Course 3 on Lorentz-Four-Contractions, Last Test, Part 1

1) if an object is traveling along a specific axis in general at .5c, describe what strings will be contracted according to the equation I gave, which strings would not be contracted at all lengthwise as a unit, and which strings would contract moderately in the globally distinguishable.

2) Why does matter and kinetic energy contract relative to light?

3) What are the basic equations for Lorentz-Four-Contractions?

4) If an object were to travel at .8c, how would its length, width, mass, and time be effected by a stander by?

5) Why can't a mass travel at light speed if it has a Kaluza-Klein light-cone-gauge topology?

6) A perfect "X" of two strings travels in the direction of the gap between them at .8c, describe the contraction of both lines that comprise the "X." (The strings would never collide.)

7) If an object is traveling in a different direction than that direction that is changing at close to light speed, yet certain of its strings are moving at the quicker string's speed, how will that object contract quantitatively?

8) Will any spherical object Lorentz-Contract uniformally if it is traveling in one direction at less than light speed? Why?

Course 3 on Lorentz-Four-Contractions, Session 15, Part 2

Think of the speed of the object as constant once it enters the given field. The direction of the speed is the general path directoral that the object went in once it has traveled. One may predict this based on where it is planned to go. Strings that are exactly in the direction of the given arbitrary path that the object is going are contracted as normally in the globally distinguishable. Strings that are not quite in the said direction of the path bear a sense of tangency at each moment that this is measured under consideration. For instance, if one detects the observed string within 10^(-20)seconds, and the string is vibrating uniformally within the object for this whole time, then we need to detect how the direction of the string interacts with all of the summed tangential changes of the path of the object as it moves along its arched path. If the string is trigonometrically away from the path of motion of the object during the "moment", then it will be contracted less than if it is moved along the path of directoralization. Another aspect to discerning this is the degree of vibration of the given with the vibration of the object as a unit as it radially and transversely kinematically differentiates through the path operand which is where the object went in the given field.

Course 3 on Lorentz-Four-Contractions, Session 15, Part 1

Think of an object. It contains strings that are distributed throughout all 32 dimensions of the set of parallel universes that it is in. Some of the said strings cut through all 32of the dimensions. Some of the strings only exist in one dimension. The strings of the given object are thus arbitrarily assorted within any parameters which include directorals that fall in the dimensional fields that exist within the Continuum at that general region. Say, for instance, that the object given is not moving in an exact given dimension that we would call "forward holomorphically", "side-to-side", or "up-and-down." Let us think that a tangential motion relative to the earth was considered as a: Directoral axis (thickness of earth) based on a three-dimensional axes that included an earth associated axis that is tangential to it; associated, while the axis going "up-and-down" would arbitrarily be the k directoral. Let us arbitrarily define the dimensional situation and placement of the strings of the object based on the given directorals and the other 29 dimensions that one may define based upon the proscribed assortment of the directoral indices that we have shown. Make the axial size down to the discrete level of the width of a string, and the length of the axes as to include the field that defines the scope of the total range of motion of the given object. The object moves within its Ward boundaries. It does not move parallel to any of the given axes. It moves, say, in an arch that falls within the fields of each of the dimensions of the axes that define the region where the object moves. Since the object is always changing direction, it is constantly accelerating. I will conclude this session so as to relieve your suspense at a later time. I'm hoping that you can picture what I am describing in detail. If you can see a concept in your mind, the solution is clear.
Sincerely,
Samuel David Roach.