Wednesday, March 12, 2014

Back to Maxwell

In the last post we learned that in our sparse world the electron quant size if 377 times the magnetic.  Maxwell also assumes that the electron positive and negative fields are right angles to each other, or the magnetic is right angles to the charge fields. Hence, the straight line along the perpendicular of both.  One field has a constant phase shift, the line of curvature, the other field has the same, and straight is the line perpendicular to both. The 377 is actually the difference in the rate of curvature. That is because of the order difference, the quant size corresponds to wavelength of the curvature.

The two fields are balanced, the e field with the large quant size cannot rebalance any phase having smaller units, there is no rebalance that is better. So the magnetic takes these. Eventually the phase imbalance build up large enough to be notice by the E field, and it starts to takes large chunks out, which cause an opposite imbalance in the M field which then reveres, in smaller chunks. Everywhere this is happening at Pauli speed.  The magnetic taking out large positive pieces, the magnetic adding in small negative pieces, and then the opposite, they subdivide the phase change into large positive pieces plus small negative pieces, and visa versa.

How does Nyquist maintain the separation between quant size? Because every region is compacting, and matter, at any level of sparsity is maintaining fields quants by  order. The wavelength of matter being determine on order by order basis according to relative density in the region at big bang.

Unoriented phase changes are equalized equally without orientation.  But if a radio transmitted can define an orientation, then the phase equalization takes is done along that orientation. Along the orientation the phase change never balances, the transmitter keep imbalancing. That becomes an axis of simultaneity to Nyquist.  To keep Pauli true the rebalancing takes place along that axis. Everywhere along that orientation, the imbalance is contained within the fields, and non simultaneity is restored. There is flattened sphere  moving along that axis, and it cannot contain all the imbalance, the E field full, the balance, the M field dumping,,  and the phase imbalance is minimum along the axis and maximum perpendicular, in the EM fields.

So lets just introduce our radio as another field with a very long wavelength, say 10,000 times the electron wavelength.   Then we can see that along that straight line the rate of changes of the phase imbalance. It is 1/10000 for the radio, 1/377 for the magnetic and 1 for the charge.  The rate of balancing between the magnetic and charge is very fast compared to the radio, we will not notice.

Now what happens when the magnetic and charge are not at right angles?  That means the electric field is curve a little in one direction, the magnetic in the other. That curve is 90 - the small angle between the two, say theta.  Every sample along the straight line will introduce a theta, and the straight is no longer the path of most balance.  The path of most balance will be a curve in which sine theta is the distance of curvature per sample.  Along that curve, phase will be most balanced.  When the curve is small, then the minimum phase path is a spiral along the axis. Most free wave motion should spiral a bit.

If we increase the phase angle the curve gets tighter until a wave will not propagate.That means EM fields are compact to support waves at that rate of phase imbalance.

Lets do something else. Lets shorten the wavelength from the radio. As it gets shorter and shorter, it approaches the wavelength of the magnetic. Soon the magnetic becomes the new axis of simultaneity. But the electro, magnetic pair cannot hold the signal. The phase imbalance gets trapped, Nyquist makes matter. The process is that the Nyquist balancing just hang there, rebalancing the wave in place. What ever it cannot balance is holds as phase shift and the bundle moves. The matter creation depends on the wavelength of the electro and magnetic fields in the region. Or in general it depends on  the two orders making the wave motion in that particular region.The electron wavelength is determined by the sparsity of the standard model in our region. So, a wave breaking into matter here will become the collection of kinetic energy, wave motion, and matter that can be supported.






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