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Kirchhoff's circuit laws
Kirchhoff's circuit laws are two equalities that deal with the conservation of charge and energy in electrical circuits, and were first described in 1845 by Gustav Kirchhoff. Widely used in electrical engineering, they are also called Kirchhoff's rules or simply Kirchhoff's laws (see also Kirchhoff's laws for other meanings of that term). Both circuit rules can be directly derived from Maxwell's equations, but Kirchhoff preceded Maxwell and instead generalized work by Georg Ohm. Kirchhoff's current law (KCL) The current entering any junction is equal to the current leaving that junction.
i1 +
i4 =
i2 +
i3
This law is also called
Kirchhoff's point rule,
Kirchhoff's junction rule (or nodal rule), and
Kirchhoff's first rule.
The principle of conservation of
electric charge implies that:
At any node (junction) in an
electrical circuit, the sum of
currents flowing into that node is equal to the sum of currents flowing out of that node. or The algebraic sum of currents in a network of conductors meeting at a point is zero. (Assuming that current entering the junction is taken as positive and current leaving the junction is taken as negative). Recalling that current is a signed (positive or negative) quantity reflecting direction towards or away from a node, this principle can be stated as:
n is the total number of branches with currents flowing towards or away from the node.
This formula is also valid for
complex currents:
The law is based on the
conservation of charge whereby the charge (measured in coulombs) is the product of the current (in amperes) and the time (which is measured in seconds).
Changing charge density
Physically speaking, the restriction regarding the "capacitor plate" means that Kirchhoff's current law is only valid if the
charge density remains constant in the point that it is applied to. This is normally not a problem because of the strength of electrostatic forces: the charge buildup would cause repulsive forces to disperse the charges.
However, a charge build-up
can occur in a
capacitor, where the charge is typically spread over wide parallel plates, with a physical break in the circuit that prevents the positive and
negative charge accumulations over the two plates from coming together and cancelling. In this case, the sum of the currents flowing into
one plate of the capacitor is
not zero, but rather is equal to the rate of charge accumulation. However, if the
displacement current d
D/dt is included, Kirchhoff's current law once again holds. (This is really only required if one wants to apply the current law to a point on a capacitor
plate. In circuit analyses, however, the capacitor as a whole is typically treated as a unit, in which case the ordinary current law holds since the current that enters the capacitor on one side leaves it on the other side.)
More technically, Kirchhoff's current law can be found by taking the
divergence of
Ampère's law with Maxwell's correction and combining with
Gauss's law, yielding:
This is simply the charge conservation equation (in integral form, it says that the current flowing out of a closed surface is equal to the rate of loss of charge within the enclosed volume (
Divergence theorem)). Kirchhoff's current law is equivalent to the statement that the divergence of the current is zero, true for time-invariant ρ, or always true if the
displacement current is included with
J.
A
matrix version of Kirchhoff's current law is the basis of most
circuit simulation software, such as
SPICE.