Discussion of 378(5)

Fully agreed, the overall theory is precisely self consistent. Also agreed about Eqs. (31) and (32). This note produces the possibility of merging counter gravity with orbital theory.

To: EMyrone@aol.com
Sent: 26/05/2017 17:42:24 GMT Daylight Time
Subj: Re: 378(5): Orbital Theory and Conditions for Counter Gravitation

I see that my idea of combining the tetrad vector with kappa is even exactly possible 🙂
Shouldn’t eqs.(31,32) have the dots on the aether coordinates at the rhs?
Then the general solution for a constant omega_0 is:

where a depends on omega_0.

Horst

Am 25.05.2017 um 14:55 schrieb EMyrone:

In this note the ECE2 gravitational field potential relations of UFT318 and UFT319 are used to derive the equations of the planar orbit, Eqs. (27) and (28) in the presence of an aether momentum (5) defined by the gravitational vector potential Q bold. This appears in the ECE2 gravitational field equations but not in Newtonian gravitation. This aether momentum can result in zero gravitation according to Eq. (33) and also in counter gravitation, as first discussed in UFT318 and UFT319. Eqs. (27), (28), (31) and (32) are four simultaneous differential equations in four unknowns, and can be solved with Maxima. Counter gravitation can be induced with an electric field as discussed in UFT318. The presence of the aether momentum implies the existence of a gravitomagnetic field, so the full scope of the ECE2 gravitational field equations is being implemented. I will write up UFT378 now and in UFT379 apply the theory to a gyroscope inside a Faraday cage.

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