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Question: In the circuit shown, value of \(I\) in ampere is ![](https://www.vedantu.com/question-sets/970675...

In the circuit shown, value of II in ampere is

A. 11
B. 0.600.60
C. 0.40.4
D. 1.51.5

Explanation

Solution

Hint: The given circuit has a combination of resistors both series and parallel, to find I, simplify the resistors to RnetR_{net} and use Ohm’s law.

Resistors in series: RS=R1+R2R_{S}=R_{1}+R_{2}
Resistors in parallel: 1RP=1R1+1R2\dfrac{1}{R_{P}}=\dfrac{1}{R_{1}}+\dfrac{1}{R_{2}}
Ohm’s Law that: V=IRV=IR

Formula used:
Resistors in series: RS=R1+R2R_{S}=R_{1}+R_{2}
Resistors in parallel: 1RP=1R1+1R2\dfrac{1}{R_{P}}=\dfrac{1}{R_{1}}+\dfrac{1}{R_{2}}
Ohm’s Law that: V=IRV=IR

Complete step-by-step answer:
To find the value of II we need to simplify the diagram. This can be done by using the resistor in series and parallel formula.
Resistors in series: RS=R1+R2R_{S}=R_{1}+R_{2} and resistors in parallel: 1RP=1R1+1R2\dfrac{1}{R_{P}}=\dfrac{1}{R_{1}}+\dfrac{1}{R_{2}}
We also know from Ohm’s Law that: V=IRV=IR
Using the above, since two 4Ω4\Omega resistors are in parallel

1RP=14+14=12\dfrac{1}{R_{P}}=\dfrac{1}{4}+\dfrac{1}{4}=\dfrac{1}{2}
RP=2ΩR_{P}=2\Omega
Again, 2Ω  ,4Ω2\Omega \; , 4\Omega resistors are in series

RS=4+2=6ΩR_{S}=4+2=6\Omega
Again,4Ω  ,6Ω4\Omega \; , 6\Omega are in parallel

1RP=14+16=6+46×4=1024\dfrac{1}{R_{P}}=\dfrac{1}{4}+\dfrac{1}{6}=\dfrac{6+4}{6\times 4}=\dfrac{10}{2 4}
RP=2.4ΩR_{P}=2.4\Omega
Again, 2.4Ω  ,1.6Ω2.4\Omega \; , 1.6\Omega resistors are in series

Rnet=2.4+1.6=4ΩR_{net}=2.4 +1.6=4\Omega
Rnet=4ΩR_{net}=4\Omega
Since V=4VV=4V
From Ohm’s law; V=IRnetV=IR_{net}
4=I×44=I\times 4
I=1AI=1A
Hence the answer is A. 1

Additional Information:
Resistors are said to be in series whenever the current flows through the resistor equally. The equivalent resistance of a series resistor is equal to the algebraic sum of the individual resistances. The current in the circuit depends on the voltage supplied by the voltage source and the potential crop across the resistor. As energy is conserved, the sum of potential drop due to each resistor is equal to the voltage source.
V=V1+V2=IR1+IR2=I(R1+R2)=IRnetV=V_{1}+V_{2}=IR_{1}+IR_{2}=I(R_{1}+R_{2})=IR_{net}
I=VRnetI=\dfrac{V}{R_{net}}
Rnet=R1+R2R_{net}=R_{1}+R_{2}
Similarly, resistors are said to be in parallel when one end of the resistors are connected by a wire, and the other end by another wire, thus the potential drop across each resistor is the same. At the junction since different currents flow through the different resistors, the sum of the individual currents is equal to the current in the circuit.
I=I1+I2=VR1+VR2I=I_{1}+I_{2}=\dfrac{V}{R_{1}}+\dfrac{V}{R_{2}}
I=V(1R1+1R2)=VRnetI=V(\dfrac{1}{R_{1}}+\dfrac{1}{R_{2}})=\dfrac{V}{R_{net}}
1Rnet=1R1+1R2\dfrac{1}{R_{net}}=\dfrac{1}{R_{1}}+\dfrac{1}{R_{2}}

Note: Be careful in identifying if the resistance is connected in series or parallel, and use the proper formula. While using resistors in parallel formula, don’t forget to take the reciprocals of the resistance. Also remember the principle behind the connections.