Gauge-Invariant Topological Manifold

 When a compact Hamiltonian Topological Manifold, is to be physically transmitted through a smooth Lagrangian, while yet not acting to bear any Chern-Simons-Related Spurs, when being in the general process of this, that it will consequently tend to spontaneously occur, that the discrete energy impedance, that is here to be eminently corroborative, with the reductional process of such a respective case scenario, will tend to be gauge-invariant. 

An interstellar craft, that is round at its base, when beginning in the proximal local field, of an Anti-Gravitational field, ideally wobbles at both ends, of all four Minkowski-Associated coni axions, by a subtended angling, of ~28.274334 degrees, when preparing for the spontaneous formation, of an artificial worm-hole, yet; An interstellar craft, that is round at its base, when beginning in the proximal local field, of a Heuristic-Gravitational field, on earth, ideally wobbles at both ends, of all four Minkowski-Associated coni axions, by a subtended angling, of ~29.9792458 degrees, when preparing for the spontaneous formation, of an artificial worm-hole.This is interesting, on two different accounts: 1) On a vacuum on earth, light travels at Exactly 2.99792458*10^8 meters per second. &, 2) The apex of the pyramid of Giza, from Egypt, is at a latitude, of Exactly 29.9792458 degrees North Latitude. 

The less entropic, that a given arbitrary tense, of electrodynamic circuitry, is to be, the more likely, that the eminently corroborative net charge, of which is here to be flowing through, such a respective tense of electromotive circuitry, will entail the general likings, of a gauge-invariant flow — to where the eminently associated Hamiltonian Topological Manifold, of which is here to act, as the emanating source, via which such a respective net charge, is thence to be implicitly kinematically propagated on account of, will thereby spontaneously tend to bear the general condition, of exemplifying the reductional characteristics, of the resultant demonstrative exhibition, of behaving as a gauge-invariant topological manifold. 

Decreased energy of heat transport per Kelvin Mole, as exhibited by an eminently corroborative, kinematically propagated, Hamiltonian Topological Manifold, may often tend to spontaneously increase the likelihood, of the covariant proximal local presence of gauge-invariance, to thereby be viably existent, from within the respective Ward-Cauchy Bounds, in which such an implicit team of mass-bearing discrete energy quanta, is here to be in the general process, of being kinetically transferred, over a time span. 

The greater that the number of filled energy levels, in terms of electric shells, is hereupon to be, that there are here to be spontaneously present, in the eminently associated conductor, of the implicit energy levels, of which are in covariant proximal local association, with the electromotive circuitry, when this is taken in terms of the electrodynamic charge-based holonomic substrate, that is here to be of the Hamiltonian Topological Manifold, of which is here to be of the magnetic energy that is kinetically transferred through the conductor, via electromotive current, as taken over the duration in which the net charge, of the implicit cohesive team of magnetic mass-bearing energy eigenstates, is here to be spatially transmitted along, over time, through the structural entity that it is here to be transferring physical conduction into, that it will therefore often tend to occur, that both the entropy level will consequently tend to be lowered, as well as that the electromotive resistance will also thereby also tend to be lowered. This just implied general tendency, will consequently tend to spontaneously enhance the expectation value, that is here to be eminently involved, in increasing the chance that the earlier mentioned Hamiltonian Topological Manifold, will thus be more likely to behave, as a gauge-invariant topological entity. 

The number, of what are termed of as being Landau Lines, is tantamount to being equivocal, to the number of filled energy levels, that are proximal local in covariant association, with the latent physical conditions of the conductor, of which is to bear an electrodynamic transmission, of the charges that are to be delineated, by the eminently corroborative, kinematically propagated Hamiltonian Topological Manifold, in so as to facilitate the generation of an electromotive current, of which is here to act to convey, a corroborative tense of electrical information. 

If and when a particular isotope of a material, is to innately act to bear a relatively high number of filled electrodynamic energy levels — to where the distributional delineation of the implicitly spontaneous consequential eminently corroborative conductive bands, are here to be homogeneous in its covariant electromotive assortment, then, it will often tend to consequently occur, that such a material, may therefore tend to exhibit both a relatively strong fractal modulus & a relatively strong elastic modulus, at the same time. Also as optimal; Such an implicit material, will also tend to bear relatively low electromotive resistance, — particularly at low temperatures, since low temperatures often work to involve a lowered energy of heat transport, lowering entropy. 

Highly conductive materials, that are to spontaneously have homogeneous delineated energy levels distributed within them, will often tend to have the general tendency, of exhibiting an enhanced capacity, of being able to express a relatively strong spring constant, to where, invasive phenomena that may tend to otherwise be potentially hazardous to the externalized structure of a given arbitrary construct, that is to be externally comprised of such an implicit material, will therefore spontaneously be less viably detrimental to the structural integrity of such an implied resilient material, due to not only the relatively strong fractal and elastic modulus hereby present, yet, also, since a strong spring constant, may cause incoming potentially treacherous phenomena, to have an enhanced capacity, of simply rebounding off of the externalized structure of such an implicit material, due to the mentioned strong spring constant, as taken at its outer boundary. 

Highly insulative materials, that are here to exhibit a homogeneous distributional delineation of their electron "clouds," may often tend to work to exhibit, a relatively strong tense, of an elastic modulus.

The greater that the density of electron shells is to be, as taken into consideration, for a molecular structure, the higher that its fractal modulus, will consequently tend to be. 

The more homogeneous that the distributional delineation of electron shells is to be, as taken into consideration, for a molecular structure, the higher that its elastic modulus, will consequently tend to be. 

The more homogeneous that the distributional delineation of electron shells is to be, for a molecular structure, that is to exhibit a relatively high density of such respective electron shells, the greater that its eminently corroborative spring constant, will consequently tend to be. 

I call the general tendency of potentially recursively stabilized structural integrity, that is here to be appertaining, to the reductional effectual physical attributes, of eminently corroborative materials, that work to exhibit an unusually high spring constant, “Homotopic deformation incursion counterbalance.”

The Fourier-Related-Progression, of a net phenomenology, that works to bear, a relatively strong, Homotopic deformation incursion counterbalance, will often tend to result, in thus expressing, a relatively strong, resonant pulsation. 

Repulsion-Related Force Exhibited By Hamiltonian Operator

 The Yukawa Coupling, between the current of a given arbitrary Hamiltonian Operator, with its net discrete energy impedance, often work to be eminently associated, with the repulsion-related force, that is here to be exhibited, by the said Hamiltonian Operator.(Just as, at a reverse-fractal level, amperage has the general tendency, of pulling phenomenology towards a given arbitrary source of electricity;While voltage has the general tendency, of pushing phenomenology away form a given arbitrary source of electricity.)(1989.THANKS FOR READING!) TO BE CONTINUED! SINCERELY, SAM ROACH. 

The more stable that the equipoise is to be, between a tense of sound that is tangentially generated, as spontaneously incurred upon an eminently corroborative tense of resonant vibration, the more harmonically delineated, that the resultant transversal motion, will consequently tend to be — to where such an implicitly generated Lagrangian, will thus tend to be more efficient, over its course of motion. 

Current

 The Yukawa Coupling, between the i*PI(del) Action of a given arbitrary Hamiltonian Operator, as taken with the net resonant frequency of that self-same Hamiltonian Operator, when coupled with its frequency of kinetic motion, may tend to work to form the current, of the herein mentioned Hamiltonian Operator. SAM.

Flow Of Magnetic Charge

 The permittivity of the flow of magnetic charge, works to form current (charge per time). And; The impedance of the flow of magnetic charge, works to form resistance (energy*time per charge squared). The dot product of the permittivity of the flow of magnetic charge, With the impedance of the flow of magnetic charge, works to form voltage, (energy per charge). TO BE CONTINUED! SINCERELY, SAMUEL DAVID ROACH. 

My Current Perspective -- The Largest Viable Number

 To my current perspective -- WHEN ONE INCLUDES BOTH NEGATIVE VALUES AND ZERO, the largest numerical value that means anything, is:

[[2*e^[(infinity)^8^(infinity)^8 ]]+ 1].

Please let this sink in, before you reply. I would LOVE to hear any thoughtful replies to this! 

Sincerely, SAMUEL DAVID ROACH. (PINCKNEY, MI; U OF M; WCC; EMU).

Unbraided Cohomology

 When two different given arbitrary covariant sources of charge, have degenerated each other's magnetism, this general tense of a kinematic activity, over the durational course of a Fourier-Related-Progression, will have the general tendency, of working to unbraid that respective dual cohomology, that was here to be represented, by the charge-based flow, that was here to be of the two different and distinct covariant sources of magnetic current, of which the two different individually taken given arbitrary respective initial sources of charge, had been exhibiting at the start of this, via the initially inferred dual magnetic display of electrodynamic flow, of which was here to be attributable, to the covariant electrostatic kinetic base of action, of which these two different and distinct interdependent implied sources of current, had initially been demonstrating amongst themselves, at the onset of this particular general type of a case scenario. SAMUEL DAVID ROACH. I WILL CONTINUE WITH THE SUSPENSE SOON! LATER FOLKS! (1989).

When An Electrodynamic Current Is De-Generated

 When a given arbitrary electrodynamic current is being de-generated, such an inferred proximal local electrodynamic current, over the general durational course of such a respective process, may often tend to be consequently working, to exhibit the physical nature, of the display of a p-Adic cohomology. Sam.

Highly Magnetic Current -- Tightly Braided Cohomology

 The greater that the scalar amplitude of the magnetism is to be, for an electrodynamic current, the more tightly braided, that the directly associated superstring-related cohomology will tend to be. Samuel Roach.

Mainly Harmonic Metric-Gauge-Related Eigenstates Of Perturbative Chern-Simons Invariants -- High Conduction Of Current

 When an electrodynamic current is to involve the general flow of a tense of charged particles, that are here to be a set of individually taken Noether-Based mass-bearing cohesive sets of discrete energy quanta, that are here to be working to exhibit the functional output, of a respective set, of basically only harmonically flowing metric-gauge-related eigenstates, that are here to be generated, by the respective tense of the directly corresponding harmonic output, that is here to tangentially flow relatively outward, from the proximal local presence of those perturbative Chern-Simons Invariants, that are here to bear the inferred tendency, of a continually covariant kinematic state of an incurred recursive state of alteration, due, in part, to a respective continual alteration in the kinematic direction of its spin-orbital momentum, will tend to result, to where this whole general type of a process, is to often have the general tendency, of working to bear a relatively efficient tense, of a conductive electrodynamic flow, of those stated charged particles, that are here to be kinematically transferred, by the general facilitation of a relatively uninhibited tense of magnetic attraction, to where the resultant flow of such an electrodynamic current, is thereby to often generally tend to work to bear a relatively uninhibited conduction of its current-related net charge, through its respective tense of electrical-related circuitry, over a correlative respective duration of time. SAMUEL.

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.

More, As To Braided Cohomology Of Electrodynamic System

 The more braided that the cohomology of an electrodynamic system is to be, the more efficient that its directly associated current will consequently tend to be. TO BE CONTINUED! SINCERELY, SAMUEL.

Electrodynamic Gaussian Braided Deformative Flow

 The magnetic flux of a physical current of charge, may potentially be described of as working to express:

The Electrodynamic Gaussian Braided Deformative Flow of a correlative kinematic covariant interdependent interaction, of a directly corresponding set of cohomological eigenstates. SAM ROACH.

Homeomorphic Noether-Based Current -- Stronger Electrical Current

 The more homeomorphic that the Noether-Based Current is to be, as appertaining to the flow of a given arbitrary covariant set of electrons, as such a said flow of electrons (electricity) -- which is here to be physically transferred, through a respective given arbitrary electrical circuitry -- the stronger that the consequentially resultant directly corresponding current of electricity will therefore tend to be. (SAM).

Even more intrinsically: The more homomorphic that the Noether-Based Current is to be, as appertaining to the flow of a given arbitrary covariant set of electrons, as such a said flow of electrons (electricity) -- which is here to be physically transferred, through a respective given arbitrary electrical circuitry -- the stronger that the consequentially resultant directly corresponding current of electricity will therefore tend to be. (SAM).

More As To Noether Current, In Relation To Current

 The flow of the vibrational delineation of the i*PI(del) Action, is key at helping to work to form the Noether Current -- and the reverse-fractal of the Noether Current, is the flow of charge (current). SAM.

Perturbative External On-Shell Cohomology-Related Eigenstates

 The general phenomenology -- in which there is here to tend to be the harmonic perturbation in the allocative delineation, of the external on-shell cohomology-related eigenstates, of a mass-bearing cohesive set of discrete energy quanta, as this is here to be taken at a reference-frame, that is external to the covariant spatial translation of such a herein mentioned mass-bearing cohesive set of discrete energy quanta -- helps to work to form the typified entity, of what we tend to think of as being Charge. The general process in which charge is transmitted from one spot to another, over a span of time -- helps to work to form, what we think of as being the phenomenology of Current. I will continue with the suspense! To Be Continued!Sincerely, Samuel David Roach.

A Little Bit Of An Editorial, As To A Pondering About Electrical-Related Issues

Tell me if the following makes adequate sense;

Electrodynamic Deactivation Action is equal to: (Energy Divided By (Current Cubed)).
                                                         
                                                                OR, IN OTHER WORDS, --
   
                                                                 (E/(Current^3)).;

                                                                 OR, IN OTHER WORDS, -- (E/I^3)).

                                                                 Please Let Me Know What You Think.

                                                                Sincerely, Samuel David Roach.
                                                             

Some Interesting Stuff About Charge

As an initial ansantz (as to here to be starting with something that people would generally tend to know), current is the basic relationship of charge per time.  Yet, the "equivalence" of charge, as here to be taken at an extremely small quantity of such a general genus of phenomenology, is an analogous relationship of the "i*PI(del) Action" per time.  To Be Continued!  Sincerely, Samuel David Roach.

Cohomology And Current

Another short but good one.:
Let us consider a cohomological flow, that is here to be generated over an evenly-gauged Hamiltonian eigenmetric.  This may be reverse-fractaled out, to a charge that is generated over time.  Current is charge per time.  This means -- that the generation of a cohomological flow over time, may be reverse-fractaled out to the flow of an electrodynamic current.
I will continue with the suspense later! To Be Continued!  Sincerely, Samuel David Roach.

A Special Case Of A Reverse Fractal

When superstrings of discrete energy permittivity interact with the torsional indices of the relatively proximal localized eigenstates of the centralized knotting of the Rarita Structure -- this will tend to work to form at a more macroscopic level, more of a point-based natured tense of magnetism that is in the lines with the activity of voltage -- than in the lines with the activity of current, when this is taken over time.  Yet, when the correlative Fadeev-Popov-Trace eigenstates in the substringular, work to interact with the torsional indices of the relatively proximal localized eigenstates of the centralized knotting of the Rarita Structure -- this will tend to work to form at a more macroscopic level, more of a point-based natured tense of magnetism that is in the line with the activity of current than with the lines with the activity of voltage, when this is taken over time.

As To The Fractals Of Voltage And Current

You probably know the fact that voltage is energy per charge.  You probably also know that current is charge per time.  Voltage is more related to the condition of magnetism than current is.  A magnetic field of any given arbitrary case scenario is more related to permittivity than the electric field of the same respective given arbitrary case scenario is.  An electric field of any given arbitrary case scenario is more related to impedance than the magnetic field of the same respective given arbitrary case scenario is.  Superstrings act as discrete quanta of energy permittivity.  Fadeev-Popov-Trace eigenstates act as discrete quanta of energy impedance.  Superstrings act as the basis of the particle-based nature of discrete energy permittivity.  Fadeev-Popov-Trace eigenstates act as the basis of the particle-based nature of discrete energy impedance.  The correlative counterstrings -- that are directly corresponding to the respective superstrings of any given arbitrary case -- act as the basis of the wave-based nature of discrete energy permittivity.  The correlative light-cone-gauge eigenstates that are directly corresponding to the respective Fadeev-Popov-Trace eigenstates of any given arbitrary case -- act as the basis of the wave-based nature of discrete energy impedance.  The discrete energy quanta of any given arbitrary specific case are of a lower scalar amplitude than the discrete quanta of charge.  Therefore, one is able to have a definitive quantity of discrete energy before one is to have any discrete charge at all.  Superstrings are the key to the basis of discrete energy.  Yet -- current requires the existence of at least a certain amount of charge, in order to be of any tangible extrapolation or consideration.  This works to indicate --  that the functional basis of superstrings, is more related to energy per charge than to charge per time.  The magnetic field is more of a direct correspondence to the voltage of any respective given arbitrary case scenario, than to the correlative current of the same said case.  This is why superstrings are here said to be of the nature of the discrete quanta of energy permittivity.  The electric field is more of a direct correspondence to the current of any respective given arbitrary case scenario, than to the correlative voltage of the same said case.  This is why Fadeev-Popov-Trace eigenstates are here said to be of the nature of the discrete quanta of energy impedance.  I will continue with the suspense later!  To Be Continued!  Sincerely, Sam Roach.