Circuits Question - Thevein & Norton Equivalents

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In summary: Not sure how much that helps so I'll check back in a few minutes to see how you're doing.In summary, the conversation discusses finding the Thevenin and Norton equivalents of a circuit using the node voltage method. One user is confused by the problem and asks for help understanding how current travels through a wire in the circuit. Another user provides a helpful explanation and helps the first user find the equivalent resistance and voltage using the node voltage method. The conversation then shifts to discussing using source conversions to find the equivalent circuit, with one user providing guidance on eliminating parallel resistors and wires in order to simplify the circuit.
  • #1
GreenPrint
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Homework Statement



http://img69.imageshack.us/img69/1973/captureyxs.png

Find the Thevenin and Norton equivalent of the circuit above between A and B using the node voltage method.

Homework Equations





The Attempt at a Solution



I place the ground reference at the node with where the two 10 ohm resistors, 30 volt supply, 40 ohm resistor, and 1 amp source meet in the upper right hand corner.

I'm confused by this problem. If I put a wire between A and B to find the short circuit current than the equivalent resistance between the 100 ohm resistor and the wire is zero ohms so I can just ignore this particular resistor. However I don't understand how any current is traveling though this part of the wire since it's just one giant node with one voltage so how can any current travel through it? Thanks for any help.
 
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  • #2
GreenPrint said:
I'm confused by this problem. If I put a wire between A and B to find the short circuit current than the equivalent resistance between the 100 ohm resistor and the wire is zero ohms so I can just ignore this particular resistor. However I don't understand how any current is traveling though this part of the wire since it's just one giant node with one voltage so how can any current travel through it? Thanks for any help.

Currents flow through wires. The resistance of an ideal wire is zero, and multiplied by any current it gives zero voltage across. And you can make that wire short, even shrink it to a node, the same current flows through. But it is better to keep that wire between A and B and find the current through it.

The internal resistance both for Norton-equivalent or Thevenin-equivalent sources can be got also as the resistance of the circuit between A and B by replacing all voltage and current sources by their internal resistance (zero for ideal voltage source and infinite for an ideal current source).

ehild
 
  • #3
Ok so I built it in Circuit Lab to confirm that the node voltages I found where correct.

http://img59.imageshack.us/img59/9217/capturegvro.png

Node 9 = -61 Volts
Node 11 = 5 Volts
Node 12 = 128.75 Volts
Node 13 = -76.25 Volts

So agrees with what I calculated.

[itex]V_{Th} = V_{13} - V_{12} = -76.25 V - (-128.75 V) = 52.5 Volts[/itex]
[itex]V_{Th}[/itex] has an orientation of
A + - B
Where node 13 or A is more positive than node 12 or B

I than calculated [itex]R_{Th}[/itex] by the method below
I think that the answer I get in this post is wrong for the Thevenin equivalent resistance because I forgot to disable a current source.
http://img14.imageshack.us/img14/5950/captureldq.png
http://img15.imageshack.us/img15/2237/captureitw.png
http://img703.imageshack.us/img703/4967/captureuc.png
http://img820.imageshack.us/img820/7518/capturepvv.png
http://img651.imageshack.us/img651/774/capturezpmw.png
http://img401.imageshack.us/img401/3530/capturekva.png

As you can see I get [itex]R_{Th} = 76.19 Ω[/itex]. Below is what I get for the Thevenin and Norton equivalents of the circuit.

http://img853.imageshack.us/img853/7579/capturedi.png
http://img266.imageshack.us/img266/6669/captureyus.png

As you can see I get [itex]I_{Th} = 689.1 mA[/itex]. I think however that I'm doing something wrong but I'm not sure what.
 
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  • #4
Oh I think I forgot to take out one current source.
So I think it should be
[itex]R_{Th} = 100 Ω[/itex]
[itex]I_{N} = .525 A[/itex]
[itex]V_{Th} = 52.5 V[/itex]

I still think I'm doing something wrong though.
 
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  • #5
Your Vth looks okay, but Rth is a problem. Check to make sure that you suppressed all the sources correctly.
 
  • #6
Shouldn't it just be the equivalent of this circuit?

http://img845.imageshack.us/img845/6814/capturessle.png
 
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  • #7
GreenPrint said:
Shouldn't it just be the equivalent of this circuit?

http://img845.imageshack.us/img845/6814/capturessle.png

Yup. That looks better. What's Rth then?
 
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  • #8
I still get 100. Am I supposed to include the resistor between nodes A and B as part of the equivalent resistance?
 
  • #9
GreenPrint said:
Am I supposed to include the resistor between nodes A and B as part of the equivalent resistance?

Absolutely.
 
  • #10
So the answers I get for using the node voltage method is as follows:

http://imageshack.us/photo/my-images/259/capturexdf.png/

The picture won't load but it's the same voltage already found with a 200 ohm resistor.

Now when I try to use source conversions I get a different answer. I'm really confused by source conversions and hate using this method. Any help would greatly appreciate me.

http://img715.imageshack.us/img715/1055/capturehav.png

Here's my attempt

http://img255.imageshack.us/img255/3316/capturexhh.png

http://img842.imageshack.us/img842/3083/captureobp.png

http://img19.imageshack.us/img19/4566/capturezu.png

[PLAIN]http://img208.imageshack.us/img208/3541/capturezop.png

[PLAIN]http://img208.imageshack.us/img208/3541/capturezop.png

http://img593.imageshack.us/img593/9273/captureezc.png

As you can see this answer is wrong as it dosen't match up.

Thanks for any help!
 
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  • #11
I don't know how you got from the second diagram in your attempt to the third. Looks like some rules were badly bent out of shape... like adding current sources that are not in parallel.
 
  • #12
Well like what can i do from the second one? I know that I can add that one set of parallel resistors. on the left but I don't see what else I can go from there.
 
  • #13
GreenPrint said:
Well like what can i do from the second one? I know that I can add that one set of parallel resistors. on the left but I don't see what else I can go from there.

Yes, definitely put those two resistors in parallel.

Something helpful to know: A resistor in series with a current source has no effect -- an ideal current source will produce its specified current no matter what its load is. What does that mean in practical terms? Since it doesn't matter what values those resistors have they might as well be zero! You can eliminate those resistors entirely, replacing them with wires. That should get you going.
 
  • #14
http://img252.imageshack.us/img252/4772/captureopx.png

When I get down to here and covert the to a voltage source and a resistor in series I don't get the same answer =( is the above circuit above correct?
 
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  • #15
How did the 26.19Ω resistance evolve? It doesn't look right to me.
 
  • #16
Ok so it should be 50, this would give me the correct resistance, but that still dosen't give me equivalent voltage, it would give me 105 volts.
 
  • #17
GreenPrint said:
Ok so it should be 50, this would give me the correct resistance, but that still dosen't give me equivalent voltage, it would give me 105 volts.

Yes, but 105 Volts spread across two 100Ω resistances...
 
  • #18
Ya but isn't Rth 200 ohms and it's just two 100 ohm resistors in series with a 105 voltage source so I don't see how it gives me the correct answer it's still 105 volts across 200 ohms?

I guess I'm just seeing this wrong. Each 100 ohm resistor experiences .525 amperes which isn't I Norton either.
 
  • #19
GreenPrint said:
Ya but isn't Rth 200 ohms and it's just two 100 ohm resistors in series with a 105 voltage source so I don't see how it gives me the correct answer it's still 105 volts across 200 ohms?

I guess I'm just seeing this wrong. Each 100 ohm resistor experiences .525 amperes which isn't I Norton either.

The two 100 Ω resistances are in parallel -- remember that you're to "look" at the circuit from the viewpoint of the A-B terminals. The Thevenin voltage is the voltage across that 100 Ω resistor sitting between the two terminals. The other 100 Ω resistance is in parallel with it from that perspective.
 

FAQ: Circuits Question - Thevein & Norton Equivalents

1. What is Thevenin's equivalent circuit?

Thevenin's equivalent circuit is a simplified representation of a complex circuit that consists of a voltage source in series with a resistor. This equivalent circuit has the same output voltage and current as the original circuit, and it is used to analyze and solve circuit problems more easily.

2. What is Norton's equivalent circuit?

Norton's equivalent circuit is another simplified representation of a complex circuit that consists of a current source in parallel with a resistor. This equivalent circuit also has the same output voltage and current as the original circuit, and it can be used to solve circuit problems in a similar way as Thevenin's equivalent circuit.

3. How do you find Thevenin's equivalent resistance?

To find Thevenin's equivalent resistance, you need to first remove all the sources (voltage and current sources) from the circuit. Then, calculate the equivalent resistance by short-circuiting all voltage sources and open-circuiting all current sources. The resulting resistance is the Thevenin's equivalent resistance.

4. How do you find Norton's equivalent current?

To find Norton's equivalent current, you need to first remove all the sources from the circuit. Then, calculate the equivalent current by short-circuiting all voltage sources and replacing all current sources with an open circuit. The resulting current is the Norton's equivalent current.

5. When should I use Thevenin's and Norton's equivalents?

Thevenin's and Norton's equivalents are used when solving complex circuit problems, especially when there are multiple sources and resistors involved. They can simplify the circuit and make it easier to analyze and solve. They are also useful in finding the maximum power transfer in a circuit.

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