KitemanSA wrote:Joseph Chikva wrote: Also, almost all tritium nuclei will react with deuterium giving 17.6MeV per event.
This is an interesting thought.
For many years this forum assumed that the alphas from the pB&J would exit the MaGrid immediately. The same assumption was held, AFAIK, regarding the fusion products from the WB6 D-D reaction. A comment by Dr Nebel lead to further examination regarding the alphas in a 7T level field and lo-and-behold, they DIDN'T exit the MaGrid immediately but bounced around a bit and left only nearer the cusps.
Has anyone done an equivalent assessment of the products of the WB6 level fields with its products? Are we WRONG to assume each D-D reaction yields HALF a neutron when it might also result in a D-T reaction that produces one?
Hmmm, maybe the D-D reaction rate is half what we've assumed by neutron count, but it is accompanied by a D-T half the time which makes a neutron ALL the time.
More math to do boys! Git bizzay!
So...
(15KeV)D+D = 50% T(1.01MeV) +P(3.02MeV) and 50% 3He(.82MeV) + N(2.45MeV)
and...the New T's AND P's running around at 50% the fusion rate means possibly...
(13.6KeV)D+T = 4He (3.517MeV) = n (14.069MeV)
P+P = D + (e+) + (v sub e) + .42MeV (But this chain produces about nil for power density...think our sun...so we can ignore it)
and possibly a little...but not likely at 58KeV, so we can discount it...
D+He = He4(3.6MeV) + p(14.7MeV)
and note the D from P + P, which in turn can chain some more...
(15KeV)D+D = negligiable power
and
(13.6KeV)D+T = negligiable power due to low input D count from P+P reaction
So overall, it would seem we can get a decent secondary chain from the initial T products acting within the D fuel construct.
In summary:
(15KeV)D+D = 50% T(1.01MeV) +P(3.02MeV) and 50% He3(.82MeV) + N(2.45MeV)
and a viable secondary chain of:
(13.6KeV)D+T = He4 (3.517MeV) + n (14.069MeV)
means that (detector dependant) for every neutron we see on a counter, it could be a D+D neutron OR a D+T neutron.
So, now we need to look at the cross sections and see how the barns stack up for the distribution probability. But without number crunching, the fact that D+T is easier than D+D, should mean to me that we would not see much of a T population accruing in a D+D machine, as it would most certainly burn off. So for arguments sake, we should see 2 neutrons for every one D+D event. But that also means that the power produced must also account for the double burn of the D+D and the D+T secondary.
On simple terms: 2.5E9 DD fus/sec should be about 5mW, not counting unburned fuel that escapes confinement.
Following on, this line of thought would argue that in a machine counting x neutrons, 50% of DD produces a n count, and the other 50% produces a T which then (assumed 100% burn) produces another n. So, that would say that every D+D makes 2 neutrons. Thus, the initial DD fusion rate is 50% of the neutron count, but then one must also account for additional energy produced by the T secondary.
In our case we thought initially that the WB6 machine produced 1.46mW, whereas looking at it this way, it produced 5mW.
2.5E9 fus/sec
1.25 T+p events/sec for a total of 5.04E15 in energy
1.25 He3 + n events/sec for a total of 4.09E15 in energy
and secondary
1.25E9 He4 + n events/sec for a total of 2.2E16 in energy
which gives
3.11E16 in total energy, converted to Watts gives
.005 Wattsecs
or
5mW
Thoughts?
This, if I am not mistaken, also means that Joel Rogers did his math wrong in his latest paper at IEC 2011.
The development of atomic power, though it could confer unimaginable blessings on mankind, is something that is dreaded by the owners of coal mines and oil wells. (Hazlitt)
What I want to do is to look up C. . . . I call him the Forgotten Man. (Sumner)