Showing posts with label plasma. Show all posts
Showing posts with label plasma. Show all posts

Monday, December 20, 2021

One Way Of Perceiving A Tense Of Tesla Energy

 One way of perceiving a tense of Tesla Energy -- Is:

From within the Ward-Cauchy-Related bounds, of a molecular-like medium, in which it may be propagated through; Tesla Energy may be thought of as being: The electro-plasma-related result, of a heuristically dispersed high energy electrodynamic current of "free-charge," in which the initial high energy electrodynamic current mentioned here, is to work to bear a multiplicity of branched-out Lagrangian-Based cohomological spurs, to where the initial De Rham cohomological setting of the said high energy electrodynamic current, is to spontaneously work to bear the tangential flow, of the multiplicity of a recursive externally propagated anharmonic set of electrodynamic delineations, that is here to be transferred in a Dolbeault-Related manner, to where such an eletro-plasma-related phenomenology, is here to interact with the external environment through which it is here to be propagated into,to where it is to often tend to form the multiplicity, of a metaphorical kinematic spatial translation, of a "laser-like fire." SAMUEL ROACH.

Monday, May 22, 2017

The Last Part Of Session 4 Of Course 20

Heat may be conveyed via convection, by annharmonic motion, which transfers heat energy through a produced differential in heat energy -- as may be measured by a temperature difference.  This may be observed by examples, such as both the strike of a match, the motion of different regions of water that work to individually bear different temperatures that touch each other, and thus, transfer a differential of heat energy, the temperature differentials of different gases that touch each other, the annharmonic motion of chemical energy that may also work to transfer heat energy, as well as other general genre of heat transfer.  The latter mentioned specific respective case, as to the transfer of heat energy, happens in part, -- because the annharmonics that exist between certain interactive chemicals, works to produce fire, which is chemical heat -- and fire is in part comprised of electromagnetic energy that exists here in particular in the form of heat or infrared energy, in such a manner by which the chemicals that are burning as fire in such a general case, are to exist here in the form of the various respective given arbitrary forms of the plasma of such a scenario.  Since heat is electromagnetic energy, that is here to be next to most commonly thought of as electromagnetic energy after white light, heat is to then exist almost everywhere where there is the presence of matter in our universe.  All electromagnetic energy works to scatter at some time, as I will continue to make even clearer soon in this course.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Thursday, May 4, 2017

The third Part Of The 4th Session Of Course 20

In general, heat may be transferred in three basic genre of manners:  Heat may be transferred by either radiation, and/or by convection, and/or by conduction.  So, in one general case, heat may be introduced into a given arbitrary area or region, simply by the implementation of an opening -- by which there may then be more of a viable scalar amplitude of a heat differential to thence be produced -- to where one may take a slant, as to this potentially being a case of either a condition of radiation, and/or of a condition of convection, and/or of a condition of conduction.  Heat may also be introduced into a given arbitrary area or region, via the resultant effects of the shining of any directly corresponding black body source (a black body, in physics, is an entity that absorbs and/or radiates a lot of heat), that is to thereby to then behave in so as to radiate infrared energy into the so-stated generally speaking given arbitrary area or region.  Heat may be transferred into a region, as well, by a chemical means of either a plasma and/or of a molecular-based differential -- to where this may then be considered as a general case of the transference of heat by the means of convection.  And heat may be transferred into a given arbitrary area or region, by a valence charge differential, -- to where this may then to be considered as the general example of the case, as to heat being transferred via the general means of conduction.  All temperature changes are related, in some manner or another, to a transfer of some sort of heat differential-based perturbation of the infrared energy that is proximal to a certain general locus of an area or region.  Heat is an actual general phenomenology.  "Cold" is NOT an actual phenomenology. (Back to basics).  What "cold" is, is a relatively low scalar amplitude of heat.  I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.