![]() Fig. 987.230 |
987.230
Symmetries #1 & 3; Cleavages #1 & 2
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987.231
Of the seven equatorial symmetries first employed in
the progression of self-
fractionations or cleavages, we use the tetrahedron's
six mid-edge poles to serve as the
three axes of spinnability. These three great-circle
spinnings delineate the succession of
cleavages of the 12 edges of the tetra-contained octahedron
whose six vertexes are
congruent with the regular tetrahedron's six midedge
polar spin points. The octahedron
resulting from the first cleavage has 12 edges; they
produce the additional external surface
lines necessary to describe the two-frequency, non-time-size
subdividing of the primitive
one-frequency tetrahedron. (See Sec.
526.23, which describes
how four happenings' loci
are required to produce and confirm a system discovery.)
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987.232
The midpoints of the 12 edges of the octahedron formed
by the first cleavage
provide the 12 poles for the further great-circle spinning
and Cleavage #2 of both the tetra
and its contained octa by the six great circles of Symmetry
#3. Cleavage #2 also locates
the center-of-volume nucleus of the tetra and separates
out the center-of-volume-
surrounding 24 A Quanta Modules of the tetra and the
48 B Quanta Modules of the two-
frequency, tetra-contained octa. (See Sec.
942
for orientations
of the A and B Quanta
Modules.)
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![]() Fig. 987.240 |
987.240
Symmetry #3 and Cleavage #3
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![]() Fig. 987.241 |
987.241
Symmetry #3 and Cleavage #3 mutually employ the six-polar-paired,
12
midedge points of the tetra-contained octa to produce
the six sets of great-circle
spinnabilities that in turn combine to define the two
(one positive, one negative) tetrahedra
that are intersymmetrically arrayed with the common-nuclear-vertexed
location of their
eight equi-interdistanced, outwardly and symmetrically
interarrayed vertexes of the
"cube"__the otherwise nonexistent, symmetric, square-windowed
hexahedron whose
overall most economical intervertexial relationship
lines are by themselves unstructurally
(nontriangularly) stabilized. The positive and negative
tetrahedra are internally trussed to
form a stable eight-cornered structure superficially
delineating a "cube" by the most
economical and intersymmetrical interrelationships of
the eight vertexes involved. (See
Fig.
987.240.)
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![]() Fig. 987.242 |
987.242
In this positive-negative superficial cube of tetravolume-3
there is combined
an eight-faceted, asymmetric hourglass polyhedron of
tetravolume-l½, which
occurs interiorly of the interacting tetrahedra's edge
lines, and a complex asymmetric
doughnut cored hexahedron of tetravolume 1½, which surrounds
the interior
tetra's edge lines but occurs entirely inside and completely
fills the space between the
superficially described "cube" defined by the most economical
interconnecting of the eight
vertexes and the interior 1½-tetravolume hourglass core.
(See Fig. 987.242E987.242E.)
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987.243
An illustration of Symmetry #3 appears at Fig.
455.11A.
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987.250
Other Symmetries
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987.251
An example of Symmetry #4 appears at Fig.
450.10. An
example of
Symmetry #5 appears at Fig.
458.12B.
An example of Symmetry #6 appears at Fig.
458.12A.
An example of Symmetry #7 appears at Fig.
455.20.
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987.300
Interactions of Symmetries: Spheric Domains
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987.310
Irrationality of Nucleated and Nonnucleated Systems
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987.311
The six great circles of Symmetry #3 interact with
the three great circles of
Symmetry # 1 to produce the 48 similar-surface triangles
ADH and AIH at Fig.
987.21ON.
The 48 similar triangles (24 plus, 24 minus) are
the surface-system set of the
48 similar asymmetric tetrahedra whose 48 central vertexes
are congruent in the
one__VE's__nuclear
vertex's center of volume.
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![]() Fig. 987.312 |
987.312
These 48 asymmetric tetrahedra combine themselves into
12 sets of four
asymmetric tetra each. These 12 sets of four similar
(two positive, two negative)
asymmetric tetrahedra combine to define the 12 diamond
facets of the rhombic
dodecahedron of tetravolume-6. This rhombic dodecahedron's
hierarchical significance is
elsewhere identified as the allspace-filling domain
of each closest-packed, unit-radius
sphere in all isotropic, closest-packed, unit-radius
sphere aggregates, as the rhombic
dodecahedron's domain embraces both the unit-radius
sphere and that sphere's rationally
and exactly equal share of the intervening intersphere
space.
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987.316
With the nucleated set of 12 equi-radius vertexial
spheres all closest packed
around one nuclear unit-radius sphere, we found we had
eight tetrahedra and six Half-
octahedra defined by this VE assembly, the total volume
of which is 20. But all of the six
Half-octahedra are completely unstable as the 12 spheres
cornering their six square
windows try to contract to produce six diamonds or 12
equiangular triangles to ensure
their interpatterning stability. (See Fig.
987.240.)
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987.324
When the tetrahedron is unity of tetravolume-1 (see
Table
223.64), then (in
contradistinction to the vector-radiused VE of tetravolume-20)
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![]() Fig. 987.326 |
987.326
This positive-negative tetrahedron complex defines
a hexahedron of overall
volume-3__1½ inside and 1½ outside its intertrussed system's
inside-and-outside-vertex-defined domain.
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987.327
Repeating the foregoing more economically we may say
that in this hierarchy
of omnisymmetric primitive polyhedra ranging from I
through 2, 2 , 3, 4, 5,
and 6 tetravolumes, the rhombic dodecahedron's 12 diamond-face-midpoints
occur at the
points of intertangency of the 12 surrounding spheres.
It is thus disclosed that the rhombic
dodecahedron is not only the symmetric domain of both
the sphere itself and the sphere's
symmetric share of the space intervening between all
closest-packed spheres and therefore
also of the nuclear domains of all isotropic vector
matrixes (Sec.
420), but the rhombic
dodecahedron is also the maximum-limit-volumed primitive
polyhedron of frequency-l.
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| Next Section: 987.400 |