Let's go back to what I was saying in one post, -- when I had mentioned about metaphorically "standing" on a spinning paraboloid. Let's next say, that one was to remain perfectly still on this said metaphorical paraboloid. Consequently, you are now to be in touch with a constantly differentiating norm-vector, that is kept in the sequential pattern of the spinning of the paraboloid. Consider the rate of the spinning to be holomorphic to the surface area of the paraboloid. Consider the rate of the spinning to be maintained at a constant speed. Of course, since you are spinning, your direction is always changing, so that you are constantly accelerating. Think of the translation of phenomena that is besides yourself -- to where, again, you are staying "put" -- that was at one point touching the paraboloid, from within the physical bounds of the surface area of it, as being proportional to the differentiation in the speed of the correlative spinning. This would then mean, that the discharge from the said surface, would be transferred at a constant rate. Consequently -- since this is true for the whole topology given, it is certainly true for the potential spot at which you would be at. You are in line with a potential discharge of residue, from the surface of the paraboloid, -- which would then be a translocation of the surrounding phenomena. This would then mean, that the earlier mentioned norm-vector, that is interactive at each point along the surface, would be constant in magnitude -- although it would be constantly changing in direction. Wouldn't this mean, then, that the norm conditions of the surface area of the given paraboloid, would be constantly altering part of the correlative Cauchy-related norm conditions, while yet constantly maintaining the others? (Additional Cliffhanger).
To Be Continued! Sincerely, Samuel David Roach.
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