To End A Little Bit Of Confusion

When there is a Lorentz-Four-Contraction that is applied upon a given arbitrary two-dimensional superstring of discrete energy permittivity, there is one general strand that works to form the topology of the so-eluded-to holonomic substrate (the said superstring) -- with one partition from within the mappable tracing of its Ward-Neumman bounds.  When the Lorentz-Four-Contraction that is applied upon the same given two-dimensional superstrings is two, there are two general strands, of which are basically of just a curved nature, that work to form the  topology of the so-eluded-to holonomic substrate -- with two partitions from within the mappable tracing of its Ward-Neumman bounds.  The more that the given arbitrary two-dimensional superstring of discrete energy pemittivity is  Lorentz-Four-Contracted, the more general strands that work to form the topology of the so-eluded-to holonomic substrate, and, as well, the less of a curved nature that would then work to make-up the topological phenomenology of the so-eluded to holonomic substrate.  So, if the so-stated two-dimensional superstring bears a Lorentz-Four-Contraction of 3*10^8, the 3*10^8 general strands that work to make-up the topology of the holonomic substrate -- being the given arbitrary two-dimensional superstring of discrete energy permittivity --  will then here be of a linear nature that approximates a closed-loop phenomenology,  except that the general strands will here be curved, as is the natural space-time-curvature that would naturally be applied to the Ward-Caucy bounds -- as to where the locus of the said superstring is at over any  proscribed given arbitrary covariant group metric.  To Be Continued!  'Till Tommorow!  Sam Roach.