Let us initially consider a mass-bearing cohesive set of discrete energy quanta, that is here to be working to form the mappable tracing, of a De Rham cohomology. If both the said mass-bearing cohesive set of discrete energy quanta, As Well As the given arbitrary particular Legendre (co)homology, that is here to be working to kinetically transfer the said set of discrete energy that is of such a case, are to both bear the general physical condition, of being of an isotropically stable nature, then, it will follow, that the resultant Lagrangian-based flow of motion, that is in this particularly mentioned case, to be directly associated with the mapping-out of a De Rham cohomology, will then consequently have a greater chance of working to bear the general physical condition of being of a homeomorphic nature, than if both the mass-bearing cohesive set of discrete energy that is here to be transferred, And, that Legendre (co)homology, that is here to be in the respective process of working to kinetically transfer it, through its correlative Hamiltonian operand, were to otherwise Not be of an isotropically stable nature. To Be Continued! Sincerely, SAMUEL ROACH. (1989).
No comments:
Post a Comment