![]() Fig. 462.00 |
462.00
Rotation of Triangle in Cube
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462.02
Wave-propagating action is cyclically generated by
a cube with a triangle
rotating in it.
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463.00
Diagonal of Cube as Wave-Propagation Model
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![]() Fig. 463.01 |
463.01
There are no straight lines, only waves resembling
them. In the diagram, any
zigzag path from A to C equals the sum of the sides
AB and BC. If the zigzag is of high
frequency, it may look like a diagonal that should be
shorter than ABC. It is not.
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463.02
As the triangle rotates in the cube, it goes from
being congruent with the
positive tetrahedron to being congruent with the negative
tetrahedron. It is an oscillating
system in which, as the triangles rotate, their corners
describe arcs (see
Sec. 464.02)
which convert the cube's 12 edges from quasistraight
lines to 12 arcs which altogether
produce a dynamically described sphere (a spherical
cube) which makes each cube to
appear to be swelling locally. But there is a pulsation
arc-motion lag in it exactly like our
dropping a stone in the water and getting a planar pattern
for a wave
(see Sec. 505.30),
but in this model we get an omnidirectional wave pulsation.
This is the first time man has
been able to have a conceptual picture of a local electromagnetic
wave disturbance.
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463.03
The cube oscillates from the static condition to the
dynamic, from the
potential to the radiant. As it becomes a wave, the
linear becomes the second-power rate
of grc wth. The sum of the squares of the two legs =
the square of the hypotenuse=the
wave. The 12 edges of the cube become the six diagonals
of the tetrahedron by virtue of
the hypotenuse: the tetrahedron is the normal condition
of the real (electromagnetic)
world. (See Sec. 982.21.)
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463.04
There is an extraordinary synergetic realization as
a consequence of
correlating (a) the arc-describing, edge-pulsing of
cubes generated by the eight triangles
rotating in the spheres whose arcs describe the spherical
cube (which is a sphere whose
volume is 2.714__approximately three__times that of the
cube) and (b) the deliberately
nonstraight line transformation model
(see Sec. 522),
in which the edges of the cube
become the six wavilinear diagonals of the cube, which
means the cube transforming into a
tetrahedron. Synergetically, we have the tetrahedron
of volume one and the cube of
volume three__as considered separately__in no way predicting
that the cube would be
transformed into an electromagnetic-wave-propagating
tetrahedron. This is an energy
compacting of 3 1; but sum-totally this means an energetic-volumetric
contraction from
the spherical cube's volume of 8.142 to the tetrahedron's
one, which energetic compacting
serves re-exp__nsively to power the electromagnetic-wave-propagating
behavior of the
wavilinearedged tetrahedron.
(See Sec. 982.30.)
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463.05
We really find, learning synergetically, from the
combined behaviors of the
tetrahedron, the cube, and the deliberately-nonstraight-line
cubical transformation into a
tetrahedron, how the eight cubical corners are self-truncated
to produce the vector
equilibrium within the allspace-filling cubical isotropic-vector-matrix
reference frame; in so
doing, the local vacatings of the myriad complex of
closest-packing cube truncations
produce a "fallout" of all the "exterior octahedra"
as a consequence of the simultaneous
truncation of the eight comers of the eight cubes surrounding
any one point. As we learn
elsewhere
(see Sec. 1032.10),
the exterior octahedron
is the contracted vector equilibriurn
and is one of the spaces between spheres; the octahedron
thus becomes available as the
potential alternate new sphere when the old spheres
become spaces. The octahedra thus
serve in the allspace-filling exchange of spheres and
spaces (see Sec. 970.20).
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464.00
Triangle in Cube as Energetic Model |
![]() Fig. 464.01 |
464.01
The triangle CDE formed by connecting the diagonals
of the three adjacent
square faces surrounding one corner, A, of the cube
defines the base triangular face of one
of the two tetrahedra always coexisting within, and
structurally permitting the stability of,
the otherwise unstable cubic form. The triangle GHF
formed by connecting the three
adjacent faces surrounding the B corner of the same
cube diametrically, i.e. polarly,
opposite the first triangulated corner, defines the
triangular face GHF of the other of the
two tetrahedra always coexisting within that and all
other cubes. The plane of the green
triangle CDE remains always parallel to the plane of
the red triangle GHF even though it
is rotated along and around the shaft AB (see drawings
section).
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