Why is R1 Open in Short Circuit?

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Discussion Overview

The discussion revolves around the behavior of a resistor (R1) in a circuit when a voltage source (Vs) is replaced with a short circuit, particularly in the context of steady-state DC conditions. Participants explore the implications of this scenario on current flow through R1 and the role of an inductor in parallel with R1.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Mathematical reasoning

Main Points Raised

  • Some participants question why no current passes through R1 when Vs is shorted, suggesting it should be in parallel with the short.
  • Others argue that since both ends of R1 are at the same potential due to the short, there is no current flow.
  • A participant raises a point about the distinction between open and short circuits, noting that an open branch can have a potential difference without current.
  • Some assert that R1 is not open but rather bypassed by the short circuit.
  • Questions are posed regarding the conditions under which a component in parallel with a short can be treated as a short itself for calculation purposes.
  • One participant emphasizes that while R1 may be considered a short for calculations, the inductor has no DC resistance, leading to no voltage across R1 and thus no current.
  • Another participant discusses the application of superposition and current division, illustrating how current flows through the path of least resistance.
  • Concerns are raised about the theoretical nature of the discussion and its applicability to real-world scenarios, highlighting the importance of considering non-zero resistance in practical systems.

Areas of Agreement / Disagreement

Participants express differing views on whether R1 is effectively open or shorted in the given scenario. There is no consensus on the interpretation of current flow through R1 versus the inductor, and the discussion remains unresolved regarding the conditions under which components in parallel with a short can be treated as shorts.

Contextual Notes

Participants acknowledge the limitations of theoretical discussions, particularly the assumption of ideal components with zero resistance, which may not hold in practical applications.

peripatein
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Hi,
Would someone care to please explain why no current passes through R1 (see attachment) in case Vs is replaced with a short and the inductor is considered a short too (in the steady state, for DC)? Why would the R1 branch be open and not short? Is it not in parallel with short under the above circumstances?
 

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If Vs is replaced with a short, what is the voltage across R1?
 
Yes, it is parallel with short so both termination of the resistor have the same potential. Therefore there is no current.
 
Why open? Doesn't zero potential mean short, rather than open? You can measure a potential between two terminations of an open branch, and the answer would not necessarily be zero. Whereas open means infinite resistance, hence current is zero.
 
It isn't open but bypassed by short.
 
Alright, so let me ask this then: when may a component in parallel with short be rendered a short?
 
This is not short nor open. Just: no potential difference = no current.
 
I got that, I am now asking a more general question, namely: when does a short turn a component in parallel to it into a short? In other words, if I take a component and connect it in parallel to a short - under what circumstances will that component, for calculation purposes, may be considered a short?
 
Under any circumstances.
 
  • #10
Well, why isn't that then what we have in the circuit in the attachment? Isn't R1 in parallel to a short? Following that reasoning why won't it then be considered a short itself, for calculation purposes?
 
  • #11
I think there is a slight misconception thinking of the situation as either a short or an open. An open can have a potential difference but no current flows, a short has no potential difference but has current flow.

In the R1 branch you have both no potential difference (because the two ends are connected by a short) and no current flow (because all the current flow will take the short due to it having less resistance).
 
  • #12
For calculation purposes you can replace it with a short. This branch doesn't affect rest of the circuit.
 
  • #13
But if the resistor is considered a short (or may be considered a short), then both the branch with the inductor is a short and the branch with R1. Therefore, why would the current "prefer" flowing through the branch of the inductor? I mean, are they not both merely wires (for calculation purposes)?
 
  • #14
No, you treat whole part of circuit with inductor and resistor as a short. Current flows through inductor - because it is a short for DC - and doesn't flow through resistor.
 
  • #15
Please don't get annoyed by all my questions (in case you are); am simply trying to understand this properly.
Didn't you just write that the resistor may be considered a short as well? Why won't the current consider both the resistor and the inductor to be a short? If it does, why then would the inductor (now a short, but so is the resistor) get current and not the resistor (if they are both a short then both of them have zero resistance)?
 
  • #16
I'm not annoyed :smile: Inductor has no DC resistance so it is a real short. This causes no voltage on resistor and thus no current. So you can get rid of resistor and nothing changes in the rest of the circuit. This is what I mean.
 
  • #17
I think I truly got it now. Thank you very much! :-)
 
  • #18
When using superposition in this case, the AC voltage source is shorted. The inductor in that branch also turns into a short in DC steady state.

So when current travels from the DC source, it first sees the cap which is an "open" in steady state DC. So it ignores it and travels to VA. At VA it has a choice between a non resistive wire and a resistor. It surely takes the path of zero resistance and has no interest in the resistor. So the short we just created has zero resistance, so there is no voltage there. Since it's parrallel to that resistor, there is zero voltage acrross resistor, therefore zero current thru resistor R4 according to V=IR.

Lets do current division as well. We'll call your inductor and VS sources (now shorted for superpostion) R0.

So we have R4=10 ohms and R0=0 ohms.

Let's just say that the current heading into node VA from DC source is 5 amps (just random guess for this exercise)

So current division thru R4 would be:
5*(0/(10+0)= 0 current thru R4.

So that's the DC case. The VAC source is going to put current thru each and every branch!
 
Last edited:
  • #19
That was a very clear explanation. Thank you, psparky!
 
  • #20
I should have figured the exact amps coming from DC source...is very simple in the case.

It's just going to be 10 volts/50 ohms which equals .2 amps leaving DC source...and .2 amps going back to source. (KCL)

50 ohms is the only resistance it encounters in this loop.
 
  • #21
It is important that this theoretical discussion - not be taken too far. ANY real system will have a non-zero resistance/impedance. So asking too many "what if" cases for a theoretical position is pointless, if not counter productive, because you may "learn" something that you later apply to a real world case and be led astray by your thinking.
 
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