Sound/Heat -- Synapsis --- Harmonic/Anharmonic Strain -- Yin(g)/Yang

 When a tense of sound, is to bear an eminent spontaneous covariant interdependent incursion, upon the quantized energy per charge, that is here to be proximal local, to the general region of a set of those synapsis, that are here to belong to the nervous system of a biological entity, this may, at times, be potentially capable, of tending to work to facilitate, the formation of a harmonic strain, upon its immediate surroundings, as this is here to be potentially imparted, upon the thought energy of such a said biological entity, -- to where, such a harmonic strain, that is here to be embellished upon the said thought energy of the nervous system, of such an inferred life form, may consequentially have at least some sort of potential tendency, of working to facilitate, the thence tangentially propagated covariant kinematically delineated presence, of what may here be thought of here, as the kinematically flowing phenomenology of Yin(g). It follows, that; When a tense of heat, is to bear an eminent spontaneous covariant interdependent incursion, upon the quantized energy per charge, that is here to be proximal local, to the general region of a set of those synapsis, that are here to belong to the nervous system of a biological entity, this may, at times, be potentially capable, of tending to work to facilitate, the formation of an anharmonic strain upon its immediate surroundings, as this is here to be potentially imparted, upon the thought energy of such a said biological entity, -- to where, such an anharmonic strain, that is here to be embellished upon the said thought energy, of the nervous system of such an inferred life form, may consequentially have at least some sort of potential tendency, of working to facilitate, the thence tangentially propagated covariant kinematically delineated presence, of what may here be thought of here, as the kinematically flowing phenomenology of Yang. I WILL CONTINUE WTIH THE SUSPENSE LATER! SAMUEL ROACH.

Incurred Electrodynamic Pressure

 Let us initially consider two different and distinct analogous covariant charges, that are here to each be initially equivocally conducted, through two different and distinct respective analogous individually taken circuitry paths, as this is here to be mathematically considered, over the course of a dual tense, of a respective Fourier Transformation. Both of such tenses of covariant circuitry paths, are to have the same "electrodynamic pressure," applicably incurred upon them, when individually taken. One of such inferred tenses of current, is to be basically left alone. The other of such inferred tenses of current, is to have a heightened tense of entropy, applicably incurred upon it (which often works to imply added heat applied). That kinematically exhibited electrodynamic circuitry path of current of the two, that is here to have a heightened tense of applicable entropy, that is here to be incurred, upon the the general flow of the multiplicity of topological manifold of those moving charges, of which are here to work to form the more entropic electrodynamic current of the two, will consequently often tend to have a greater resistivity and a lower conductivity, than the other of the two individually taken kinematically exhibited electrodynamic circuitry paths of current. I WILL CONTINUE WITH THE SUSPENSE LATER! TO BE CONTINUED! SAM ROACH.