Kirchhoff's law consists of two rules that apply to the current and potential difference in electrical circuits:
1. Kirchhoff's Current Law (KCL): The total current entering a junction equals the total current leaving the junction. Mathematically:
\[
\sum I_{\text{in}} = \sum I_{\text{out}}
\]
2. Kirchhoff's Voltage Law (KVL): The sum of the electrical potential differences (voltages) around any closed loop or circuit is zero. Mathematically:
\[
\sum V = 0
\]
Now, for the second part of the question, we use the principle of the metre bridge. The balance condition for a metre bridge is given by:
\[
\frac{R}{S} = \frac{l_1}{l_2}
\]
Where:
- \(R\) and \(S\) are the resistances in the bridge,
- \(l_1\) is the length on one side of the bridge,
- \(l_2\) is the length on the other side.
Given:
- The original balance point occurs at \(l_1 = 34~\text{cm}\) and \(l_2 = 52~\text{cm}\). Thus, the equation becomes:
\[
\frac{R}{S} = \frac{34}{52} = \frac{17}{26}
\]
Now, when a resistance of 12 ohms is connected in parallel to \(S\), the balance point shifts to a new position. The equivalent resistance of the parallel combination of \(S\) and \(12~\Omega\) is:
\[
S' = \frac{S \times 12}{S + 12}
\]
The new balance condition is:
\[
\frac{R}{S'} = \frac{l_1'}{l_2'}
\]
Given the new lengths:
- \(l_1' = 34~\text{cm}\) and \(l_2' = 68~\text{cm}\), the ratio becomes:
\[
\frac{R}{S'} = \frac{34}{68} = \frac{1}{2}
\]
Now, we solve for \(S'\):
\[
\frac{R}{S'} = \frac{1}{2} $\Rightarrow$ S' = 2R
\]
Substituting the expression for \(S'\):
\[
\frac{S \times 12}{S + 12} = 2R
\]
Now, substitute \(R = \frac{17}{26}S\) from the earlier equation:
\[
\frac{S \times 12}{S + 12} = 2 \times \frac{17}{26} S
\]
Simplifying the equation, we solve for \(S\) and find the values of \(R\) and \(S\).