It may possibly help understanding if I amplify my previous
remarks with the following explanation of proton-electron
interaction outside and inside palladium.
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.........External Beta-atmosphere pressure...........
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...O O O O O O O.....................................
...O O. . . . . . . . . . . . o o o o o....
...O O . . . > . . . . > . . o o....
...O PROTON O. . . . . . . . . . . . o e o....
...O O . . . < . . . . < . . .o o....
...O O. . . . . . . . . . . . o o o o o....
...O O O O O O O.....................................
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Fig.1 Bernoulli pressure drop between P and e
relative to the external environment
Fig.1 shows the difference in pressure brought about
by the electric and magnetic flow and counter flow
(vortex tube) between the proton and the electron
when the hydrogen atom is outside the palladium and
subjected to full external Beta-atmosphere pressure.
The concentration of dots represents the magnitude
of the pressure. Because of the Bernoulli pressure
drop between the proton and the electron they are
pushed together by the external beta atmosphere
pressure.
. . . . . . . . . . . . . . . . . . . . . . . . . . .
. . . . . . . . . . . . . . . . . . . . . . . . . .
. . . .Internal Beta-atmosphere pressure. . . . . . .
. . . . . . . . . . . . . . . . . . . . . . . . . .
. . . . . . . . . . . . . . . . . . . . . . . . . . .
. . . . . . . . . . . . . . . . . . . . . . . . . .
. . . . . . . . . . . . . . . . . . . . . . . . . . .
. O O O O O O O . . . . . . . . . . . . . . . . . .
. .O O. . . . . . . . . . . . o o o o o . .
. O O . . . . . . . . . . . o o. .
. .O PROTON O. . . . . . . . . . . . o e o . .
. O O . . . . . . . . . . . .o o. .
. .O O. . . . . . . . . . . . o o o o o . .
. O O O O O O O . . . . . . . . . . . . . . . . . .
. . . . . . . . . . . . . . . . . . . . . . . . . . .
. . . . . . . . . . . . . . . . . . . . . . . . . .
. . . . . . . . . . . . . . . . . . . . . . . . . . .
. . . . . . . . . . . . . . . . . . . . . . . . . .
. . . . . . . . . . . . . . . . . . . . . . . . . . .
Fig.2 No Bernoulli pressure drop between P and e
relative to the internal environment
Figure 2 show the situation inside the palladium.
The Beta-atmosphere pressure surrounding the proton
-electron complex is reduced to the point that the
Bernoulli pressure drop disappears. The electron is
no longer pushed towards the proton and is free to
wander about in an analogous way, and for the same
reason that ions are free to wander about in aqueous
solutions.
Obviously, I have represented a boundary case, but
this in essence is what is going on inside the
palladium.
Cheers,
Frank Grimer
