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.
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