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Question: Find the potential difference between points \(A\) and \(B\) i.e. (\({V_A} - {V_B}\)) in the network...

Find the potential difference between points AA and BB i.e. (VAVB{V_A} - {V_B}) in the network shown in figure.

Explanation

Solution

We shall assume the resistance of the middle resistance as RR and the current flowing through it as II. We will also need to assume another current which has been assumed as I1{I_1} flowing in the branch C  AC\;A. The new diagram is as shown below with the currents shown as applicable. Next, we shall apply KVL in the loops AC  BAAC\;BA and AD  BAAD\;BA to get two equations from which we calculate II.

Complete step by step solution:
The diagram has been redrawn with the currents assumed in the respective branches. All the assumed currents and resistance have been shown in red.
We have assumed the value of the resistance in the branch A  BA\;B as RR. The voltage between the points AA and BB i.e. (VAVB{V_A} - {V_B}) in the network shown will be dependent on the value of the resistance RR.

The values of the currents in each branch have been shown. We will apply Kirchhoff's Voltage Law in the loop AC  BAAC\;BA and AD  BAAD\;BA respectively to get the required values of I1{I_1} and II.
After applying Kirchhoff's Voltage Law in the loop AD  BAAD\;BA, we will get
IR+2(2+II1)=3(I1I)IR + 2(2 + I - {I_1}) = 3({I_1} - I)
IR+4+2I2I1=3I13I\Rightarrow IR + 4 + 2I - 2{I_1} = 3{I_1} - 3I
Now on rearranging the terms, we get
IR+5I=5I14\Rightarrow IR + 5I = 5{I_1} - 4
I=5I14R+5\Rightarrow I = \dfrac{{5{I_1} - 4}}{{R + 5}}
Again applying Kirchhoff's Voltage Law in the loop AB  CAAB\;CA, we get
2I1+IR=(2I1)32{I_1} + IR = (2 - {I_1})3
Now substituting the value of II in the above equation, we get
2I1+(5I14R+5)R=(2I1)32{I_1} + (\dfrac{{5{I_1} - 4}}{{R + 5}})R = (2 - {I_1})3
(R+5)2I1+R(5I14)=(2I1)3(R+5)\Rightarrow (R + 5)2{I_1} + R(5{I_1} - 4) = (2 - {I_1})3(R + 5)
2RI1+10I1+5RI14R=6R+303I1R15I1\Rightarrow 2R{I_1} + 10{I_1} + 5R{I_1} - 4R = 6R + 30 - 3{I_1}R - 15{I_1}
On rearranging the terms, we get
10RI1+25I1=10R+30\Rightarrow 10R{I_1} + 25{I_1} = 10R + 30
I1=2R+62R+5\Rightarrow {I_1} = \dfrac{{2R + 6}}{{2R + 5}}
Now, substituting this value of I1{I_1} in II, we get
I=1R+5(10R+302R+54)I = \dfrac{1}{{R + 5}}(\dfrac{{10R + 30}}{{2R + 5}} - 4)
I=1R+5(10R+308R202R+5)\Rightarrow I = \dfrac{1}{{R + 5}}(\dfrac{{10R + 30 - 8R - 20}}{{2R + 5}})
I=1R+5(2R+102R+5)\Rightarrow I = \dfrac{1}{{R + 5}}(\dfrac{{2R + 10}}{{2R + 5}})
Upon solving further we get
I=22R+5I = \dfrac{2}{{2R + 5}}.
Now the voltage drop between the points AA and BB i.e. (VAVB{V_A} - {V_B}) is given by
VAVB=IR{V_A} - {V_B} = IR
VAVB=2R2R+5\Rightarrow {V_A} - {V_B} = \dfrac{{2R}}{{2R + 5}}
This is the required potential difference between the two given points.
Thus the required answer is 2R2R+5V\dfrac{{2R}}{{2R + 5}}{\mkern 1mu} V.

Note:
We have assumed the resistance of the middle resistor, as the voltage drop will be dependent on the resistance of the resistor. This is already shown by the answer found as VAVB=2R2R+5{V_A} - {V_B} = \dfrac{{2R}}{{2R + 5}} is an equation dependent on the value of the assumed resistance RR. We can also see that since the product of the diagonal resistances is not equal in the above bridge-circuit, some current will flow, assumed II.