Kirchoff’s Circuit Law
We saw in the Resistors tutorial
that a single equivalent resistance, ( RT ) can be found
when two or more resistors are connected together in either series, parallel or
combinations of both, and that these circuits obey Ohm’s Law.
However, sometimes in complex circuits such as
bridge or T networks, we can not simply use Ohm’s Law alone to find the
voltages or currents circulating within the circuit. For these types of
calculations we need certain rules which allow us to obtain the circuit
equations and for this we can use Kirchoffs Circuit Law.
In 1845, a German physicist, Gustav Kirchoff developed a pair or set of rules or laws which deal
with the conservation of current and energy within electrical circuits. These
two rules are commonly known as: Kirchoffs Circuit Laws with
one of Kirchoffs laws dealing with the current flowing around a closed
circuit, Kirchoffs Current Law, (KCL) while the other law deals with the voltage sources
present in a closed circuit, Kirchoffs Voltage Law, (KVL).
Kirchoffs First Law – The Current Law, (KCL)
Kirchoffs Current Law or KCL, states that the “total current or charge
entering a junction or node is exactly equal to the charge leaving the node as
it has no other place to go except to leave, as no charge is lost within the
node“. In other words the algebraic sum of ALL the currents entering and
leaving a node must be equal to zero, I(exiting) + I(entering) = 0.
This idea by Kirchoff is commonly known as the Conservation of
Charge.
Kirchoffs Current Law
Here, the 3 currents entering the node, I1, I2, I3 are
all positive in value and the 2 currents leaving the node, I4 and
I5 are negative in value. Then this means we can also rewrite
the equation as;
I1 + I2 + I3 – I4 – I5 = 0
The term Node in an electrical
circuit generally refers to a connection or junction of two or more current
carrying paths or elements such as cables and components. Also for current to
flow either in or out of a node a closed circuit path must exist. We can use
Kirchoff’s current law when analysing parallel circuits.
Kirchoffs Second Law – The Voltage Law, (KVL)
Kirchoffs Voltage Law or KVL, states that “in any closed loop network,
the total voltage around the loop is equal to the sum of all the voltage drops
within the same loop” which is also equal to zero. In other words the
algebraic sum of all voltages within the loop must be equal to zero. This idea
by Kirchoff is known as the Conservation of Energy.
Kirchoffs Voltage Law
Starting at any point in the loop continue in
the same direction noting the direction of all the
voltage drops, either positive or negative, and returning back to the same
starting point. It is important to maintain the same direction either clockwise
or anti-clockwise or the final voltage sum will not be equal to zero. We can
use Kirchoff’s voltage law when analysing series circuits.
When analysing either DC circuits or AC circuits
using Kirchoffs Circuit Laws a number of
definitions and terminologies are used to describe the parts of the circuit
being analysed such as: node, paths, branches, loops and meshes. These terms are
used frequently in circuit analysis so it is important to understand them.
Common DC Circuit Theory Terms:
• Circuit – a circuit is a closed loop conducting path in
which an electrical current flows.
• Path – a single line
of connecting elements or sources.
• Node – a node is a
junction, connection or terminal within a circuit were two or more circuit
elements are connected or joined together giving a connection point between two
or more branches. A node is indicated by a dot.
• Branch – a branch is
a single or group of components such as resistors or a source which are
connected between two nodes.
• Loop – a loop is a
simple closed path in a circuit in which no circuit element or node is
encountered more than once.
• Mesh – a mesh is a
single open loop that does not have a closed path. There are no components
inside a mesh.
Note that:
Components are said to be
connected together in Series if the same current value flows through all the
components.
Components are said to be
connected together in Parallel if they have the same voltage applied across
them.
A Typical DC Circuit
Kirchoffs Circuit Law Example No1
Find the current flowing in
the 40Ω Resistor, R3
The circuit has 3 branches, 2 nodes
(A and B) and 2 independent loops.
Using Kirchoffs Current Law, KCL the
equations are given as;
At node A : I1 + I2 = I3
At node B : I3 = I1 + I2
Using Kirchoffs Voltage Law, KVL the
equations are given as;
Loop 1 is given
as : 10 = R1 I1 + R3 I3 = 10I1 + 40I3
Loop 2 is given as : 20 = R2 I2 + R3 I3 = 20I2 + 40I3
Loop 3 is given
as : 10 – 20 = 10I1 – 20I2
As I3 is the sum of I1 + I2 we
can rewrite the equations as;
Eq. No
1 : 10 = 10I1 + 40(I1 + I2) = 50I1 + 40I2
Eq. No
2 : 20 = 20I2 + 40(I1 + I2) = 40I1 + 60I2
We now have two “Simultaneous Equations” that can be reduced to give us the
values of I1 and I2
Substitution of I1 in terms
of I2 gives us the value of I1 as -0.143 Amps
Substitution of I2 in terms
of I1 gives us the value of I2 as +0.429 Amps
As : I3 = I1 + I2
The current flowing in resistor R3 is
given
as : -0.143 + 0.429 = 0.286 Amps
and the voltage across the resistor R3 is
given
as : 0.286 x 40 = 11.44 volts
The negative sign for I1 means
that the direction of current flow initially chosen was wrong, but never the
less still valid. In fact, the 20v battery is charging the 10v battery.
Application of Kirchoffs Circuit Laws
These two laws enable
the Currents and Voltages in a circuit to be found, ie, the
circuit is said to be “Analysed”, and the basic procedure for using Kirchoff’s
Circuit Laws is as follows:
1. Assume all voltages and resistances are
given. ( If not label them V1, V2,… R1, R2, etc. )
2. Label each branch with a branch current.
( I1, I2, I3 etc. )
3. Find Kirchoff’s first law equations for each
node.
4. Find Kirchoff’s second law equations for each
of the independent loops of the circuit.
5. Use Linear simultaneous equations as required
to find the unknown currents.
As well as using Kirchoffs
Circuit Law to calculate the various voltages and
currents circulating around a linear circuit, we can also use loop analysis to
calculate the currents in each independent loop which helps to reduce the
amount of mathematics required by using just Kirchoff's laws. In the next
tutorial about DC circuits, we will look at Mesh Current Analysis to do just that.
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