Peter and Jones--

Spin flipping may be a coupling mechanism to create phonic vibrations and heat. 
 However what is the source of energy causing the spin flipping? 

You suggest it may be gluon mass loss.  I would agree, and it shows up as a new 
nuclei in the coherent system where flipping occurs, with lower binding energy 
reflecting the loss of gluons and rest mass of the new nucleus.

We need instrumentation to monitor spin flipping to test the theory.  Measuring 
gluon loss is hard.  However NMR may be able to identify the growth of new 
nuclei that appear in the reactor with time.  

The ability to shutdown and restart may allow such NMR measurements with fuel 
depletion. 

Bob Cook


From: Peter Gluck 
Sent: Tuesday, June 23, 2015 7:55 AM
To: VORTEX 
Subject: Re: [Vo]:Resonance in a ceramic tube reactor



Thanks for this answer! 
Peter

On Tue, Jun 23, 2015 at 4:28 PM, Jones Beene <[email protected]> wrote:

  From Peter Gluck’s blog


  "Identifying the Problem is a crucial step"


  There’s been discussion about resonance, coherence and cavity oscillators in 
the context of the Hot-Cat. The related question is whether the ceramic tube is 
required for some unknown reason, and if so – can it can be optimized by 
geometry? Obviously, thermal stability is one benefit of ceramics. Since Rossi 
has used at least three different form factors with the Hot-Cat, and the 
claimed COP has gone down instead of up - according to his own statements – he 
may have downplayed the issue of resonance (due to cavity oscillation) as being 
harder to control at high temperature.


  But there could be a place for a resonant reactor design in a lower 
temperature regime. One detail worth noting, in the design of any hydrogen 
reactor when the goal is achieving resonance, is identifying the kind of 
resonance. It would be a mistake to assume that only EM resonance is the answer 
to the problem. Phonon resonance is arguably more important in LENR - the 
entire subfield of sonofusion is built on phonon resonance. Magnetic waves will 
be assumed to be a subset of phonon resonance.

  It would be ideal to match up the two– phonon (magnon) and photon wavelengths 
– and arrive at a resonant standing wave design which is mutually reinforcing. 
In fact, the general size of these reactors is one of the few possible ranges 
where EM waves and sound waves can reasonably share a common wavelength – and 
there is one candidate that stands out – 21 cm. Larger and smaller geometries 
are harder to match.

  One way to think about this is by example. Let’s say we want to exploit a 
known resonance level for hydrogen. The ultimate goal doesn’t need to be 
fusion, necessarily, and we should assume that protons in resonance can better 
achieve thermal gain in several different ways – such as through manipulation 
of electron angular momentum, or the zero point field, or sequential Lamb shift 
(QED), or QCD mass depletion of gluons, etc. (the usual suspects). 

  The most notable resonant wavelength for hydrogen is 21 cm- the Universe is 
bathed in microwaves of this and similar frequencies – the CMB. With this 
glaring fact all around us, it could be no accident that the axial dimension of 
the E-Cats is in this range. Is that merely luck, or was it planned that way?

  In the case of the Lugano device, we should be more likely to achieve EM 
resonance for hydrogen if a larger diameter tube was to be implemented (say 
quarter wavelength, or 5.25 cm.) The “pre-Lugano” hot cat was indeed  in this 
diameter range and also had a higher claimed COP. Why change? (possible answer: 
going smaller to avoid runaway) 

  
http://4.bp.blogspot.com/-XuKgtxpqL9U/UYQSyPJP-OI/AAAAAAAAJYI/96mRUBJjs1w/s1600/hot-cat.JPG


  This 21 cm wavelength corresponds to GHz photon radiation (1420 MHz) but 
apparently no one has seen this kind of radiation in the Lugano or other 
similar experiments. GHz radiation would promote the Lamb shift, which is one 
of several ways that thermal gain could enter the system. Any competent 
research team would have looked for GHz because of the negative health issues – 
and we can be fairly certain none was seen or used, since at any rate, alumina 
will not contain or reflect microwaves in this range.


  One of the most respected physicists to support cold fusion was Julian 
Schwinger, whose name is associated with the Lamb Shift and QED. Microwaves 
would be ideal to maximize a sequential Lamb shift spin-flip reaction, in a 
hydrogen reactor, but curiously – have not been considered relevant in the 
past, since the energy per “flip” is very low - and the reverse reaction may 
not be asymmetric in a closed loop system. 

  Few theorists have reasoned that a "ringing-Lamb-shift" which would be 
happening at THz frequency and is asymmetric – powered by the zero point field 
– is feasible, since it is a different beast from fusion – the default 
assumption. However, the net energy derived spin-flipping could be substantial 
- even larger than "normal" nuclear energy since there is no dependence on the 
mass of reactants. Several prominent names turn up in LENR history for past 
advocacy of a Lamb shift modality, instead of fusion, but it is a definite 
minority view. 

  In a future post, it will be shown that the same 21 cm wavelength for 
hydrogen photon emission due to spin flipping can be achieved at an ultrasonic 
frequency for phonons. This ultrasound would be in the 25kHz to 50 KHz range 
(predicated by the speed of sound in the media). In the simplest case, this 
frequency is available using SCRs… which can be seen in many Rossi photos. 
Coincidental?

  All of this leads in to the question of the day for revisionist LENR theory. 
If 21 cm radiation can be shown to stimulate an asymmetric Lamb shift, can 
phonon (magnon) waves of the same wavelength do the same stimulation with no 
photon component? Or alternatively, why not use a steel sleeve and heat the 
reactor internally with low power 1420 MHz radiation (tens of watts) looking 
for gain at a more modest temperature?






-- 

Dr. Peter Gluck 
Cluj, Romania
http://egooutpeters.blogspot.com

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