....Electrons also have speed profiles that depend on radius, only they are slowest at min r. How these two profiles intersect is not a straight forward matter, in terms of scattering and thermalization. To me, it would not be all that surprizing if the normal calculation methods used for "thermal" systems like the tokomak were very far off from reality....
I agree that yields and losses etc cannot be even guessed at from Tokomak (or old Stellarator) experience; however, given (or with assumed) local density of electrons and ions only one can do a lot with confidence.
For example, calculate the electric potential everywhere. From this and the nature of the electrons injected (current and energy) one can then get good idea of the energy density everywhere. How this energy is distributed among the particles is a little more speculative but not much unknown if you work hard at the calculations. One can be confident that the electrons do have a local temperature (I.e. a Maxwellian distribution) everywhere, except for the few that have just been injected into that local volume. - They will very rapidly also take their place in the distribution.
For example if some of those injected do make it into the center and turn around they will not make it back even once to the edge of the well but the stopping them is a "pressure" that can build the well.
By design, we know that there is an excess of electrons everywhere (if there were more ions in some small delta r spherical shell then the electric potential would be going up, not down as you pass from R greater thru that net positive shell. (actually as some if not all, of the Boron is multiply ionized there could even be less that 20% the ion density as the electron density everywhere.
I think it is likely that any ion sort of at rest at the edge of the well will fall quite far into the well and not strongly collided with others but will be scattering (accelerating, producing radiation) the electrons as it does so without transfer of much energy to the electrons because of the mass difference. Thus it is reasonable to think that in the outer parts of the well the ions may not be thermal and even if they are, may not have the same temperature as the electrons at least the first time they enter the plasma region. (I am not clear on how the ions are introduced - perhaps boiled out of a tiny tub into vacuum?)
If the device is to have significant fusion making collision there will be plenty of non-fusion collisions among the ions to make most of them have a temperature, but for reasons stated, even in the center of the well they will not quite make neutral plasma. There will be a lot of recombination occurring and this is a loss of energy via UV and soft X-rays which with the assumed densities and temperatures can be computed. (True these assumed values, which are a function of radial location, may not be the ones actually present, but with them one can also compute the fusion rate, along the lines I suggested with consideration of the impact parameters these distributions imply.)
Thus for many assumed distributions, including some obviously too favorable, one can compare the radiative loss rate to the fusion energy production rate. That is what needs to be done. Perhaps there is some distribution for which the losses do not exceed the energy production rate, but I doubt it as with large number of multiple charged ions the radiation is intense. -I initially told how this blocked the old Stellarator form achieving even the much lower temperature for the DT reaction until the diverters were added (to "skim off" the influx of out gassing molecules, which were quenching the plasma via this radiation.) but the fact that highly charged ions in a hot plasma radiate like crazy is not device dependent.
It is a simple fact, always true, built on the well understood binary interactions taking place. It will be true in Bussards device as it is in all others - even the shock tube plasma I used for my Ph.D. which only had neutral and one stage of ionization Argon gas in it. Ions do recombine with electron in plasmas and radiate. X-rays or at least harsh UV if they have 4 or 5 electrons missing as is Bussard's hope with B+++++ ions.