On Fri June 7th Axil said [snip] Why does a Ni/H reactor form a Bose-Einstein condensate throughout its entire volume? STANIS LAW J. SZAREK provides the answer; the dipoles throughout the reactor are forced to become totally entangled when the percentage of dipole entanglement exceeds 20%. [/snip]
Axil, Does this mean that 20% of the hydrogen must be in a redundant ground state, F/h? On one hand it seems like the confinement must be small and conductive to fractionalize but on the other it must reach 20% of the gas to reach entanglement... I keep going back to a relativistic interpretation of casimir effect and Naudt's relativistic explanation of the hydrino to fit the requisite percentage of atoms into a space that appears too small from our macro perspective.. My posit is that hydrogen fractions approaching h/137 see the macro world as slow moving as we see the Paradox twin orbiting an event horizon.. I chose the equivalent acceleration of the black holes gravity well instead of near luminal velocity of an object because it is nearer the situation inside the NAE where fractional hydrogen acting as a local observer sees itself at the top of a gravity well where the bottom of the well is the macro world outside the NAE. My posit is that vacuum engineering at the nano scale via suppression is free and far easier than modifying the isotropy with velocity or gravity wells at the macro scale, It is still partially subject to square law but is trumped by Casimir effect in this geometry - I think there is also some inherent advantage in "shielding" a zone from longer vacuum wavelengths in that you are segregating a reservoir that wants to equalize without pouring any energy into the construction, it sets the stage for us to employ gas as the mediator between the reservoirs of different potentials present inside the cavity.. like Rossi's tubules the geometry should form a tapestry of different suppression levels. I suspect that f/H2 takes on different values proportional to the tapestry dimensions where the h atoms first associate. As these fractional molecules disassociate and quickly reform they migrate toward a negative minimum of h/137, I can see the 20% threshold being reached as the gas population in the cavity approaches this minimum and there also remains the open question if fractional molecules / IRH can persist for a time outside the geometry in the lattice. Fran From: Axil Axil [mailto:[email protected]] Sent: Friday, June 07, 2013 4:31 PM To: vortex-l Subject: EXTERNAL: [Vo]:ENTANGLEMENT THRESHOLDS FOR RANDOM INDUCED STATES References: http://phys.org/news/2013-05-einstein-spooky-action-common-large.html Einstein's 'spooky action' common in large quantum systems, mathematicians find If you like mathematics that can choke an elephant try this as follows: http://arxiv.org/pdf/1106.2264v3.pdf ENTANGLEMENT THRESHOLDS FOR RANDOM INDUCED STATES Why does a Ni/H reactor form a Bose-Einstein condensate throughout its entire volume? STANIS LAW J. SZAREK provides the answer; the dipoles throughout the reactor are forced to become totally entangled when the percentage of dipole entanglement exceeds 20%. The Ni/H reactor will formulate a very large entangled system when it is in operation. As a large system, it has no choice but to become totally entangled. Infrared Photon tunneling between the individual Nano-cavities is the method by which quantum entanglement is spread Josephson like from one nano-cavity to its immediate neighbors. When the Ni/H reactor is not totally entangled, it renders the nuclear energy it produces from the decoherent nano-cavities as gamma radiation. However, if the 20% entanglement threshold is reached, the energy produced by the LENR reaction is thermalized through the process of frequency sharing as in a large super atom. When a Ni/H reactor is not yet totally entangled, it will produce gamma radiation. This can happen when the reactor is heating up upon startup or cooling down at shutdown. In the LeClair reactor, the 20% entanglement threshold is never reached and a significant proportion of its energy output is rendered as gamma radiation. A Ni/H reactor must exceed this 20% dipole entanglement threshold before its energy production phase is initiated to avoid the inconvenience of gamma production.
