As usual, updating of the gravimagnetic theory article continues on a
regular basis.
The figures have been moved to the end. Figure 3, a figure of galaxy
587742782068817961 of the Sloan Digital Sky Survey:
http://cas.sdss.org/astro/en/tools/explore/obj.asp?id=587742782068817961
has been added as a possible example of a fairly aged galaxy having
normal matter black holes which produce mirror matter. The effects
of the mirror matter are (1) the repulsion of the inner portions of
the galatic arms into a ring, and (2) the repulsion of some ordinary
matter to the periphery of the spherical shaped mass of mirror matter
which surrounds the galaxy, thus making the spherical shell visible.
Changes have occurred relating to dimensional analysis, unitization
in relativity, and virtual particle gravitational mass.
In many circumstances, many applications, due to the small
gravitational constant, it is adequate to treat gravitational
quantities completely independently for computational purposes, and
then consolidate with Coulomb force results if that is even
necessary. The exact same Coulomb based equations can be
independently applied to the gravitational portion of the
computation in order to derive the gravitational forces, energies,
waveforms, etc. The gravitational formulations are completely
independent of the electromagnetic formulations. They are
isomorphic, so the same equations are used, though using the
isomorphism substitutions as defined. The results, however, are not
similar in handedness or magnitude, because, though the equations are
all formally identical, there are imaginary values coming into play,
and h_g = - h, G is used instead of the Coulomb constant, etc.
Because the gravitational charge and EM charge are bound together,
the forces can be summed to characterize a fermion, or to
characterize a boson-fermion interaction as a whole.
When full relativistic effects are involved, or a correct formalism
is required, then it is decessary to dispense with MLTQ units in
favor of the full definition over the field of complex numbers, LT(a
QM + b Q_g ), where the value of real and b are determined by
particle type(s) involved, and Q and the imaginary Q_g are units of
Coulomb and gravitational charge, M is inertial mass. This in
effect provides a fully unified field theory, as unified as possible
at this point that is.
The Dirac equation, the Dirac Hamiltonians for field interaction,
etc, the Rarita-Schwinger equation used for spin 3/2 fermions,
etc. , must be defined over the full imaginary field, not just real
numbers with units.
It is noteworthy that the technique of normalization of units,
commonly used in relativity, can not necessarily be used when
applying gravimagnetic theory as unified over the imaginary field.
It is not necessarily true that c = c_g, so it is not possible to
set both c = 1 and c_g = 1. Q and Q_g exist in differing proportions
in differing particles, and one of the values is imaginary.
Photons, or bosons in general, are bound entities, having both an
electromagnetic portion and a gravimagnetic portion. Photons have
an electromagnetic potion and corresponding gravimagnetic charge.
Graviphotons have a gravimagnetic portion and corresponding Coulomb
charge. Virtual photons don't have a gravimagnetic portion and
gravitons don’t have an electromagnetic portion. Virtual particles
do not have a gravitational charge. This then provides a description
of gravity consistent with both Newton and special relativity.
Horace Heffner
http://www.mtaonline.net/~hheffner/
