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| Author |
Message |
| Jack Sarfatti |
 Posted: Thu May 19, 2005 5:37 am |
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Guest
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On the extended space structure of a single electron
On May 13, 2005, at 7:46 AM, Ken Shoulders wrote:
A paper by Ken Shoulders entitled "EVOs And The Hutchison Effect" will
be presented at the 2005 Conference on Cold Fusion to be held at MIT on
May 21. A 1 MB .PDF file showing some of the graphics slides to be used
in that presentation can now be downloaded from:
http://www.svn.net/krscfs/
Ken
For a shell of N electrons
N(h/mc)^2 = 4piro^2
N^1/2(h/mc) = (4pi)^1/2ro
ro^3 = (Ne)^2/(2mc^2/\zpf)
N^3/2(h/mc)^3/(4pi)^3/2 = N^2e^2/2mc^2/\zpf
(h/mc)^3/(4pi)^3/2 = N^1/2e^2/2mc^2/\zpf
/\zpf = (4pi)^3/2N^1/2(e^2/2mc^2)/(h/mc)^3
e^2/hc ~ (1/137) = (classical electron radius)/(Compton radius)
/\zpf ~ (4pi)^3/2N^1/2(e^2/hc)(mc/h)^2
For a SINGLE ELECTRON N = 1 (Bohm hidden variable)
This solves a 100 year old problem from Lorentz.
The electron is a shell of charge with a dark energy core.
The zero point stress energy density tensor of the dark energy core is
tuv(ZPF core) = (c^4/8piG)/\zpfguv
On May 18, 2005, at 10:02 PM, Jack Sarfatti wrote:
bcc
PS for uniform /\zpf > 0 of negative pressure (dark energy core)
F/m = -dV/dr = -2c^2|/\zpf|ro + (Ne)^2/mro^2 = 0
ro^3 = (Ne)^2/2mc^2/\zpf
stability
d^2V/dr^2 = +2c^2|/\zpf| + 2(Ne)^2/mro^3 > 0
On May 18, 2005, at 9:42 PM, Jack Sarfatti wrote:
Note that my theory of Ken Shoulders charge clusters also has a dark
energy core that stabilizes the shell of N electrons. The dark energy
core potential ~ + c^2|/\zpf|r^2 holds the repulsive Coulomb barrier +
(Ne)^2/mr in check!
Similarly for Pioneer 10 & 11 anomaly, galactic halo & other phenomena. |
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