![]() Fig. 1032.30 |
1032.30
Complementary Allspace Filling of Octahedra and Vector
Equilibria:
The closest packing of concave octahedra, concave vector
equilibria, and spherical vector
equilibria corresponds exactly to the allspace filling
of planar octahedra and planar vector
equilibria (see Sec.
470). Approximately half of the
planar vector equilibria become
concave, and the other half become spherical. All of
the planar octahedra become concave
(see Illus.
1032.30).
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![]() Fig. 1032.31 |
1032.31
Concave octahedra and concave vector equilibria close-pack
together to
define the voids of an array of closest-packed spheres
which, in conjunction with the
spherical vector equilibria, fill allspace. This array
suggests how energy trajectories may be
routed over great-circle geodesic arcs from one sphere
to another, always passing only
through the vertexes of the array__which are the 12 external
vertexes of the vector
equilibria and the only points where the closest-packed,
uniradius spheres touch each other
(see Illus.
1032.31).
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1033.00
Intertransformability Models and Limits
[1033.00-1033.92 Involvement Field Scenario]
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1033.010
Generation of the Involvement Field in Which Synergetics
Integrates
Topology, Electromagnetics, Chemistry and Cosmology
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|
1033.011
Commencing with the experimentally demonstrated proof
that the
tetrahedron is the minimum structural system of Universe
(i.e., the vectorially and
angularly self-stabilizing minimum polyhedron consisting
of four minimum polygons in
omnisymmetrical array), we then discover that each of
the four vertices of the tetrahedron
is subtended by four "faces," or empty triangular windows.
The four vertices have proven
to be only whole-range tunable and point-to-able noise
or "darkness" centers__which are
primitive (i.e., as yet frequency-blurred), systemic
somethings (see Secs.
505.65,
527.711,
and
1012.33) having six unique angularly intersightable
lines of interrelationship whose
both-ends-interconnected six lines produce four triangular
windows, out through which
each of the four system-defining somethings gains four
separate views of the same
omninothingness of as-yet-untuned-in Universe. As subtunable
systems, points are
substances, somethings ergo, we have in the tetrahedron
four somethings symmetrically
arrayed against four nothingnesses. (Four INS versus
four OUTS.)
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1033.017
We have elsewhere reviewed the progressive tangential
agglomeration of
other "spherical" somethings with the otherness observer's
spherical something (Secs.
411.01-08)
and their four-dimensional symmetry's systemic
intermotion blocking and
resultant system's interlockage, which locking and blocking
imposes total system integrity
and permits whole-system-integrated rotation, orbiting,
and interlinkage with other system
integrities.
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1033.018
Since we learned by experimental proof that our four-dimensional
symmetry
accommodates three axial freedoms of rotation motion
(see the Triangular-cammed, In-
out-and-around, Jitterbug Model, Sec.
465), while also
permitting us to restrain3 one of
the four axes of perpendicularity to the four planes,
i.e., of the INS most economically__
or perpendicularly__approaching the tensor relationship's
angularly planed and framed
views through to the nothingness, we find that we may
make a realistic model of the
omniinvolvement field of all eight phases of the tetrahedron's
self-intertransformability.
(Footnote 3: "Restrain" does not mean motionless or "cosmically at rest." Restrain does mean "with the axis locked into congruent motion of another system." Compare a system holding in relative restraint one axis of a four-axis wheel model.) |
![]() Fig. 1033.019 |
1033.019
The involvement field also manifests the exclusively
unique and inviolable
fourfold symmetry of the tetrahedron (see Cheese Tetrahedron,
Sec.
623), which permits
us always to move symmetrically and convergently each__and
inadvertently any or all__of
the four triangular window frames perpendicularly toward
their four subtending
somethingness-converging-point-to-able IN foci, until
all four planes pass through the
same threshold between INness and OUTness, producing
one congruent, zerovolume
tetrahedron. The four inherent planes of the four tensegrity
triangles of Anthony Pugh's
model4* demonstrate the nothingness of their four planes,
permitting their timeless__i.e.,
untuned__nothingness congruence. (See Fig.
1033.019.)
The tuned-in, somethingness
lines of the mathematician, with their inherent self-interferences,
would never permit a
plurality of such lines to pass through the same somethingness
points at the same time (see
Sec.
517).
(Footnote 4: This is what Pugh calls his "circlit pattern tensegrity," described on pages 19-22 of his An Introduction to Tensegrity (Berkeley: University of California Press, 1976.) |
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1033.020
Four-triangular-circuits Tensegrity: The four-triangular-circuits
tensegrity
relates to the four great circles of the vector equilibrium.
The four great circles of the
vector equilibrium are generated by the four axes of
vector equilibrium's eight triangular
faces. Each of the four interlocking triangles is inscribed
within a hexagonal circuit of
vectors__of four intersecting hexagonal planes of the
vector equilibrium. These tensegrity
circuits relate to the empty tetrahedron at its center.
(See Secs.
441.021,
938.12, and
1053.804.)
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1033.022
The involvement field also identifies the unique cosmically
inviolate
environment domain of convergent-divergent symmetrical
nuclear systems, i.e., the vector
equilibrium's unique domain provided by one "external"
octahedron (see Sec.
415.17),
which may be modeled most symmetrically by the 4-tetravolume
octahedron's symmetrical
subdivision into its eight similar asymmetric tetrahedra
consisting of three 90-degree
angles, three 60-degree angles, and six 45-degree angles,
whose 60-degree triangular faces
have been addressed to each of the vector equilibrium's
eight outermost triangular
windows of each of the eight tetrahedra of the 20-tetravolume
vector equilibrium.
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| Next Section: 1033.030 |