ZapperZ said:
Again, this has produced no new concepts or even addressed the original set of problems that I laid out in another thread on accelerator-driven fusion reactor. Those of us who work in accelerator systems, and as someone who is also familiar with the beam dynamics of a synchrotron center, we simply shake our heads when something like this is being proposed. It appears that these things are thought up by people who are not working in this field.
I reviewed some of the older threads to which you refer and it appears that part of the issue is nomenclature: the word accelerator in your context means nothing less than a GeV or TeV particle smasher, with large (m or km) mean free path. Fair enough, 'accelerator' is so defined. Certainly that type of apparatus has no practical application to fusion.In the links on
confinement I posted above, 'accelerator' refers merely to accelera
tion, as in F=m
a where the F is typically provided by a kV sized electrostatic field applied to charged particles, and appropriate for nuclear coulomb barriers.
A Tokamak certainly has never been classified as an accelerating structure.
Agreed, a Tokamak is a completely thermal device in concept and has almost nothing in common with electrostatic acceleration inertial confinement (IEC) fusion approaches to which I refer. Now, IEC does have much in common with 'accelerators', or particle smashers as many of the physics issues you reference below here still obviously apply to these kV confinement cases:
1. Luminosity problems. To get any significant "fusion", you need a large number of collisions. This is the "luminosity" issue that even places like the Tevatron faced. It is very hard to do this with neutral particles such as neutrons because you can't direct them to where you want to go. If you do this with protons, god help you because...
2. You will need a LOT of protons, and thus, you encounter SPACE CHARGE problems. Since you want to tightly confine the protons to a very thin beam (to increase the luminosity), you encounter A LOT of space charge problems that simply want to blow up the beam, thus reducing your luminosity
Electrostatic confinement concepts use deuteron's, tritium, He3, or even p-11B because of the much greater fusion reactivity cross section (just as in Tokamaks of course).
Luminosity and space charge are issues here as well (density is the common term in the referenced literature, but perhaps luminosity is more apt as its still beam physics that apply). Hence, some degree of neutrality is usually proposed by inclusion of electrons. If the electrons are allowed to thermalize w/ the ~50kV ions they radiate all the power way, so clever schemes have been proposed to prevent this (unrealized so far) such as keeping the electron life times short, etc.
4. If you want to fuse protons (which is one of the silliest thing to do for a fusion reactor), you will need collide them at such a high energy that you will require accelerating structures powered by klystrons, etc.. This will simply KILL your wall-plug efficiency. In other words, the energy you get out of the fusion reaction is LESS than the energy you put in in the first place. Transferring RF power from a klystron to a structure can be highly inefficient, and large accelerator complex requires several of these things to power a number of LINACs.
Again nobody is trying to fuse protons in my references, and drive power is provided by the electrostatic field for my cases, not much mention of RF though there's some resonance inducing attempts via RF.