Kirchhoff's Law and current Sources?

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Discussion Overview

The discussion revolves around the application of Kirchhoff's voltage law (KVL) in circuits that include ideal current sources. Participants explore how to treat current sources in voltage equations and the implications of their presence in circuit analysis.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants question whether an ideal current source can be ignored in KVL equations, suggesting that it does not contribute a voltage drop due to its ideal nature.
  • Others argue that a current source does not project a voltage difference but instead defines a current, and cannot be simply replaced with a voltage source without considering the circuit's configuration.
  • One participant suggests that treating the current source as an unknown voltage is necessary to solve for all variables in the circuit, emphasizing the need for additional equations when a current source is present.
  • There is mention of using Kirchhoff's current law (KCL) as an alternative approach to circuit analysis, with some expressing a preference for KCL over KVL.
  • A later reply discusses the relationship between the current source and the load it drives, indicating that the voltage across the current source is influenced by the load rather than being an inherent property of the source itself.
  • Participants reference concepts such as Thevenin and Norton equivalents to illustrate how current sources interact with circuit elements.

Areas of Agreement / Disagreement

Participants express differing views on how to incorporate current sources into KVL equations, with no consensus reached on the best approach. Some advocate for treating current sources as separate entities, while others suggest integrating them into the overall circuit analysis.

Contextual Notes

The discussion highlights the complexity of circuit analysis involving current sources, including the assumptions about ideal behavior and the implications of load conditions. There are unresolved mathematical steps regarding the treatment of current sources in KVL.

Who May Find This Useful

This discussion may be of interest to students and practitioners in electrical engineering and physics, particularly those dealing with circuit analysis and the application of Kirchhoff's laws.

dphysics
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When you are using Kirchhoff's voltage law and you come across a current source, what are you supposed to include that as? Pretending that it is an ideal current source, there will be no resistance and thus no voltage drop. So, do you just ignore it in the voltage equation? (Ex: V1+V2+V3=0)

Because of the fact that you can re-arrange a resistor and voltage source in parallel to a current source and resistor in series, I'm a little confused.

Any help much appreciated.
 
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A current requires there be an electric field, which in turn, requires there be a potential difference.
 
dphysics said:
When you are using Kirchhoff's voltage law and you come across a current source, what are you supposed to include that as? Pretending that it is an ideal current source, there will be no resistance and thus no voltage drop. So, do you just ignore it in the voltage equation? (Ex: V1+V2+V3=0)

Because of the fact that you can re-arrange a resistor and voltage source in parallel to a current source and resistor in series, I'm a little confused.

Any help much appreciated.

That's one of the reasons I use KCL to solve circuits. I never liked KVL...
 
Gear, would you treat the current source as a separate voltage source altogether or combine it with the surrounding resistor and use it in the equation V=IR?
 
A current source does not project a voltage difference, just a current. You cannot replace it with a voltage source unless you re-imagine the circuit as a Thevenin equivalent circuit. Use the KCL rule for the branches that have current sources as the current source forces the current in that branch.
 
dphysics said:
Pretending that it is an ideal current source, there will be no resistance and thus no voltage drop.
This will get you the wrong answer almost every time. Current sources typically have very high impedance. The current source supplies whatever voltage is required in order to maintain the set current.

dphysics said:
When you are using Kirchhoff's voltage law and you come across a current source, what are you supposed to include that as?
Include it as what it is, an unknown voltage that you have to solve for. In such a problem you have one more unknown (the voltage across the current source) and one more equation (the sum of the loop currents through the current source equals the set current). You still have enough equations to solve for all of your unknowns.

berkeman said:
That's one of the reasons I use KCL to solve circuits. I never liked KVL...
I agree!
 
Born2bwire said:
A current source does not project a voltage difference, just a current. You cannot replace it with a voltage source unless you re-imagine the circuit as a Thevenin equivalent circuit.

Wouldn't there be a voltage difference to induce the current source?
 
Gear300 said:
Wouldn't there be a voltage difference to induce the current source?

Not exactly, as DaleSpam stated, the sourced current would create a voltage offset through the source's load. It does not apply a voltage difference, it applies a current source, the resulting voltage difference is dependent upon the load on the current source.

Take a look at a MOSFET current mirror. The voltage across the sourcing transistor in a current mirror is not created (in the ideal case) by the transistor but entirely by the load connected to the mirror. In fact, with a current mirror, your load needs to create a sufficient voltage drop to force the sourcing transistor into saturation for the mirror to work properly. Actually, the current mirror itself is a Norton source, with a large but finite Norton resistance due to what is called channel length modulation. Ideally, the Norton resistance would be infinite, in which case the current mirror would not have any voltage drop associated across it (since the resistance branch would become an open circuit).

A simpler example is the Thevenin and Norton circuits. You can see that in the Norton circuit, the parallel load resistance creates the voltage drop.
 

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