}_{1}}\ \text{is 36V}\text{.}
C. The unknown emf E2 is 54V.\text{C}\text{. The unknown emf }{{\text{E}}_{2}}\ \text{is 54V}\text{.}
D. The resistance R is equal to 9Ω.\text{D}\text{. The resistance R is equal to 9}\Omega \text{.}

Explanation

Solution

The given problem has a very long solution since we have to find the values of many things. Make use of the Ohms’ law when required. We also need the junction law to solve this problem. Start with assuming the potential at anyone point as zero.

Formula used:
V = iR

Complete step-by-step answer:
In this solution we will be the junction law for current and the Ohm’s law. According to the Ohm’s law, the potential difference across a resistance R, through which a current I is flowing is given as V = iR.
Let us first assume that the potential at point O is zero. Then the potential at points A and F is E2{{E}_{2}} , potential at point E is E1{{E}_{1}}.
It is given that the potential difference of the 6Ω6\Omega resistance is 10V. Then with ohm’s law, the current in this resistance is i=106=53Ai=\dfrac{10}{6}=\dfrac{5}{3}A. The direction of this current is from A to B because the current always flows from the higher potential to a lower potential
Since the 3Ω3\Omega is parallel with this resistance, the potential difference will be 10V. In this resistance also the current will be in the downwards direction and its value will be i=103Ai=\dfrac{10}{3}A.
Then from the junction law, we get that the current in the adjacent 4Ω4\Omega (between D and B) is 103+53=153=5A.\dfrac{10}{3}+\dfrac{5}{3}=\dfrac{15}{3}=5A.
Therefore, the current flowing in the 4Ω4\Omega resistance between C and B is 5A.
Hence, the option is true.
Now, the potential difference across this 4Ω4\Omega resistance will be V=5(4)=20VV=5(4)=20V.
We know that the potential at A is E2{{E}_{2}} and VAVB=10V{{V}_{A}}-{{V}_{B}}=10V.
E2VB=10V\Rightarrow {{E}_{2}}-{{V}_{B}}=10V
VB=E210\Rightarrow {{V}_{B}}={{E}_{2}}-10 …. (i).
Form point B, there is a potential drop of 20V when we reach point D.
This means that VBVD=20V{{V}_{B}}-{{V}_{D}}=20V ….. (ii).
From (i) and (ii) we get,
E210VD=20V{{E}_{2}}-10-{{V}_{D}}=20V
VD=E230\Rightarrow {{V}_{D}}={{E}_{2}}-30.
By applying junction law at point D, we get that the current in the 3Ω3\Omega is 3+5=8A3+5=8A.
Then the potential difference across this resistance will be 8(3)=24V8(3)=24V.
This means that VDVO=24V{{V}_{D}}-{{V}_{O}}=24V.
But VO=0V{{V}_{O}}=0Vand VD=E230{{V}_{D}}={{E}_{2}}-30
E230=24V\Rightarrow {{E}_{2}}-30=24V.
E2=54V\Rightarrow {{E}_{2}}=54V
Hence, option C is true.
The potential at C and D are equal.
VC=E230=5430=24V\Rightarrow {{V}_{C}}={{E}_{2}}-30=54-30=24V.
And
VE=E1{{V}_{E}}={{E}_{1}}.
Therefore, the potential difference across the 4Ω4\Omega resistance is E124=12V{{E}_{1}}-24=12V.
E124=12V\Rightarrow {{E}_{1}}-24=12V
E1=36V\Rightarrow {{E}_{1}}=36V.
Hence, option is B is true.
Now, the potential difference across the resistance R will be E2E1=2R{{E}_{2}}-{{E}_{1}}=2R.
And
E2E1=5436=18V{{E}_{2}}-{{E}_{1}}=54-36=18V
18=2R\Rightarrow 18=2R
R=9Ω\Rightarrow R=9\Omega .
Hence, option D is also true.
Therefore, the correct options are A, B, C and D.

So, the correct answers are “Option A,B,C and D”.

Note: We have solved the question by using Ohm’s law and junction law. One can use the Kirchhoff‘s voltage law for the required loops. The law is also called a loop law.
Remember that current always flows higher potential to a lower potential. Hence, there is a potential drop across a resistance in the direction of the current.