Kirchhoff’s Laws:
Some time we encounter
circuit where simplification by series and parallel combination is impossible.
Consequently, Ohm’s law cannot be applied to solve such circuits. Kirchhoff
gave two laws to solve such complex circuits, namely:
1. Kirchhoff’s Current Law (KCL) 2.
Kirchhoff’s Voltage Law (KVL)
Kirchhoff’s Current Law (KCL):
The algebraic sum of the currents meeting at a junction in an
electric circuit is zero.

(I1) + (I4) + (-I2) + (-I3) = 0
I1 + I4 = I2 + I3
i.e., Sum of incoming current = sum of outgoing
currents
Hence, Kirchhoff’s current
law may also started as under:
The sum of current flowing towards any junction in an electrical
circuit is equal to the sum currents flowing away from the junction.
Note: Kirchhoff’s
current law also called junction rule.
Kirchhoff’s Voltage Law (KVL):
This
laws relate to e.m.fs and voltage drops in a closed circuit or loop and may be
started as under:
In any closed
electrical circuit or mesh, the all algebraic sum of all the electromotive
forces (e.m.fs) And the voltage drops in resistor is equal to zero, i.e.,
Algebraic sum all e.m.fs + Algebraic sum of voltage drops = 0
The validity of Kirchhoff’s
voltage law can be easily established by referring to the loop ABCDA show in
figure (2). If we start from any point (say point A) in this closed circuit and
go back to the point(i.e., point A) after going round the circuit, the there is
no increase or decrease in potential. This means the algebraic sum of the
e.m.fs of all the sources (here only one e.m.f. source is consider) met on the
way plus the algebraic sum of the voltage drops in resistances must be zero.
Kirchhoff’s voltage law based on the law of *conservation of energy, i.e., net
change in the energy of a charge after completing the closed path is zero.
Note:
Kirchhoff’s voltage law is also called loop rule.
Sign convention:
Sign convention:
While applying Kirchhoff’s
voltage law to a close circuit, algebraic sum are considered. Therefore, it is
very important to assign proper signs to e.m.fs and voltage drops in the closed
circuit. The flowing sign convention may be followed:

Thus in figure (3a) as go
from A to B (i.e., from negative terminal of the cell to the positive
terminal), there is a rise in potential.
In figure (3b) as we go from
A to B, there is a rise in potential.
In figure (3c) as we go from
C to D, there is a fall in potential.
In figure (3d) as we from C to D, there is again
a fall in potential.
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