Sunday, March 21, 2010

Course 3 on Lorentz-Four-Contractions, Session 12, Part 1

Strings move to form themselves and larger objects/phenomena. When strings move, they may move either dependently, independently, or interdependently with certain other superstrings. If a group of strings move in such a way that a certain specific string needs the action of the other strings, even though the other strings have no direct need for that individual string, then the given individual string is dependent on the group of strings that it is associating with in the course of its kinematic differentiation. (If a string ceased to differentiate kinematically, it would cease to exist.) If a string moved around in such a fashion so as to not need the direct influence of certain other arbitrary strings as part of what would allow it to exist as a stringular entity at all, then the given individual string that I mentioned would be independent of any of the stated arbitrary strings in terms of direct influence. This Independence would mean that, although everything has some relationship to everything else, the string mentioned above would not be directly interacting with and influenced by certain other strings. If a string is dependent upon other certain strings yet not interdependent upon them, then the other strings would be able to maintain their shape and behavior without the other individual strings. If a set of strings were interdependent, then the set of such strings would need each other to allow for the maintenance of their shape and behaviours in general. I will conclude with the purpose of this session with my next post.

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