On Oct 8, 2009, at 6:58 PM, [email protected] wrote:

In reply to Horace Heffner's message of Thu, 8 Oct 2009 13:02:07 -0800:
Hi,
[snip]
If the D(D,gamma)He4 branch is highly favored and the D(D,p)T and D
(D,n) He3 reactions highly suppressed, it is reasonable to expect the
lower energy branches are being energetically suppressed by a lack of
energy to make them feasible.
[snip]
He4 is far more stable than either He3+n or T+p, and the only reason that it doesn't form all the time is because the excited He4 nucleus doesn't have any fast energy removal channel available to it (quadrupole gamma radiation is very slow compared to energy loss via a fast particle). That means that the excited nucleus usually breaks up releasing the energy as fast particles long before the
gamma ray could dispose of the energy.

However in your deflation fusion model there is *always* an electron present in the newly formed He4* (because that's what catalyzed the reaction in the first place). There is therefore nothing to hinder the formation of He4 by disposing of the excess energy as kinetic energy of the electron, which has to be expelled anyway. That neatly explains the change in branching ratios without resorting to
any exchange with the ZPE.

Your assertion demonstrates the diagnostic importance of tritium doping to determination of the reaction mechanism. The correlation of heat with He4 is difficult due to the difficulty of measuring the total amount of He4 produced, and specifically the amount remaining in the lattice. See:

http://lenr-canr.org/acrobat/Hagelsteinnewphysica.pdf

Which, for example, states:

• The rate of helium production (atoms/s) varies linearly with excess power (see Figure 6). • The amount of helium observed in the gas stream is generally within a factor of about 2 less than would
be expected for a reaction mechanism consistent with D+D → 4He.
• Helium is partially retained, and dissolved helium is released only slowly to the gas phase for analysis.

It simply is very difficult to establish with high sigma results whether energy is produced at 23.8 MeV or 18.8 MeV per He4, or something in between.

In the case of the fusion reaction:

   D + T -> He4 (3.5 MeV) + n (14.1 MeV)

it is much easier to determine if the energy spectrum of the neutrons, which result from every such reaction, is consistent with a mean of 14.1 MeV. I think there is in fact some indication that the neutrons resulting from cold fusion are considerably less than 14.1 MeV on average. This is because only a few percent are above 9.4 MeV. It remains for the spectrum to be nailed down. I think this is the most important experimental work at hand.

There is also the theoretical question of whether the electron is capable of radiating away the energy released by the strong force when the helium nucleus is formed. It strikes me as likely in ordinary D-D hot fusion that an energetic helium nucleus is momentarily formed prior to the release of either a proton or neutron. That means the nucleus momentarily contains the full 23.9 MeV of a D-D fusion heat, of strong force binding of the deuterons. The breaking of strong force bonds, fission of the He4*, to release an n or p then saps away some of that heat. In the case of D(D,p)T the energy required to fission off a proton is 23.9 MeV - 4.03 MeV = 19.87 MeV. In the case of the D(D,n)He3 reaction the fission energy to produce the neutron is 23.9 MeV - 3.27 MeV = 20.63 MeV. This results in the classic hot fusion energies:

D(D,p)T   4.03 MeV
D(D,n)He3   3.27 MeV
D(D,gamma)He4   23.9 MeV

Now, if a small electron is present in the fused nucleus, the nucleus kinetic energy is reduced a priori, the nuclear temperature is reduced. The energy of fusion does not have to be radiated away. No time is required for photon creation, or for that matter neutrino creation or any other weak reaction, prior to the He4* nucleus fission. The heat is simply not there to begin with. The amount of energy so removed from the He* depends on the wavelength of the electron at the moment of wavefunction collapse, so is a stochastic variable.

I think only the D-T reaction energy data can be expected to provide a precise answer to what mechanism is at work in cold fusion.

Best regards,

Horace Heffner
http://www.mtaonline.net/~hheffner/




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