Just to be picky, KitemanSA is accurate when he mentions the difference in the Polywell. I doubt it will chang Jos's vitrified viewpoints, but an expansion of what was said may be helpfull. First off mirror machines have not been abondoned, there are some adherants that hope some manipulation may still work. In the Pollywell there are two considerations. First cusp confinement is perhaps ~8-10 times better than biconic mirror machines in terms of the volume of plasma contained vs the cusp loss rates. This is an improvement but not a game changing one. The Wiffleball inflation is a game changer. High beta inflation of the Wiffleball increases the 'cusp' confinement an additional ~ 100 X (to values in the thousands) . This leakage would apply to the ions and electrons in a neutral plasma. But the plasma is not neutral. The excess electrons produce an electrostatic potential well that contains the ions to even better levels of perhaps several orders of magnitude or more. This requires MFP for the fuel ions that approach or probably exceed the diameter of the machine combined with annealing which combined retard the upscattering of ions so that the potential well can continue to retain enough of the ions so that the ~ 100x- 1000 X less efficient Wiffleball containment losses only applies to the relatively small portion of ions that have managed to overcome the annealing process.KitemanSA wrote:If the Polywell were trying to confine the plasma with magnetic fields, it would be forgotten now too. But that is the GENIUS of the Polywell. It is confining the plasma with an electrodynamic well, not a magnetic field. ED wells are quite stable against minor perturbations.Joseph Chikva wrote: ....
Convex field had all mirror kind of machines. All them are forgotten now.I have looked the general history a bit, enough to understand the failings of most of the big money machines to date. Polywell doesn't have those failings. It may have OTHERS, but not those....Joseph Chikva wrote: Studying only Polywell history may be better if you get studied also what has been done in fusion research during past 60 years.
The crossfield transport of these upscattered electrons may be an issue, but I suspect the cusp losses still dominate for the upscattered ions as the effective density of these ions are substantially less than the population of of electrostatically contained ions deeper within the magnet grid. These ions are not reaching the magnetic domain, so they are not contributing to the random walk of the upscattered ions doing the ExB drift through the magnetic field. The point is mostly moot though as either the drift or cusp escape of these upscattered ions is desireable. The ExB drift is one reason why magnatized plasma machines need to be large as ion confinement time is limited by this process (assuming macro instabilities do not occur). The Polywell overcomes this by only confining the electrons in this manner. Things changes some when the Wiffleball forms, but initially this applies. This allows for electron confinement to be dominated by the cusp losses, even in small machines where the thicknes of the magnatized layers small. With ions in a neutral plasma with no potential well the ExB drift losses may even dominate over cusp losses in these small machines. The non neutral plasma is the key. This mostly removes the ions from ExB drift considerations. They are electrostatically retained within the magnetic shell. This allows for the magnetic constraints to apply mostly only to the electrons and with their ~ 60X or greater difference in momentum the ExB drift limits allows for smaller machines with significantly increased densities- especially with Wiffleball confinement greatly improving the cusp confinement. This allows for larger contained electron densities at acceptable losses (with recirculation) and this leads to electrostatic ion containment at almost equal densities. This ~ 1000 fold increased density leads to n^2 fusion rates a million times higher, with constant B and volume. This occurs with loss rates of ExB transport of electrons and cusp loss of electrons similar to the starting lower density conditions of the non wiffleball configuration. This ~ 1000 fold improvement in density with resultant ~ 1 million fold improvement in fusion makes up for much of the deficiency of Elmore Tuck type fusors which is the baseline from which the Polywell is derived. Recirculation of the elecrons then pushes the energy balance into the positive region, if the system works as advertized. Add to that further gains from increasing the B field strength ( B* n^2). Density scales as the square of the B field. Fusion scales as the density squared, thus the B^4 scaling.
There are all sorts of permutations that effect the final configuration and interacting physics, thus the difficulty is modeling the system without extensive experimental data. The same has been found to apply to the tokamak. But the complications are hoped to be much less than in the tokamak (such as the macro instabilities, asymmetry conditions, MHD stability issues, etc. WB 8 will/ has answered much of these questions, but a larger machine would have done better, once again illustrating Bussard and Nebels reasoning for going to to a near full size machine. Also, it illustrates the comparative dollar costs based on ~ r^3 scaling between the Polywell and tokamak.
Dan Tibbets