Course 3 on Lorentz-Four-Contractions, Session 11, Part 2

Now, if a phenomenon has a trillion closed strings, and these all traveled in a unitary Cartesian direction at .8c, all of the strings of the given phenomenon would be .6 of their normal length in the direction of the phenomenon's motion, the mass index of all of the closed strings of that phenomenon would multiply by 1 and 2/3 relative to an observer standing still, which would increase the measurable mass of the overall phenomenon by a factor of 1 and 2/3. The time elapsed for the phenomenon in general would be .6 that of what an observer would have observed along the side of its trajectory. Open strings, being vibrating hoops in the substringular, amount to no mass even though every superstring has a mass index associated with it, since open superstrings account for just kinetic energy that is not in the form of electromagnetic energy. Electromagnetic energy consists of photons, and photons are comprised of certain bosonic superstrings. Bosonic superstrings are vibrating hoops of topological substance. Things that have no mass do not change in mass. Certain closed strings, and all closed strings are bosonic superstrings, cause mass. Thus, these closed strings that cause mass change in mass when they differentiate in the globally distinguishable relative to light. (Course 4 is on The Substringular Verses the Globally Distinguishable.) Any change in action relative to a constancy in light is a differentiation relative to light. So, whenever a closed string accelerates or decelerates in the confines of our three-dimensional delineation, its Newmann parameters change relative to a stationary observer. (This would only be if the given stationary observer were able to perceive of the moving phenomenon.) Newmann parameters are the physical boundaries of a phenomenon before you take derivatives of the motion of the phenomenon.)