Opening switch on inductor circuit in absolute vacuum

Click For Summary
SUMMARY

The discussion centers on the behavior of inductors in circuits when a switch is opened, particularly in the context of an absolute vacuum. It is established that opening a switch in an inductor circuit causes a voltage spike, allowing current to briefly continue flowing across the gap, which can lead to a spark. In a perfect vacuum, the absence of air reduces the likelihood of a spark, but the inductive effect still causes a significant voltage increase to maintain current flow. The mathematical representation of this phenomenon is captured in the equation I(t) = I_0e^{-Rt/L}, illustrating the relationship between current, resistance, and inductance.

PREREQUISITES
  • Understanding of inductance and its role in electrical circuits.
  • Familiarity with the concept of voltage and current in electrical engineering.
  • Knowledge of differential equations as they apply to electrical circuits.
  • Basic principles of vacuum physics and its implications in electrical contexts.
NEXT STEPS
  • Explore the effects of inductance on circuit behavior during switch operations.
  • Study the mathematical modeling of LR circuits and their transient responses.
  • Investigate the implications of vacuum conditions on electrical discharges.
  • Learn about the role of resistance in electrical circuits and its impact on voltage spikes.
USEFUL FOR

Electrical engineers, physicists, and students studying circuit theory who are interested in the dynamics of inductors and the effects of vacuum conditions on electrical phenomena.

osnarf
Messages
207
Reaction score
0
So, a professor in class a about a year ago mentioned that opening a switch in a circuit that an inductor is providing power to would cause a breakdown in the air and a spark would jump across it because the current can't change instantaneously to zero in an inductor. Something just made me think about that. But anyways, what would happen if it was in a perfect absolute vacuum?
 
Physics news on Phys.org
osnarf said:
So, a professor in class a about a year ago mentioned that opening a switch in a circuit that an inductor is providing power to would cause a breakdown in the air and a spark would jump across it because the current can't change instantaneously to zero in an inductor. Something just made me think about that. But anyways, what would happen if it was in a perfect absolute vacuum?

Very likely it would have little effect since the dielectric effect of a tiny amount of air as the circuit opened would only make it a tiny bit easier for the spark to fly across the gap than it would do it without the air there.
 
osnarf said:
So, a professor in class a about a year ago mentioned that opening a switch in a circuit that an inductor is providing power to would cause a breakdown in the air and a spark would jump across it because the current can't change instantaneously to zero in an inductor. Something just made me think about that. But anyways, what would happen if it was in a perfect absolute vacuum?

I thought it was the opposite, that having an inductor prevents an instantaneous change of current through the circuit which would be disastrous, since an instantaneous change in current would create an infinite voltage which would lead to sparks.
 
RedX said:
I thought it was the opposite, that having an inductor prevents an instantaneous change of current through the circuit which would be disastrous, since an instantaneous change in current would create an infinite voltage which would lead to sparks.

You have it right but seem to misunderstand the effect. The inductance in the circuit prevents an instantaneous change in current so what happens, as the OP described, is that a spark occurs when the circuit opens because the voltage goes WAY up in order to provide a current across the gap for a VERY brief time so that the current can go to zero quickly but NOT instantaneously. That is, the current CAN'T change instantaneously, and the voltage in the circuit is NOT going to be enough to drive a spark across a gap, so the inductive effect causes the voltage to rise dramatically very quickly so that the current can decrease very quickly. It doesn't take infinite voltage to create a gap spark.
 
phinds said:
You have it right but seem to misunderstand the effect. The inductance in the circuit prevents an instantaneous change in current so what happens, as the OP described, is that a spark occurs when the circuit opens because the voltage goes WAY up in order to provide a current across the gap for a VERY brief time so that the current can go to zero quickly but NOT instantaneously. That is, the current CAN'T change instantaneously, and the voltage in the circuit is NOT going to be enough to drive a spark across a gap, so the inductive effect causes the voltage to rise dramatically very quickly so that the current can decrease very quickly. It doesn't take infinite voltage to create a gap spark.

I think I see what you mean, but in an LR circuit, upon disconnection, the current goes as:

I(t)=I_0e^{-Rt/L}

so that the voltage across the gap with high resistance R is:

V(t)=-L*I'(t)=RI_0e^{-Rt/L}

so it seems that this effect doesn't depend on the value of L at all, just the value of the gap resistance R. The maximum voltage drop across the gap will always be RI_0 at time zero, regardless if you have an inductor or just have the self-inductance of the wires.
 
By opening the switch the gap width is not constant.
The value of resistance across the gap is thus not a constant value of R, but is increasing from 0 at the time the switch is thrown to a greater and greater resistance.
Subsequently, the voltage across the gap increases to a higher and higher value.

From your second equation V(t)=−L∗I′(t)=RI0e−Rt/L , with the R being variable and increasing, the voltage itself increases alongside the gap becoming wider if an inductance is included in the circuit..
 
256bits said:
By opening the switch the gap width is not constant.
The value of resistance across the gap is thus not a constant value of R, but is increasing from 0 at the time the switch is thrown to a greater and greater resistance.
Subsequently, the voltage across the gap increases to a higher and higher value.

From your second equation V(t)=−L∗I′(t)=RI0e−Rt/L , with the R being variable and increasing, the voltage itself increases alongside the gap becoming wider if an inductance is included in the circuit..

That certainly makes sense, and is very perceptive. If you include a time-varying gap resistance, then the equation for the voltage drop across the gap:

V(t)=I_0 R(t) e^{-(1/L) \int R(t) dt}
If R(t) is increasing with time, then a huge inductance L will allow the factor of R(t) in front to increase with time without much drop in the exponential as time passes, so the voltage attains higher value with increasing L.

That is strange though as I thought inductors were good things and prevented sparks, but were bad for things like signal processing as they smooth out waveforms.
 
A slight segue here. An absolute vacuum? Really? Really? Do you mean a partial vacuum? Absolute vacuums are the realm of theoretical physics. Example: Present definition of a vacuum is "http://www.thefreedictionary.com/vacuum" " Since mass/energy, space and time all seem to be intertwined, perhaps a better definition might be that an absolute vacuum is "A volume devoid of space." (The volume only being defined and described by space surrounding the absence.)
This is frontier stuff, mostly dealt with in far-fetched scientific papers and http://www.youtube.com/watch?v=2fdhyhPu6PY".
 
Last edited by a moderator:

Similar threads

  • · Replies 24 ·
Replies
24
Views
8K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 19 ·
Replies
19
Views
2K
  • · Replies 9 ·
Replies
9
Views
3K
  • · Replies 10 ·
Replies
10
Views
1K
  • · Replies 4 ·
Replies
4
Views
2K
  • · Replies 10 ·
Replies
10
Views
3K
  • · Replies 52 ·
2
Replies
52
Views
13K
  • · Replies 14 ·
Replies
14
Views
4K
  • · Replies 4 ·
Replies
4
Views
3K