Reverse-Polarity Of E(8)XE(8) Stringular Oscillation-Based Tendency

When the E(8)XE(8) stringular oscillation-based tendency is to reverse in its polarity, this general process will consequently tend to reverse the direction -- in which that general motion that works to cause the fortification-related activity, by which the main influences of physical nature are to be implemented, are thence to be able to happen as needed, over time. To Be Continued! Samuel David Roach.

Unorientable Strings And The E(8)XE(8) Stringular Oscillation-Based Tendency

Let's consider a mass-based orbifold eigenset.  When the superstrings of discrete energy permittivity, that work to comprise such a said eigenset, are to be unorientable -- both during any one particular given arbitrary iteration of the Betti Action, and the immediately ensuing correlative Regge Action, -- such an inferred set of strings, will then subsequently ensue to become of a tachyonic nature.  This will then work to consequently result, in a reverse-polarity of the holomorphicity of the correlative Fourier-related codifferentiable placements of those partition-based discrepancies, that are here to work to be most directly associated with the directly correlative process, of the here pertinent i*PI(del) action.  This will then work to consequently cause a reverse-polarity in the Fourier-related translation, of the directly corresponding E(8)XE(8) stringular oscillation-based tendency, -- since the E(8)XE(8) stringular oscillation-based tendency, is most associated with the eminent relationship that is here to exist -- between the Betti Action and the correlative i*PI(del) action.Samuel David Roach.

Polarity Of Legendre Homology

Let us initially consider a tense of a discrete overall quantum of Legendre homology, that is here to be delineated by the generation of the Lagrangian-related activity of an electromagnetic source.  Next, let us say that the voltage (energy per charge) that is to be directly associated with the said electromagnetic source, is to be of a positive polarity. This will then mean -- that the directoral-related angular momentum of the earlier mentioned delineated Legendre homology, will be directed as a cross-product-related operation of kinetic energy, -- to where the kinetic energy that is here to be produced by the said electromagnetic source (in the form of voltage, or, energy per charge), will here be directed relatively outward.  However, -- if the voltage is to, instead, to be directly associated with a negative polarity, then, this will mean -- that the directoral-related angular momentum of the so-eluded-to Legendre homology, will then, in this ulterior case, be directed as a dot-product-related operation of kinetic energy, -- to where the kinetic energy that is here to be produced by the said electromagnetic source (in the form of voltage, or, energy per charge), will here be directed relatively inward.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Sychronized Ward-Polarity

Let us initially say that one were to have an orbifold eigenset, that was comprised of by a relatively large number of discrete energy quanta -- as such a said given arbitrary orbifold eigenset were to be traveling over a relatively large evenly gauged metric.  The more synchronized that the Ward-Cauchy-related polarity is here to be -- when this is in consideration of the general holomorphic direction of the integration of those discrete energy quanta, that are here to work to comprise the said eigenset, when this is taken into consideration the general condition just stated alone, -- the more likely that such a respective given arbitrary eigenset is then to be able to at least approach the speed of light, over the so-eluded-to evenly gauged metric.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.