Tuesday, March 30, 2010

Course 3 on Lorentz-Four-Contractions, Session 14, Part 3

Each time that a string is iterated, it forms a ghost eigenbasis in terms of the form of "imaginary" residue that the quaternionic-instanton-field-impulse-range can not use for a while in the given tori-sector. These ghosts will quantify until either the substring changes its relative tori-sector or until some of these ghosts may be reused in other strings. Light detects what light effects. So, since these ghosts are like a "sculpture" of what the strings have been and where these strings have been over the span that it takes for any detection of that string, what we really detect is the residue that that string has left behind. This is indicative of the electron. What we mainly detect of matter is the electron and its product, electromagnetic energy. Even if you could somehow detect stuff within the movement of light's transfer, (The Planck Moment), the substrings are basically constantly on the go. By understanding how strings interact relative to light helps one to see behind the mask of what strings are and how these really behave! What I have just written in this post should reveal to a greater extent than before why all motion is relative to electrodynamics.
You may ask, why are Lorentz-Four-Contractions existent based on the equations that I have shown in earlier sessions? Here is why. Light in a vacuum (where there is no matter in the way of the propagation of the light) travels at 3*10^8 meters per second. At the speed of the fastest electron, which is just under light speed, the Lorentz-Four-Contraction is 3*10^8.
So, based on what the speed of the fastest electron is and the prior conditions that I have just mentioned, Lorentz-Four-Contractions behave as according to the equations that I indicated in past sessions.
I appreciate all of the comments and all of the support provided to this blog.
I am trying to teach others.
Sincerely,
Samuel David Roach.

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