On Feb 27, 2011, at 12:32 PM, [email protected] wrote:

In reply to Horace Heffner's message of Sun, 27 Feb 2011 00:28:04 -0900:
Hi,
[snip]
Ni has roughly the following isotopes/percentages:-

Ni-58   68%
Ni-60   26%
Ni-61    1%
Ni-62    4%
Ni-64    1%

If 30% of the Ni is converted to copper over the long term, then
it's possible
that it's just the heavier isotopes that are reacting and that
Ni-58 is not
involved.

It does not look to me to be credible that this happens, unless maybe
very large hydrogen clusters are involved - and that is not credible
for a mechanism that is so effective it can consume 94% of the
available consumable isotopes and convert all that to copper.

The main problem lies with 60Ni28.  Looking at every strong force
reaction energetically feasible involving 4 or fewer protons:

60Ni28 + 2 p* --> 32S16 + 30Si14 + 00.554 MeV [-16.327 MeV] (B_Ni:2)
60Ni28 + 2 p* --> 34S16 + 28Si14 + 1.530 MeV [-15.351 MeV] (B_Ni:3)
60Ni28 + 2 p* --> 50Cr24 + 12C6 + 00.365 MeV [-16.516 MeV] (B_Ni:4)
60Ni28 + 2 p* --> 58Ni28 + 4He2 + 7.909 MeV [-8.973 MeV] (B_Ni:5)
60Ni28 + 3 p* --> 32S16 + 31P15 + 7.851 MeV [-18.205 MeV] (B_Ni:6)
60Ni28 + 3 p* --> 35Cl17 + 28Si14 + 7.901 MeV [-18.155 MeV] (B_Ni:7)
60Ni28 + 3 p* --> 36Ar18 + 27Al13 + 4.823 MeV [-21.233 MeV] (B_Ni:8)
60Ni28 + 3 p* --> 39K19 + 24Mg12 + 5.135 MeV [-20.921 MeV] (B_Ni:9)
60Ni28 + 3 p* --> 40Ca20 + 23Na11 + 1.771 MeV [-24.285 MeV] (B_Ni:10)
60Ni28 + 4 p* --> 32S16 + 32S16 + 16.715 MeV [-18.997 MeV] (B_Ni:11)
60Ni28 + 4 p* --> 36Ar18 + 28Si14 + 16.408 MeV [-19.304 MeV] (B_Ni: 12) 60Ni28 + 4 p* --> 40Ca20 + 24Mg12 + 13.464 MeV [-22.248 MeV] (B_Ni: 13)

You seem to have not included the reactions involving 1 proton.
Consider that if your own model is correct, then the likely result of 1 proton fusion is first a fast strong force mediated fusion, followed by a "slow" weak force mediated capture of the trapped electron. However the "slow" weak force reaction is still likely to be have a much shorter half life than the usual positron decay reaction because it has a 1 MeV advantage (2 electron masses) and the electron is already trapped, so the nucleus doesn't need to wait for the occasional appearance of a K shell electron (which IMO is what usually make EC
less likely than positron decay).
The normal half life of 61Cu29 is 3.3 hours (the energy of the decay is 2.2 MeV), so if this is enhanced (the decay energy increases by at least 50%), then we could be looking at mere seconds, or perhaps even much less than that if the nucleus is still in an excited state due to the proton fusion. (There is a rough
correlation between decay energy and half life.)

It's very possible that a similar logic applies to any of the shrunken species
under consideration.

BTW another possibility with clusters is direct conversion to Zn (or even
higher) with no Cu intermediary.


there appears to be no energetically feasible reaction that can
produce copper from 60Ni without creating radioactive nuclei.

True, but the half-life could be very short. However that still leaves the "problem" of gamma radiation, unless the new nucleus is either formed in the ground state or has a faster energy disposal mechanism available than gamma
radiation.


Actually, according to deflation fusion theory, there is an initial energy deficit of around 4.84 MeV that would suppress the initial gamma:

  60Ni28 + p* --> 61Cu29 * + 4.801 MeV [-4.840 MeV]

So, I don't see that as a problem. The problem to me is the lack of any evidence that heavy element LENR ever results in radioactive nuclei. Maybe this would be a first.

The 61Cu29 decays to 61Ni29 in 3.333h, but the 4.84 MeV trapped electron may stimulate that immediately. Now we are back to copper with:

  61Ni28 + p* --> 62Cu29 * + 5.866 MeV [-3.722 MeV]





The close proximity of many other "free" particles (as in a cluster),
could provide a means of rapidly disposing of the energy as kinetic energy of the particles rather than as gamma radiation, or could also mean that the newly
forming nucleus can go directly to the ground state by ejecting fast
particle(s). The latter may technically also be considered a form of
fusion/fission, though not one commonly considered, particularly as some of
those fast particles may be electrons.

However we don't know for sure that no gamma radiation was produced during the run that resulted in 30% Cu. This is especially so, considering that Rossi includes a Pb shield, so he certainly expects it, which in turn seems to imply that he has previously detected it (not to mention that has said that it is
present in some places).

Same
is true considering weak reactions, which take an extra 782.353 kEv
away. If radioactive nuclei are created then some will remain in the
leftover material, but it was denied that there was any such
radioactive "ash".

See above re. half-life. Consider the situation where the heavier Ni isotopes are the first to transmute. Ni-64 goes directly to Cu-65 and stays there. Ni-62 goes directly to Cu-63 and stays there. Ni-61 goes (perhaps much more slowly) to Cu-62 which rapidly decays to Ni-62, which then has a better chance of proton fusion, so it converts to Cu-63. Slower even still to capture a proton is Ni-60, which converts to Cu-61 (decays to Ni-61; and follows on from there). Slowest of all to capture a proton is Ni-58, which barely manages it, resulting overall in
roughly a 30% conversion to stable Cu.

58Ni creates 59Cu:

   58Ni28 + p* --> 59Cu29 * + 3.419 MeV [-6.329 MeV]

59Cu positron decays in 81.5 s (normally) to 59Ni which has a 76,000 yr half-life.

I believe there was a statement by Rossi that there was no residual radiation, so this should rule out 59Ni in the leftovers.

However, it may be a reasonable hypothesis that the initially trapped electron (by 6.329 MeV deficit) stimulates the nucleus to the point where 59Co is created quickly from the 59Cu. Now we can have:

   59Co27 + p* --> 60Ni28 + 9.533 MeV [1.588 MeV]

but we have now moved up the ladder sufficiently to convert everything to copper. This reaction might produce 1.588 MeV gammas by the way. Non-radiating alternatives might be:

   59Co27 + 2 p* --> 60Ni28 + 1H1 + 9.533 MeV [-6.856 MeV]
   59Co27 + 3 p* --> 58Ni28 + 4He2 + 17.441 MeV [-7.881 MeV]

The key question I think is whether the initially trapped electron has the kinetic energy to stimulate a very short half-life of a radioactive composite nucleus. Clearly it does! The trapped electron *initially* has the kinetic energy it had when it was in the very small deflated hydrogen state, a very high kinetic energy, low potential energy. This explains why radioactive products are not observed from heavy element LENR, at least not from the simple single decay elements that have been experimentally involved. This may not be true of very heavy elements like those in the actinide decay chain, for example. This could be a very interesting line of research concerning nuclear remediation.




This sort of scenario is not unreasonable because the most stable nuclei are those that are close to the middle of the isotope range for any given element, hence neutron heavy isotopes are more likely to "want" a proton than neutron
light (or "proton rich") isotopes.
[snip]
Regards,

Robin van Spaandonk

http://rvanspaa.freehostia.com/Project.html


Best regards,

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




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