Norton's Theorem and Thevenin's theorem

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SUMMARY

This discussion focuses on applying Norton's Theorem to find the Norton equivalent source between terminals A and B in a circuit involving a 20V source and resistors of 4kΩ and 6kΩ. The solution involves calculating the short circuit current (Isc) and Thevenin resistance (Rth) using Kirchhoff's Current Law (KCL) and Kirchhoff's Voltage Law (KVL). The final Norton equivalent is determined to be -2mA in parallel with Rth = 12k/5Ω. The discussion emphasizes the utility of source transformations for simplifying circuit analysis.

PREREQUISITES
  • Norton's Theorem and Thevenin's Theorem
  • Kirchhoff's Current Law (KCL)
  • Kirchhoff's Voltage Law (KVL)
  • Circuit analysis techniques including source transformations
NEXT STEPS
  • Study the application of Norton's Theorem in complex circuits
  • Learn about Thevenin's Theorem and its relationship with Norton's Theorem
  • Explore advanced circuit analysis techniques using superposition
  • Investigate practical applications of source transformations in electrical engineering
USEFUL FOR

Electrical engineering students, circuit designers, and professionals involved in circuit analysis and design will benefit from this discussion, particularly those looking to deepen their understanding of Norton's and Thevenin's theorems.

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Homework Statement



For some reason I don't use this theorem since Thevenin's theorem is more common. I'm asked to find the Norton equivalent source between the terminals ##A## and ##B## for the following:

Screen Shot 2014-12-11 at 4.23.33 PM.png


Homework Equations

The Attempt at a Solution



The first step is to short ##R_2##, and to find the short circuit current across that wiring.

Screen Shot 2014-12-11 at 4.23.33 PM.png


I believe KCL at the node above the ##3 mA## would be useful:

##\sum I = 0 \Rightarrow 3mA + I_{sc} - I_R = 0 \Rightarrow I_{sc} = I_R - 3mA = \frac{V_{Node} + 20V}{4k} - 3mA##

Now ##V_{Node}## is the voltage across the ##3 mA##. Applying KVL around the left loop using the current source as a constraint:

##\sum V = 0 \Rightarrow 20V + V_R + V_{Node} = 0 \Rightarrow V_{Node} = -(20V + V_R) = -(20V + (3mA)(4k)) = - 32V##

This implies that ##I_{sc} = \frac{-32V + 20V}{4k} - 3mA = - 6mA##.

Is this reasonable?
 
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You went astray when you wrote equations with ##V_{Node}##. The short circuit forces ##V_{Node}## to be zero volts. If you think about the Superposition Principle you can take advantage of that, since it makes calculating the current contribution of the 20 V source quite simple.

If I may suggest another approach? Start by converting the 20V source and R1 to their Norton equivalent. Then take advantage of parallel connections to simplify...
 
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Ah source transforms, those are awfully useful and I hardly ever use them.

First, ##V = -IR \Rightarrow I = \frac{-20V}{4k} = -5mA## so ##-5mA## points up or ##5mA## points down. Also, the ##5 mA## is in parallel with the ##4k## now.

So the combined current in parallel is ##-5mA + 3mA = -2mA##. This is the only current in this new circuit (comprised of the current source, 4k resistor and shorted 6k resistor). Hence ##I_{sc} = -2mA##.

Now going back to the original circuit, short circuiting the voltage and open circuiting the current source, we find:

##R_{th} = (\frac{1}{4k} + \frac{1}{6k})^{-1} = \frac{12k}{5}##

Hence the norton equivalent would be ##-2mA## pointing up in parallel with ##R_{th}##.
 
There you go! Much less brain sweat required :)
 

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