When a mass-bearing discrete quantum of physical energy, is to work to exhibit a relatively strong tense of permittivity, this general condition will tend to reverse-fractal, into the existence of mass-bearing cohesive sets of discrete energy quanta — that are consequently to result, in tending to Externally display a relatively strong scalar magnitude of charge per time (amperage). Furthermore; when a mass-bearing discrete quantum of physical energy, is to work to exhibit a relatively strong tense of permeability, this general condition will tend to reverse-fractal, into the existence of mass-bearing cohesive sets of discrete energy — that are consequently to result, in tending to Externally display a relatively strong scalar magnitude of energy per charge (voltage). The microscopic condition of increased “amperage,” may often reverse-fractal into the physical condition, by which a physical entity, at the vantage-point of a much larger scale of measurement, may then tend to work to bear a stronger fractal modulus. Furthermore; the microscopic condition of increased “voltage,” may often reverse-fractal into the physical condition, by which a physical entity, at the vantage-point of a much larger scale of measurement, may then tend to work to bear a stronger elastic modulus. Consequently; a strong tense of super string-related energy permittivity, may often tend to be able to reverse-fractal, in a vast manner, into the presence of a strong tense of fractal modulus. Furthermore; a strong tense of super string-related energy permeability, may often tend to be able to reverse-fractal, in a vast manner, into the presence of a strong tense of elastic modulus. SAM.
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