Agreed with this, Note 380(4) can be appleid to this anti gravity problem in order to simulate the apparatus and optimize conditions for counter gravitation. Note 380(4) used the homogeneous field equations of ECE2 gravitation:

del cap omega = 0

curl g + partial cap omega / partial t = 0

and the antisymmetry laws from

cap omega = curl Q – omega x Q

Here cap omega is the gravitomagnetic field, g is the gravitational field, Q is the gravitational vector potential, and omega the space part of the spin connection four vector. The inhomogeneous laws of ECE2 gravitation were not used in Note 380(4), and it was shown that the above three equations are sufficient to completely determine Q and the spin connection four vector. Having found them, they can be used in the inhomogeneous laws, the ECE2 gravitational Coulomb law and Ampere Maxwell law. Exactly the same remarks apply to ECE2 electromagnetism, and combinations of electromagnetism and gravitation. This ought to produce efficient counter gravitational designs. We can describe any existing counter gravitational apparatus with these powerful ECE2 equations.

To: EMyrone@aol.com

Sent: 25/06/2017 16:01:12 GMT Daylight Time

Subj: Another suggestion for solving the antigravity problem

There are rumours out that antigravity can be achieved by rotating

magnetic fields (like in a 3-phase motor). In this case the spin

connection is the vector of the rotation axis if I see this right. So we

have a predefined bold omega and can apply the Faraday and/or

Ampere-Maxwell law to find bold A and bold Q. Perhaps worth a thought. I

am not sure if the coupling from e-m to gravity can be applied in the

same way as before.

Horst

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