Using Norton's Theorem to Solve for Io in a Complex Circuit

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In summary, the conversation discussed different methods for finding Io using Norton's Theorem, including using Thevenin's Theorem and Nodal Analysis. The conversation also mentioned a follow-up question about creating a current controlled voltage source in QUCS.
  • #1
raddian
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Homework Statement


Find Io using Norton's Theorem

Homework Equations


Screenshot - 06112015 - 11:09:31 AM.png


The Attempt at a Solution


I broke it into the following circuit:
Snapshot.jpg

I would like to break it down some more but if I open the node between 3k and 6k (ohms), and 6k and 6k (ohms), I run into problems...

What should I do to make sure I stick to Norton's Theor
 

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  • #2
I don't think you're restricted to using Norton's Theorem exclusively. It should be sufficient to determine the Norton equivalent of the network driving the current through the 6 k "load" using whatever means you wish. You might begin by suppressing all the sources and determining the Norton resistance.

By the way, 2 k + 3 k is not 6 k :wink:
 
  • #3
I just took a while and solved the problem by hand using mesh analysis with a supermesh and then put the circuit into QUCS and verified my answer.

I am having a hard time seeing how it would be easily done with norton's theorem or thevenin's theorem. I got a value for the equivalent resistance seen by the load resistor but breaking down the circuit to find the voltage across the terminals of the load resistor would lead me back to using mesh.

supermesh.png
 
Last edited:
  • #4
I'd go for a Thevenin approach and Nodal Analysis. Finding the Thevenin resistance (same as Norton resistance) is pretty easy with the sources suppressed. Removing the 6k load to open-circuit the output (For Thevenin you want the open-circuit voltage) leaves a single essential node. The rest is just finding particular potentials along branches.
 
  • #5
Yeah I agree that would be another way. converting the thevenin equivalent into a norton equivalent. The equivalent resistance is easy to find

supermesh.png


The difference in voltages Vx and Vy is the thevenin equivalent voltage
 
  • #6
gneill said:
I don't think you're restricted to using Norton's Theorem exclusively. It should be sufficient to determine the Norton equivalent of the network driving the current through the 6 k "load" using whatever means you wish. You might begin by suppressing all the sources and determining the Norton resistance.

By the way, 2 k + 3 k is not 6 k :wink:

At first I didn't know what you meant by "driving the current through the 6 k "load" using whatever means you wish." but with FOIWATER's picture:

supermesh-png.84725.png


I am able to understand now. Thank you! I will try my best to solve this using the techniques you suggested!
 
  • #7
I was able to find the Voltage between the open circuit using Thevenin and Node analysis: I got Vth = ~10.8 V (making Vy facing positive and Vx near negative), and Rth = 33/5. So the short circuit current is 10.8/6.6=1.6464 and current division between the load and 6.6 KOhms makes the load current 0.857. This hsould be negative because of the way the current is facing and the way I had my voltages set up. Thanks everyone!

(Btw FOIWATER, your R6 resister should be 3k)
 
  • #8
Glad you figured it out friend.
 
  • #9
Follow up question on using QUCS:
I'm trying to make a current controlled voltage source matching this diagram...:
Screenshot - 06122015 - 01:09:17 PM.png

Im not sure how exactly the current controlled voltage source is used in qucs.. Examples help, but I didnt know the right name for it in the examples given in qucs

Screenshot - 06122015 - 01:10:27 PM.png

Code:
<Qucs Schematic 0.0.18>
<Properties>
  <View=-50,-814,893,-265,1,287,0>
  <Grid=10,10,1>
  <DataSet=5.11.dat>
  <DataDisplay=5.11.dpl>
  <OpenDisplay=1>
  <Script=5.11.m>
  <RunScript=0>
  <showFrame=0>
  <FrameText0=Title>
  <FrameText1=Drawn By:>
  <FrameText2=Date:>
  <FrameText3=Revision:>
</Properties>
<Symbol>
  <.ID -20 -16 SUB>
  <Line -20 20 40 0 #000080 2 1>
  <Line 20 20 0 -40 #000080 2 1>
  <Line -20 -20 40 0 #000080 2 1>
  <Line -20 20 0 -40 #000080 2 1>
</Symbol>
<Components>
  <R R1 1 230 -450 15 -26 0 1 "3000 Ohm" 1 "26.85" 0 "0.0" 0 "0.0" 0 "26.85" 0 "US" 0>
  <R R2 1 440 -450 15 -26 0 1 "6000 Ohm" 1 "26.85" 0 "0.0" 0 "0.0" 0 "26.85" 0 "US" 0>
  <R R4 1 530 -630 -26 15 0 0 "2000 Ohm" 1 "26.85" 0 "0.0" 0 "0.0" 0 "26.85" 0 "US" 0>
  <Idc I1 1 80 -450 18 -26 0 1 "8 mA" 1>
  <IProbe Pr1 1 600 -430 16 -26 1 3>
  <GND * 1 430 -310 0 0 0 0>
  <CCVS SRC1 1 340 -620 34 -26 1 3 "4000" 1 "4000" 0>
  <.DC DC1 1 40 -540 0 43 0 0 "26.85" 0 "0.001" 0 "1 pA" 0 "1 uV" 0 "no" 0 "150" 0 "no" 0 "none" 0 "CroutLU" 0>
  <Idc I2 1 420 -780 -26 18 0 0 "2 mA" 1>
</Components>
<Wires>
  <440 -580 500 -580 "" 0 0 0 "">
  <230 -310 430 -310 "" 0 0 0 "">
  <230 -590 230 -480 "" 0 0 0 "">
  <560 -620 600 -620 "" 0 0 0 "">
  <230 -420 230 -310 "" 0 0 0 "">
  <440 -580 440 -480 "" 0 0 0 "">
  <440 -420 440 -310 "" 0 0 0 "">
  <500 -630 500 -580 "" 0 0 0 "">
  <560 -630 560 -620 "" 0 0 0 "">
  <80 -310 230 -310 "" 0 0 0 "">
  <80 -420 80 -310 "" 0 0 0 "">
  <80 -480 230 -480 "" 0 0 0 "">
  <230 -590 310 -590 "" 0 0 0 "">
  <440 -310 600 -310 "" 0 0 0 "">
  <600 -400 600 -310 "" 0 0 0 "">
  <600 -620 600 -460 "" 0 0 0 "">
  <430 -310 440 -310 "" 0 0 0 "">
  <370 -590 370 -580 "" 0 0 0 "">
  <370 -580 440 -580 "" 0 0 0 "">
  <370 -670 370 -650 "" 0 0 0 "">
  <370 -670 560 -670 "" 0 0 0 "">
  <560 -670 560 -630 "" 0 0 0 "">
  <310 -660 310 -650 "" 0 0 0 "">
  <310 -660 500 -660 "" 0 0 0 "">
  <500 -660 500 -630 "" 0 0 0 "">
  <230 -780 230 -590 "" 0 0 0 "">
  <230 -780 390 -780 "" 0 0 0 "">
  <600 -780 600 -620 "" 0 0 0 "">
  <450 -780 600 -780 "" 0 0 0 "">
</Wires>
<Diagrams>
</Diagrams>
<Paintings>
</Paintings>
 
  • #10
R4 is shorted by your wiring of the controlled current source "sense line". Note that there is a path from the top of R5 to the top of R2 that does not pass through R4!
Fig1.gif
 
  • #11
Thanks again!
 

What is Norton's Theorem?

Norton's Theorem is a fundamental principle in circuit analysis that states that any linear, active circuit can be replaced by an equivalent circuit containing a current source, a parallel resistance, and a load resistor.

How is Norton's Theorem different from Thevenin's Theorem?

Norton's Theorem is similar to Thevenin's Theorem in that they both allow for the simplification of complex circuits. However, Norton's Theorem uses a current source instead of a voltage source.

What is the benefit of using Norton's Theorem?

Norton's Theorem allows for the simplification of complex circuits, making it easier to analyze and design circuits. It also allows for the determination of the current flowing through a load resistor without having to calculate the entire circuit.

What are the limitations of Norton's Theorem?

Norton's Theorem is only applicable to linear, active circuits. It also assumes that the circuit is in steady-state conditions and that there are no reactive elements present.

How do you apply Norton's Theorem in circuit analysis?

To apply Norton's Theorem, you first need to find the Norton equivalent circuit by determining the Norton current and the equivalent parallel resistance. Once you have the equivalent circuit, you can use it to analyze the original circuit as if it were a simple circuit containing only a current source and a load resistor.

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