Artificial Gravity

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Artificial ElectroGravity Fields
 

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This page assumes that you have read and understood the 4 basic electrogravity axioms.  There are two things that dictate the strength of an electrogravity field:  divergence and magnitude (with direction)

Reverse Electrogravity

The reverse polarity electrogravity field (in red), will cancel and override the original field (in black).  This means that the EG field by vector addition is equal to zero.

Please also note that the reverse polarity field does not have to be divergent, as long as it de-polarizes the atom from the original field with a negative or reverse polarity EG field.

A reverse polarity field is produced by positive moving charges i.e. protons, ions, nucleus including alpha-particles or any man-made objects that have been made to carry a positive electric charge, and moving at a high speed.  (This effect is also suggested by Prof. Tom Chalko and Michel Desmarquet)

Convergent Positive Electrogravity

The convergent positive polarity electrogravity field (in green), can also cancel and override the original field (in black).  It may be hard to generate in practical far field applications, but it is available for use.

The cancellation works by having a convergence which cancels out the original divergence field (in black).  The non-divergent field strength can still be strong, but it has no dielectric effect on the atoms if the net field is not divergent.

Electrostatic Decoupling

As in the Townsend Brown experiments, it is possible to decouple the electrogravity field by using a strong electrostatic field on certain dielectric materials. 

This technique will not work on metals, but it could be quite effective on high dielectric constant materials, such as barium composites, and other dielectric materials, most often found in capacitors.

Read more about this effect on the Townsend Brown page.

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