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Question: The circuit is shown. ![](https://www.vedantu.com/question-sets/ca602ee4-73ba-40e2-8f4f-c3b1e73a7...

The circuit is shown.

What is current through 3Ω3\Omega resistance ??

Explanation

Solution

In this problem, first we need to find the equivalent resistance to find the value of current flowing through the resistor of resistance 3Ω3\Omega . In series combination the current remains the same and voltage will be different whereas in parallel combination the current will be different and voltage will be the same we use this concept to solve the problem.

Formula used:
\to For series combination, the equivalent resistance is given by
Rs=R1+R2+......+Rn{R_s} = {R_1} + {R_2} + ...... + {R_n}
\to For parallel combination, the equivalent resistance is given by
1Rp=1R1+1R2+.......+1Rn\dfrac{1}{{{R_p}}} = \dfrac{1}{{{R_1}}} + \dfrac{1}{{{R_2}}} + ....... + \dfrac{1}{{{R_n}}}
According to ohm’s law,
V=IRV = IR
I=VR\Rightarrow I = \dfrac{V}{R}

Complete step by step answer:
Step 11 :-

In above circuit 2Ω2\Omega , 5Ω5\Omega and 2Ω2\Omega are connected in series because the current is the same in these resistors as shown in above circuit. Therefore,
Rs1=R1+R2+R3{R_{s1}} = {R_1} + {R_2} + {R_3}
Rs1=2+5+2\Rightarrow {R_{s1}} = 2 + 5 + 2
Rs1=9Ω\Rightarrow {R_{s1}} = 9\Omega ………. (1)\left( 1 \right)
Step 22 :-

In the above circuit 9Ω9\Omega and 9Ω9\Omega are connected in parallel because the current is different in these resistors as shown in the above circuit. Therefore,
1Rp=1R1+1R2\dfrac{1}{{{R_p}}} = \dfrac{1}{{{R_1}}} + \dfrac{1}{{{R_2}}}
On substituting we get
1Rp1=19+19\dfrac{1}{{{R_{p1}}}} = \dfrac{1}{9} + \dfrac{1}{9}
On simplifying we get
1Rp1=29\dfrac{1}{{{R_{p1}}}} = \dfrac{2}{9}
Therefore, Rp1=4.5Ω{R_{p1}} = 4.5\Omega ………..(2)\left( 2 \right)

Step 33 :-

In above circuit 2Ω2\Omega, 4.5Ω4.5\Omega and 2Ω2\Omega are connected in series because the current is the same in these resistors as shown in above circuit.Therefore,
Rs2=R1+R2+R3{R_{s2}} = {R_1} + {R_2} + {R_3}
Rs2=2+4.5+2\Rightarrow {R_{s2}} = 2 + 4.5 + 2
Rs2=8.5Ω\Rightarrow {R_{s2}} = 8.5\Omega ………. (3)\left( 3 \right)

Step 44 :-

In the above circuit 8.5Ω8.5\Omega and 8.5Ω8.5\Omega are connected in parallel because the current is different in these resistors as shown in the above circuit. Therefore,
1Rp=1R1+1R2\dfrac{1}{{{R_p}}} = \dfrac{1}{{{R_1}}} + \dfrac{1}{{{R_2}}}
On substituting we get
1Rp2=18.5+18.5\dfrac{1}{{{R_{p2}}}} = \dfrac{1}{{8.5}} + \dfrac{1}{{8.5}}
On simplifying we get
1Rp2=28.5\dfrac{1}{{{R_{p2}}}} = \dfrac{2}{{8.5}}
Therefore, Rp2=4.25Ω{R_{p2}} = 4.25\Omega ………..(4)\left( 4 \right)

Step 55 :-

In above circuit 3Ω3\Omega , 4.25Ω4.25\Omega and 2Ω2\Omega are connected in series because the current is the same in these resistors as shown in above circuit.Therefore,
Req=R1+R2+R3{R_{eq}} = {R_1} + {R_2} + {R_3}
Req=3+4.25+2\Rightarrow {R_{eq}} = 3 + 4.25 + 2
Req=9.25Ω\Rightarrow {R_{eq}} = 9.25\Omega ………. (5)\left( 5 \right)
Step 66 :-
According to ohm’s law
V=IRV = IR
I=VR\Rightarrow I = \dfrac{V}{R}
Substituting the value of VV and RR
Therefore, I=99.25I = \dfrac{9}{{9.25}}
I=0.973A\therefore I = 0.973A

Hence current flow through 3Ω3\Omega resistor is 0.973A0.973A.

Note: In an electric circuit, various components can be connected either in series or in parallel manner to produce different resistive networks. Sometimes, in the same circuit, resistors can be connected in parallel and series, across different loops to produce a more complex resistive network. Resistors are said to be in series if they are joined end to end such that the same current flows through all of them.