Basic Electrical & Electronics Engineering — Network Theorems, NEC licence examination syllabus (Nepal Engineering Council).
The same idea as Thevenin, asked the other way round — and one line converts between them.
Thevenin asks: what voltage does this circuit offer, and what resistance sits behind it?
Norton asks a different question about the same circuit: if I short the terminals with a thick wire, how much current pours out?
Both descriptions are complete. It is like describing a car by its top speed or by its engine power — different numbers, same car, and either can be worked out from the other.That is genuinely all of it. If you can do Thevenin, you can do Norton — find the Thevenin form and divide.
TheveninVoltage source in series with R.
NortonCurrent source in parallel with the same R.
A 24 V source with 4 Ω, a 12 Ω to ground, and an 8 Ω load. Thevenin gave 1.636 A. Let us watch Norton reach the same number by a different route.
Identical to R_th. Same circuit, same sources killed, same resistance looking in:
Put a wire across a–b. That wire has zero resistance, so it is a far easier path than the 12 Ω beside it — essentially all the current takes the wire, and the 12 Ω is bypassed entirely.
The conversion formula agrees, as it must:
Norton is a current source with R_N in parallel, so the 6 A splits between R_N and the load. We want the load's share, so the other branch (R_N) goes on top:
TheveninWhen the sources are voltages in series, and when the question asks for a voltage.
NortonWhen there are current sources or many parallel branches, and when the question asks for a current.
Source transformation"Convert this to its Norton equivalent" — one division and a redraw. Nearly free marks.
Same-circuit-both-waysSolve by Thevenin and by Norton, and show they agree. Say explicitly that R is unchanged.
Common slipForgetting the current divider at the end. Norton's R is in parallel, so the load never gets all of I_N.
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