TallDave wrote:Ah, so such screening would only apply to charges on stuff within the Magrid, not on the Magrid itself (at least to the extent the Magrid is like a conducting sphere). That seems to makes sense, but then do you disagree with Dan's perspective of Gauss' Law being the result of charges on the sphere cancelling within the sphere? Presumably if they are cancelling at a given point in the sphere, they can also be screened from that point, but what you're saying sounds more like they just don't exist inside the sphere at all. Or is it just not possible to screen forces in such a way as to "reveal" the charges on the sphere to stuff inside?
The charge carriers on a conducting shell will automatically distribute themselves so that there is no electric field
anywhere inside the shell due either to the charge on it
or any additional external charge concentrations. This is indeed a 'cancelling' effect; it arises from the fact that this is the minimum-energy distribution.
Thus the wiffleball plasma doesn't 'see' (electrostatically speaking) the magrid,
or any other electrostatic influences external to the magrid (to first order, obviously). If there were no plasma, the electric potential inside the magrid would be flat.
Now, the plasma will have an effect on the charge distribution on the magrid, because the magrid charges can see the plasma charge. But the effect is symmetric and the upshot is the same.
Debye screening would apply to the charged wiffleball,
if it were a thermal plasma - the potential drop would occur mostly within a debye length or three from the wiffleball edge, resulting in a rectangular well. But the kinetic energy of the injected electrons is what forms the well, and it is larger than the maximum electric potential energy difference in the plasma (rather than being much smaller than it), as well as having a highly nonthermal distribution, and thus a Polywell plasma as it is predicted to form breaks the assumptions underlying debye screening theory.
Notice what happened there - a thermal plasma can shield its own interior via debye screening, but it can't change what happens outside it - screening is a matter of charge cancellation via superposition, and if you have a spherically-symmetric plasma ball with a charge q, it really doesn't matter what it does internally; from the outside it's going to look like a point charge q.
Do you understand the Principle of Superposition?