Instant change of current in an inductor

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Discussion Overview

The discussion revolves around the behavior of an inductor in a DC circuit when a switch is opened, particularly focusing on the theoretical implications of instantaneous changes in current and the resulting voltage. Participants explore concepts of energy storage in inductors compared to capacitors, the effects of arcing, and practical applications in circuits.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant questions whether an inductor could theoretically create any voltage by disconnecting it rapidly, suggesting that the resistance of air could influence the time constant of the voltage's existence.
  • Another participant argues that an infinite voltage spike cannot occur due to arcing at the switch when opened.
  • Some participants propose that the energy storage analogy for inductors is akin to shorting the ends of the inductor, noting that energy dissipates due to the resistance in the coil.
  • One participant mentions experiments with superconductors where current is induced in a superconducting loop and observed over time, highlighting practical challenges in using inductive energy storage compared to capacitive storage.
  • Another participant emphasizes that even superconducting inductors have capacitance, which affects energy discharge when the switch is opened.
  • Discussion includes the use of parasitic capacitance in flyback DC-DC power supplies and how it influences peak output voltage and energy transfer dynamics.
  • Concerns are raised about the relationship between the peak voltage across parasitic capacitance and the arc-over voltage of the switch, introducing a dynamic interplay between switch operation and circuit resonance.

Areas of Agreement / Disagreement

Participants express differing views on the feasibility of achieving high voltages through rapid disconnection of an inductor, the role of arcing, and the implications of parasitic capacitance. The discussion remains unresolved with multiple competing perspectives.

Contextual Notes

Participants note limitations related to assumptions about ideal versus real inductors, the influence of parasitic elements, and the conditions under which energy storage and discharge occur.

iceman_ch
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Ok, here is a goofy question. Say you have an inductor that is connected in a simple DC circuit and has been there for a "long time". Now if you had a switch that you could move at any speed that you wanted to and could be any distance from the terminal that you wanted it to be what would happen when you disconnected it? Since an inductor resists any change in current would it be able to create any voltage you wanted it to by opening that switch as far as you wanted to. I believe theoretically the answer is yes. You could use the resistance in the air and the distance for the resistive part of the time constant and that would tell you the amount of time that the voltage would exist. Does this mean that when an inductor is removed from a circuit it could never store energy like a capacitor could?
 
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you can never get that infinite voltage spike by opening the switch because the switch would just arc.

i think the energy storage analogy would be to short the ends of the inductor (you open the ends of the cap to store energy). the problem is, the flux induces a current in the coil, and that coil also has resistance, so your energy dissipates.
 
Proton Soup said:
i think the energy storage analogy would be to short the ends of the inductor (you open the ends of the cap to store energy). the problem is, the flux induces a current in the coil, and that coil also has resistance, so your energy dissipates.

This is pretty much exactly what's done in experiments with superconductors, though. They induce a current into a superconducting loop (which has some inductance), and then come back years later and see if it's still flowing.

Inductive energy storage as a practical alternative to capacitive energy storage still hasn't made many inroads, though.
 
Even if the windings of the inductor are superconducting, there is always a capacitance. If the inductor is carrying current for a long time, then the switch is opened, in an attempt to quickly interrupt the current, the energy will discharge into the winding capacitance.

In an analogous manner, a perfect cap with superconducting plates and leads is charged to a steady dc voltage. If shorted with a zero ohm termination, superconducting, what happens? The self-inductance of the cap limits the current. Energy is transferred from the electric field between the plates, to the magnetic field in the closed loop.

Does this answer the question?

Claude
 
Last edited:
cabraham said:
Even if the windings of the inductor are superconducting, there is always a capacitance. If the inductor is carrying current for a long time, then the switch is opened, in an attempt to quickly interrupt the current, the energy will discharge into the winding capacitance.

In fact, this technique is used in "flyback" topology DC-DC power supplies, like the ones that generate the high voltage for the picture tube in (ancient) TVs. The capacitance is explicit in these supplies, and is sized to give the peak output voltage that is rectified to generate the output high voltage.

But as cabraham says, if you have just a real inductor alone, the peak output voltage will be determined by the parasitic capacitance of the inductor -- the energy stored in the inductor current gets transferred into the peak voltage across the parasitic capacitance, and then that energy is transferred back into a reverse current through the inductor, and so on. There is also a DCR (parasitic resistance) associated with the inductor, and that is the R element in the lossy RLC resonant circuit of the real inductor all by itself.

The arcing effect mentioned will come into play if the peak voltage across the parasitic capacitance exceeds the arc-over voltage across the (partially) open switch... the race is how quickly the gap opens on the switch versus the RC resonance half-period on the first ring-up.
 

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