Archive for August, 2011
Friday, August 26th, 2011
Feed: Dr. Myron Evans
Posted on: Friday, August 26, 2011 10:30 AM
Author: metric345
Subject: Analysis by Marion and Thornton
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Friday, August 26th, 2011
Feed: Dr. Myron Evans
Posted on: Friday, August 26, 2011 7:19 AM
Author: metric345
Subject: Another test of EGR
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Friday, August 26th, 2011
Feed: Dr. Myron Evans
Posted on: Friday, August 26, 2011 1:10 AM
Author: metric345
Subject: 193(8): The Parabola and Conic Section in Cartesian Coordinates
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Tuesday, August 16th, 2011
Feed: Dr. Myron Evans
Posted on: Monday, August 15, 2011 1:14 AM
Author: metric345
Subject: 192(3), Final Version: m(r) Function for a Precessing Ellipse
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Thursday, August 11th, 2011
Feed: Dr. Myron Evans
Posted on: Thursday, August 11, 2011 6:57 AM
Author: metric345
Subject: Artwork by Robert Cheshire from the Precessing Ellipse
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Thursday, August 11th, 2011
Feed: Dr. Myron Evans
Posted on: Thursday, August 11, 2011 6:53 AM
Author: metric345
Subject: Artwork from the Precessing Ellipse and Logarithmic Spiral
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Thursday, August 11th, 2011
Feed: Dr. Myron Evans
Posted on: Thursday, August 11, 2011 3:57 AM
Author: metric345
Subject: 192(5): Comparison of Solar System and Whirlpool Galaxy m(r) Functions
These are given in this table, and are similar functions, suggesting that the dynamics of the solar system and whirlpool galaxy have an underlying cause, i.e. a new cosmology based on ECE theory. The next note will develop this theme in terms of
m(r) = 2 – exp(2exp( r / R))
obtained from the correct torsional geometry with a single antisymmetric connection. Various analytical curves can be used to produce their own m(r) functions in spherical spacetime. In UFT 108 the binary pulsar was considered, a precessing ellipse spiralling inwards. This also has its own m(r) function and is a precessing ellipse with alpha getting smaller, where 2 alpha is the latus rectum, a characteristic of the ellipse. Ray Delaforce and Horst Eckardt could graph this function. It is, for a fixed eccentricity epsilon:
r = alpha(r) / (1 + epsilon cos(x theta))
where alpha decreases with r. For example
alpha = alpha sub 0 exp ( – r / R0)
where R0 is a characteristic radial length. This ought to be a precessing ellipse spiralling inwards and that can be checked graphically. Its m(r) function can then be found.
a192ndpapernotes5.pdf

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Thursday, August 11th, 2011
Feed: Dr. Myron Evans
Posted on: Wednesday, August 10, 2011 5:42 AM
Author: metric345
Subject: 192(2): Proof that General Relativity does not give a Static Ellipse
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Thursday, August 11th, 2011
Feed: Dr. Myron Evans
Posted on: Wednesday, August 10, 2011 7:37 AM
Author: metric345
Subject: 192(3) : Einsteinian GR never produces a precessing elliptical orbit
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Monday, August 8th, 2011
Feed: Dr. Myron Evans
Posted on: Monday, August 08, 2011 3:51 AM
Author: metric345
Subject: 192(1): Simple Angular Velocity Test of General Relativity
This is a suggestion for an angular velocity (omega = dtheta / dt) test of general relativity by measuring to maximum precision possible the change in angle theta over time t of an object such as the moon, and measuring the distance to the moon directly with a laser. Repeat all around the orbit. According to the standard model the result should en eq. (10). However the correct result is
m(r) = omega r squared / y
where
y = L c squared / E = constant of motion
a192ndpapernotes1.pdf

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