Course 2, Session 13

We are now going to examine what the tori sector for a given world-tube looks like during the metric in which the strings that were encoded for that sector during the occurring iteration are in their singularized form. The strings that form here form in either an instantaneous moment or else these form in a sequence of arrival that may include some instantaneous impulse eigenvalues in terms of the achieved locus of the given strings as well as the push that these strings delineate toward their surrounding neighborhoods. If new strings that were not included in the tori sector in the previous iteration were to become integrated within that tori sector during what would be a current iteration, then the metric neighborhood in which the strings would form would probably not be instantaneous. Yet, as the strings of the given tori sector are homotopically formed within the Caucy boundaries of that sector, the sway of the commuting residue from each string is pulled to the center state of string homotopy in such a way that all of the residue that does not become re fed back into other strings reaches the center state instantaneously relative to each overall world-sheet of each of the strings as those strings "inhale" again by taking in that unwanted Real residue that forms a wave mode that opens an operand that allows these strings to have minimal resistance in recycling the ultimon. The strings of a world-tube are one and two dimensional. There are six Royal Arc world-tubes that are tangent in the Continuum. These world-tubes are half-circles that majorize into semicircle tubes that also circle the Continuum. There are three sets of tubes, each set consisting of one tube "above" another. These sets are connected by Mobius Twists that twist back upon itself via the bases of light, the heterotic string, and the encodement strings. This causes there to be two sides to the general morphology. Each tori sector half has one Mobius Twist associated with it. If you integrate the tori sector out to both tangent world-tubes and their similar ones on the bottom, these four world-tubes share one covalent set of Mobius Twists whose one sidedness is undone by the Bases of Light, the main heterotic strings, and the encodement strings. And the "tori sector" as described here is a more general way of looking at a tori sector. The metric as to when the other two sets of world-tubes related also allow their strings to leave their quaternion is also the same instant. Each world-tube is involved by one "quarter." Once the residue is received by all four, it goes to the top of the arc newly instantaneously (or to the relative bottom). The recycled ground residue at that "top"becomes a raw material for norm state waves. Here, some of it begins on what will be a joining to become norm states. I will not go into all of the details now, yet, I will say this. What changes into norm states goes along a figure-eight path, and what goes back into ground againg follows a Chi path. The residue that reaches the figure-eight path travels in its "lane", "up" to the "top" of the Arc. As quickly as the Arc went to the "top", it goes to the other side of the Chi. This is basic idea behind the recycling of differential geometries.