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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:
In the example, the total current Itotal is given by:
I_\mathrm{total} = {15 \mathrm{V} \over 2\,\mathrm{k}\Omega + 1\,\mathrm{k}\Omega \| (1\,\mathrm{k}\Omega + 1\,\mathrm{k}\Omega)} = 5.625 \mathrm{mA} <math> The current through the load is then:
I = {1\,\mathrm{k}\Omega + 1\,\mathrm{k}\Omega \over (1\,\mathrm{k}\Omega + 1\,\mathrm{k}\Omega + 1\,\mathrm{k}\Omega)} \cdot I_\mathrm{total} <math>
= 2/3 \cdot 5.625 \mathrm{mA} = 3.75 \mathrm{mA} <math> And the equivalent resistance looking back into the circuit is:
R = 1\,\mathrm{k}\Omega + 2\,\mathrm{k}\Omega \| (1\,\mathrm{k}\Omega + 1\,\mathrm{k}\Omega) = 2\,\mathrm{k}\Omega <math> So the equivalent circuit is a 3.75 mA current source in parallel with a 2 kΩ resistor. See alsoExternal links
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