The interesting for me to note is that the non square integrable feature of
the Dirac
solution is perhaps a key feature, It can (I'm not an expert) mean that you
generally do not see single live hydrinos but clusters of hydrogen that
take advantage of x number of hydrino states to keep the cluster bounded by
demanding the hydrinos to have a non localized part. The main effect would
then be a BEQ like state that could be the main driving force to generate
energy. But a certainly a few hydrinos could escape and keep that state for
so long to do other nuclear reactions as the paper you showed suggested. I
would also not expect these clusters to live long because they would
trigger a nuclear reaction as Kim suggests and due to the energy release
break up.

Does this make sense?


On Thu, Jan 16, 2014 at 5:14 PM, Jones Beene <[email protected]> wrote:

>  A number of observers have observed this “deep Dirac” (DDL) layer to be
> the real source of Mills’ “hydrino” since it is similar in ways - but not
> the same - and its presence leads to a nuclear reaction. (which is a
> drastic departure from Mills).
>
>
>
> See Meulenberg,
>
>
>
>
> http://newenergytimes.com/v2/conferences/2012/ICCF17/papers/Meulenberg-Femto-Atoms-And-Transmutation-ICCF17-ps.pdf
>
>
>
> The other alternative which I have been promoting is the DDL as the
> predecessor state to RPF (reversible proton fusion).
>
>
>
> RPF (diproton reaction) would provide a smaller amount of energy (much
> smaller than fusion) via QCD color charge dynamics from excess proton mass,
> but with no fusion.
>
>
>
>
>
> *From:* Stefan Israelsson Tampe
>
>
>
> BLP being real or not, here is something that I find intriguing,
>
>
>
> http://arxiv.org/abs/physics/0507193
>
> QUOTE
>
> The Klein-Gordon equation of the hydrogen atom has a low-lying eigenstate,
> called hydrino state, with square integrable wavefunction. The
> corresponding spinor solution of Dirac's equation is not square integrable.
> For this reason the hydrino state has been rejected in the early days of
> quantum mechanics as being unphysical. Maybe it is time to change opinion.
>
> UNQUOTE
>
>
>
> Can we spin on this? Note
>
> 1.  Not being square integrable means probably that the wave function has
> "thick tails" and that it basically describes a non-localized electron that
> happens to get close very very seldom. E.g. quite an unlikely state.
>
>
>
> 2. Solutions to Klein Gordon equations is most probably a combination of
> spinor states for which the thick tails cancels. This may mean that you can
> have a hydrino state, but it's basically impossible to reach it because it
> depends on a delicate balance.
>
>
>
> But what if we combine a cluster of N hydrogen atoms, what happens then?,
> well we could view this as a possibility to bend the space into a compact
> manifolds of various forms and for applying these states on that system,
> one could perhaps trigger the formation of these hydrino states, for that
> case one would expect the electron will be partly bound closely, more
> closely than ordinary hydrogen but also have a component of delocalisation
> e.g. an affinity for the system to behave as a strongly coupled system just
> as with a BEQ state.
>
>
>
> So assuming the active sites have an ability to catalyze clusters of
> hydrino clusters, the next step to take is to note that for these hydrino
> clusters that could very well be close in nature to BEQ clusters, but more
> combact due to the close proximity of the electrons to the nucleus, the
> mechanism Kim describes could very well trigger nuclear reactions.
>
>
>
> At least that's my 2c of what's happens.
>
>
>
> Have fun!
>
>
>
>
>
>
>
>
>
>
>
>
>
> On Thu, Jan 16, 2014 at 4:20 PM, Jones Beene <[email protected]> wrote:
>
> In earlier BLP filings - on what constitutes a hydrino catalyst, it turned
> out to be possible to fit two thirds of the periodic table into their
> expansive definition. Talk about “over-reaching” …
>
>
>
> USPTO examiners detest these painfully long and over-reaching
> applications. Many observers have commented on how poorly worded BLP’s
> efforts turn out - and how little value they actually have in defensible
> IP, having paid top dollar for poor work. BLP will probably not fare well
> if it ever comes to litigation.
>
>
>
> A few years ago it was noted here that the company had overlooked “gas
> phase” in all of their voluminous filings – that is, up until Rossi’s
> patent application showed up in which his claim was for only gas phase… at
> which time BLP altered a previous filing, once which had only claimed
> liquid and plasma phase, to include gas phase. It was obvious that they
> were trying to cover up a glaring mistake in coverage.
>
>
>
> I suppose that they were hoping no one would take notice, but instead the
> effect was to announce to the world how badly they had screwed up.
>
>
>
> *From:* David Roberson
>
>
>
> It appears to me that they have most of the possible current levels
> covered.  Why list ranges that include each other?
>
> Magnetic fields that are changing in magnitude or direction generate
> electric fields that can impart energy upon charged particles.  A steady
> magnetic field is not able to supply energy to these charged objects, but
> can change their direction of motion.
>
> Dave
>
>
>
>
>
>
>
> -----Original Message-----
>
> The BLP website is down as I write this, but yesterday the
>
> "What’s New" tab on their homepage led to this entry dated 1/14/14 -
>
>
>
> Patent Application – Power Generation Systems and Methods Regarding Same.
>
> http://www.blacklightpower.com/wp-content/uploads/presentations/Power%20Generation%20Systems%20and%20Methods%20Patent%20Application.pdf
>
>
>
> I am unsure whether this untitled 324 page document is an existing
>
> patent application, one just submitted, or is pending submission.
>
>
>
> What I found especially interesting is that it credits the anomalous
>
> energy generation, and hydrino formation to an extremely wide range of
>
> plasma currents, and current pulse widths.  For example, on p.107,
>
> the following excerpt appears -
>
>
>
>
>
>   "The current density may be in the range of at least one of
>
>   100A/cm^2 to 1,000,000 A/cm^2, 1000 A/cm^2 to 100,000 A/cm^2,
>
>   [...]
>
>   The pulse time may be in at least one range chosen from about
>
>   10^-6 s to 10s, 10^-5s to 1s, 10^-4s to 0.1s, and 10^-3s to 0.01s.
>
>   [...]
>
>   The magnetic flux may be in the range of about 10 G to 10 T,
>
>   100 G to 5 T, or 1 kG to 1 T."
>
>
>
>
>
> The huge current densities and sharp rise/fall times should create
>
> very large magnetic forces that, if focused, impart huge momenta
>
> and energies to charged particles that are in, or impacted, by the
>
> plasma current filaments.
>
>
>
>
>
> Possibly, BLP's upcoming demo will be a more systemic version of
>
> the 1922 Wendt-Irion experiment that vindicates W-I's conclusions?
>
>
>
> -- Lou Pagnucco
>
>
>
>
>
>
>
>
>

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