Equating Voltage/Current of Associated Sources: A Comprehensive Guide

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Discussion Overview

The discussion revolves around the methods for equating the voltage and current of associated sources, specifically focusing on the behavior of voltage and current sources in series and parallel configurations. Participants explore theoretical and practical implications of these configurations, including ideal versus non-ideal sources.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Experimental/applied

Main Points Raised

  • Some participants explain that for voltage sources in series, the voltages add up, while in parallel, the voltage remains the same as any single source, with current divided among them.
  • Others argue that for ideal sources of equal voltage in parallel, the current distribution is not guaranteed to be equal, and unequal voltage sources can lead to large currents flowing backwards through lower voltage sources.
  • A participant notes that for current sources in series, the current remains the same, while in parallel, the currents add up.
  • Some express that cases involving unequal voltages or currents for ideal sources are impossible, while cases with equal values are straightforward.
  • One participant highlights the risks of using non-ideal sources in real circuits, suggesting that improper configurations could lead to short circuits or equipment damage.
  • Another participant mentions that while cases 2 and 3 can theoretically be done in the real world, they require caution, providing an example of jump-starting a car with batteries in parallel.

Areas of Agreement / Disagreement

Participants generally agree on the basic principles of combining sources but express disagreement regarding the feasibility of certain configurations, particularly with unequal voltages and currents. The discussion remains unresolved on the practical implications of these configurations.

Contextual Notes

Limitations include the assumptions about ideal versus non-ideal sources, and the potential for large currents in configurations that do not meet the ideal conditions. The discussion also reflects varying interpretations of when certain cases are possible or advisable.

Who May Find This Useful

This discussion may be useful for students and practitioners in electrical engineering, physics, or related fields who are exploring the behavior of electrical sources in circuit design and analysis.

Jhenrique
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How equate the voltage/current of the associated sources with the voltage/current equivalent?

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For voltage sources in series, simply add the voltages up. In parallel, the voltage of the circuit is the same as any single source, but each source will have a fraction of the total current. So if you have three 9-volt batteries in parallel, there's 9 volts applied to the circuit and each battery supplies 1/3 of the total current.

For current sources it's the opposite. The current through each current source in series is the same, while you would add the current sources together if they are in parallel.
 
Drakkith said:
In parallel, the voltage of the circuit is the same as any single source, but each source will have a fraction of the total current. So if you have three 9-volt batteries in parallel, there's 9 volts applied to the circuit and each battery supplies 1/3 of the total current.
The parallel situation is not quite this simple. For ideal sources of equal voltage connected in parallel by ideal wires there is no guarantee that each supplies 1/3 of the total current. Any combination adding up to 1 will satisfy the relevant equations. For ideal sources of unequal voltage connected in parallel by ideal wires, there is no way to satisfy the relevant equations.

For near-ideal sources, connected in parallel, small details matter. If the sources have equal voltage then the current will be distributed based on the (small) internal resistance in each source and in the connecting wires. If the sources have unequal voltage than there will be large currents as the high voltage sources run current backwards through the low voltage sources. The result is a kind of averaging of the voltages of the component sources. The currents will become as large as is needed to prevent the voltage sources from behaving in an ideal fashion. The result is that the voltage of the parallel combination is some sort of average of the [nominal] voltages of the individual sources.

For current sources it's the opposite. The current through each current source in series is the same, while you would add the current sources together if they are in parallel.

Similar caveats apply for current sources. Perfectly ideal current sources connected in series must have equal values. Any other choice will fail. Near-ideal current sources connected in series will have extremely high potential differences created as the conflicts result in the accumulation or depletion of charge in the connections between. These voltage differences will become as large as is needed to prevent the current sources from behaving in an ideal fashion. The result is that the current through a series of current sources is some sort of average of the [nominal] currents of the individual sources.

Edit: Added the word "nominal" for a bit of clarity.
 
Last edited:
Ah, you are correct Jbriggs. I forgot to say that my explanation only applies when the voltage sources in parallel are equal in voltage and the current sources in series are equal in current.
 
In real life you don't want voltage sources in parallel, or current sources in series ... !
 
I don't understand...

Yeah, I1 ≠ I2 ≠ I3 so like V1 ≠ V2 ≠ V3, and the sources are ideal.

I don't want to divide the total current/voltage for each source, I want that when given I1, I2 and I3, or V1, V2 and V3, find the Ieq and Veq for every four cases above.

You're saying that this is impossible?
 
Jhenrique said:
I don't understand...

Yeah, I1 ≠ I2 ≠ I3 so like V1 ≠ V2 ≠ V3, and the sources are ideal.

I don't want to divide the total current/voltage for each source, I want that when given I1, I2 and I3, or V1, V2 and V3, find the Ieq and Veq for every four cases above.

You're saying that this is impossible?

Yes. Cases 2 and 3 are impossible for ideal sources with unequal voltages/currents.

Cases 1 and 4 are trivial. Add the voltages or currents respectively.
 
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jbriggs444 said:
Yes. Cases 2 and 3 are impossible for ideal sources with unequal voltages/currents.

Cases 1 and 4 are trivial. Add the voltages or currents respectively.

And if you use non-ideal sources in real circuits for cases 2 and 3 just to see what happens something really bad might happen like a short circuit that might damage equipment/start a fire. Hard to guess since it would depend on the particular design of the sources.
 
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Now I liked of the answers!
 
  • #10
Cases 1 and 4 are possible only if I1 = I2 = I3 and V1 = V2 = V3 ?
 
  • #11
Jhenrique said:
Cases 1 and 4 are possible only if I1 = I2 = I3 and V1 = V2 = V3 ?

That should be... Cases 2 and 3 are only possible if...
 
  • #12
CWatters said:
That should be... Cases 2 and 3 are only possible if...

what? 2 and 3 are absolutely impossibles!
 
  • #13
Looks like I misunderstood your post.

Case 1: Possible. Veq=V1+V2+V3 and I1=I2=I3.

Case 2: Possible but only if V1=V2=V3=Veq. Not recommended in the real world

Case 3: Possible but only if I1=I2=I3=Ieq. Not recommended in the real world.

Case 4: Possible. Ieq=I1+I2+I3 and V1=V2=V3
 
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  • #14
Case 2 and 3 can be done in the real world but care is needed. An example of case 2 is jump starting a car by placing two batteries in parallel. This works because they are not ideal voltage sources (no such thing as an ideal voltage source in the real world).
 
  • #15
CWatters said:
Looks like I misunderstood your post.

Case 1: Possible. Veq=V1+V2+V3 and I1=I2=I3.

Case 2: Possible but only if V1=V2=V3=Veq. Not recommended in the real world

Case 3: Possible but only if I1=I2=I3=Ieq. Not recommended in the real world.

Case 4: Possible. Ieq=I1+I2+I3 and V1=V2=V3

Good! Existe some book that gives those explanations too? Cause I never see...
 

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