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Norton's Theorem

The objective of the Norton theorem is to simplify a complex linear circuit into an equivalent circuit consisting of a single current source in parallel with a resistance, making analysis between two terminals (A and B) easier.

Norton's Theorem
Norton's Theorem

Any linear circuit located between points A and B can be modeled by an equivalent generator (IN,RN)(I_{N}, R_{N}), where:

  • INI_{N} is the short-circuit current between A and B
  • RNR_{N} is the equivalent resistance seen between A and B when the sources are deactivated
Norton's Theorem - part 1

Determination of INI_N with a short-circuit

Norton's Theorem - part 2
IAB=ERI_{AB} = \frac{E}{R}

Determination of RNR_N without the sources

Norton's Theorem - part 3
RN=RRR+R=RR2R=R2R_N = \frac{R \cdot R}{R + R} = \frac{R \cdot R}{2R} = \frac{R}{2}

Finally, you can replace the original circuit with the Thévenin equivalent generator, which consists of a current source IN=ERI_{N} = \frac{E}{R} in series with a resistance RN=R2R_{N} = \frac{R}{2}.

Norton's Theorem - part 3