Archive for May, 2013
Saturday, May 25th, 2013
Feed: Dr. Myron Evans
Posted on: Friday, May 24, 2013 4:19 AM
Author: metric345
Subject: Munich Discussions on the B(3) Field and RFR
Pleasure, if developed, RFR could lead to ESR, NMR and MRI without magnets, and a multi billion dollar industry. The resolution is much higher, the chemical shift pattern is unique, and there is no need for expensive cooled magnets. I discussed this with both Ernst and Anderson (joint Wolf Prize winners 1990). Ernst won the Nobel Prize in 1991 for FTNMR, just as I got back to Cornell Theory Center. I lectured to Ernst’s group at ETH and he was very encouraging. With the gear available today it should be straightforward and Simon Clifford has many good ideas as usual.
To: EMyrone@aol.com
CC: simon@mrclifford.org
Sent: 24/05/2013 08:40:35 GMT Daylight Time
Subj: Re: Typo in List of RFR items
Many thanks, we discussed RFR and other experiments basing on the B(3) field here in Munich last week. Simon Clifford visited a trade show in Munich last week and met with Bernhard and me. We will continue our discussions at the conference.
Horst
Verschickt: Fr, 24 Mai 2013 7:53 am
Betreff: Typo in List of RFR items
It should be: OO446, OO572, OO582, OO585, UFT80, UFT81, UFT83, and UFT84.

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Saturday, May 25th, 2013
Feed: Dr. Myron Evans
Posted on: Friday, May 24, 2013 4:02 AM
Author: metric345
Subject: FOR POSTING: UFT242 and Background Notes
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Saturday, May 25th, 2013
Feed: Dr. Myron Evans
Posted on: Friday, May 24, 2013 11:34 PM
Author: metric345
Subject: Daily Report 24/5/13
There were 2,166 hits from 508 distinct visits, 41.9% spiders from google and MSN. Auto1 91, Auto2 42, CEFE25, Englynion 20. National University of La Plata F3(Sp); Johennes Kepler University Linz Finite Photon Mass; Xarxa State Education System Catalonia UFT168(Sp); National Vocational Training Institute Chile Essay 28(Sp); University of the Frontier Chile Connection antisymmetry (Sp); National University of Colombia UFT16; Technical University of Bolivar Colombia F12(Sp); Fujitsu Corporation United States UFT41; Audi Corporation Germany Homopolar; Oberwolfach Mathematics Research Institute UFT88, UFT102; Technical University Darmstadt UFT85; Junta de Andalucia (Andalucian Parliament) UFT160(Sp); University of Lorraine Nancy UFT88; University of Poitiers general; University of Rennes 1 UFT88; International Centre for Theoretical Physics Trieste Italy Dan8; State Education Secretariat San Luis Potosi Mexico SU2 Quantum Electrodynamics; United States National Archives general; Royal Society of Chemistry publications, Journal Leaflet; Technical University of Peru UFT144 (Sp); Power Engineering Company Bucharest Romania Johnson Magnets; Bristol University UFT149. Intense interest all sectors, updated usage file attached for May 2013.

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Saturday, May 25th, 2013
Feed: Dr. Myron Evans
Posted on: Friday, May 24, 2013 10:26 AM
Author: metric345
Subject: Kurata Process
UFT183 and UFT184 in the UFT papers section of www.aias.us summarized my analysis of the use of the B(3) field in the Kurata process. The Kurata catalytic process has resulted in full scale production in Spain, and many entries on my blog deal with this. That type of Kurata process is a faily conventional catalytic process resulting in the production of clean burning fuel from olive waste and other kinds of waste. Kurata was an AIAS Fellow and claimed that my B(3) concept could be useful in his type of process. However he never gave any convincing details and so I produced UFT183 and UFT184. Sophie Jones of GET knows all about the Spanish plants, which are described on the net.
In a message dated 24/05/2013 13:28:25 GMT Daylight Time, writes:
Dear Dr. Evans,
While trying to find some peer reviews of the Kurata Technology I seem to be getting referred back to you
as someone who understands the process.
I would like to find out more independently of what Kurata Systems say on the web site can you point me in a particular direct that may assist me
or a contact with Kurata Japan.
Thanking you,
Regards: Patsy Edgers

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Wednesday, May 15th, 2013
Feed: Dr. Myron Evans
Posted on: Wednesday, May 15, 2013 2:57 AM
Author: metric345
Subject: 242(6): Polar Angle Theta for any Planar Orbit and any Force law
This is given in eq. (22) as a function of r for any force law F(r) between a mass m orbiting a mass M. There is an unknown constant of integration x as shown, but the result is perfectly general. For simplicity it has been assumed that the constant of integration y is zero. In the Newtonian theory the area is given by eq. (4), and this is how epsilon enters the analysis. The Newtonian force law is
F(r) = – mMG / r squared
and the Newtonian L sub 0 is
L sub 0 squared = alpha m squared MG
The time T is the time for one complete orbit. For the Earth this is one year. Eq. (25) is a new diffusion equation of astronomy. The integrals in Eqs. (22) and (23) are not analytical so must be evaluated with numerical integration as done by Dr. Horst Eckardt in the last note from him. This is no problem with contemporary software and hardware. This is a completely new discovery and method in astronomy so it will take some experimentation to fine tune it. We are just at the beginning of this procedure now.
a242ndpapernotes6.pdf

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Wednesday, May 15th, 2013
Feed: Dr. Myron Evans
Posted on: Tuesday, May 14, 2013 11:25 PM
Author: metric345
Subject: Computing Note 242(5)
Many thanks very good work as usual. I would say that both constants of integration A and B have to be used to obtain the Newtonian result. I would suggest going back a little bit and checking eq. (3) of note 242(4) for t against the Newtonian result for t . I will calculate the Newtonian result for t this morning. This procedure determines the constants of integration A and B. Then having determined the constants A and B the true anomaly can be found.
To: EMyrone@aol.com
Sent: 14/05/2013 22:30:05 GMT Daylight Time
Subj: Re: 242(5): The True Anomaly for a Given Distance R between m and M for any Force
I did some calculations for this note. The outer integral is not solveable analytically for the Newton force unless the integration constant is A=0. This solution is %o12 and is plotted in %t14. This does not look like theta(R) for an ellipse.
After that I solved the integral numerically. %t24 shows a plot of the integrands for A>0, A=0, A<0. Only for A<0 the integrandremains finite, in accordance with my earlier findings for the integration constant A.
The numerical results of the integral and the function theta ~ integral / R^2 are plotted in %t35. theta drops like 1/R, also this does not look likely for an ellipse. This needs further checks and study.
The known solution (8) contains a parameter epsilon. I wonder where this comes from in the general solution (2).
Horst
Am 14.05.2013 17:50, schrieb EMyrone
This note gives some more details of the method, notably the inner integral must be an indefinite integral as in eqs. (2) and (4). The outer integral is a definite integral from 0 to R. This note also gives another baseline check of the method in the Newtonian theory, in which eqs. (1) and (9) must be the same. When the baseline checks are complete the theory may be used to compute the perihelion precession for any force and any planar orbit.
242(5).pdf

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Wednesday, May 15th, 2013
Feed: Dr. Myron Evans
Posted on: Tuesday, May 14, 2013 11:05 PM
Author: metric345
Subject: Daily Report 14/5/13
There were 1,724 hits from 508 distinct visits, 41.2% spiders from google, MSN, yandex and sistrix. Auto1 40, Auto2 20, Englynion 15, CEFE 12. Argentine Ministry of Economics and Finance Space Energy (Sp); University of Sidney UFT42, Physics Pontifical Catholic University of Chile UFT133 (Sp); Max Planck Institute for Mathematics in the Sciences Leipzig Proof 2; Students of the Universities of Bonn and BonnRheinSieg UFT88; Aarhus University Denmark UFT149; University of Wisconsin UFT171; University of Seville UFT166; IberoAmerican University Mexico UFT150(Sp); Christiana Care Health System Delaware UFT14; Wellcome Trust Sanger Institute UFT77; Physics Strathclyde University UFT88; University of Sussex Proof2. Intense interest all sectors, updated usage file attached for May 2015.

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Wednesday, May 15th, 2013
Feed: Dr. Myron Evans
Posted on: Monday, May 13, 2013 11:51 PM
Author: metric345
Subject: Checking the New Orbital Equation by Computer
We seem to have discovered a very rich new area of orbital theory. The computer is a great help, especially when controlled in the incisive way demonstrated here by co author Dr. Horst Eckardt. The new equation is a novel combination of the two orbital Lagrangian equations, which have been well known since the late eighteenth century. It is also interesting that the diffusion equation has a structure similar to the diffusion equations of Brownian motion theory such as the Fick, Smoluchowski and Kramers equations which are known to have a very rich mathematical structure and many classes of solution. These are also similar to the Schroedinger equation structure and solutions. In this theory, the precession of the perihelion is computed exactly to machine precision, so the near circular approximation is not needed. For the Newtonian potential there should be no precession of the ellipse, but for other force laws, there should be a precession. Using this method r can be computed as a function of t and t as a function of r and theta. So this method can be used for animation. It can also be applied to galaxies and used with any force law. The heavy calculational work is all done by the computer. This approach would be impossible by hand because of all the calculations.
To: EMyrone@aol.com
Sent: 13/05/2013 17:32:31 GMT Daylight Time
Subj: Re: 242(3): Equation for Theta for Any Planar Orbit and Any Force Law
I checked the analytical solution. First the original harmonic oscillator gives a real solution, but this does not matter.
In the second section the general solution is developed.
In the third section the equation is rewritten with F(r) instead of Omega.
The fourth section is a check with both constants = 0 and a constant Omega. The complex solution
r = exp(i omega t)
appears. Obviously the first constant is needed to allow for a radius scaling required for correct physical dimensions.
Setting
%k1 = – 1/2 * v0
(this is a velocity) leads to the (real) result
r = v0/omega * sin(omega t)
so we have
r0 = v0/omega.
I used the second solution, anyhow the sign seems to play a role. It is also important that %k1 is negative, otherwise a complex radius comes out.
Horst.
242(3).pdf

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Wednesday, May 15th, 2013
Feed: Dr. Myron Evans
Posted on: Monday, May 13, 2013 11:14 PM
Author: metric345
Subject: Daily Report 13/5/13
There were 2,773 hits from 519 distinct visits, 29.8% spiders from google, MSN and yandex. Auto1 46, Auto2 18, Englynion 14, CEFE 12. University of Sydney Australia UFT33; Dalhousie University Canada UFT142; Niels Bohr Institute Copenhagen University UFT33; McDaniel College Maryland UFT85; University of Wisconsin UFT177; Ecole des Ponts Paris Tech. UFT88; Alaska Weather Center UFT241; Ritsumei University Japan Overview; United States National Archives general; Piura National University Peru UFT177(Sp); Antenor Orrega University Peru Essay52(Sp), UFT32, Book Store, Life of MWE, UFT100, 200, 201, 203, 204, 209, 210, 213, 214, CEFE, Essay61(Sp); University of Cambridge UFT38; University of Southampton UFT237; Mathematics University College London UFT172, CV. Intense interest all sectors, updated usage file attached for May 2013.

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Wednesday, May 15th, 2013
Feed: Dr. Myron Evans
Posted on: Tuesday, May 14, 2013 10:05 AM
Author: metric345
Subject: Einstein Debye Theory of Specific Heats
This theory calculates the heat capacity function using the Planck distribution. Einstein assumed that all the oscillators have the same frequency and the energy of the oscillators was quantized to integral multiples of the photon h bar omega. Excitation occurs in the Einstein theory when a least amount of energy, the quantum of radiation or photon, is supplied. So the concept is similar to the photoelectric effect. Debye corrected the theory to allow for interactions. So the basic idea of the theory is similar to that of the photoelectric effect and the Compton effect, developed in ECE theory in UFT158 ff. So the same kind of development can be applied to the Einstein Debye theory. After writing up UFT242 I will probably develop the Einstein Debye theory of specific heats as requested by Kerry Pendergast. UFT158 ff have been studied intensely for a number of years. The daily report sent out each morning is just the tip of a very big iceberg with which the standard model of physics has collided. It does not know as yet that it has sunk without trace.

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