Torque Free Precession

Agreed with this procedure for calculation and computation. I have just sent over the Euler equations of fluid dynamics, and it can be seen that there are many new torques in Eq. (10), providing plenty of scope for comparison with the data.

To: EMyrone@aol.com
Sent: 06/01/2017 12:55:34 GMT Standard Time
Subj: Re: Torque Free Precession

In the paper by Swanson (referencing Braithwaite and Shipov) a formula is given for the force generated by the non-classical momentum. It would be favourable if we could find a method for computing the spin connection instead of adapting it to an experimental value. Perhaps we should analyze how Shipov obtained his formula, although he has a free “adaptation factor” between 0.1 and 0.01 in it.

Horst

Am 06.01.2017 um 09:09 schrieb EMyrone:

Eq. (13) are the Euler equations as in Marion and Thornton, who use the term “torque free precession”. The torque is defined in a rotating frame, giving rise to omega x L. The Euler equations are fundamentally extended by fluid dynamics, giving rise to many new effects. Hopefully the effects observed by Braithwaite and Shipov (paper sent over by Michael Jackson) can be described by a choice of spin connections. My next task is to extend Eq. (16) to three dimensions and calculate the precession frequency or frequencies of the Euler equations of fluid dynamics. There may be more than one precession frequency.

To: EMyrone
Sent: 05/01/2017 18:05:47 GMT Standard Time
Subj: PS: Re: 367(1): Fluid Dynamic Theory of Gyroscopes

PS: Is the case you described what in the literature is called “torque-free precession?”. There is no external torque.

Horst

Am 04.01.2017 um 13:02 schrieb EMyrone:

The attached notes shows that the well known Euler Equations are fundamentally modified in ECE2 fluid dynamics, and become Eqs. (22). They can be simplified to Eq. (27) with the assumptions (25) and (26) and show that there are new precessional effects in a gyroscope when the angular momentum becomes a vector field of ECE2 fluid dynamics, i.e. when the motion takes place in a fluid spacetime, aether or vacuum. Eq. (27) could be applied to the experimental results recently sent over by Michael Jackson, to attempt to explain the experimental data with this new theory. It is assumed that the data are reproducible and repeatable and there is no reason to doubt it. The standard classical dynamics cannot explain the data. This new theory can be applied to the precessions of the earth or any rigid object such as a symmetric top (see Marion and Thornton pp. 388 ff., third edition).

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