Some Relations Between Static Force and Flow

The fractal of a static friction that exists as the entity of the oscillating discrete permittivity along the topology of superstrings works to act as the modulae that works to allow superstrings to be able to move through the Hamiltonian operands through which the said strings move in order to go from one spot to another.  The fractal of a kinetic friction that exists as the entity of the oscillating discrete impedance along the topology of Fadeev-Popov-Trace eigenstates works to act as the modulae that works to allow the mentioned discrete units of energy impedance to be able to move through the Hamiltonian operands through which the said phenomena of discrete energy impedance move in order to go from one spot to another.  When a superstring becomes more of a "swivel"-like shape, the mentioned fractal of static friction that acts as a holonomic substrate bears less of a holomorphism of blockage when in terms of the Hamiltonian operand in which it is projected through, allowing such a superstring to be less inhibited by the amplitude of the Ricci Scalar via the entity of the Rarita Structure.  This lack of physically-based inhibition works to allow less of a graviational limitation to the directly related superstring, thereby producing more of a potential for a conversion fom Noether Flow to tachyonic flow.  The inverse condition that directly relates to the lack of inhibitions of certain given arbitrary Fadeev-Popov-Trace eigenstates likewise works to allow less of a limitation for the eluded to discrete units of energy impedance from keeping these from moving into a state of tachyonic flow.  The more that a superstring is swivel-like shaped, the more of a tendancy for its directly related Fadeev-Popov-Trace eigenstates to also become tachyonic over the same duration in which these directly link in such a manner that these may be converted from a Noether Flow into a tachyonic flow.  So, the less the fractal of static friction in superstrings, the less the fractal of kinetic friction in its corresponding Fadeev-Popov-Trace eigenstates.  This goes for both bosonic strings (closed strings) and fermionic strings (open strings).  I will continue with the suspense later!
Sincerely, Sam Roach.