4 ms·
I think for my objection to apply in the 2D case, you'd need for the force law to be 1/r instead of 1/r^2. That would happen in a truly 2D world, but not in thi
by c1ccccc1 5y ago
I think for my objection to apply in the 2D case, you'd need for the force law to be 1/r instead of 1/r^2. That would happen in a truly 2D world, but not in this case where we have charges confined to a 2D plane, but with 3D electric fields extending above and below that plane.
I think charge still goes to the surface, even if not induced. A spherical conductor with a net charge would have a uniform distribution of charge on its surface, and 0 charge density inside the bulk. Any net charge density inside the conductor would create a diverging electric field around itself, which would cause a current to flow, dissipating that net charge in the process. The same argument should apply to a bunch of free electrons, shouldn't it?
- contravariant 5y agoAh you're right by definition a conductor does have a current provided there's any electrical field inside it (divergent or not). So indeed they can't have charges inside them in equilibrium. However if you induce an electrical field in a vacuum then no charges at all will flow because a vacuum is the perfect insulator. And even if there is nonzero electric field in and around an individual electron they won't move as long as things cancel out at their exact position. Really the theory of conductors and charge densities seems to break down somewhat once you get to the point of individual electrons near absolute zero in a vacuum. One way to put this to the test would be to charge a conductor to its absolute limit, basically removing all free charges from it and seeing if the rest will crystalize. This might require an impractical amount of energy.