Wind 8.54%, speed 1 – 18 mph

June 29, 2016

This is about as much as the wind turbines will ever produce, so the propaganda is compete deception. The 18 mph wind happens to be over West Wales and is the highest speed in the British Isles today.

Graphics of paper 349

June 29, 2016

They are very interesting graphics, and this shows how meticulous is Horst Eckardt in his work.

In a message dated 29/06/2016 14:23:14 GMT Daylight Time, writes:

I just found a calculational fault in my code, will re-compute the results of paper 349. The results remain essentailly the same, but I used a scalar where a vector was required.

Horst

Am 29.06.2016 um 10:09 schrieb EMyrone:

Kambe’s hydrodynamic electric field is Eq. (25) of this note, it is E = (v dot del)v in units of acceleration, metres per seconds squared. Here v is the velocity field v(r, t) of a fluid continuum. This fluid is considered to be the aether or spacetime, which is geometry. So Kambe’s E can be translated in to the electric field stength in volts per metre of electrodynamics through a proportionality constant detemined by a units analysis. This constant or coefficient is volts per metre divided by acceleration. Whether E is turbulent or not depends on whether v is turbulent or not. Kambe’s E can be expressed in terms of the vorticity w through Eq. (27) of the note. The vorticity equation including the Reynolds number is Eq. (40) of the note. Kambe assumes that the right hand side of Eq. (40) is zero, and that is a special case. So Kambe leaves out the Reynolds number in his paper but the note reinstates it. I checked that his neglect of the Reynolds number does not affect his field equations. By units analysis the electrodynamic equivalent of the vorticity equation (40) is Eq. (46). Kambe uses Gaussian units in his field equations, and these have to be translated into S. I. units of ECE and ECE2. Kambe’s H is defined as the vorticity w = curl v. So whether or not H is turbulent depends again on whether or not v is turbulent. The geometrical condition for the Aharonov Bohm vacuum in Kambe’s analysis is the same as in electrodynamics:

d ^ q = – omega ^ q

where
T = d ^ q + omega ^ q

is the Cartan torsion in minimal notation. Under this condition there are potentials but no fields (the Aharonov Bohm vacuum). Eq. (46) can be expressed in terms of the W potential of ECE2 by using:

B = curl W

When considering the Aharnov Bohm vacuum this equation must be extended to complex valued W, so that it becomes possible to have finite W and zero B. Alternatively one can use (UFT317 and UFT318):

B = curl A + 2 omega x A

In Eq. (46) of the note. The Aharonov Bohm vacuum is defined by

curl A = 2 A x omega = – 2 omega x A

so
B = 0

but A is not zero. Then one has a vacuum vorticity equation with Reynolds number R. So conditions for turbulent vacuum A can be defined.

Discussion of Note 351(1).

The existence of an electric field requires a spacetime pressure but no turbulence. Additionally there are vacuum waves that even do not require electric or magnetic fields.
Horst

Von meinem Samsung Gerät gesendet.

351(2): Translation of Fluid Dynamics into Electrodynamics

June 29, 2016

All the equations of fluid dynamics can be translated into hitherto unknown equations of electrodynamics using the conversion table on page 4. For example the well known Euler equation of fluid dynamics becomes Eq. (8), a new relation between the scalar potential phi sub W and the vector potential W of ECE2 electrodynamics. So to describe electrodynamic turbulence, google up or otherwise find the well known hydrodynamic equations that govern the transition to turbulent flow, and translate directly into turbulent electrodynamics, or turbulent gravitation. These are manifestations of turbulent spacetime or aether in ECE2 unified field theory. The turbulent Aharonov Bohm vacuum for example may be used as in UFT311 and the turbulence observed experimentally. Osamu Ide may be observing this turbulence at present. So the next note will translate the well known and traditional Navier Stokes equations into entirely new equations of classical electrodynamics. All the relevant S. I. units are given on page one of the note.

a351stpapernotes2.pdf

Graphics of Turbulence

June 29, 2016

I think that UFT351 will be a well studied paper, especially with graphics of turbulence by co author Horst Eckardt, worked out with boundary conditions in the usual way. I think that Norman Page is right in describing spacetime as being in general turbulent. Leonardo da Vinci thought in much the same way in his famous left handed drawings. So we can have turbulent geometry, but this is always causal, there is no indeterminacy of the Copenhagen type. Nothing about geometry is “unknowable”. Turbulence is very interesting and ideal for graphics, there are eddies, vortices and so on. The subject of non Newtonian rheology can also be translated into electrodyamics and gravitation. This shows the power of a unified field theory based on geometry, and not 167 and a quarter adjustables, all totally unknowable forever.

Work by Hans Albert Einstein

June 29, 2016

Many thanks, it would be very interesting to calculate a turbulent vacuum A and graph the transition to turbulence.

Sent: 28/06/2016 23:12:27 GMT Daylight Time
Subj: Here is one reference

Einstein, H. A. (1963). “Engineering derivation of the Navier-Stokes
equations.”
J. Eng. Mech. Div., 89(3), 1–8. Discussion by T. Sarpkaya, E. O.
Macagno, and R. Schmidt, 89(4), 99–102; Ramsey, H., and W. D. L. Finn,
89(5), 105–106; G. H. Toebes, 90(1), 163–166; and closure by Einstein,
H. A., 90(4), 151–155.

Norman

Einstein Junior and Turbulent flows

June 29, 2016

Very interesting, this must be Hans Albert Einstein. His younger brother Edouard was initially a good student but developed schizophrenia when about twenty and spent his entire later life in a Sanatorium after his mother Mileva Maric died. His father never saw him again after 1933. So there was an aspect of Albert Einstein’s character that was decidedly unpleasant. If I had a son I would certainly have brought him over to Princeton. They had an older sister Lieserl (Elizabeth) who was illegitimate, and in those days that was a stigma. She was apparently born in Novi Sad, and was kept a secret. Her existence was not known until thirty years after Einstein died. Lieserl was mentioned for the last time on Sept. 19th 1903 in a letter from Albert Enstein to Mileva Maric and then disappeared from history. Apparently Lieserl was also disabled psychologically at birth. In those days that was also a stigma. So this is a very rough side of both Albert Einstein and Mileva Maric, and of course, hypocritical society.

Sent: 28/06/2016 23:06:21 GMT Daylight Time
Subj: Turbulent flows

Myron Horst it is interesting to note that Einstein’s son spent his
career working on hydraulic flows and turbulence from a very empirical
angle. Norman

http://ascelibrary.org/doi/pdf/10.1061/9780784413302.bm03

Discussion of Note 351(1), Part 2.

June 29, 2016

Kambe’s hydrodynamic electric field is Eq. (25) of this note, it is E = (v dot del)v in units of acceleration, metres per seconds squared. Here v is the velocity field v(r, t) of a fluid continuum. This fluid is considered to be the aether or spacetime, which is geometry. So Kambe’s E can be translated in to the electric field stength in volts per metre of electrodynamics through a proportionality constant detemined by a units analysis. This constant or coefficient is volts per metre divided by acceleration. Whether E is turbulent or not depends on whether v is turbulent or not. Kambe’s E can be expressed in terms of the vorticity w through Eq. (27) of the note. The vorticity equation including the Reynolds number is Eq. (40) of the note. Kambe assumes that the right hand side of Eq. (40) is zero, and that is a special case. So Kambe leaves out the Reynolds number in his paper but the note reinstates it. I checked that his neglect of the Reynolds number does not affect his field equations. By units analysis the electrodynamic equivalent of the vorticity equation (40) is Eq. (46). Kambe uses Gaussian units in his field equations, and these have to be translated into S. I. units of ECE and ECE2. Kambe’s H is defined as the vorticity w = curl v. So whether or not H is turbulent depends again on whether or not v is turbulent. The geometrical condition for the Aharonov Bohm vacuum in Kambe’s analysis is the same as in electrodynamics:

d ^ q = – omega ^ q

where
T = d ^ q + omega ^ q

is the Cartan torsion in minimal notation. Under this condition there are potentials but no fields (the Aharonov Bohm vacuum). Eq. (46) can be expressed in terms of the W potential of ECE2 by using:

B = curl W

When considering the Aharnov Bohm vacuum this equation must be extended to complex valued W, so that it becomes possible to have finite W and zero B. Alternatively one can use (UFT317 and UFT318):

B = curl A + 2 omega x A

In Eq. (46) of the note. The Aharonov Bohm vacuum is defined by

curl A = 2 A x omega = – 2 omega x A

so
B = 0

but A is not zero. Then one has a vacuum vorticity equation with Reynolds number R. So conditions for turbulent vacuum A can be defined.

Discussion of Note 351(1).

The existence of an electric field requires a spacetime pressure but no turbulence. Additionally there are vacuum waves that even do not require electric or magnetic fields.
Horst

Von meinem Samsung Gerät gesendet.

Discussion of Note 351(1).

June 29, 2016

In general I would say that the equations of electrodynamics can be expressed as equations of flow, so all the well studied aspects of hydrodynamics apply to electrodynamics. Both subjects are expressions of the geometry of spacetime. The same is true of gravitational and nuclear physics.

In a message dated 28/06/2016 14:18:53 GMT Daylight Time, writes:

Myron Is it not perhaps more fruitful to think of space time as being generally turbulent ? The Reynolds number of interest is then that which marks the transition to observable structures. Norman Page
On 6/28/2016 7:06 AM, EMyrone wrote:

Many thanks, it would also be interesting to have some graphics of turbulent aether flow for various boundary conditions (boundary of the aether with the circuit).

To: EMyrone
Sent: 28/06/2016 12:56:26 GMT Daylight Time
Subj: Re: 351(1): Energy from a Turbulent Spacetime

Very interesting – needless to say!

Sent from my Samsung device

Wind 4.04%, 0828 local time, speed across the British Isles 0 – 18 mph

June 29, 2016

It is already clear that wind turbines fluctuate wildly and will never be of any real use. The were useless from the start because the mean wind speed is below their optimal range and sometimes they are becalmed or switched off. They were forced through undemocratically and have dragged down the economy.

Daily Report 27/6/16

June 29, 2016

The equivalent of 195,690 printed pages was downloaded (713.484 megabytes) from 2949 downloaded memory files (hits) and 585 distinct visits each averaging 4.9 memory pages and 16 minutes, printed pages to hits ratio for the day of 66.36, main spiders cnsat(China), google, MSN and Yahoo. Collected ECE2 1709, Top ten 1503, Collected Evans / Morris 891 (est), Collected scientometrics 609, Barddoniaeth / Collected Poetry 393, Eckardt / Lindstrom papers 359, Principles of ECE 339, F3(Sp) 338, Collected Proofs 222, Autobiography volumes one and two 222, Evans Equations 128, UFT88 117, Principles of ECE (typeset) 111, Engineering Model 111, CEFE 109, UFT321 73, UFT311 69, Self charging inverter 48, Llais 45, List of prolific authors 26, Three world records by MWE 23, Lindstrom Idaho lecture 18, UFT313 39, UFT314 40, UFT315 53, UFT316 38, UFT317 57, UFT318 63, UFT319 65, UFT320 49, UFT322 59, UFT323 44, UFT324 70, UFT325 70, UFT326 51, UFT327 38, UFT328 56, UFT329 44, UFT330 49, UFT331 48, UFT332 57, UFT333 45, UFT334 42, UFT335 42, UFT336 61, UFT337 38, UFT338 40, UFT339 41, UFT340 39, UFT341 40, UFT342 32, UFT343 43, UFT344 38, UFT345 54, UFT346 61, UFT347 56, UFT348 38, UFT349 9 to date in June 2016. Physics State University of Rio de Janeiro Brazil UFT157(Sp); Technical University Ilmenau UFT238b; Cornell University AIAS Staff; Science and Technology Keio University Japan UFT165, large downloads unresolved domain. Intense interest all sectors, updated usage file attached for June 2016.


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