Harmonic/Anharmonic Spin-Orbital Momentum Of Mass-Bearing "Teams" Of Discrete Energy

 Let us initially consider a given arbitrary kinematic spatially transferred  gyrating Noether-Based mass-bearing cohesive set of discrete energy quanta, that is to work to bear a certain tense of a constant transversal velocity over time, even though it is to be accelerated, on account of the physically proscribed conditions, that since it is gyrating, it is here to be constantly altering in its direction, over time. (An acceleration, is when there is to be a eminent tense of changes, in either the speed And/Or the direction, of a particular physical phenomenon.) Anything that is to be gyrating, will thereby work to bear a viably associated set of spin-orbital conditions. This  more harmonic that the consistently incurred effect of such a tense of a spin-orbital momentum is to behave, in the course of the transferable inferred Fourier-Related-Progression, that is of the recursively kinematic spatial translation of such an earlier stated mass-bearing cohesive set of discrete energy quanta, over the span of the earlier inferred duration of a proscribed tense of time, the more viable of a charge-related output, that such an inferred "team" of mass-bearing discrete energy quanta, will consequently tend to be tangentially emitted, in such a manner that is here to tend to be delineated relatively outward and away, from the bearings of its cohomology-related Lagrangian-Based flow, as this is here to be initially produced, by the multiplicity of a general tense, of a given arbitrary internal covariant kinematically transferred motion of the said "team" of mass-bearing energy quanta, that is here to work to bear the general tense, of a relatively piecewise continuous iterative gauge-related-action, in which the directly corresponding Chern-Simons Invariants are here to be consistently altered, due to a constant change in direction, that such an electrodynamic current-related flow is to be exhibiting in its physical display -- as it is here to be "tugged"into the path of its correlative Lagrangian-Based motion. (Again; You see: Chern-Simons Invariants are only "invariant," when the "team" of discrete energy quanta  of such a given arbitrary case, are to be maintaining the exact same speed and direction all of the time, in its relation to the motion of electromagnetic energy.) TO BE CONTINUED! SINCERELY, SAM ROACH.