Friday, February 12, 2010

Course 2, Session 15

The Mobius Twist completing itself of a tori-sector-range integrates at the local neighborhood where the residue reaches the center state of stringular homotopy of that tori-sector-range. This is because the indices of supplementation between the fields of the residue and the fields of the mini bases of light bear a maximum potential at the relative locus that is delineated there thru the concurrence of their differential metrics, taken as a group time dependent differential that sways as a sub-energy metric. Once the Mobius Twist singularizes at the given locus, the strings "find their places" and the residue of these strings move toward the center state of stringular homotopy of the given tori-sector-range while other residue searches for a "home" among other strings of that sector. Recycling indices are then exchanged, and the strings are free to "inhale" and dissociate.
As said before, the "inhaling" is the reappropriation of homotopic delineation after the "exchanging", or the release of residue by the strings. when the strings dissociate, the residue flow is desingularized. this action desingularizes the Mobius Twist by freeing up the transpiration of the metric that was prior in a state of static equilibrium. The breaking up of the stringular condition of superstrings into point particles is through equal and opposite reaction to a force acting in the opposite direction. For instance, if I took all of the air out of a balloon, it would collapse inward. Likewise, when the strings of a tori-sector-range dissociate, the given basis of ligt folds in while breaking down into mini bases of light. This dissingularization opens up the path operand of the Mobius Twist that completes itself to allow it to propagate as many miniature particles. This is fascilitated by the increase of surface area of the given Basis of Light. When the singularized Basis touches a string via an abelian and direct yet unborne tangency via mini strings, this string is illuminated prior to iteration.
When electromagnetic waves of Planck Phenomena (mini bases of light), which are Planck Phenomena that fluctuate between their electric and magnetic field in a manner that obeys the right hand rule, touch a physical phenomenon, that physical phenomenon is illuminated during an iteration. This touch helps scatter the Planck Phenomenons locus because it allows for a path for recycling norm and ground states. As the mini traces move without singularizing, these are globally scattered to their subsequent locus and distribution along the ultimon. When these bases singularize at all during instanton, this when these quantize. So, for every 10^(-43) second, some light from a substringular beam is scattered, and some light from a subsringular beam is quantized. This does not mean, however, that a specific globally distinguishable beam is scattered at every locus of the beam every second even, since light in the vacuum of space is often unscattered. Photons are interchanged with indistinguishable difference. This means that photons of the same nature replace each other in our realm all of the time in various loci. The described Planck Phenomena are the field trajectory of the bosons which act as the discrete permittivity eigenstates of photons, since these given Planck Phenomena are the discrete impedance eigenstates of photons.
A photon is a photon. Anything illuminated scatters light. scattered light indicates that it is being "recycled." Recycled light means recycled phenomena. and recycled phenomena allows there to be any phenomena at all. The recycling of substringular phenomena is due to Cassimer Invariance.

No comments: