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Tuesday, July 15, 2014

NLT-the next step Part 34: PRE-EQUATION ANALYSIS: COMPRESSION, SCALE AND BLACK HOLES (2 OF 2 SCALE)

I'm listening to a new book on tape.  It is a good book, but it would be impossible for me to sound as pompous as the author who is also reading his book.  Now I am not complaining, because I'm enjoying the subject matter as well as the presentation.  Ah, but if I could only sound as pompous as that, but it is impossible without an English aristocrat's accent.
I know you are thinking that I seem totally bombastic, but I can't "sound" that way.  The guy reading his book, now he can sound pretentious and annoying in that special, British way.
It's about the Atlantic Sea, traveling, especially on the sea and I'm traveling again.  But it makes it sound like only stuffy, pretentious people know how to travel right or maybe they are the only ones who should be allowed to travel, I'm not far along enough to get the ambiance of the novel.  It's nice to be a distance swimmer while reading a book about the sea.  During the long, empty spans of water; the stories of the sea drift in and out like a tide.

But you're here to get the second part of the Scale section, so here it is:

Any transition that is used in this example may well turn out to be “staged” so that the scale is doubled at any stage. The solution of the exact transition steps (e.g. gravity-photonic-electromagnetic energy-nuclear forces with clock time-unknown forces associated with CT5) is a primary question of inquiry. While it is “assumed the corresponding change is known (one dimension-two dimension-three-dimension-clock time) we should not rule out that a less obvious transition takes place nor should we discount the possibility that dimensional and time changes are staged, such as a three dimensional framework without spin and one with spin or singular three dimensional frame work (or singular two dimensional framework) to multiple three dimensional (or two dimensional) frameworks.
From a scale perspective, if we ignore possible staging, if we have consistent compression, and if we're looking at d2-f2 to d3-f3 having a scale of c^2 and d2-f-2 to d4-f4 being on the scale of c^4. Mass doesn't exist at these scales and neither does standard clock time, but since time is conserved the potential for both coordinates to change with a corresponding drop in the other coordinate rates of change remains for each quantum point.
The point charge along a single vector (vectors being dimension, the creation of space/time can be viewed from one of these at a time) can be viewed as F(e)=(q/4pier^2)r' where q=electric charge, r is the position (in terms of x, y and z), r' is the unit vector of r (for one set of positions).
Going back one step (the creation of space and gravity from time going non-linear d1+f1 to d2+f2) you can assume F(g)=m(-GMr'/r^2).
The scales of transition where r corresponds to c applies only to CT3 to CT4 transitions in theory.
According to NLT these vector numbers change according to the distance (size of coordinate change) between them which are, for CT(0) to CT(1) seen as planck length changes, suggested to be on the scale of the square of plank lengths. The reason these transitions are hard to see. They are really small, but they should still be quantum changes.   
Existence defined by NLT can be shown in this equation: P(d1+f1, d2+f2,d3+f3,d4+f4)dt where the forces are negative numbers in this representation. Positive and negative have an unusual relationship in non-dimensional space and determining how they should be viewed is a part of the undertaking.
Time is non linear dt=0.
Time goes non linear (step one in the big bang) and d1 + f1 is no longer zero since the time coordinates for both change.
P(d1+f1)dt which is a function of m(-gmr'/r^2) for gravity and therefore for space; dt=zero for all the other d(s) and f(s).
When space transitions into energy, p1(d1+f1)=p2(d1+f1,d2+f2)dt, f2 being photon force that is created from space having 2 dimensions.

Next we'll get to rotational movement, but that will have to wait till later.

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