Force-Fields are sets of inter-laced braided steady-state electrostatic eigenstates, that are Not super-conformally invariant at an internal reference-frame. TO BE CONTINUED! SINCERELY, SAM ROACH.
Showing posts with label force-fields. Show all posts
Showing posts with label force-fields. Show all posts
Tuesday, February 15, 2022
Sets Of Inter-Laced Braided Steady-State Electrostatic Eigenstates -- Not Super-Conformally Invariant -- Force Fields
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eigenstates,
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force-fields,
inter-laced,
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steady-state,
super-conformally invariant
Saturday, May 9, 2020
A Lesson About Permittivity And Impedance
The Main Influence that is to be formed by the point-commutative force, is the i*PI(del) Action. The i*PI(del) Action, indirectly helps to work to allow for the conservation of homotopic residue. Consequently; the i*PI(del) Action indirectly works to allow for the substringular-related proximal local presence of discrete energy permittivity. Furthermore; the Main influence that is to be formed by the force of pressurized vacuum, is the condition of force-fields. Such just mentioned force-fields, indirectly help to work to form the needed multiplicit gauging of the Polyakov Action. The multiplicit condition of force-fields, also indirectly helps to work to allow for the substringular-related proximal local presence of discrete energy impedance. Such a general case in the multiplicit presence of the inferred metric-gauge-related force-fields, is basically equivalent to the condition of the quotient of the Majorana-Weyl-Invariant-Mode when divisible by the i*PI(del) Action. Sam.
Tuesday, September 24, 2019
Here's Why The Seven Main Influences Are As These Are
Here's why the seven main influences of physical nature upon reality, are as these are:
1) Ideas, or, Thought -- Works to allow for any semblance of order or reality.
2) Force-Fields -- Works to allow for any physical interaction.
3) The i*PI(del) action -- Works to allow for the existence of prolonged physical interaction.
4) The Majorana-Weyl-Invariant-Mode -- Works to allow for the existence of mass.
5) Charge -- Works to allow for there to be an attraction between the various masses.
6) Inertia -- Works to allow for the kinetic motion of attracted mass-bearing phenomenology.
& 7) Entropy -- Works to allow for enough disorder to occur, so that a re-organization of a multiplicit resultant order may consequently occur.
1) Ideas, or, Thought -- Works to allow for any semblance of order or reality.
2) Force-Fields -- Works to allow for any physical interaction.
3) The i*PI(del) action -- Works to allow for the existence of prolonged physical interaction.
4) The Majorana-Weyl-Invariant-Mode -- Works to allow for the existence of mass.
5) Charge -- Works to allow for there to be an attraction between the various masses.
6) Inertia -- Works to allow for the kinetic motion of attracted mass-bearing phenomenology.
& 7) Entropy -- Works to allow for enough disorder to occur, so that a re-organization of a multiplicit resultant order may consequently occur.
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charge,
entropy,
force-fields,
i*Pi(del) Action,
ideas,
inertia,
thought
Sunday, September 22, 2019
More As To The Embedding Of Chern-Simons Invariants
When Chern-Simons Invariants are to be embedded upon the holonomic substrate of the force of pressurized vacuum, -- this tends to work to form force-fields.
When Chern-Simons Invariants are to be embedded upon the holonomic substrate of the point- commutative force, -- this tends to work at helping to form the i*PI(del) Action.
When Chern-Simons Invariants are to be embedded upon the holonomic substrate of the strong force, -- this tends to work to help at forming the multiplicit Majorana-Weyl-Invariant-Mode.
When Chern-Simons Invariants are to be embedded upon the holonomic substrate of the electromotive force, -- this tends to work to help form, what may be generally thought of as being charge.
When Chern-Simons Invariants are to be embedded upon the holonomic substrate of the weak force (spontaneous radioactive decay), -- this tends to help at working to form entropy as a whole.
To Be Continued! Sincerely, Samuel David Roach.
When Chern-Simons Invariants are to be embedded upon the holonomic substrate of the point- commutative force, -- this tends to work at helping to form the i*PI(del) Action.
When Chern-Simons Invariants are to be embedded upon the holonomic substrate of the strong force, -- this tends to work to help at forming the multiplicit Majorana-Weyl-Invariant-Mode.
When Chern-Simons Invariants are to be embedded upon the holonomic substrate of the electromotive force, -- this tends to work to help form, what may be generally thought of as being charge.
When Chern-Simons Invariants are to be embedded upon the holonomic substrate of the weak force (spontaneous radioactive decay), -- this tends to help at working to form entropy as a whole.
To Be Continued! Sincerely, Samuel David Roach.
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charge,
Chern-Simons Invariants,
entropy,
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holonomic substrate,
i*Pi(del) Action,
static
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