Thursday, January 29, 2015
Part One of As to the Fractal of Electric Current
So, what is the fractal of an electric current? Here is a start to an explanation of this. An electric current is a flow of electrons. What is it about any given arbitrary charge -- whether such a charge here is respectively of either a static or of a viably kinetic genus, that would here work to form the so-eluded-to electric field? The basis of all of the phenomenology that would here appertain to the multiplicit array of the eigenstates of holonomic substrate, is the condition of both the existence and the covariant activity of pointal-based phenomena. Initially, let us pervay the concept of the Heisenburg Uncertainty Principle. By the so-stated Heisenburg Uncertainty Principle, any given arbitrary point particle -- that is to be considered in any respective given arbitrary case scenario -- is an approximated extrapolation of holonomic substrate, that is viable at the Poincaire level -- that may be considered to be comprised of a segment of what is here to be a certain discrete quanta of the condensed oscillation that is existent at the general locus of whatever the general microcosmic "neighborhood" that such an eluded-to pointal-based phenomenon happens to be kinematically existent at, over time. Such a general region or neighborhood is one that may be considered to bear indices of discrete Hamiltonian operand -- when this said operand is to be considered, relative to both the Laplacian-based codifferentiability and the Fourier-based codifferentiability of both the Poincaire-based codetermination and the Lagrangian-based codetermination of whatever the so-stated or so-eluded-to pointal-based phenomena incurs, via the activity of the said point particle, over the metrical eigenbase that the said particle devolves upon -- over the correlative sequential series of instantons that directly appertain to any of such respective given arbitrary case scenarios in which this is pertinent. When one is to discuss the nature of such a so-eluded-to point particle, one may be here describing anything that may fit the directly prior general case scenario -- down to those point particles that may be thought of in any given arbitrary discussion involving string theory.
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8:30 AM
Labels:
Heisenburg Uncertainty Principle,
holonomic substrate,
instantons,
Lagrangian,
Poincaire,
superstrings
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