Friday, January 15, 2010

Course 3, Session 1, Lorentz-Four-Contractions

We live in a vast world of three observable dimensions. So, when things we can fully detect go from one spot to another, these also must move in our three-dimensional realm as these are detected as a complete entity. In order for things to happen at all, there must be an interdependent coordination of procedures that allow room for the transporation of any occurrence, yet alone the interplay between all of the different occurrences that we have a clue are happening thruout the Continuum. So, if we know all of the boundaries of an object or a phenomena physicswise, and the boundaries that limit that item within the three-dimensional delineation of our apparent realm do not include extra dimensions of space, then the other dimensions you would need to know (physicswise) in order to predict how that object will differentiate is one that measures the order of circumstances that define the procedure as to the prior, current, and subsequent arrangement of interactions that allow the static and differentiating kinematisms of the given object to differentiate as a group action period. Such an added dimension is time. Time is the procedure in which action takes place.
Our Continuum is not round. It is a toroidal disc. Our visible universe is approximately round in so far as we as people fave found, yet the Overall Physical Continuum is a lot bigger than the visible universe. Space, thence likes to curve. Whenever something moves, there is curve involved. One may add, this is because everything involves radial motion. Mmm, Yeah. Yet it is also because of the "integration of the bike" concept. What I mean is this: Remember how I explained in the last course that the different norm indices between ground and norm Or smooth curvedness and jointedness must work toward supplementation in order for the net result to be the universe having any energy at all? Well, the supplementation is linear motion. Linear motion that is delineated by radial indices which act as a basis for both its cause and effect describes the basic idea of the distribution impetus of a majorized plane. A majorized plane means that there are eigenbases of Majorana matrices that describe the path of the field of majorization. The propagation of this majorization in the operands of empty space causes this space to curve and at least bear a potential action.

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