The Fourteenth Session of Course 13 On Stringular Transformations, Part one

One and two-dimensional superstrings may both have a swivel shape at various different times.  For a one-dimensional superstring, such a swivel shape is like the basic vibrating strand of an open string, except that the said string curves in a sinusoidal manner into a general format of a general condition of a curved standing wave at the respective iterations of instanton -- in which such superstrings are topologically delineated under the general condition of being shaped in a swivel-like manner.  For a two-dimensional superstring of discrete energy permittivity, such a swivel-based shape of a vibrating hoop of phenomenon is like the basic round shape of a closed string, except that the given arbitrary string here curves in a sinusoidal timeless-based mapping of topology into a general format of a curved standing wave at the respective iterations of instanton in which such superstrings are topologically delineated under the general condition of being shaped in a swivel-like manner.  The counterstrings of a one-dimensional superstring that are swivel-shaped are also curved in a sinusoidal-based manner, except that the said sinusoidal-based curvature of the said counterstring of the mentioned one-dimensional superstring that is swivel-shaped are 90 degrees out of phase with the sinusoidal-based curved standing waves of the said one-dimensional strings that are topologically delineated under the general condition of being shaped in a swivel-like manner.