Kirchoff's loop rule with multiple voltage sources

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Discussion Overview

The discussion revolves around understanding Kirchoff's loop rule in the context of circuits with multiple voltage sources. Participants explore the implications of different current values and how they relate to the voltage sources in the circuit, focusing on both theoretical and practical aspects of circuit analysis.

Discussion Character

  • Exploratory, Technical explanation, Conceptual clarification, Debate/contested

Main Points Raised

  • One participant expresses confusion about how the current I1 is influenced by both voltage sources and how this relates to Kirchoff's loop rule.
  • Another participant suggests that the current I3 affects I2, implying that the interaction between currents is significant in understanding the overall circuit behavior.
  • A different participant acknowledges the influence of both voltage sources on I1 but struggles with the application of the loop rule, particularly regarding the omission of ε2 in the first equation.
  • One participant attempts to clarify that the equations for the circuit do not require I2 in the loop equations, suggesting that I2 is derived from I1 and I3 instead.
  • Another participant emphasizes the importance of using multiple equations to solve for multiple unknowns in circuit analysis, indicating that the relationship between the currents and voltage sources is more complex than it appears.

Areas of Agreement / Disagreement

Participants do not reach a consensus, as there are differing interpretations of how the voltage sources affect the currents and how to apply Kirchoff's loop rule effectively. The discussion remains unresolved with multiple competing views on the topic.

Contextual Notes

There are limitations in the discussion regarding the assumptions made about the relationships between the currents and voltage sources, as well as the mathematical steps involved in applying Kirchoff's loop rule. Some participants express uncertainty about the completeness of their equations in representing the circuit behavior.

Avatrin
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Hi

Let's look at this:

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The issue I am having is that while I know that this is accurate:
img715.png


I just cannot wrap my head around why. I1 is a result of both voltage sources. So, while the equations clearly tell me that the voltage drop across the resistor R1 is I1R1, I cannot wrap my head around how this works in terms of Kirchoff's loop rule.
 
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Doesn't I3 steal from I2 to make I1 different? Surely you accept that I3 is affected by E2.
 
Yes, I get that part. It is the Kirchoff's loop rule that I cannot wrap my head around.

I1 is affected by both ε1 and ε2. Yet, I can use the equation above ignoring ε2. It is true regardless of ε2. That part I cannot wrap my head around.
 
Ahhh i see.

I think it's not an electrical ambiguity, rather a temporary memory lapse in translating from the algebra you know well to the electricity that seems unfamiliar.

Back to algebra basics: It takes more than one equation to solve for more than one unknown.
So that one equation isn't the whole story.

We all stumble over these little difficulties. Work lots of homework problems..

old jim
 
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If I understand correctly, your trouble seems to be the fact that the ε2 source is not represented in the first equation. The issue is that I2 is not a part of the loop equations in their most basic form. Rather I2 = I1 - I3, and there are only two equations that are necessary for the drawn circuit. Those loop equations need only use I1 & I3, so while ε2 is not directly reflected in the loop 1 equation, it is a part in as much as it factors into the 2nd loop equation as a boundary condition of I3's loop.

Follow Jim's advice and use the math and you will see that a change in ε2 does cause a change in the first equations value.
 

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