Sunday, October 11, 2015

Another Interim In-Between Parts To Session 11 of Course 19 -- The Klein Bottle and Orbifold Differentiation

Let us say that one were to have a given arbitrary case scenario -- in which a given orbifold eigenset, that is moving in its Ward-Caucy-based Majorana-Weyl-Invariant-Mode, to where such a said orbifold were to have a charge of one electron volt (1.6*10^(-19) of one Coulomb) -- that would here be propagated away from its so-eluded-to Ward-Neumman bounds.  Let us say that the so-mentioned propagated charge -- was delineated, as a cross-product that would here go away from the Ward-Neumman bounds of the said orbifold eigenset, in both the here relatively holomorphic direction, and, through a discrete Lagrangian, that was here to move through what would here be the relative Real Reimmanian Plane.  This would then mean that, in such a case, there would then be a simultaneous charge (through the vantage point of a central conipoint), of one Imaginary electron volt -- being propagated in a directoral-based manner -- in both a direction that would then be both orphoganal and Njenhuis to the here relatively holomorphic direction of such an arbitrary case, as well as such an Imaginary charge being both orphoganal and Njenhuis to the discrete Lagrangian of the said propagation of the here stated Real Reimmanian charge, that is here Gliossi to the relatively Real Reimmanian Plane, that is of this here respective given arbitrary so-stated case scenario.
To Be Continued!  I will continue with the suspense later!  Sincerely, Sam Roach.

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