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Question: Derive the condition for balance of a Wheatstone's bridge using Kirchhoff's rules....

Derive the condition for balance of a Wheatstone's bridge using Kirchhoff's rules.

Explanation

Solution

Draw the Wheatstone bridge circuit diagram first and then try to analyse the condition. By using the notion of current flow and voltage division, try to understand the concept of the bridge and obtain the required balanced condition. The circuit laws of Kirchhoff are two equalities dealing with the current and potential difference in the electrical circuit lumped element model.

Complete answer:
It can be mathematically expressed, as per Kirchhoff's first rule, as:
Σi=0\Sigma i=0
Where Σi\Sigma i is the sum of current entering the junction and current leaving the junction.
It can be mathematically expressed, as per Kirchhoff's first rule, as:
ΣiR=ΣE\Sigma i R=\Sigma E
Where ΣR\Sigma R is the resistance at the junction and ΣE\Sigma E is the emf at the junction.

Here GG is the galvanometer and it is used to measure the current flowing across two points.
And R1,R2,R3R_{1}, R_{2}, R_{3} and RxR_{x} are the resistances connected as shown in the above diagram.
Across the points and as shown, the resistances are related. If the current flows through the circuit and the circuit,
No deflection is provided by the galvanometer, so the bridge is balanced. We must have the conditions for a balanced bridge.
as:
RxR3=R1R2\dfrac{R_{x}}{R_{3}}=\dfrac{R_{1}}{R_{2}}
Let the total current flowing in the circuit be I. Now this current is divided into two parts i1i_1 and i2i_2 flowing through
Rx,R3R_{x}, R_{3} and R1,R2.R_{1}, R_{2} . When the Wheatstone is balanced, the galvanometer shows zero deflection, that is the potential
of BB and CC will be equal. In the closed circuit ABCD, by Kirchhoff's second law, we will have:
i1R1i2Rx=0\Rightarrow i_{1} R_{1}-i_{2} R_{x}=0
i1R1=i2Rx\Rightarrow i_{1} R_{1}=i_{2} R_{x} - -equation 1
And
i1R2i2R3=0i_{1} R_{2}-i_{2} R_{3}=0
i1R2=i2R3\Rightarrow i_{1} R_{2}=i_{2} R_{3} - -equation 2
Dividing equation 1 by equation 2, we have i1R1i1R2=i2Rxi2R3\dfrac{i_{1} R_{1}}{i_{1} R_{2}}=\dfrac{i_{2} R_{x}}{i_{2} R_{3}}
R1R2=RxR3\therefore \dfrac{R_{1}}{R_{2}}=\dfrac{R_{x}}{R_{3}}
Which is the required condition.

Note:
Remember that Kirchhoff's law has two rules. Using both the rules, the condition for balanced Wheatstone may be obtained. The laws of Kirchhoff are used to study any type of circuit, whether the circuit is simple or complex.