Pages

Friday, May 19, 2017

Transitioning between book1 and book 2 part 1 (note I've changed the name but not the content of this post)

Today I hit the half-way point in the edit of the second edition of book 1.
As you can imagine, there is increasing overlap with book 2, although I try to keep the two separate.
There is a lot going on as the universe tries to distract me from finishing the project but since I may or may not have that luxury (certainly this isn't putting any food on the table); I share with you, in celebration of hitting the half way mark; a portion of the section dealing with curvature of space.
In this section, the ideas from book 2 on the arising forces from ct change (see the book, since you were too lazy to give any comments) are applied to the curvature equations and analysis of book 1.
Spoiler alert:  The last paragraph is the one with the big bang in it.
Enjoy:
a)     Curvature changes from one ct state to the next.  The preferred formula for pi in AuT is:
Pi=n+(from 2 to max x)N/F(pix)
f(pix)=[(-1)^x]+[2x(-1)^x-1]
note this is a type of the f-series (x and x-1); it is also a reflection of following out along positive and negative spirals outward from a central point.
Pi is considered to be a function of separation as well as the overall value of x, but is driven by the primary equation.
N changes according to the amount of coordinate compression for the given value of N.
b)     The relevance of the order of solution to defining location is fixed by the mechanism of stacking the two prior universes to get the next universe.  
c)     The closer two solutions occur together the closer the proximity; diverging and converging spirals ensures separate points may come together.  The sharing of ct1 states in particular ensures higher CT states can remain together for very long periods.  The longest carriers are multiples of the life of any intermediary period between big bangs because of exponential stacking in F-series solutions to make carriers.
d)     This separation is important because the solution for any intersection of any two spirals of pi for that intersection involves both the separation (based on the order in which the solutions are solved) and amount of information possible based on state of the proximate information in question.  The basic equation for gravity m1*m2/r^2 averaged over the entire universe is relevant to the inquiry but it is solved with a Lorentz equation so that distant solutions can have a disproportionate effect.  Because of the density (16^32) of information in black holes two black holes separated by galactic distances might have a greater effect on one another than the matter in between just as two bodies of matter have a greater effect on one another notwithstanding the wave, photonic and space effects between them.
e)     The equations defining pi for different ct spiral states are suggested by the size and direction of the phase shift related to coordinate change.  This could result in a reversal of the calculation process which is not considered likely but is worth setting out:
Ct1 -1+1/3-1/5+1/7….
Ct2 2-2/3+2/5-2/7…
Ct3 -3+3/3-3/5+3/7…
Ct4 4-4/3+4/5-4/7…
Ct5 -5+5/3-5/5+5/7
While pi builds in this fashion, Pi=n+(from 2 to max x)N/F(pix), when measuring it, a backwards look might make more sense given the strength of the more highly compressed ct5 state.
Perhaps the most important part of this, covered in more detail in book 2, is that the electromagnetic force seems to result from ct2 being exposed to pi from ct4; the weak nuclear force (slowed emf) is caused from having ct2 exposed to pi from ct5; and the strong nuclear force results from ct3 being exposed to pi from ct5.  The exact mechanism for this is the variation in the geo function for solutions where a certain concentration achieves a critical concentration inflection point.

The second edition of book 1 should be available by June 1, in the interim, please enjoy book 2 and this blog.


No comments:

Post a Comment