What happens to surface charges when conductors/dielectrics touch?

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Discussion Overview

The discussion centers around the behavior of surface charges when conductors and dielectrics come into contact. Participants explore the implications of charge movement, polarization, and the effects of electrochemical potential differences in various materials, including ideal and real-world scenarios.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • Some participants suggest that when conductors or dielectrics touch, surface charges may move or cancel each other out.
  • Others argue that in a perfect dielectric, charges cannot move, and thus no exchange occurs between dielectrics upon contact.
  • It is proposed that charges in dielectrics can shift slightly due to polarization, but they remain bound and do not flow freely.
  • Some participants question the nature of charge movement in conductors, suggesting that a double-charge layer may form due to electrochemical potential differences.
  • There is a discussion about whether the conductors involved are the same or different, with implications for the electrochemical potential and charge distribution.
  • Some participants express uncertainty about the concept of "cancellation" of charges and how it applies to real versus ideal situations.
  • Concerns are raised about the presence of gaps between surfaces and how that affects charge distribution and potential gradients.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the behavior of charges in dielectrics or conductors when they touch. Multiple competing views remain regarding the movement and cancellation of charges, particularly in the context of ideal versus real materials.

Contextual Notes

Limitations in the discussion include assumptions about ideal conditions, the nature of dielectric materials, and the effects of external electric fields. The complexity of real-world materials versus theoretical models is acknowledged but not resolved.

feynman1
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When 2 conductors/dielectrics touch, will surface charges move away from their original conductor/dielectric to the other?
 
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Yes, they meet and cancel charges.
 
anuttarasammyak said:
Yes, they meet and cancel charges.
How could any charge move in a perfect dielectric? You are implying that something happens differently, the instant when they 'touch', compared with when there's a small gap. The Capacitance that the conductor will 'see', starts with an air spaced capacitor in series with a dielectric space. As the gap decreases, the capacitance of the air space increases without limit until all that's there is the dielectric layer. Can any charges flow onto or off the dielectric surface? By definition, I don't think so.

I think that the clue to the perceived paradox here is that the conductor is a real one and 'all the charges do not occupy an infinitely small region on the surface (the row of +++ signs that we draw in diagrams). The molecular fields in a real dielectric will not be uniform at the surface either.
 
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sophiecentaur said:
How could any charge move in a perfect dielectric? You are implying that something happens differently, the instant when they 'touch', compared with when there's a small gap. The Capacitance that the conductor will 'see', starts with an air spaced capacitor in series with a dielectric space. As the gap decreases, the capacitance of the air space increases without limit until all that's there is the dielectric layer. Can any charges flow onto or off the dielectric surface? By definition, I don't think so.

I think that the clue to the perceived paradox here is that the conductor is a real one and 'all the charges do not occupy an infinitely small region on the surface (the row of +++ signs that we draw in diagrams). The molecular fields in a real dielectric will not be uniform at the surface either.
I too disagree that charges in dielectrics can move, as there's no free charge there. But what about conductors?
 
Of course, in a dielectric the charges move a bit, but they are all bound, i.e., they don't move very far but are hold back by the binding forces (also electromagnetic). That's how a dielectric gets polarized by an external electric field. At a positively charged plate you due to this shift of charges in the dielectric you have a thin layer of negative charges at the boundary of the dielectric adjacent to the positively charged plate, and that's why the net effect of an dielectric within a capacitor enhances its capacitance by a factor ##\epsilon_r## compared to the capacitance of a "vacuum filled" capacitor, i.e., to get the same voltage difference ##U## you need to bring more charge ##Q=CU## to the plate in a dielectric-filled capacitor than in a vacuum-filled one.
 
By 'I too disagree that charges in dielectrics can move', I mean if 2 dielectrics touch, charges shouldn't exchange from dielectric to dielectric? Agree?
 
No, they are not exchanged but are bound but still they move a little bit leading to polarization of the dielectrics. Without external electric field that's due to the electro-chemical-potential difference between the different media.
 
Even dialectics can have a few free electrons, and only a few may need to move to redistribute the charge.

In real life, we don't have pure conductors, insulators, semiconductors, or dielectrics.
 
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If everyone agrees that 2 dielectrics won't exchange surface charges when touching, what happens to 2 conductors then?
 
  • #10
There will build up a thin double-charge layer at the surface due to the electrochemical potential difference between the metals.
 
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  • #11
Can anyone draw a brief graph to illustrate this electrochemical potential difference between the metals? Thanks in advance.
 
  • #12
Are the metals (conductors) the same or different? The electrochemical potential seems to unnecessarily complicate the discussion, but certainly is necessary for different metals.
 
  • #13
hutchphd said:
Are the metals (conductors) the same or different? The electrochemical potential seems to unnecessarily complicate the discussion, but certainly is necessary for different metals.
Different conductors.
 
  • #14
Say you connect a wire to the charged plates of conductor, charges move through wire so short circuit takes place. I do not see much difference on what take place in touching and in short circuiting.

I am not sure at all your setting of touching dielectric e.g. with E field keep working, touching with same/different polarity ?

In the usual case of sandwiching dielectric with condenser plates, surface charges of dielectric are cancelled, more exactly over cancelled, by charges of condenser plates.
 
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  • #15
anuttarasammyak said:
surface charges of dielectric are cancelled,
I'm not sure why you mean by "cancelled". For two ideal dielectrics the electrons from one side will not flow onto the other side. But, as I wrote before, it is not fruitful to try to reconcile ideal situations with reality. It's called a discontinuity, I think.
 
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  • #16
sophiecentaur said:
I'm not sure why you mean by "cancelled".
Please find an attached figure to show "cancel" I mean in post #14. Dielectric is also insulator, touching condenser plates.

2020-06-09 17.16.33.jpg
 
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  • #17
anuttarasammyak said:
Please find attached figures to show "cancel" I mean in post #14.
That's fine as an intuitive picture of it but how is that 'cancellation' any different from the same +- patterns that you have drawn all over the dielectric? Wouldn't you expect the gradient of the potential 'within' each molecule to be the same as the gradient of the potential between them? If it were not, there would be movement of charge to make it so.

In terms of field, you have a situation with constant field through the dielectric and Zero field within the conductor. It's just a matter of how 'micro' you want to go in describing the transition. Also, a real situation will have gaps between the two surfaces with a few points of contact. In those gaps you would have Air? or even a Vacuum?. Where would your "cancellation" be there?
 
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  • #18
It's of course not completely cancelled. Since here the battery is connected to the capacitor you have a given voltage difference across the capacitor. That voltage difference leads to a charge ##\pm Q## on the plates with $$Q=C U = C_{\text{vac}} \epsilon_{\text{rel}} U,$$
i.e., you need more charge on the plate to get that voltage difference in the steady state than if the capacitor is filled with vacuum (because ##\epsilon_{\text{rel}}>1##). This is due to this "cancellation of charges" by polarization of the dieelectric.
 

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