Nortons Theorem |
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Nortons Theorem
In some ways Norton's Theorem can be thought of as the opposite to "Thevenins Theorem", in
that Thevenin reduces his circuit down to a single resistance in series with a single voltage. Norton on the other
hand reduces his circuit down to a single resistance in parallel with a constant current source. Nortons Theorem
states that "Any linear circuit containing several energy sources and resistances can be replaced by a single Constant
Current generator in parallel with a Single Resistor". As far as the load resistance, RL
is concerned this single resistance, RS is the value of the resistance looking back into
the network with all the current sources open circuited and IS is the short circuit current
at the output terminals as shown below.
Nortons equivalent circuit.
The value of this "Constant Current" is one which would flow if the two output terminals where
shorted together while the source resistance would be measured looking back into the terminals, (the same as Thevenin).
For example, consider our now familiar circuit from the previous section.
To find the Nortons equivalent of the above circuit we firstly have to remove the centre
40Ω load resistor and short out the terminals A and
B to give us the following circuit.
When the terminals A and B are shorted
together the two resistors are connected in parallel across their two respective voltage sources and the currents
flowing through each resistor as well as the total short circuit current can now be calculated as:
with A-B Shorted Out

If we short-out the two voltage sources and open circuit terminals A
and B, the two resistors are now effectively connected together in parallel. The value
of the internal resistor Rs is found by calculating the total resistance at the
terminals A and B giving us the following circuit.
Find the Equivalent Resistance (Rs)

Having found both the short circuit current, Is and equivalent internal
resistance, Rs this then gives us the following Nortons equivalent circuit.
Nortons equivalent circuit.
Ok, so far so good, but we now have to solve with the original 40Ω
load resistor connected across terminals A and B as shown below.
Again, the two resistors are connected in parallel across the terminals A
and B which gives us a total resistance of:

The voltage across the terminals A and B with
the load resistor connected is given as:

Then the current flowing in the 40Ω load resistor can be found as:

which again, is the same value of 0.286 amps, we found using
Kirchoff´s circuit law in the
previous tutorials.
Nortons Analysis Summary.
The basic procedure for solving Nortons Analysis equations is as follows:
- 1. Remove the load resistor RL or component concerned.
- 2. Find RS by shorting all voltage sources or by open circuiting all the current sources.
- 3. Find IS by placing a shorting link on the output terminals A and B.
- 4. Find the current flowing through the load resistor RL.
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