Added Torque Towards Cohomology-Related Generation

Let us consider two different mass-bearing orbifold eigensets -- of which are then to work to bear a Majorana-Weyl-Invariant-Mode, which is thereby super conformally invariant at an internal reference-frame. Each of these said given arbitrary orbifold eigensets, are here to be in the process of being translated through a Lagrangian, at an external reference-frame,  by a Legendre homology -- at a relatively high rate of speed.  Both of said such orbifold eigensets are here to work to bear both the same relativistic mass, as well as the Ward-Cauchy-related condition -- that both of such said orbifold eigensets are here to work to bear the same relativistic transversal velocity, when this inferred transversal velocity is here to be considered, as relative to the motion of electromagnetic energy.  Next, let's say that both of these respective given arbitrary eigensets, are to be transferred at such a so-eluded-to velocity -- over the same duration of an evenly-gauged Hamiltonian eigenmetric, -- in a manner that is simultaneous, via the vantage-point of a central conipoint.  One of these just mentioned mass-bearing orbifold eigensets, is to simply be in the process of being translated in a transversal manner, over the proscribed time that is being implied here; whereas -- the other mentioned mass-bearing orbifold eigensets, is to be in the process of being translated in a manner that is both of a transversal nature and of a radial nature, over the proscribed time that is being implied here.  That orbifold eigenset of the two, that has been discussed in this case, that is here to bear both a radial and a transveral motion -- over the course of its projected trajectory, which is over the same duration of time, -- will then tend to work to bear an added tense of torque, than the other said orbifold eigenset.  This will then work to help at tending to cause this said respective eigenset -- that is here to work to bear a greater tense of torque than the other of the two said respective eigensets, to then act, in so as to work to generate more cohomology over time, than the other orbifold eigenset that is being discussed here.  When one is then to consider a reverse-fractaled-out condition, of the just mentioned cohomology being translated into a tense of charge, -- this will then mean, that this may then elude to the condition, that the said orbifold eigenset of such a respective given arbitrary case, that is here to bear an added tense of torque, than the other of such inferred eigensets, to where this will then tend to potentially work to help at forming a greater scalar magnitude of charge generation over time, at a relatively speaking more macroscopic level than the subatomic level, than the other of the two different said orbifold eigensets.  To Be Continued!  Sam Roach.