On Nov 18, 2008, at 7:13 AM, Jones Beene wrote:
Horace
Today I learned an interesting factoid in passing: the internal
magnetic field for the sodium atom has been measured to be on the
order of ~30 MG (million Gauss) = ~3,000 T !!
"This is not a large value for near nucleus field strength. The
dipole field has a ~ 1/r^3 field intensity, so grows arbitrarily
large as the the dipole distance r goes to zero."
But it would seem that r cannot ever go to zero or near zero for
measurement purposes - because of the strong force, which would
overwhelm any other force long before it could attain that kind of
value. The strong interaction is typically 100 times the strength
of the electromagnetic force
There is no strong force exchange between hadrons and leptons. I
stated: "For example, the 9.2x10^-17 m de Broglie wavelength electron
in the deflated state hydrogen in my theory imposes a 1.5x10^17 T
field on the proton at a distance of 1.8x10^-16 m."
and I am assuming that the range for this measurement was outside
the region where there would be interference. It is not clear how
the measurement was made, but it was probably by deflection of an
electron beam.
I would guess by neutron scattering - because the neutron is neutral
so magnetic influences can more clearly be seen.
When you say that this 30 T is not a large value, do you have a
reference for that ? or are you basing the conclusion of the
"arbitrarily large" supposition?
Jones
My statement is based upon ordinary *calculations*. See:
http://mtaonline.net/~hheffner/DeflateP1.pdf
for the proton deflated state calculation,
http://www.mtaonline.net/~hheffner/FusionSpreadDualRel.pdf
for the deuteron deflated state calculation,
and:
http://www.mtaonline.net/~hheffner/DeflationFusion2.pdf
for background information.
As I noted earlier, these calculations are based on simple
relativistic mechanics, and ignore the extreme virtual particle flux
that would clearly be involved in the necessarily high energy near
nucleus traverses of an electron.
Best regards,
Horace Heffner
http://www.mtaonline.net/~hheffner/
