986.870 Nuclear and Nonnuclear Module Orientations
986.871 The rhombic triacontahedron may be fashioned of 120 trivalently bonded T Quanta Module tetrahedra, or of either 60 bivalently interbonded positive T Modules or of 60 bivalently interbonded negative T Modules. In the rhombic triacontahedron we have only radiantly arrayed basic energy modules, arrayed around a single spheric nuclear-inadequate volumetric domain with their acute “corners” pointed inwardly toward the system’s volumetric center, and their centers of mass arrayed outwardly of the systemergo, prone to escape from the system.
986.872 In the tetrahedron constructed exclusively of
986.8721 In the case of the rhombic dodecahedra we find that the centers of volume of their half-Couplers’ A and B Modules occur almost congruently with their respective closest-packed, unit-radius sphere’s outward ends and thereby concentrate their energies at several spherical-radius levels in respect to a common nuclear-volume-adequate centerall of which suggests some significant relationship of this condition with the various spherical-radius levels of the electron “shells.”
986.873 The tetrahedron and octahedron present the “gravitational” model of self-and-otherness interattractive systems which inherently provide witnessable evidence of the systems’ combined massive considerations or constellations of their interbindings.
986.874 The highly varied alternate A and B Module groupings permitted within the same primitive rhombic dodecahedron, vector equilibrium, and in the Couplers, permit us to consider a wide spectrum of complexedly reorientable potentials and realizations of intermodular behavioral proclivities lying in proximity to one another between the extreme radiational or gravitational proclivities, and all the reorientabilities operative within the same superficially observed space (Sec. 954). All these large numbers of potential alternatives of behavioral proclivities may be circumferentially, embracingly arrayed entirely within the same superficially observed isotropic field.