Lloyd wrote:If a current is moving through space, I assume it's moving toward the nearest or strongest opposite charge concentration, although bipolar jets are currents too, aren't they?, and they're moving away from the poles of a body, rather than toward opposite charge, I guess.
It all depends on the model. In my model of bipolar jets, ejecta from "natural tokamaks" move because of the momentum they got from the nuclear fusion going on in the core of the reactor. They are +ions, and they drag electrons along with them, in a parallel but separate charge stream. CMEs are likewise +ions, which drag electrons along with them, but CMEs typically balloon outward -- they don't stay collimated like bipolar jets, so they don't drag a parallel but separate stream of electrons along with them. Rather, CMEs simply increase the voltage between the Sun and the heliosphere, which increases the electron drift out of the photosphere.
Lloyd wrote:The theoretical galactic current in the EU model, is it supposed to be moving toward an opposite charge concentration? It doesn't seem so.
I don't know -- I haven't heard anybody say specifically.
Lloyd wrote:I heard that AC current moves on the surface of conductors, while DC moves within conductors. Do you agree?
I think that all currents (AC/DC) flow on the surface of the conductors.
Lloyd wrote:Would there be vacuum channels in either of those locations?
That depends on who you're talking to. Most EEs don't seem to acknowledge any sort of vacuum between atoms in the crystal lattice of a conductor -- they think of the whole thing at a higher granularity, where the valence bands have fused into a continuous conductor, and the electron cloud is free to slosh around all it wants. But if you step down one notch in granularity, you see the atoms, and the electron shells, and the void between the atoms. So every time an electron hops from one atom to the next, it has to exceed the work function of the previous atom (as if it were an electrode) to get out of that electron shell and into the next one. But it does this easily, because the atoms are close enough together that all of the electric forces are superposing, so the shells present little resistance. At the end of the conductor -- at the electrode staring off into a vacuum -- there is no next atom to hop onto, so the electron somehow has to be broken completely out of the valence band of the conductor. That takes additional work (known as the work function of the electrode). But that doesn't mean that the vacuum is providing "resistance" -- it's just that the crystal lattice came to an end, and the binding energy of the electrons inside the conductor had to be overcome. Once this happens, the electrons can drift through the vacuum unimpeded.