Having forged a clear understanding in UFT386 of the induction of a vacuum current density by the vector spin connection in ECE2 magnetostatics, UFT387 will extend the methodology to the induction of a vacuum charge density in ECE2 electrostatics. Following papers will extend the method to ECE2 electrodynamics. August 2017 will see a new record high interest in ECE2 (UFT313 – UFT385 to date) and also in my prose and poetry. The record set in July 2017 will be exceeded by a very large margin. Many thanks to all concerned!

## Archive for August, 2017

### Plans for UFT387

Thursday, August 31st, 2017### FOR POSTING: UFT386 Sections 1 and 2 and Notes

Thursday, August 31st, 2017This paper shows that conservation of ECE2 antisymmetry leads to the inference of a vacuum current density (20). The paper shows that this can be computed for any material A. Eqs (5) to (7) are used to compute the vector spin connection from any A, while rigorously conserving antisymmetry. It would be very interesting to graph a few examples of a vector spin connection and a vacuum current density from a few material potentials, for example A for a static magnetic field and A from a current loop, and the A inferred by Horst Eckardt for this paper. In general J and J(vac) can be computed from any material A using Eq. (11) and numerical integration. This is a great advance in understanding of energy from spacetime.

### Daily Report 29/7/17

Thursday, August 31st, 2017The equivalent of 124,271 printed pages was downloaded (453.092 megabytes) from 2,503 downloaded memory files (hits) and 573 distinct visits each averaging 3.6 memory pages and 7 minutes, printed pages to hits ratio of 49.65, top referrals total of 2,292,434, main spiders Baidu, Google, MSN and Yahoo. Collected ECE2 3881, Top ten 2505, Collected Evans Morris 957, Autobiography volumes One and Two 714, F3(Sp) 679, Barddoniaeth (Collected Poetry) 645, Collected scientometrics 611, CV 338, Collected Eckardt / Lindstrom 236. Principles of ECE 220, Evans Equations 136, Collected Proofs 119, Engineering Model 105, UFT88 104, PECE2 82, PLENR 69, CEFE 65, MJE 61, UFT311 58, PECE 54, UFT321 51, ADD 47, SCI 45, Llais 44, 83Ref 42, UFT313 45, UFT314 60, UFT315 73, UFT316 32, UFT317 59, UFT318 28, UFT319 64, UFT320 50, UFT322 48, UFT323 38, UFT324 64, UFT325 51, UFT326 34, UFT327 25, UFT328 55, UFT329 46, UFT330 32, UFT331 48, UFT332 50, UFT333 35, UFT334 39, UFT335 55, UFT336 40, UFT337 22, UFT338 34, UFT339 32, UFT340 46, UTF341 53, UFT342 33, UFT343 55, UFT344 50, UFT345 48, UFT346 52, UFT347 73, UFT348 72, UFT349 39, UFT351 50, UFT352 72, UFT353 61, UFT354 93, UFT355 71, UFT356 60, UFT357 64, UTF358 65, UFT359 58, UFT360 57, UFT361 50, UFT362 54, UFT363 87, UFT364 70, UFT365 63, UFT366 82, UFT 367 58, UFT368 75, UFT369 59, UFT370 74, UFT371 65, UFT372 61, UFT373 67, UFT374 75, UFT375 45, UFT376 43, UFT377 57, UFT378 65, UFT379 50, UFT380 67, UFT381 48, UFT382 82, UFT383 75, UFT384 49, UFT385 29 to date in August 2017. Paul Scherrer Institute Switzerland general; Regional Computer Centre University of Erlangen UFT383, UFT177; City University of Hong Kong general; RailTel Government of India UFT169; University of Guadalajara F3(Sp); Science Museum National Autonomous University of Mexico Essay 24(Sp); International Peace Bureau Namibia general; Wayback Machine (www.archive.org) spidering, National University of Singapore UFT8. Intense interest all sectors, updated usage file attached for August 2017.

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### Discussion of 386(9)

Wednesday, August 30th, 2017Many thanks. The computer algebra and discussions for this note were very useful. Conservation of antisymmetry in ECE2 magnetostatics implies the vacuum current density:

J (vac) = curl (omega x A) / mu0

The material current density is

J = curl (curl A) / mu0

and both exist on the ECE2 level. A two dimensional analysis can always be made. So I will proceed to writing up Sections 1 and 2 of UFT386.

To: EMyrone@aol.com

Sent: 29/08/2017 17:48:24 GMT Daylight Time

Subj: Re: 386(9): Rigorous General Solution for ECE2 MagnetostaticsThis is a very clear description of the general implications of antisymmetry. We can comment that the general solution (4-6) requires all components of A to be different from zero. In our examples this is not the case, therefore we had to make special assumptions on omega x A.

The special example 3 for A which I found (constant field B=B0) is of the general form. The total charge density nabla x B is zero, but the constitutents from nabla x A and omega x A are not. This is an example for the vacuum current density. To my understanding it is counter-acted by a “real” charge density. So the total charge density is always a sum of both terms. Can we conclude this in general?Horst

Am 29.08.2017 um 15:13 schrieb EMyrone:

This procedure uses the unique solution (4) to (6) of the vector antisymmetry equations (1) to (3). This is an exactly determined problem. The solution (4) to (6) was found by co author Horst Eckardt using computer algebra. If more equations are added to the set of three equations (1) to (3) there is no solution because the problem becomes over determined. Horst and I discussed this point and are agreed. The ECE2 equations of magnetostatics are eqs. (7) to (10). So the well known material vector potential A may be found for any material current density using Eq. (10). In general this must be done by computer, but there are well known analytical solutions such as the circular current loop and magnetized sphere. Having found A, the vector spin connection is found from Eqs. (4) to (6), so omega x A can be calculated for any material J. Conservation of antisymmetry combined with del B = 0 implies that there exists a spacetime, vacuum or aether current density J(vac) defined by Eq. (17). So J(vac) can be computed from Eq. (17). The vacuum current density contributes to the total magnetic flux density B through Eq. (14), so a magnetic flux density is induced in material matter by spacetime, Q. E. D. Similarly, an electric field strength is induced by spacetime in the patented and replicated Ide circuit and the new circuits of UFT382 and UFT383 (UFT311, UFT321, UFT364, UFT382, UFT383), QED. I will now write up UFT386. In the standard model the spin connection does not exist and there is no vacuum current density, contrary to observation. Therefore given any material current density, the vacuum current density can be computed. The latter induces an extra magnetic flux density not present in the standard model (Maxwell Heaviside theory). A similar theory can be developed for ECE2 electrostatics as in immediately preceding UFT papers and notes. From Eq. (17) the vector spin connection is the link between the material vector potential A and the vacuum current density.

### Daily Report 28/7/17

Wednesday, August 30th, 2017The equivalent of 100,030 printed pages was downloaded (364.711 megabytes) from 2,649 memory files downloaded and 570 distinct visits each averaging 3.2 memory pages and 6 minutes, printed pages to hits ratio of 37.76, top referrals total 2,291,933 main spiders Baidu, Google, MSN and Yahoo. Collected ECE2 3970, Top ten 2443, Collected Evans Morris 924, Autobiography volumes one and two 708, Barddoniaeth (Collected Poetry) 641, F3(Sp) 636, Collected scientometrics 609, CV 337, Collected Eckardt Lindstrom 230, Principles of ECE 229, Evans Equations 128, Collected Proofs 116, UFT88 102, Engineering Model 101, PECE2 80, PLENR 68, CEFE 62, MJE 60, UFT311 55, PECE 52, UFT321 47, ADD 44, SCI 43, Llais 41, 83Ref 40, UFT313 43, UFT314 59, UFT315 71, UFT316 32, UFT317 58, UFT318 28, UFT319 63, UFT320 47, UFT322 47, UFT323 36, UFT324 61, UFT325 49, UFT326 34, UFT327 25, UFT328 53, UFT329 45, UFT330 31, UFT331 48, UFT332 47, UFT333 33, UFT334 39, UFT335 53, UFT336 37, UFT337 22, UFT338 33, UFT339 31, UFT340 46, UFT341 53, UFT342 33, UFT343 55, UFT344 47, UFT345 47, UFT346 51, UFT347 70, UFT348 71, UFT349 39, UFT351 51, UFT352 71, UFT353 61, UFT354 92, UFT355 70, UFT356 59, UFT357 62, UFT358 63, UFT359 55, UFT360 54, UFT361 49, UFT362 52, UFT363 83, UFT364 68, UFT365 62, UFT366 80, UFT367 57, UFT368 73, UFT369 58, UFT370 72, UFT371 63, UFT372 59, UFT373 65, UFT374 71, UFT375 44, UTF376 41, UFT377 55, UFT378 63, UFT379 48, UFT380 66, UFT381 47, UFT382 81, UFT383 70, UFT384 48, UFT385 26 to date in August 2017. Physics University of Adelaide UFT149; Physics University of Constanz UFT110; Physics University of Massachusetts UFT88; Univeristy of Eastern Finland UFT88, City University of Hong Kong general; University of Guadalajara Mexico F3(Sp); Wayback Machine (www.archive.org) spidering; UCW Swansea Civil List Pension. Intense interest all sectors, updated usage file attached for August 2017.

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### 3-D Plot of spin connection on the blog of www.aias.us

Tuesday, August 29th, 2017It looks clear and very well prepared, and is a three dimensional map of the spin connection. The spacetime current is:

J (spacetime) = curl (omega x A) / mu0

where “spacetime” is equivalent to “aether” or “vacuum”. Clearly, omega is the intermediary between J (spacetime) and A, the usual material vector potential.

### 386(9): Rigorous General Solution for ECE2 Magnetostatics

Tuesday, August 29th, 2017This procedure uses the unique solution (4) to (6) of the vector antisymmetry equations (1) to (3). This is an exactly determined problem. The solution (4) to (6) was found by co author Horst Eckardt using computer algebra. If more equations are added to the set of three equations (1) to (3) there is no solution because the problem becomes over determined. Horst and I discussed this point and are agreed. The ECE2 equations of magnetostatics are eqs. (7) to (10). So the well known material vector potential A may be found for any material current density using Eq. (10). In general this must be done by computer, but there are well known analytical solutions such as the circular current loop and magnetized sphere. Having found A, the vector spin connection is found from Eqs. (4) to (6), so omega x A can be calculated for any material J. Conservation of antisymmetry combined with del B = 0 implies that there exists a spacetime, vacuum or aether current density J(vac) defined by Eq. (17). So J(vac) can be computed from Eq. (17). The vacuum current density contributes to the total magnetic flux density B through Eq. (14), so a magnetic flux density is induced in material matter by spacetime, Q. E. D. Similarly, an electric field strength is induced by spacetime in the patented and replicated Ide circuit and the new circuits of UFT382 and UFT383 (UFT311, UFT321, UFT364, UFT382, UFT383), QED. I will now write up UFT386. In the standard model the spin connection does not exist and there is no vacuum current density, contrary to observation. Therefore given any material current density, the vacuum current density can be computed. The latter induces an extra magnetic flux density not present in the standard model (Maxwell Heaviside theory). A similar theory can be developed for ECE2 electrostatics as in immediately preceding UFT papers and notes. From Eq. (17) the vector spin connection is the link between the material vector potential A and the vacuum current density.

### Posted UFT366, Final version of PECE2

Tuesday, August 29th, 2017Readings of this book are strongly recommended of course. It will now go for printing.

To: EMyrone@aol.com

Sent: 29/08/2017 07:22:02 GMT Daylight Time

Subj: Re: FOR POSTING AS UFT366: Final version of PECE2 bookPosted today

Dave

On 8/21/2017 12:46 AM, EMyrone wrote:

Many thanks to all concerned! The final monograph is a significant advance in knowledge and is a challenge to many aspects of the standard model of physics. Particular thanks are due to Douglas Lindstrom, Robert Cheshire, Russ Davis and Steve Crothers for helping to fund the production. Therefore is an important chapter ten by Ulrich Bruchholz on his theory of elementary particles, a theory that is able to calculate elementary particle masses where the standard model fails, and a landmark chapter eleven by Stephen Crothers on the refutation of the fundamentals of Big Bang and black hole theory, combined with criticisms of the Planck theory. This chapter complements criticisms of the Planck theory in the Evans / Morris papers on www.aias.us and www.upitec.org We must question in order that we may understand. Finally the book was collated, edited, and mainly funded by Dr. Horst Eckardt, who has made many fundamental contributions of his own in the last twelve years or so.

Sent: 20/08/2017 18:43:58 GMT Daylight Time

Subj: Final version of PECE2 bookDear authors,

I finished editing of the book. Please check that you chapters are

completely valid and let me know if something needs to be changed.Best regards,

Horst

### Graphics for paper 386

Tuesday, August 29th, 2017These are very interesting graphics as usual, especially the spin connections, which do not exist in the standard model, and which are fundamentally important to ECE2 , a generally covariant unified field theory. This is again excellent work by co author Horst Eckardt. Wit the use of Maxima it does not matter if formulae get very complicated, because they can be reduced to clear graphics. Therefore it has been proven that magnetostatics requires antisymmetry laws and conservation of antisymmetry. The latter is a rigorous requirement of physics, a new and important discovery. The standard model of electrodynamics violates antisymmetry, and therefore must be improved and upgraded to the ECE2 level. The understanding of how to obtain energy from spacetime is based on a knowledge and mapping of spin connections. This another major advance in physics.

To: EMyrone@aol.com

Sent: 28/08/2017 19:43:09 GMT Daylight Time

Subj: Graphics for paper 386I succeeded in computing all quantities for the magnetic current loop.

The formulas are highly complicated but it worked with the combination

of independent antisymmetry equations and components of omega x A in

the same way as for the far field dipole.

The figures are:

Fig. 1 – Fig. 3: magnetic far field dipole

Fig. 4 – Fig. 7: magnetic current loop

Fig. 8 – Fig. 12: special potential example, giving a constant magnetic

field.In particular we should compare Figs. 3 and 6. The far field dipole is

like the electric dipole, the current loop field is dipole-like but in

the plane are two cuts through the conducting line. The current density

(Fig. 7) changes direction at the loop.The spin connection has planes with diverges in all examples. For the

third example, the two components B1 and B2, resulting in a constant

field B, are quite complicated and there are also currents cancelling

each other.

Horst

### Daily Report Sunday 27/7/17

Tuesday, August 29th, 2017The equivalent of 85,622 printed pages was downloaded (312.176 megabytes) from 1,907 memory files downloaded (hits) and 515 distinct visits each averaging 3.4 memory pages and 6 minutes, printed pages to hits ratio of 44.90, top referrals total 2,291,707, main spiders Baidu, Google, MSN and Yahoo. Collected ECE2 3934, Top Ten 2373, Collected Evans Morris 891, Autobiography volumes One and Two 706, Barddoniaeth (Collected Poetry) 636, F3(Sp) 585, Collected scientometrics 579, Collected Eckardt / Lindstrom 236, Principles of ECE 209, Evans Equations 126, Collected Proofs 115,Engineering Model 101, UFT88 99, PECE2 79, CEFE 60, MJE 59, UFT311 54, PECE 50, UFT321 46, UFT321 46, SCI 43, Llais 41, 83Ref 39, UFT313 43, UFT314 57, UFT315 67, UFT316 30, UFT317 58, UFT318 27, UFT319 60, UFT320 47, UFT322 47, UFT323 35, UFT324 61, UFT325 49, UFT326 34, UFT327 25, UFT328 51, UFT329 44, UFT330 31, UFT331 47, UFT332 37, UFT333 34, UFT334 39, UFT335 52, UFT336 37, UFT337 22, UFT338 33, UFT339 31, UFT340 35, UFT341 52, UFT342 33, UFT343 52, UFT344 47, UFT345 46, UFT346 49, UFT347 68, UFT348 71, UFT349 37, UFT351 50, UFT352 69, UFT353 60, UFT354 87, UFT355 69, UFT356 58, UFT357 59, UFT358 61, UFT359 55, UFT360 54, UFT361 48, UFT362 52, UFT363 81, UFT364 66, UFT365 62, UFT366 79, UFT367 55, UFT368 71, UTF369 58, UFT370 72, UFT371 63, UFT372 59, UFT373 65, UFT374 70, UFT375 45, UFT376 41, UFT37752, UFT378 62, UFT379 48, UFT380 66, UFT381 47, UFT382 81, UFT383 70, UFT384 47, UFT385 22 to date in August 2017. College of Engineering and Computing University of South Carolina AIAS Fellows; City University Hong Kong general; University of Cambridge UFT100, AIAS Staff, publications; International Peace Bureau Namibia general. Intense interest all sectors, updated usage file attached for August 2017.

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