986.870 Nuclear and Nonnuclear Module Orientations

986.871 The rhombic triacontahedron may be fashioned of 120 trivalently bonded T Quanta Modul e tetrahedra, or of either 60 bivalently interbonded positive T Modules or of 60 bivalently interbonded negativeTModules. In the rhombic triacontahedron we have only radiantly arrayed basic energy modules, arrayed around a single spheric nucl ear-inadequate volumetric domain with their acute “corners” pointed inwardly to ward the system’s volumetric center, and their centers of mass arrayed outwardly of the systemergo, prone to escape from the system.

986.872 In th e tetrahedron constructed exclusively of24 AModules, and in the octahedron co n structed of48 Aand48 BModules, the asymmetric tetrahedral modules are in rad ical groups, with their acute points arrayed outwardly of the system and their ce nters of mass arrayed inwardly of the systemergo, prone to maintain t heir critical mass interattractive integrity. The outer sharp points of theAandBM odules are located at the centers of the four or six corner spheres defining the tetrahedron and octahedron, respectively. The fact that the tetrahedron’s and oct ahedron’sAandBModules have their massive centers of volume pointing inwardly of the system all jointly interarrayed in the concentric layers of theV E, where as in the rhombic triacontahedron (and even more so in the half-Couplers of the r hombic dodecahedron) we have the opposite condition which facts powerf ully suggest that the triacontahedron, like its congruent icosahedron’s nonnuclea r closest-possible-packed omniarray, presents the exclusively radiational aspect of a “one” or of a “no” nuclear-sphere-centered and isolated most “spheric” polyhedral system to be uniquely identified with the nonnuclear bubble, the one-m olecule-deep, kinetically-escape-prone, gas-molecules-containing bubble.

986.8721 In the case of the rhombic dodecahedra we find that the centers of vol ume of the ir half-Couplers’AandBModules occur almost congruently with their r espective closest-packed, unit-radius sphere’s outward ends and thereby concentra te their energies at several spherical-radius levels in respect to a common nucle ar-volum e-adequate centerall of which suggests some significant relat ionship of this condition with the various spherical-radius levels of the electro n “she lls.”

986.873 The tetrahedron and octahedron present the “gravitat ional” model of self-and-otherness interattractive systems which inherently pro vide wit nessable evidence of the systems’ combined massive considerations or con stellati ons of their interbindings.

986.874 The highly varied alternateAan dBModu le groupings permitted within the same primitive rhombic dodecahedron, ve ctor eq uilibrium, and in the Couplers, permit us to consider a wide spectrum of c omplex edly reorientable potentials and realizations of intermodular behavioral pr ocliv ities lying in proximity to one another between the extreme radiational or g ravi tational proclivities, and all the reorientabilities operative within the sam e s uperficially observed space (Sec. 954). All these large numbers of potential a lt ernatives of behavioral proclivities may be circumferentially, embracingly arra y ed entirely within the same superficially observed isotropic field.