| Exactly, but the fuel cycle is actually more subtle than that: When compressing the D+He3 plasma, inevitabily some D will also fuse together. And since one in two D+D reaction yields He3+n, if you fine tune the proportion D/He3, the D+He3 reaction will in total (ie taking into account the D+D side reaction) produce more He3 than it consumes. But D+D also yields T+p, and T eventually decays into He3 (T half life is 12.5 years) The total fuel cycle has 3 fusion reactions: D+He3 -> He4 + p (50%) D+D -> He3 + n (25%) D+D -> p + T (25%) (T=He3, after decay) As you can see the only input is deuterium. The thing is that you want to avoid D+D -> He3 + n because 1. It produces less energy 2. It produces neutrons that damages your machine. Hence the proposal of splitting the fuel cycle in two reactors, one doing the clean and powerful D+He3 and the other doing the dirty D+D. So one reactor will consume He3 and the other will produce He3 in excess. |
What you want to avoid is D + T on the T generated from the other D + D reaction. In Helion's scheme, I believe the ions do not equilibrate during a pulse, so that tritium doesn't slow down before the plasma reexpands and is exhausted to the divertor. The DT fusion cross section peaks around a 60 keV center of mass energy, so keeping the T energetic can reduce its fusion rate somewhat.
This is another reason to have "field reactors" burning 3He generated elsewhere, with a high 3He/D ratio. The lower D concentration reduces DD reactions, but it also reduces DT reactions on any T that are produced.
There's an additional problem of purifying and reusing the D in the exhaust of the machines. You don't want to have to filter out all the tritium from this before every cycle. It's possible the field machines could have many go-arounds of this gas before sending the sufficiently contaminated D back to be filtered (or used in the dirty DD machines).