As To The Substringular About The Exchange Of Electrons

How about if we consider here -- what is going on in the substringular, when one or more electrons are exchanged in an ionic manner -- from one given arbitrary atom, to a respective other given arbitrary atom in time and space.  Let us then consider -- in this specific given case -- one extra atom that is from one initially negatively charged atom, that is being pulled, in an ionic manner, (due to one excessive electron in its valence shell), into the Ward-Neumman bounds of another atom -- that is initially positively charged, due to a lack of one electron in its respective valence shell.  This situation would here, in this given case at hand, involve the exchange of one negative charge of one electron volt from one atom (1.6*10^(-19) of one Coulumb of negative charge) -- to another atom, that initially bears a positive charge of one electron volt (1.6*10^(-19) of one Coulumb) of positive charge.  Initially, with the so-stated beginning valence charges, that would here exist before the so-eluded-to ionic exchange of one electron from one atom to another atom -- there would be, subtended and stemming from the initially stated negatively-based one electron volt, that is from the initially stated atom, a Njenhuis valence  charge of one negatively-based Imaginary electron volt -- that would be both orphoganal to both the respective given arbitrary Real Reimmanian Plane -- that the said charge is being pulled through, in a Lagrangian-base manner, while also being orphoganal to the directoral-based wave-tug/wave-pull of the J (S+L), by which what is here meant as a tangency that works to bear a stemming from the specific Laplacian-based directoral-based overall angular momentum, that may be mapped-out from the projection of the trajectory of the Hamiltonian-based activity of the field of the said initially stated negatively-charged electron volt of field-based disturbance.  Likewise, there will be a similar but different situation for the propagation of the so-eluded-to positively-based electron volt -- that would stem from the initially stated positively charged atom of this scenario.  There would be a Njenhuis valence charge of one Imaginary-based electron volt -- that would stem from both the here relatively Real Reimmanian-based field, as well as stemming from the directoral-based wave-tug/wave-pull of the overall angular momentum of J (S+L), by which is here meant as a tangency that works to bear a stemming from the specific Laplacian-based Hamiltonian operation of the field-networking -- that may here be mapped-out from the second stated atom of such a case -- when in terms of the electrodynamic field of the said initially stated positively-charged electron valence field-based disturbance.  Once the said ionic-based charges are exchanged -- then, as well, the respective given arbitrary Njenhuis-based valence charges are negated -- in so as to work to conform to what is here, a relative conservation of charge.
I will continue with the suspense later! To Be Continued!  Sincerely, Sam Roach.