Concept:
A Wheatstone bridge is used to determine an unknown resistance by comparing it with known resistances.
It consists of four resistors arranged in a diamond shape with a galvanometer connecting the middle junctions.
Let:
- \( P, Q \) be resistances in one branch
- \( R, S \) be resistances in the other branch
- Galvanometer connects junctions \( B \) and \( D \)
The bridge is said to be balanced when no current flows through the galvanometer.
Step 1: Balanced Condition
If no current flows through the galvanometer:
\[
I_g = 0
\]
This means the potentials at points \( B \) and \( D \) are equal:
\[
V_B = V_D
\]
Step 2: Apply Kirchhoff’s Law
Let current \( I_1 \) flow through branch \( P \to Q \),
and current \( I_2 \) flow through branch \( R \to S \).
Potential drop from \( A \) to \( B \):
\[
V_{AB} = I_1 P
\]
Potential drop from \( A \) to \( D \):
\[
V_{AD} = I_2 R
\]
Since \( V_B = V_D \):
\[
I_1 P = I_2 R \quad \cdots (1)
\]
Step 3: Consider lower arms
Potential drop from \( B \) to \( C \):
\[
V_{BC} = I_1 Q
\]
Potential drop from \( D \) to \( C \):
\[
V_{DC} = I_2 S
\]
Again using equal potentials:
\[
I_1 Q = I_2 S \quad \cdots (2)
\]
Step 4: Divide equations (1) and (2)
\[
\frac{I_1 P}{I_1 Q} = \frac{I_2 R}{I_2 S}
\]
Cancel currents:
\[
\frac{P}{Q} = \frac{R}{S}
\]
\[
\boxed{\frac{P}{Q} = \frac{R}{S}}
\]
This is the condition for a balanced Wheatstone bridge.
Physical Meaning:
- No current flows through the galvanometer.
- Potential difference between its terminals is zero.
- The bridge behaves like two independent voltage dividers.
Application:
If one resistance is unknown (say \( S \)):
\[
S = \frac{RQ}{P}
\]
Thus Wheatstone bridge is used for precise resistance measurement.