nsaspook
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FeynmanFtw said:No, not about the light bulb, but about the non uniform surface charge. That paper simply goes on to show how we can see A surface charge. It doesn't explain anything about how it varies across the wire's length.
As explained in the Sefton paper, the circuit is a loop with turns or bends instead of a infinitely thin straight wire.
At bends in the wire there must be some additional unbalanced charge in order to change the
direction of the field and the current. To see how a distribution of surface charge can direct the flow
of mobile charges and also adjust itself to achieve that result, imagine an electron drifting a long a
wire and approaching a bend. The only way that it can get around the bend on a smooth path is for it
to be pushed or pulled around the corner by some other charged particles that are lying in wait for it.
If that were not so, the electron would keep going and run into the surface of the wire. If it does that
and sticks there it may, in turn, lie in ambush for another electron coming along behind it. So the
first electron, which does not quite make it around the bend, will help to push the next one around.
This process may continue until the surface charge builds up just enough to keep all the conduction
electrons on track. In ways like this the whole system will very quickly adjust itself until there is
just the right distribution of surface charge to ensure a smooth and continuous drift of conduction
charge along the wire. The reason that everything adjusts so quickly is that changes in electric field
propagate at the speed of light.
Another good article.
http://www.matterandinteractions.org/Content/Articles/circuit.pdf
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