Norton's theorem for electrical networks states that any collection of voltage sources and resistors with two terminals is electrically equivalent to an ideal current source I in parallel with a single resistor R. The theorem can also be applied to general impedances, not just resistors.

The theorem was published in 1926 by Bell Labs engineer Edward Lawry Norton (1898-1983).

To calculate the equivalent circuit:

1. Replace the load circuit with a short.
2. Calculate the current through that short, I, from the original sources.
3. Now replace voltage sources with shorts and current sources with open circuits.
4. Replace the load circuit with an imaginary ohm meter and measure the total resistance, R, with the sources removed.
5. The equivalent circuit is a current source with current I in parallel with a resistance R in parallel with the load.

In the example, the total current I_total is given by:

The current through the load is then:

And the equivalent resistance looking back into the circuit is:

So the equivalent circuit is a 3.75 mA current source in parallel with a 2 kΩ resistor.

See also

• Thevenin's theorem

External links

• Origins of the equivalent circuit concept
• Norton's theorem at allaboutcircuits.com