Re: Contrary current flow within a radiator
- From: Jim Lux <james.p.lux@xxxxxxxxxxxx>
- Date: Wed, 14 Jan 2009 14:18:43 -0800
Roy Lewallen wrote:
I don't want to add ammunition to support Art's gibberish, but it's interesting and not widely known that current *does* flow in the opposite direction to the main flow, at certain depths in a homogeneous conductor.
In a solid conductor, the current density does, of course, decrease exponentially with depth. The depth at which it's decayed to 1/e (about 37%) of the surface density is the "skin depth". This is why a hollow tube is just as good a conductor as a solid one, providing only that the tube wall is at least several skin depths thick.
But the *phase* of the current changes with depth, too, quite dramatically. As you go each skin depth deeper below the surface, the phase becomes one radian (about 57 degrees) more lagging. So at pi skin depths below the surface, the current is completely out of phase with the surface current, i.e., it's flowing in the opposite direction. Of course, the current density at this point is very small, only 1/e^pi ~ 4% of the surface density, so only a small fraction of the total current flows completely backward. (Good thing!) At two pi skin depths, the current is again in phase with the surface current, but its magnitude is only 1/e^(2*pi) ~ 1/500 of the surface density. And so forth.
This isn't of much immediate practical use, and it's certainly not offered as supporting in any way Art's fanciful theories (whatever they might be). But it is an interesting fact.
I wonder if one could set up some sort of interesting demonstration of this. If you could, for instance, have a 1 foot diameter conductor with skin depth of an inch or so, and some (probably not feasible) way to indicate current flow. (yes, in order for this to happen it has to be AC, etc.)
.
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