Kirchhoff’s laws are fundamental tools for analysing complex electric circuits. They allow us to relate currents and voltages in any network of resistors, batteries and other components.
KCL states that the algebraic sum of currents meeting at a node (junction) is zero:
$$\sum I_{\text{in}} - \sum I_{\text{out}} = 0$$In words, the total current entering a junction equals the total current leaving it.
K \cdot L states that the algebraic sum of the potential differences (voltages) around any closed loop is zero:
$$\sum V_{\text{rise}} - \sum V_{\text{drop}} = 0$$This reflects the conservation of energy for a charge moving around the loop.
When resistors are connected end‑to‑end, they form a series circuit. The same current flows through each resistor, and the total voltage across the series combination is the sum of the individual voltage drops.
The combined (equivalent) resistance $R_{\text{eq}}$ of $n$ resistors $R_1, R_2, \dots , R_n$ in series is given by:
$$R_{\text{eq}} = R_1 + R_2 + \dots + R_n$$Consider a simple series loop containing a battery of emf $E$ and three resistors $R_1$, $R_2$, $R_3$. Applying K \cdot L:
$$E - I R_1 - I R_2 - I R_3 = 0$$Factorising the current $I$ gives:
$$E = I (R_1 + R_2 + R_3) = I R_{\text{eq}}$$Hence the current in the loop is:
$$I = \frac{E}{R_{\text{eq}}}$$| Concept | Mathematical Form | Key Point for Series Circuits |
|---|---|---|
| KCL | $\displaystyle \sum I_{\text{in}} = \sum I_{\text{out}}$ | Current is the same through all series elements. |
| K \cdot L | $\displaystyle \sum V_{\text{rise}} = \sum V_{\text{drop}}$ | Sum of voltage drops equals the source emf. |
| Series Resistance | $\displaystyle R_{\text{eq}} = \sum_{i=1}^{n} R_i$ | Resistances add directly. |
| Current in Series Loop | $\displaystyle I = \dfrac{E}{R_{\text{eq}}}$ | Same current flows through each resistor. |