19Kirchhoff’s Laws: Circuit Analysis

19.1 Introduction

In this chapter, we will examine the Kirchhoff’s laws, created by the German physicist Gustav Robert Kirchhoff (1824–1887) and how these laws can be used to find unknowns in electric circuits.

19.2 Kirchhoff's Laws

To use the Kirchhoff’s laws, it is necessary to understand two concepts: nodes and meshes.

19.2.1 Nodes or Junctions

It is a point where two or more wires connect.

Figure 19.1 shows a circuit with two nodes, A and B, where all components connect.

A circuit having a voltage source labeled V1 (20 V), a current source labeled I4 (3 A), resistors labeled R1 (5Ω), R2 (5Ω), R3 (20Ω), and R4 (2Ω), DC voltage source labeled B2 (10 V), and two nodes labeled A and B.

Figure 19.1 Two nodes, A and B.

19.2.2 Mesh

It is any closed path in which current circulates.

Figure 19.2 shows dashed lines that represent the three meshes possible for the circuit: M1, M2, and M3.

A circuit having a voltage source labeled V1 (20 V), current source labeled I4 (3 A), DC voltage source labeled B2 (10 V), resistors labeled R1 (5Ω), R2 (5 Ω), R3 (20 Ω), and R4 (2 Ω). Dashed lines represent 3 meshes for M1, M2, and M3.

Figure 19.2 Three meshes, M1, M2, and M3.

19.2.3 Kirchhoff's First Law

Kirchhoff's first law, also known as the Kirchhoff’s current law (KCL), postulates that at any junction in a circuit, the sum of the currents arriving at the junction is equal to the sum of the currents leaving the same junction.

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