Kirchhoff laws are essential for resistor network theory. They were formulated by the German scientist Gustav Kirchhoff in 1845. The laws describe the conversation of energy and charge in electrical networks. They are also called Kirchhoff’s circuit laws. Kirchhoff contributed also to other fields of science, therefore the generic term Kirchhoff law can have different meanings. Both circuit laws, the Kirchhoff Current Law (KCL) and the Kirchhoff Voltage Law (KVL), will be explained in detail.
Kirchhoff Current Law (KCL)
The Kirchhoff Current Law (KCL) states that the sum of all currents leaving a node in any electrical network is always equal to zero. It is based on the principle of conservation of electric charge. The law is also referred to as Kirchhoff’s first law. In formula form this is given by:
The KCL is easier to understand with an example. Look at an arbitrary “node A” from a resistor network. Three branches are connected to this node. Two of the currents are known: I1 is 2 amperes and I2 is 4 amperes. The current law states that the sum of I1, I2 and I3 must be zero:
Kirchhoff Voltage Law (KVL)
The second law is also called Kirchhoff’s voltage law (KVL). It states that the sum of the voltage rises and voltage drops over all elements in a closed loop is equal to zero. In formula form:
Let’s take an example to explain the second law. Consider a part of a resistor network with an internal closed loop, as shown in the picture below. We want to know the voltage drop between node B and C (VBC). The sum of voltage drops in the loop ABCD must be zero, so we can write:
The two circuit laws are explained in the video below.
Kirchhoff law example
The Kirchhoff laws form the basis of network theory. Combined with Ohm’s law and the equations for resistors in series and parallel, more complex networks can be solved. Several examples of resistor circuits are given to illustrate how Kirchhoff can be used.
Example 1: the bridge circuit
Bridge circuits are a very common tool in electronics. They are used in measurement, transducer and switching circuits. Consider the bridge circuit below. In this example will be shown, how to use Kirchhoff’s laws to determine the cross current I5. The circuit has four bridge sections with resistors R1 – R4. There is one cross bridge connection with resistor R5. The bridge is subject to a constant voltage V and I.
The first Kirchhoff law states that the sum of all currents in one node is zero. This results in:
The second Kirchhoff law states the sum of all voltages across all elements in a loop is zero. This leads to:
The six sets of equations above can be rewritten using normal algebra to find the expression for I5 (the current in the cross branch):
The equation shows that the bridge current is equal to zero the bridge is balanced:
Example 2: the star delta connection
Kirchhoff’s laws can be used to convert a star connection to a delta connection. This is often done to solve complex networks. A widely used application for star delta connections is to limit the starting current of electric motors. The high starting current causes high voltage drops in the power system. As a solution, the motor windings are connected in the star configuration during starting and then change to the delta connection.
The star connection as shown in the figure above, has the same voltage drops and currents as the delta connection shown on the right side, only when the following equations are valid: