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Question: A balanced Wheatstone's bridge is shown in the figure. Find the value of the currents \({i_1}\) and ...

A balanced Wheatstone's bridge is shown in the figure. Find the value of the currents i1{i_1} and i2{i_2}.

A) 0.9A0.9{\text{A}} and 0.6A0.6{\text{A}}
B) 0.3A0.3{\text{A}} and 0.2A0.2{\text{A}}
C) 0.5A0.5{\text{A}} and 0.7A0.7{\text{A}}
D) 0.7A0.7{\text{A}} and 0.6A0.6{\text{A}}

Explanation

Solution

In a balanced Wheatstone's bridge, the ratio of the resistances of the two arms will be the same. Here branches ABC and ADC are connected in parallel but the resistors in each branch form a series connection. So we can find the effective resistance of the circuit which will give us the total current in the circuit. The currents i1{i_1} and i2{i_2} can be then found out using the balance condition of the bridge.

Formulae used:
The effective resistance when two resistors are connected in series is given by, Reff=R1+R2{R_{eff}} = {R_1} + {R_2} where R1{R_1} and R2{R_2} are the resistances of the two resistors.
The effective resistance when two resistors are connected in parallel is given by, Reff=R1R2R1+R2{R_{eff}} = \dfrac{{{R_1}{R_2}}}{{{R_1} + {R_2}}} where R1{R_1} and R2{R_2} are the resistances of the two resistors.
The current through a circuit is given by, I=VReffI = \dfrac{V}{{{R_{eff}}}} where Reff{R_{eff}} is the effective resistance of the circuit and VV is the voltage across the circuit.

Complete step by step answer:
Sketch the given circuit diagram and list its parameters.

From the above diagram we have, RAD=3Ω{R_{AD}} = 3\Omega , RDC=6Ω{R_{DC}} = 6\Omega , RAB=2Ω{R_{AB}} = 2\Omega and RBC=4Ω{R_{BC}} = 4\Omega .
The internal resistance of the battery is r=0.4Ωr = 0.4\Omega .
The emf of the battery is V=6VV = 6{\text{V}} .
Here i1{i_1} is the current through ABC and i2{i_2} is the current through ADC.
Let II be the total current through the circuit.
Obtain the effective resistances of the two branches to find the effective resistance of the circuit.
In branch ADB, RAD{R_{AD}} and RDC{R_{DC}} are connected in series and so the effective resistance of branch ADB will be RADC=RAD+RDC{R_{ADC}} = {R_{AD}} + {R_{DC}} ------- (1)
Substituting RAD=3Ω{R_{AD}} = 3\Omega and RDC=6Ω{R_{DC}} = 6\Omega in equation (1) we get, RADC=3+6=9Ω{R_{ADC}} = 3 + 6 = 9\Omega
So the effective resistance of branch ADC is RADC=9Ω{R_{ADC}} = 9\Omega .
Similarly, in branch ABC, RAB=2Ω{R_{AB}} = 2\Omega and RBC=4Ω{R_{BC}} = 4\Omega are connected in series and so the effective resistance of branch ABC will be RABC=2+4=6Ω{R_{ABC}} = 2 + 4 = 6\Omega .
Now the reduced circuit is given below.

In this circuit RADC=9Ω{R_{ADC}} = 9\Omega and RABC=6Ω{R_{ABC}} = 6\Omega are connected in parallel and the internal resistance of the battery is connected in series with it.
So the effective resistance of the circuit will be Reff=RADCRABCRADC+RABC+r{R_{eff}} = \dfrac{{{R_{ADC}}{R_{ABC}}}}{{{R_{ADC}} + {R_{ABC}}}} + r -------- (2)
Substituting RADC=9Ω{R_{ADC}} = 9\Omega , RABC=6Ω{R_{ABC}} = 6\Omega and r=0.4Ωr = 0.4\Omega in equation (2) we get, Reff=9×69+6+0.4=4Ω{R_{eff}} = \dfrac{{9 \times 6}}{{9 + 6}} + 0.4 = 4\Omega
Thus the total resistance of the circuit is Reff=4Ω{R_{eff}} = 4\Omega .
Using Ohm’s law obtains the total current through the circuit.
Ohm’s law gives the current through the given circuit as I=VReffI = \dfrac{V}{{{R_{eff}}}} -------- (3)
Substituting for Reff=4Ω{R_{eff}} = 4\Omega and V=6VV = 6{\text{V}} in equation (3) we get, I=64=1.5AI = \dfrac{6}{4} = 1.5{\text{A}}
Thus the current through the circuit is I=1.5AI = 1.5{\text{A}} .
Using Kirchoff’s junction rule and the balanced condition of the bridge we can find the currents i1{i_1} and i2{i_2} .
According to Kirchoff’s junction rule at point A, the total current II splits into the currents i1{i_1} and i2{i_2} .
i.e., I=i1+i2I = {i_1} + {i_2} ------- (4)
Also, the given Wheatstone's bridge is said to be balanced.
i2RAD=i1RAB\Rightarrow {i_2}{R_{AD}} = {i_1}{R_{AB}} --------- (5)
Substituting for RAB=2Ω{R_{AB}} = 2\Omega and RAD=3Ω{R_{AD}} = 3\Omega in equation (5) we get, 3i2=2i13{i_2} = 2{i_1}
i2=2i13\Rightarrow {i_2} = \dfrac{{2{i_1}}}{3} ------- (6)
Substituting equation (6) in (4) we get, I=i1+2i13=5i23I = {i_1} + \dfrac{{2{i_1}}}{3} = \dfrac{{5{i_2}}}{3}
i1=3I5\Rightarrow {i_1} = \dfrac{{3I}}{5} and on substituting for I=1.5AI = 1.5{\text{A}} we get, i1=3×1.55=0.9A{i_1} = \dfrac{{3 \times 1.5}}{5} = 0.9{\text{A}}
Then back-substituting i1=0.9A{i_1} = 0.9{\text{A}} in equation (6) we get, i2=2×0.93=0.6A{i_2} = \dfrac{{2 \times 0.9}}{3} = 0.6{\text{A}}
Thus the values of the currents are i1=0.9A{i_1} = 0.9{\text{A}} and i2=0.6A{i_2} = 0.6{\text{A}}.

So the correct option is A.

Note: Here the Wheatstone’ bridge is mentioned to be a balanced bridge. In a balanced bridge, the potential drop at points C and D in the given circuit diagram will be the same. This is given by equation (5). Also since the potential drop at C and D are the same, the potential difference between these two points will be zero and so no current will flow through the galvanometer.