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Question: Seven resistors are connected as shown in the diagram: The equivalent resistance in ohms of this net...

Seven resistors are connected as shown in the diagram: The equivalent resistance in ohms of this network between AA and BB is:

A. 6Ω6\Omega
B. 8Ω8\Omega
C. 12Ω12\Omega
D. 20Ω20\Omega

Explanation

Solution

: Identify the parallel and series connection in the given circuit. First solve for the resistors in parallel connection, then the circuit will become a Wheatstone bridge. Check the condition for a balanced Wheatstone bridge.

Formula used:
Resistors connected in series, equivalence resistance Req=R1+R2+R3+...{R_{eq}} = {R_1} + {R_2} + {R_3} + ...
Resistors connected in parallel, equivalence resistance 1Req=1R1+1R2+1R3+...\dfrac{1}{{{R_{eq}}}} = \dfrac{1}{{{R_1}}} + \dfrac{1}{{{R_2}}} + \dfrac{1}{{{R_3}}} + ...

Complete step by step answer:
First name the resistances and redraw the circuit diagram.

In the above circuit, we have to find the equivalent resistance between the terminal A and B.The resistors R6{R_6} and R7{R_7} are connected in parallel.Equivalence of R6{R_6} and R7{R_7} is given as
R67=R6R7R6+R7{R_{67}} = \dfrac{{{R_6} \cdot {R_7}}}{{{R_6} + {R_7}}}
Substitute the values of R6{R_6} and R7{R_7} in the above formula.
R67=8×108+10Ω\Rightarrow {R_{67}} = \dfrac{{8 \times 10}}{{8 + 10}}\Omega
R67=409Ω\Rightarrow {R_{67}} = \dfrac{{40}}{9}\Omega
The resistors R1{R_1} and R5{R_5} are connected in parallel.
The equivalent resistor of R1{R_1} and R5{R_5} is given as
R15=R1R5R1+R5{R_{15}} = \dfrac{{{R_1} \cdot {R_5}}}{{{R_1} + {R_5}}}
Substitute the values of R1{R_1} and R5{R_5} in the above formula.
R15=30×630+6Ω\Rightarrow {R_{15}} = \dfrac{{30 \times 6}}{{30 + 6}}\Omega
R15=5Ω\Rightarrow{R_{15}} = 5\Omega

Now the equivalent circuit of above the circuit is as follows

The equivalent circuit of the given circuit is a Wheatstone bridge circuit.
The Wheatstone bridge is balanced because it satisfies the condition R15R4=R2R3\dfrac{{{R_{15}}}}{{{R_4}}} = \dfrac{{{R_2}}}{{{R_3}}}
Therefore, no current flows through the resistor R67{R_{67}}. Remove the R67{R_{67}} from the Wheatstone bridge. The final circuit is as follows.

R15{R_{15}} and R2{R_2} are in series.
The equivalent resistance of R15{R_{15}} and R2{R_2} is R152=R15+R2{R_{152}} = {R_{15}} + {R_2}
R152=5Ω+4Ω=9Ω\Rightarrow {R_{152}} = 5\Omega + 4\Omega = 9\Omega
R4{R_4} and R3{R_3} are in series connection.
The equivalent resistance of R4{R_4} and R3{R_3} is R45=R4+R5{R_{45}} = {R_4} + {R_5}
R45=10Ω+8Ω=18Ω\Rightarrow {R_{45}} = 10\Omega + 8\Omega = 18\Omega
Now R152{R_{152}} and R45{R_{45}} are in parallel connection.
The equivalent resistance of R152{R_{152}} and R45{R_{45}} is Req=R152R45R152+R45{R_{eq}} = \dfrac{{{R_{152}} \cdot {R_{45}}}}{{{R_{152}} + {R_{45}}}}.
Substitute the values of R152{R_{152}} and R45{R_{45}} in the above formula.
Req=9×189+18Ω\Rightarrow {R_{eq}} = \dfrac{{9 \times 18}}{{9 + 18}}\Omega
Req=6Ω\therefore {R_{eq}} = 6\Omega
The equivalent resistance of the given circuit is 6Ω6\Omega .

Hence the correct option is A.

Note: Alternative method:Alternatively, we can solve the circuit by drawing an equivalent circuit of the given circuit with some extra consideration as follows.

To solve the above equivalence circuit, Let the current II enter junction A and leave junction B. A battery of VV voltage is connected across the terminals A and B. For simplification let terminal A is at VV voltage and terminal B is at 00 voltage. Let the junctions C and D are at V1{V_1} voltage and V2{V_2} voltage respectively. Now apply Kirchhoff's current law at the junction A in the above equivalence circuit.
I=I1+I2I = {I_1} + {I_2}

Apply Kirchhoff's current law at the junction C in the above equivalence circuit.
I1=I3+I4{I_1} = {I_3} + {I_4}
From the above circuit diagram, I1=VV15{I_1} = \dfrac{{V - {V_1}}}{5}
I3=V104{I_3} = \dfrac{{{V_1} - 0}}{4}
I3=V14\Rightarrow {I_3} = \dfrac{{{V_1}}}{4}
I4=V1V2409\Rightarrow {I_4} = \dfrac{{{V_1} - {V_2}}}{{\dfrac{{40}}{9}}}
I4=940(V1V2)\Rightarrow {I_4} = \dfrac{9}{{40}}\left( {{V_1} - {V_2}} \right)
Therefore,
VV15=V14+940(V1V2)\dfrac{{V - {V_1}}}{5} = \dfrac{{{V_1}}}{4} + \dfrac{9}{{40}}\left( {{V_1} - {V_2}} \right)
On simplification
27V19V2=8V\Rightarrow 27{V_1} - 9{V_2} = 8V …… (1)
Now apply Kirchhoff's current law at junction D in the above equivalence circuit.
I2+I4=I5{I_2} + {I_4} = {I_5}

From the above circuit diagram, I2=VV210{I_2} = \dfrac{{V - {V_2}}}{{10}}
I5=V208{I_5} = \dfrac{{{V_2} - 0}}{8}
I5=V28\Rightarrow {I_5} = \dfrac{{{V_2}}}{8}
Therefore,
VV210+940(V1V2)=V28\dfrac{{V - {V_2}}}{{10}} + \dfrac{9}{{40}}\left( {{V_1} - {V_2}} \right) = \dfrac{{{V_2}}}{8}
On simplification
9V1+18V2=4V\Rightarrow - 9{V_1} + 18{V_2} = 4V …… (2)
Now solve the two equations (1) and (2) and find the values of V1{V_1} and V2{V_2} in terms of VV. We got,
V1=4V9{V_1} = \dfrac{{4V}}{9},
V2=4V9\Rightarrow {V_2} = \dfrac{{4V}}{9}

Now calculate the value of I1=VV15{I_1} = \dfrac{{V - {V_1}}}{5}
I1=V4V95{I_1} = \dfrac{{V - \dfrac{{4V}}{9}}}{5}
I1=V9\Rightarrow {I_1} = \dfrac{V}{9}
And calculate the value of I2=VV210{I_2} = \dfrac{{V - {V_2}}}{{10}}
I2=V4V910{I_2} = \dfrac{{V - \dfrac{{4V}}{9}}}{{10}}
I2=V18\Rightarrow {I_2} = \dfrac{V}{{18}}
Now we have I=I1+I2I = {I_1} + {I_2}
Substitute the values of I1{I_1} and I2{I_2} in the above formula for II.
I=V9+V18I = \dfrac{V}{9} + \dfrac{V}{{18}}

Further calculating
I=V6\Rightarrow I = \dfrac{V}{6}
The equivalent resistance of the above equivalence circuit between the two terminals A and B is given by
Req=VBVAI{R_{eq}} = \dfrac{{{V_B} - {V_A}}}{I}
Substitute all the required values in the above formula
Req=V0V6{R_{eq}} = \dfrac{{V - 0}}{{\dfrac{V}{6}}}
On further simplification
Req=6Ω{R_{eq}} = 6\Omega
Hence the correct option is (A).