1020.00
Compound Curvature: Chords and Arcs
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1021.10
Convexity and Concavity of Tetrahedron
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1022.10
Minimum Sphere
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1023.10
Systematic Enclosure
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1023.19
Not until we have four othernesses do we have macrocosmic
volumetric
awareness. Four is required for substantive awareness.
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1024.10
What Is a Bubble?
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1025.10
Closest Packing of Bubbles
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1030.11
The sphere is a convex vector equilibrium, and the
spaces between closest-
packed uniradius spheres are the concave vector equilibria
or, in their contractive form,
the concave octahedra. In going contractively from vector
equilibrium to equi-vector-
edged tetrahedron (see Sec.
460), we go from a volumetric
20-ness to a volumetric
oneness, a twentyfold contraction. In the vector-equilibrium
jitterbug, the axis does not
rotate, but the equator does. On the other hand, if
you hold the equator and rotate the
axis, the system contracts. Twisting one end of the
axis to rotate it terminates the
jitterbug's 20-volume to 4-volume octahedral state contraction,
whereafter the contraction
momentum throws a torque in the system with a leverage
force of 20 to 1. It contracts
until it becomes a volume of one as a quadrivalent tetrahedron,
that is, with the four edges
of the tetrahedron congruent. Precessionally aided by
other galaxies' mass-attractive
tensional forces acting upon them to accelerate their
axial, twist-and-torque-imposed
contractions, this torque momentum may account for the
way stars contract into dwarfs
and pulsars, or for the way that galaxies pulsate or
contract into the incredibly vast and
dense, paradoxically named "black holes."
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1031.10
Dynamic Symmetry
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1031.14
In other words, the planar symmetrical is projected
outwardly on the sphere.
The sphere is simply a palpitation of what was the symmetrical
vector equilibrium, an
oscillatory pulsation, inwardly and outwardly__an extension
onto an asymmetrical surface
of what is inherently symmetrical, with the symmetricals
going into higher frequency. (See
Illus.
1032.12,
1032.30, and
1032.31.)
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1031.16
Asymmetry is a consequence of the phenomenon time and
time a
consequence of the phenomenon we call afterimage, or
"double-take," or reconsideration,
with inherent lags of recallability rates in respect
to various types of special-case
experiences. Infrequently used names take longer to
recall than do familiar actions. So the
very consequence of only "dawning" and evolving (never
instantaneous) awareness is to
impose the phenomenon time upon an otherwise timeless,
ergo eternal Universe.
Awareness itself is in all these asymmetries, and the
pulsations are all the consequences of
just thought itself: the ability of Universe to consider
itself, and to reconsider itself. (See
Sec.
529.09.)
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1032.00
Convex and Concave Sphere-Packing Intertransformings
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1032.10
Convex and Concave Sphere-Packing Intertransformings
as the Energy
Patterning Between Spheres and Spaces of Omni-Closest-Packed
Spheres and Their
Isotropic-Vector-Matrix Field: When closest-packed uniradius
spheres are interspersed
with spaces, there are only two kinds of spaces interspersing
the closest-packed spheres:
the concave octahedron and the concave vector equilibrium.
The spheres themselves are
convex vector equilibria complementing the concave octahedra
and the concave vector
equilibria. (See Secs.
970.10
and
970.20.)
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1032.11
The spheres and spaces are rationally one-quantum-jump,
volumetrically
coordinate, as shown by the rhombic dodecahedron's sphere-and-space,
and share sixness
of volume in respect to the same nuclear sphere's own
exact fiveness of volume (see Secs.
985.07 and
985.08),
the morphological dissimilarity
of which render them one-quantumly
disequilibrious, i.e., asymmetrical phases of the vector
equilibrium's complex of both
alternate and coincident transformabilities. They are
involutionally-evolutionally, inward-
outward, twist-around, fold-up and unfold, multifrequencied
pulsations of the vector
equilibria. By virtue of these transformations and their
accommodating volumetric
involvement, the spheres and spaces are interchangeably
intertransformative. For instance,
each one can be either a convex or a concave asymmetry
of the vector equilibrium, as the
"jitterbug" has demonstrated (Sec.
460). The vector
equilibrium contracts from its
maximum isotropic-vector-matrix radius in order to become
a sphere. That is how it can
be accommodated within the total isotropic-vector-matrix
field of reference.
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![]() Fig. 1032.12 |
1032.12
As the vector equilibrium's radii contract linearly,
in the exact manner of a
coil spring contracting, the 24 edges of one-half of
all the vector equilibria bend
outwardly, becoming arcs of spheres. At the same time,
the chords of the other half of all
the vector equilibria curve inwardly to produce either
concave-faced vector-equilibria
spaces between the spheres or to form concave octahedra
spaces between the spheres, as
in the isotropic-vector-matrix field model (see Illus.
1032.12). Both the spheric aspect of
the vector equilibrium and the "space" aspect are consequences
of the coil-spring-like
contraction and consequent chordal "outward" and "inward"
arcing complementation of
alternately, omnidirectionally adjacent vector equilibria
of the isotropic-vector-matrix
field.
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1032.13
In a tetrahedron composed of four spheres, the central
void is an octahedron
with four concave spherical triangular faces and four
planar triangular faces with concave
edges. This can be described as a concave octahedron.
In an octahedron composed of six
closest-packed spheres, the central void is a vector
equilibrium with six concave spherical
square faces and eight triangular faces with concave
edges: a concave vector equilibrium.
The vector equilibrium, with edges arced to form a sphere,
may be considered as a convex
vector equilibrium. Illus.
1032.12D
shows the vector
equilibrium with arcs on the
triangular faces defined by spheres tangent at vertexes:
a concave vector equilibrium.
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1032.22
Physics thought it had found only two kinds of acceleration:
linear and
angular. Accelerations are all angular, however, as
we have already discovered (Sec.
1009.50).
But physics has not been able to coordinate its mathematical
models with the
omnidirectional complexity of the angular acceleration,
so it has used only the linear,
three-dimensional, XYZ, tic-tac-toe grid in measuring
and analyzing its experiments.
Trying to analyze the angular accelerations exclusively
with straight lines, 90-degree
central angles, and no chords involves pi ( )
and other
irrational constants to correct its
computations, deprived as they are of conceptual models.
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| Next Section: 1032.30 |