cramming work?
tiny-tim said:
Doesn't the electrostatic force mean that the charges on the two plates of the same capacitor are
always equal (and opposite),
whatever happens?
atyy said:
So what about the rule tiny-tim cites about the charges on opposite plates of a capacitor always being the same? Perhaps this is a rule from circuit theory, and only works under conditions in which the opposite plates are connected within some closed circuit? …
This electrostatic force has really been bugging me …
I think you're right, atty, and exact equality occurs only in a "circuit", and then only from
conservation of charge.
I think this is how it works:
Imagine an isolated metal sphere N, already holding a negative charge, of 100 electrons.
Those 100 electrons will be repelling each other, and will try to get as far away from each other as possible, so they'll be fairly uniformly distributed around the sphere.
Attach a metal wire to N … only one or two of the electrons will go into the wire, because the wire is small, and any more would be repelled back onto the sphere.
Connect the wire to the earth, E … now all 100 electrons will be able to go to E, because E is so large (or will 1 electron remain on N, simply because it has no reason to move?

).
In other words, the electrons move from N to E not because of any potential difference, but because they repel each other, and E is a great place to hide!

Now start again, with the same negatively charged sphere N and a positively charged sphere P with 200 "holes".
Bring them close together … the closer they are, the more the electrons on N will be attracted to the holes on P, so the electrons and holes will no longer be uniformly distributed.
Connect the wire to N as before, and then connect E to the wire.
This time, the 100 electrons will still be repelling each other, but they will also be attracted to the 200 holes on P. So not all will want to get away.
How many will stay on N? Will any more arrive from E?
I don't know …
Perhaps we can work it out like this … suppose P and N (in their final position) were originally charged, in the same circuit, so as to have 200 holes and electrons respectively.
So the 200 electrons on N
could have gone a long way away (to the battery, which we'll assume is as good as infinitely far away, so far as electrostatic force is concerned). But they didn't, 'cos their natural repulsion for each other was exactly balanced by their attraction for the holes on P
plus the "pressure" from the battery.
Now disconnect the battery, and connect N to E … the "pressure" has gone, but the attraction from P is still there!
So some of the electrons on N will go to E, but some will remain crammed on N, attracted by P.
So the questions seem to be,
i] what is the work is done by moving a charge Q though a voltage V, compared with the work done by cramming a charge Q (made up of many mutually repelling electrons) into a small volume? and
ii] what is the electrostatic attraction compared with the battery "pressure"?
At this point, I have no idea how to calculate either.
Though it seem obvious that the smaller the area A of the plate, the more the cramming work … and capacitor plates are
very small compared with metal spheres … and that a "positive feedback" means that the larger Q is, the more the electrostatic attraction is "helping".
I've never even seen cramming work mentioned … but it seems an essential part of the operation of a capacitor.
Dimensionally, one would expect it to be something like Q²/ε√A (which is much
larger than the standard work done, Q²d/εA).
Or is it insignificantly tiny?
