DCE, PEC and TiH2Jones--

If I understand the crux of your theory, there is a phase change going on that 
harvests energy from some source.

In the cases where a plasma is apparent, what is the nature of the phase change 
you indicate is happening?  

Maybe the “plasmas” in some of the active experiments are really charged 
nano-scale particles, big enough to exhibit phases and stay together during 
changes.  The same sort of thing may happen in a large molecule with changes 
associated with the left-right-handedness induced by a  resonant magnetic or 
electric field.  

There might be a nuclear source of the extra energy as well as your suggestion 
of the creation of virtual photons by DCE.   

me356’s Vortex-l email this morning is interesting in this regard—particularly 
the purple glow in his quartz see-in reactor.  It seems like there may be a 
resonance of some sort there.   Me356 notes that it does not happen without 
tuning his control, whatever that is?

The art of LENR is all important!

Bob Cook 

From: Jones Beene 
Sent: Sunday, May 01, 2016 2:23 PM
To: [email protected] 
Subject: RE: [Vo]:DCE, PEC and TiH2

One interesting detail to add: It is somewhat outrageous to imagine that 
cyclical loading/unloading of hydrogen into a hydride storage metal such as 
palladium - and that alone - can cause temperature increase in both directions.

Mainstream physics, and most hands-on experimentation, teaches that there is 
symmetry and that conservation of energy prevails in such a common system - and 
that exotherm on loading is balanced by endotherm on unloading.

But here is a understated paper found by Jack Cole, from a couple of years ago 
where George Miley, Xiaoling Yang and their postgrads at Illinois-Urbana manage 
to easily find and document a massive and glaring asymmetry with 
loading/unloading of deuterium in palladium… and hello… somehow the mainstream 
of physics manages to ignore the profound implications. Go figure.

http://www.lpi.usra.edu/meetings/nets2012/pdf/3051.pdf

----------------------------------- 

This is the first part of a formative hypothesis for anomalous thermal gain, 
which explains terminology and acronyms but does not dig deeply into Holmlid’s 
past work, nor into Mills, but instead presents a hybridized alternative to 
thermal gain. The gain is ostensibly non-nuclear so long as the laser is not 
used.

The dynamical Casimir effect, DCE - is a proved relativistic effect of 
nanoscale geometry. It was first demonstrated in 2011 as a mechanism for 
anomalous energy gain involving photons being “created” (from virtual photons). 
Heretofore that type of gain has been too small to use in a practical device. 
Curiously, the DCE was first seen in Gothenburg, the home of Leif Holmlid, but 
the Professor has not yet seen the connection of DCE to hydrogen densification 
- nor to excess energy which will be presented here. This proposed route does 
not involve a vacuum or the laser per se, but is a new route using what is 
called PEC and would be powered by DCE.

PEC is short for photo-electric-catalysis and is one of the hottest topics in 
chemistry these days, thanks to nano-geometry. PEC has been most often used to 
split water using solar radiation, but that is the tip of an iceberg of 
applications. PEC - at least as it will be used in this hypothesis, can be 
employed without vacuum condition - as the major pathway for hydrogen 
densification, leading to UDH or to an intermediate form of f/H (fractional 
hydrogen) operating in the gas phase (as opposed to plasma phase). PEC is 
boosted by the surface plasmon polariton, or else is intrinsic to SPP – but 
operates without the substantial ionization necessary for Mills version - which 
means low temperature operation. 

TiH2 is the nominal hydride of titanium when fully loaded, but the average 
amount of hydrogen per atom of Ti can vary substantially, causing major 
structural changes and stress in the packing arrangement of the crystal 
structure as the ratio changes. TiH(1.95) is a typical ratio as supplied 
commercially. Note that with palladium, the loading of hydrogen almost never 
gets to a full 1:1 but with Ti it is relatively easy to get to 2:1, but the 
important thing is that phase-change accompanies the various ratios, and this 
has profound thermal repercussions without invoking nuclear reactions.

TiHx approaches stoichiometry as TiH2 and it wants to adopt a distorted 
body-centered tetragonal structure but there are at least two other phase 
structures “competing for space” along the way, and in a narrow range. At 
ratios of H:Ti which are between 1.5:1 and 1.9:1 this crystal can become 
unstable with respect to isothermal decomposition (dehydrogenation). The 
crystal can rapidly decompose even at room temperature until an approximate 
composition of TiH(1.74) is reached. Normally dehydrogenation is endothermic 
but some of the phases of titanium hydride are unique, and this points to 
eventual asymmetry. 

If there is an intrinsic asymmetry in titanium hydride, in sequential cycles of 
loading-unloading, and one unloading is isothermal but the loading is 
exothermic, then the stage is set. Gibbs “free energy” for the first time 
becomes really free. There can be a further boost in the exotherm of loading – 
if and when UDU expands on loading.

It is worthwhile to take a moment to reintroduce “recalescence” as a known 
example of an surprisingly intense thermal anomaly of certain hydrides. 
Recalescence is related to rapid phase-change in a few alloys with soaring 
temperature gain. It was known to happen with Pd systems going back to the age 
of the Zeppelin, since one Pd-Ag alloy was used in hydrogen purification which 
can heat up drastically– igniting hydrogen. 

https://en.wikipedia.org/wiki/Recalescence

Note that with recalescence there is the prospect of getting equivalent 
chemical energy of approximately an eV per atom - via hydride ratios, but with 
no redox reaction or other chemical change. As to what it takes to introduce 
asymmetry into the equation, so that that DCE can become active, that will be 
the focus of the next part of this hypothesis.

Jones 

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