- Kirchhoff’s Rule
- At any junction, the sum of the currents entering the junction is equal to the sum of the currents leaving the junction.
- The algebraic sum of the charges in potential around any closed loop involving resistors and cells in the loop is zero.
Condition of balance of a Wheatstone bridge: The circuit diagram of Wheatstone bridge is shown in fig.
P, Q, R and S are four resistance forming a closed bridge, called Wheatstone bridge. A battery is connected across A and C, while a galvanometer is connected between B and D. At balance, there is no current in galvanometer.
Derivation of Formula: Let the current given by battery in the balanced position be I. This current on reaching point A is divided into two parts I1 and I2 . As there is no current in galvanometer in balanced state, current in resistances P and Q is I1 and in resistances R and S it is I2 .

Applying Kirchhoff’s I law at point A
I - I1 - I2 = 0 or I = I1 + I2 - - - - - - - - (i)
Applying Kirchhoff’s II law to closed mesh ABDA
- I1P + I2R = 0 or I1P = I2 R - - - - - - - (ii)
Applying Kirchhoff’s II law to mesh BCDB
- I1Q + I2S = 0 or I1Q = I2S - - - - -- - (iii)
Dividing equation (ii) by (iii), we get
$\frac{\text{I}_{1}\text{P}}{\text{I}_{1}\text{Q}} = \frac{\text{I}_{2}\text{R}}{\text{I}_{2}\text{S}}\text{ or }\frac{\text{P}}{\text{Q}} = \frac{\text{R}}{\text{S}}$ - - - - - - -(iv)
This is the condition of balance of Wheatstone bridge.
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For null point at D, balance length $\ell_{1}$ = 40 cm
So, $\frac{\text{R}_{1}}{\text{R}_{2}} = \frac{\text{AD}}{\text{DC}} =\frac{40}{(100- 40)} = \frac{2}{3}$ - - - -- - (i)
If resistance 10 $\Omega$ is connected in series of R1, then balance length AD' > AD i.e. balance point shifts by length ‘y’ towards C i.e., AD = 60 cm.
$\frac{\text{R}_{1} + 10}{\text{R}_{2}} = \frac{\text{AD}"}{\text{D}'\text{C}} = \frac{60}{100-60} = \frac{3}{2}$
$\frac{\text{R}_{1}}{\text{R}_{2}} + \frac{10}{\text{R}_{2}} =\frac{3}{2}$- - - - - -- -- - -(ii)
From equations (1) and (2), we have
$\frac{2}{3} +\frac{10}{\text{R}_{2}} =\frac{3}{2}$
$\frac{10}{\text{R}_{2}} = \frac{3}{2} - \frac{2}{3} =\frac{9-4}{6} = \frac{5}{6}$
$\Rightarrow\text{R}_{2} = \frac{ 10\times6}{5} = 12\text{ ohm}$
From equation (1), we have
$\frac{\text{R}_{1}}{12} = \frac{2}{3}\Rightarrow\text{R}_{1} = \frac{12\times2}{3} =8\text{ ohm}.$