Kirchcoff’s Law or circuit Laws is comprised of two equality mathematical equations that deal with resistance, current and voltage in the lumped elemental model of electrical circuits. The laws are fundamental to circuit theory. They quantify how current flows and voltages vary through a loop in a circuit. Gustav Robert Kirchhoff, a German physicist, contributed to the fundamental understanding of electrical circuits.
What are Kirchhoff’s Laws?
There are two laws as follows:
 Kirchhoff’s first law, also known as the Kirchhoff’s current law (KCL) states that the current flowing into a node must be equal to the current flowing out of the node. This is a consequence of charge conservation.
 Kirchhoffâ€™s second law, also known as the Kirchhoff’s voltage law (KVL) states that the sum of all voltages around a closed loop in any circuit must be equal to zero. This again is a consequence of charge conservation and also conservation of energy.
Here in this short piece of article, we will be discussing Kirchhoffâ€™s second law.
Kirchhoff’s Voltage Law
Kirchhoff’s Second Law or the voltage law states that
The net electromotive force around a closed circuit loop is equal to the sum of potential drops around the loop
It is termed as Kirchhoff’s Loop Rule, which is an outcome of an electrostaticÂ field which is conservative.
Hence,
 If a charge moves around a closed loop in a circuit, it must gain as much energy as it loses.
 The above can be summarized as ” the gain in energy by the charge = corresponding losses in energy through resistances
 Mathematically, the total voltage in a closed loop of a circuit is expressed as \(\sum V=0\).
The below figure illustrates that the total voltage around a closed loop must be zero.
This law manages the voltage drops at different branches in an electrical circuit. Consider one point on a closed loop in an electrical circuit. If somebody goes to another point in a similar ring, he or she will find that the potential at that second aspect might be not quite the same as the first point.
On the off chance that he or she keeps on setting off to some unique point on the loop and he or she may locate some extraordinary potential in that new area. If he or she goes on further along that closed loop,Â eventually he or she achieves the underlying point from where the voyage was begun.
That implies, he or she returns to a similar potential point in the wake of the intersectionÂ through various voltage levels. It can be then again said that the gain in electrical energy by the charge is equal to corresponding losses in energy through resistances.
Related Article:
Solving circuit using Kirchhoff’s Second Law

 The first and foremost step is to draw a closed loop to a circuit. Once done with it draw the direction of the flow of current.
 Defining our sign convention is very important
 Using Kirchhoff’s first law, at B and A we get, \(I_{1}+I_{2}=I_{3}\)
 By making use of above convention and Kirchoffâ€™s Second Law
From Loop 1 we have:
\(10=R_{1}*I_{1}+R_{3}*I_{3}\)
\(=10I_{1}+40I_{3}\)
\(1=I_{1}+4I_{3}\)
From Loop 2 we have :
\(20=R_{2}*I_{2}+R_{3}*I_{3}\)
\(20I_{2}+40I_{3}\)
\(1=I_{2}+2I_{3}\)
From Loop 3 we have :
\(1020=10I_{1}20I_{2}\)
\(1=I_{1}+2I_{2}\)
 By making use of Kirchhoff’s First law \(I_{1}+I_{2}=I_{3}\)
Equation reduces as follows (from Loop 1 ) :
\(1=5I_{1}+4I_{2}\)
Equation reduces as follows ( from Loop 2 ) :
\(1=2I_{1}+3I_{2}\)
 This results in the following Equation: \(I_{1}=\frac{1}{3}I_{2}\)
 From last three equations we get, \(1=\frac{1}{3}I_{2}+2I_{2}\) \(I_{2}=0.429A\) \(I_{1}=0.143A\) \(I_{3}=0.286A\)
Advantages and Limitations of Kirchhoffs Law
The advantages of the laws are:
 It makes the calculation of unknown voltages and currents easy
 The analysis and simplification of complex closedloop circuits becomes manageable
Kirchhoff’s laws work under the assumption that there are no fluctuating magnetic fields in the closed loop. Electric fields and electromotive forceÂ could be induced which results in the breaking of Kirchhoff’s rule under the influence of the varying magnetic field.