Concept:
A Wheatstone bridge is used to compare resistances.
It consists of four resistors arranged in a diamond shape with a galvanometer between the middle junctions.
Let the four resistances be:
\[
P, \; Q, \; R, \; S
\]
Step 1: Bridge configuration.
\( P \) and \( Q \) in one branch
\( R \) and \( S \) in the other branch
Galvanometer connected between junctions B and D
Bridge is balanced when no current flows through galvanometer.
Step 2: Condition for balance.
If no current flows through galvanometer:
Potential at junction B = potential at junction D
So:
\[
V_B = V_D
\]
Step 3: Using potential division.
Current through branch \( P, Q \) = \( I_1 \)
Current through branch \( R, S \) = \( I_2 \)
Potential at B (between \( P \) and \( Q \)):
\[
V_B = I_1 P
\]
Potential at D (between \( R \) and \( S \)):
\[
V_D = I_2 R
\]
For balance:
\[
I_1 P = I_2 R \quad \cdots (1)
\]
Step 4: Total potential drop in branches.
Since both branches are across the same battery:
\[
I_1 (P + Q) = I_2 (R + S) \quad \cdots (2)
\]
Step 5: Divide (1) by (2).
\[
\frac{I_1 P}{I_1 (P+Q)} = \frac{I_2 R}{I_2 (R+S)}
\]
\[
\frac{P}{P+Q} = \frac{R}{R+S}
\]
Step 6: Simplify.
Cross multiplying:
\[
P(R+S) = R(P+Q)
\]
\[
PR + PS = PR + RQ
\]
\[
PS = RQ
\]
Final Condition:
\[
\boxed{\frac{P}{Q} = \frac{R}{S}}
\]
This is the condition for a balanced Wheatstone bridge.
Conclusion:
When the ratio of resistances in one branch equals the ratio in the other branch, no current flows through the galvanometer and the bridge is balanced.