Magnetic repulsion in superconductivity is caused by the generation of mass by the superconductor in the photon. This is the same mass production mechanism that is seen in the higgs field were mass is produced in the W boson.
On Thu, Nov 5, 2015 at 7:49 PM, David Roberson <[email protected]> wrote: > From what I recall the magnetic field repulsion is due to current flowing > and not on an individual atom basis. That would imply that no extra > repulsion would be seen for atoms embedded within the iron. > > Dave > > > > -----Original Message----- > From: Bob Higgins <[email protected]> > To: vortex-l <[email protected]> > Sent: Thu, Nov 5, 2015 6:39 pm > Subject: Re: [Vo]: Evidence for ultra-dense deuterium > > Jones, > > Even if true that H(-1) exists as a superfluid/RTSC (and Winterberg says > that the ultra-dense form only occurs with deuterium), then it is highly > likely that it would be a type II superconductor, like all of the > superconductors above about 40K. The type II superconductors pin a > magnetic field inside it if the field was there when the superconducting > state formed. So, you wouldn't get the instant repulsion. > > On Thu, Nov 5, 2015 at 3:56 PM, Jones Beene <[email protected]> wrote: > >> Of interest… >> >> In a 2014 paper, Holmlid says: “Ultra-dense hydrogen H(-1) is a quantum >> material and the first material which is superfluid and superconductive at >> room temperature. This has been shown in detail for the deuterium form >> D(-1).” >> >> Comment: >> As a RTSC, the dense material H(-1) will be subject to the Meissner >> effect. If it is created on a ferromagnetic catalyst which has permanent or >> applied magnetic field, which is possible to accomplish with iron oxide as >> the fill, then H(-1) should be repelled as soon as it is made. >> >> The H(-1) can made within a translucent alumina tube filled with Shell >> 105 and hydrogen, using photons shining into the tube, so as to create SPP >> on the interfacial ID surface of the tube. The H(-1) should slowly migrate >> into the walls of the alumina. This should happen as soon as it is formed >> due to Meissner repulsion. Laser light should be avoided in favor of >> diffuse monochromatic light during the fuel build-up stage. It would be >> beneficial to cool the tube as much as possible at this stage, possibly >> using a cold plate. The alumina matrix would be effectively porous to H(-1) >> at only a few picometers in diameter. >> >> This is concievably an effective way to make and store the H(-1) for >> later use. >> >> >> > >
