Note: I suck at the laws of physics, but it is my belief that with the upcoming pole shift & the changes to our electromagnetic shield – this will be enough to allow the trapped ISBEs to escape from what has been a true & real ‘prison’. The answer lies in the 1864 paper that was written on the Lorentz Force. And the solution was always right there…..found on page 77 in the alternative theories of relativity.
Hence why the numeric countdown began at 77
Quoting: ladyannie2009Where do I find this The Alternative Theories of Relativity? I did a quick google but didn't find a book title by this name. Am I looking in the wrong place?
pardon me, eireann. That should have read 'line 77' (of his equasion) not page 77.
in the pdf file, you'll find this beginning on pg 197
<snipped>
"... electromagnetic force..."
"In physics, the Lorentz force is the force on a point charge due to electromagnetic fields. Lorentz introduced this force in 1892. However, the discovery of the Lorentz force was before Lorentz's time. In particular, it can be seen at equation (77) in Maxwell's 1861 paper.
On Physical Lines of Force. Later, Maxwell listed it as equation "D" of his 1864 paper, A Dynamical Theory of the Electromagnetic Field, as one of the eight original Maxwell's equations. In this paper the equation was written as follows:
(goes into pg 198)
Significance of the Lorentz force While the modern Maxwell's equations describe how electrically charged particles and objects give rise to electric and magnetic fields, the Lorentz force law completes that picture by describing the force acting on a moving point charge q in the presence of electromagnetic fields. The Lorentz force law describes the effect of E and B upon a point charge, but such electromagnetic forces are not the entire picture. Charged particles are possibly coupled to other forces, notably gravity and nuclear forces. Thus, Maxwell's equations do not stand separate from other physical laws, but are coupled to them via the charge and current densities. The response of a point charge to the Lorentz law is one aspect; the generation of E and B by currents and charges is another.
In real materials the Lorentz force is inadequate to describe the behavior of charged particles, both in principle and as a matter of computation. The charged particles in a material medium both respond to the E and B fields and generate these fields. Complex transport equations must be solved to determine the time and spatial response of charges, for example, the Boltzmann equation or the Fokker–Planck equation or the Navier-Stokes equations.
For example, see magnetohydrodynamics, fluid dynamics, electrohydrodynamics, superconductivity, stellar evolution. An entire physical apparatus for dealing with these matters has developed. See for example, Green–Kubo relations and Green's function (many-body theory).
Although one might suggest that these theories are only approximations intended to deal with large ensembles of "point particles", perhaps a deeper perspective is that the chargebearing particles may respond to forces like gravity, or nuclear forces, or boundary conditions."
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link to exopoliticshongkong.com]
then, I also found this from cern - I'm guessing many people will find this
very interesting!
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link to indico.cern.ch]
*I'll correct the typo - thanks for bringing it to my attention!
