Current Sources in Parallel when Simplifying Circuits

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Discussion Overview

The discussion revolves around the simplification of circuits involving current sources and resistors, specifically addressing whether a parallel branch with a current source and a resistor can be treated as just the current source, and the conditions under which multiple parallel current sources can be combined. The scope includes theoretical considerations and practical applications in circuit analysis.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants suggest that if the resistance is negligible, a parallel branch with a current source and a resistor can be simplified to just the current source.
  • Others argue that multiple parallel current sources can be combined even if there are other branches present, as long as they are oriented in the same direction.
  • One participant notes that while ideal current sources do not consider series resistance, real circuits require attention to actual resistances involved.
  • A participant raises a concern about whether resistance can be ignored and questions the implications of combining sources on opposite sides of a particular wire in the circuit.
  • Another participant suggests converting voltage sources to Norton equivalents and combining them with caution regarding series resistance.
  • There is mention of using Kirchhoff's laws to analyze the circuit, with some participants expressing confidence in their approaches while others question the equivalence of their methods.

Areas of Agreement / Disagreement

Participants express differing views on the treatment of resistance in circuit simplifications and the conditions under which current sources can be combined. There is no consensus on the best approach, and the discussion remains unresolved regarding specific circuit configurations.

Contextual Notes

Participants highlight the importance of knowing the details of actual resistances and the specific branches involved when simplifying circuits. There are also references to the limitations of ideal versus real current sources.

engineer_ja
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When simplifying a circuit, can a parallel branch with a current source and a resistor in series be considered as just the current source?


Also, if two parallel current sources 'point upwards' i.e. toward the positive rail, can I add them together as one source even if there are other branches in between them?


Thanks everyone!
 
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If you can ignore the resistance - yes.
Yes add them together even if other branches are present.
 
Yes, of course. They will both end up with the same voltage across them, each one supplying the current it's been set to deliver. (There are practical limits to that statement, of course - but only along the same lines as connecting Voltage sources in series).
 
Thanks!

How do I know if I can ignore the resistance?

The question I am trying to do asks for the current in a particular wire of the circuit. Looking at my answer, It seems that i cannot combine things in parallel if they are on opposite sides of this wire. is that correct?
 
If resistance is very small (close to zero ohm) ignore it like a short circuit.

You should be specific about what kind of branch you want to combine.
 
An ideal current source doesn't care about series resistance but in a 'real' circuit, you would need to know the details of actual resistances involved.
Post a diagram to give us a better idea.
 
Hi, I've attached the circuit picture. To find current in xx I convert the 2 voltages to norton equivalents. Can I then combine the 2A with the left hand current source, ignoring its 5 ohm series resistance??

I then think that I cannot combine the left hand and right hand norton equivalents into one, as I 'lose' the link xx??

Thanks.
 

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Convert the voltage sources to Norton. Then combine everything except the current source branch to one current source and one parallel resistance. Then convert it back to Thevenin. Then the analysis is easy. Dont ignore the resistance.
 
That 2A stays as 2A - no worries there. Just do Kirchoff on the circuit and you should get the right answer. You have currents at x adding to give zero (K1) and you have three loops that you can do K2 on. I think that's enough for a solution with four equations and four unknowns.
@KS that's another approach. I don't see why mine shouldn't work too- not as clever as yours though.
 
  • #10
Thanks Guys,

@SC, that approach worked for me when I tried, but the answers gave this as an equivalent circuit, and I can't work out how they got there...!
 
  • #11
sorry file didn't attach!
 

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  • #12
It seems to me that the solution should look like this
 

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