Joseph Chikva wrote:....
First
TOKAMAKs developers do not hope on 90% burning-off fuel. But on much less. In Polywell and in other beam devices as well by idea the burning-off should be more. But not 100%. Because in reaction zone gradually will decrease the density of reacting nucleii together with appearance of other charged particles - products of reaction.
Second
The temperature in TOKAMAKs not 5keV but 10 keV reached in latest versions and 15keV projected for ITER.
Third
There is one more difference between beam method (using coherent motion of particles for overcoming barrier) and thermal method: for beam we should spend 100% required for fusion KE before reaction. In thermal methods only high energetic tail of distribution can work initially. That is "ignition". Then by idea self-heating at the expense of fusion. It is not advantage or disadvantage but only the feature of method.
Fourth
I am repeating. Till now I could not see any mechanism allowing to avoid thermalization in Polywell. But thermalization will occur obligatory. As together with each fusion event you will get thousands elastic collisions events as well. So, If you have not any dissipating mechanism better if together with mechanism returning the scattered particle to the right direction, sorry. Because you will not can save your so lovely "mono-energetism"
1St, I never said that I expected a Tokamak to burn up 90% of the fuel. I said 90% of the fusion that does occur will result from those ions at the high end thermal tail of the plasma. This is an example, please do not think that I am implying an accurate quantitative profile of fusion rates vs temperature.
2nd, I gave an example for Tokamak temperatures. Obvously, a considerable effort has been expended to boost the operating temperature of Tokamaks. I even included a example where the Tokamak had a 20 KeV temperature, in excess of your expectations.. The point was not only the average temperature reached, but also the thermal spread about that temperature.
3rd, Percisely. Tokamaks are thermal machines that depend on ignition to provide the nessisary thermal temperature against losses.
A Polywell is a power amplifier. It does not use ignition. In fact, ignition is bad as that implies that the high energy fusion ions are thermalizing within the plasma. If Coulomb collisionality and dwell times allow for high energy fusion ions thermalization, then all of the lower energy fuel ions would also be quickly thermalizing- which is not desired. Thinking about it, this may be one reason that A. Carlson thought that such high potential wells was needed (several million electron volts- because he may have assumed that the multiMeV fusion ions were contributing to the overal ion population thermalized mix.
But, fusion ions in a Polywell are expected to give up almost none of their energy to the plasma before they escape through a cusp.They are expected to make ~ 1000 passes (due to the Wiffleball traping factor- not the potential well which is of course way too weak to effect these ions much). Wven with a few thousand passes the distance traveled will only be a few thousand meters, and the MFP at >~3 MeV energies is in the tens of thousand Meter range. Also, the fusion ions would not maintain confluence for long so they would not have as much concentrating effect in the core as the fuel ions are expected to have. I can explain my reasoning on this.if you wish.
As you suggested, all, 100% of the ion energy comes from the potential well. There is no (ideally) heating from scattering collisions. There is some thermal spread ongoing but no needed boosting of the temperature. And, this thermal spread is minimal to moderate depending on machine size, operating density, effectiveness ot 'annealing', etc. Also, just as with electrons there is a mechanism for preferentially removing runaway upscattered ions, just as there is for electrons.
4th, Yes Coulomb scattering collisions will always exceed fusion collisions. But, not nessisarily by thousands. In D-T reactors, at ~ 100 KeV Coulomb collisions only exceed fusion collisions by ~ 10X. In D-D reactors this ratio at 100 KeV would be closer to ~ 100-1000, but not much more. Again, mechanism to prevent, or at least retard the thermalization process is nessisary. I have discussed two of the methods, and touched on a third.
You also seem to be stuck on beam- beam or beam- target fusion concepts where there is only one (or a few) chances for fusion collisions befor the beam energy is dispersed or absorbed into the target. While the Polywell is ideally a beam - beam machine. It is definity not a coherent* two opposing beam machine. The spherical geometry and the potential well means that basically you do not care if there is dominate Coulomb scattering over fusion ( thermalization concerns are present, but cooling concerns are negligible). The ions will scatter, but due to the potential well and the spherical geometry they (almost) always return for another try. This is obvous for anybody who has studied gridded fusors. . The difference with the Polywell is that the ions might have many thousands, or even millions of passes, where gridded fusors at best only ave <100 tries, and beam- beam, or beam- solid target systems only get essentially a few tries. before they lose their energy.
Comparing Tokamak physics to claimed Polywell physics is of course perfectly legitimate, but using Tokamak assumptions and applying them to Polywells is like comparing a vulture to a hummingbird. They both obey certain rules, but they achieve and maintain flight in different ways.
*POPS effects might chang this somewhat, but again in a spherical framework, not a collumated beam arrangement.
Dan Tibbets
To error is human... and I'm very human.