Current generally enters the given galvanometer and further divides into two equal magnitude currents which are, I1 and I2. This condition is only seen when the current passing via a galvanometer is zero.
Hence, I1P = I2R … [1]
In a balanced condition, the currents in the bridge can be represented as:
| I1 = I3= E/(P+Q)I2 = I4= E/(R+S) |
Where,
- E = emf of the battery.
Now, after replacing the value of I1 and I2 in equation [1], we can obtain:
⇒ PE/(P+Q) = RE/(R+S)
⇒ P/(P+Q) = R/(R+S)
⇒ P/(R+S)=R/(P+Q)
⇒ PR+PS = RP+RQ
Thus, PS = RQ … [2]
And, R = PQ × S … [3]
\(\therefore\) Equation [2] demonstrates the balanced condition of the bridge. And, Equation [3] specifies the value of the unknown resistance.
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