ASSOCIATION AND DISSOCIATION OF DIONS AND TRIONS

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ASSOCIATION AND DISSOCIATION
OF DIONS AND TRIONS In the study of Group Behavior, we learned that up to three configurations may occupy the same center providing that their orbital planes are orthogonal to each other, and, that the frequency of occurrence of such a condition is directly proportional to the field packing.

The field packing directly relates to the density of configurations in layers; forcing configurations into a specific alignment in close proximity so that orthonormal restorative impulses come into play.
One of these new configurations, consisting of three orthogonal two-dimensional configurations is called a TRION. Its energy image, artistically depicted, is shown adjacent. It is considered analogous to an electron or positron, consisting of three quarks.

The sharp cutoff of energy, giving the sphere a well defined spherical surface is attributed to the outside shells of three orthogonal outside-shelled spirals in combination. This link will take you to a single OSS in two dimensions, illustrating the static curvature of contributing field surfaces.

As of June 21, 2011 many references are wrong as are the quantum colors being that I chose to go with a Cartessian left-hand frame of reference.

    In this example shown, three charged spiral objects of orthonormal axes, respectively, combine to produce a TRION.    Any combination of three orthonormal field objects may combine in this way. The field objects which are permitted to combine in this way include: neutral dual-wave radial configurations, positive and negative ISSs and OSSs. By definition then, a TRION, in the least, consists of any combination of dual-wave radials, ISSs and OSSs.
    In reference to the previous illustration, any spiral whose orbital axis parallels the x-axis of a right-hand rectangular coordinate frame of reference is positive (NORTH pole pointing to the right), belongs to a class of red quantum chromodynamic field objects.   The spiral whose orbital axis parallels the y-axis of a right-hand rectangular coordinate frame of reference is negative (NORTH pole pointing out of the paper), belongs to a class of magenta quantum chromodynamic field objects. The spiral whose orbital axis parallels the z-axis of a right-hand rectangular coordinate frame of reference is positive (NORTH pole pointing up), belongs to a class of blue quantum chromodynamic field objects.
    Of the three, magenta is an opposite, or rarely occurring chroma class, or anti-objects.
    On the right, a TRION consisting of normal spirals is shown.
Using the left-hand rule, where the index finger points in the initial direction of the wave in orbit prior to becoming a standing wave, the thumb will be pointing NORTH. If two waves are in counter rotation, this rule does not apply.
    The black arrows point in the direction of each wave corresponding to its spiral configuration. Accordingly, the red spiral configuration has its NORTH pole directed to the right along the X-axis, the green spiral configuration has its NORTH pole directed into the paper (away from the observer) along the Y-axis and the blue spiral configuration has its NORTH pole directed upwards along the Z-axis.

The colors of each spiral configuration identify its source: red for the red layer, green for the green layer and blue for the blue layer, and, cyan for the cyan layer, magenta for the magenta layer and yellow for the yellow layer.

A TRION whose X-axis spiral configuration originated the cyan layer would appear as this. In its case, its directional arrow is opposite than before and its NORTH pole points to the left.

The complete opposite of the first TRION shown, would be one whose ISSs came from the negative layers cyan (x), magenta (y) and yellow (z), which, because of their opposite charges along all three planes, if in close proximity to the other, both would be drawn towards each other and undergo mutual annihilation as their centers approached coincidence.

Their attraction is comprehensive in that polar attraction and radial attraction come into play no matter their relative orientations.
An approach from any of the three planes would be facilitated as unlike spirals common to the same plane, driving them together. However their approach along any of the three axial directions would be inhibited by polar twisting of their like poles in opposition, much in the same way magnetism works. If in the case, these two TRIONS come together, it will result in a virtually instantaneous and simultaneous unwrapping of their spirals arms along all three planes, with the obvious release of great system energy as changing curvature of the field surfaces in this region of the Random Field. (See ANNIHILATION PATTERNS.)

ELEMENTARY FIELD CONFIGURATIONS

     More common than the TRION is the DION, consisting of only two configurations whose orbital planes are orthogonal.
    Essentially the primary field configuration assemblies, consisting of both the TRION and DION consist of charged ISSs and OSSs, and neutral dual-wave radials. Adjacent is a chart showing the elementary field configurations which adhere to the rules of Dynamic Geometry.
    The respective icons, at first glance, may appear to be reversed, the natural tendency to imagine inside-shell spirals smaller than outside-shelled spirals, hence their icons smaller. But remember, a great deal of the inside-shelled spiral's radius of activity exceeds that of the outside-shell's, which is why its icon is larger.
    Both ISSs and neutral dual-wave radials have larger radii of activity, and are therefore assigned the larger size icon.

    In general, all of these configurations, are assigned the symbolism C^c_d, where C represents the type of configuration, assigned the values I, O or R, where I symbolizes an ISS (inside-shelled spiral), O an OSS (outside-shelled spiral) and R a dual-wave neutral radial configuration.
    The lower case c superscript denotes the charge, + or -, and 0 in the case of R.
    The lower case d subscript denotes the orientation direction; the axial direction of each configuration, where such an axis is orthonormal to the orbital plane. The orbital plane is the plane of rotation of the simple field waves (l) comprising a dual-wave radial (R) or the plane of rotation of simple waves, prior to becoming standing waves of spiral configurations (O and I).
    As convention, all evaluation of these objects and their field behavior is confined to a finite three-dimensional polarized region of the Random Field, where within, though simple waves may be generically denoted as l_d, d must equal either x, y or z, in their correspondence to their respective layers of activity and confinement.
    In the case of I and O, their north poles are in the direction of the thumb, in the left-hand rule, where the fingers point in the direction of orbit of their simple waves before becoming standing waves.
    A positive charge corresponds to configurations whose north pole points in the direction of the positive axis they have assumed and a negative charge corresponds to configurations whose north pole points in the direction of their negative axis assumed within this finite region.
    Dual-wave radials have no north pole, and therefor their charge is zero.
    In the case of simple waves, their subscript orientation (d) in the field corresponds to the direction they travel within and limited to three orthonormal layers (x, y or z).
    The subscript designation (d) of these three orthonormal layers relates to their normals parallel to the three principle X, Y, and Z-axes of the Cartesian frame of reference utilized for this finite region of the Random Field, and to no other frame of reference, inertial or otherwise.

ELEMENTARY CONFIGURATION REACTIONS

n = x, y or z c = +, -, or 0 C = I, O or R

l_n = I⁺_n or I^-_n (spontaneous generation, not reversible)

2l_n = R^o_n (spontaneous generation, not reversible)

R^o_n = O⁺_n + I^-_n or O^-_n + I⁺_n (decay, not reversible)

PERMITTED DION COMBINATIONS

I^c_x + I^c_y I^c_y + I^c_z I^c_z + I^c_xO^c_x + O^c_yO^c_y + O^c_z O^c_z + O^c_x Combinations of I and O are not permitted though any combination of charge is allowed.
Following is a table of possible geometric combinations of spirals and radials which may form DIONS, without regard to the above rules.

DION COMBINATIONS

ANNIHILATION PATTERNS

    In the above chart, the positive base DION O⁺_x + O⁺_y (at the top of the chart in the box) is arbitrarily chosen as a permitted system DION; all other dions graded as to their persistence in its presence, those in green at the bottom of the chart being fully annihilated by its presence. This means, that within this system, the bottom four DION configurations are disallowed. Two of them are further disallowed because they are mixed between ISSs and OSSs.
    At the top of the chart in salmon color, three DIONS are greatly repelled (double repelled) by the base DION, which means that they have the greatest system persistence, except that two of them are disallowed because they are mixed OSSs and ISSs, leaving only one, the I⁺_x + I⁺_y.
    The following chart, by application of these rules shows the permitted system dions.

    At the bottom of this chart are the least likely DIONS to be present; at the top, the most common. The shaded areas may be assigned numerical values ranging from greater than zero (possible) to close to unity for salmon colored DIONS.
    The next chart shows the permitted association of these DIONS with free spiral configurations forming TRIONS. And though this process seemingly rather benign, with wondering spiral configurations, those allowed of course, in absence of any coerced annihilations, cruising everywhere about the...thus slipping into an unoccupied niche in an complete DION, in one case like a trojan horse ready to implode...such as an R^o_x.
    In its case, consisting of a naturally occurring neutral oblate glob of sorts, with an occasional faint magnetic field, though its axis impeccably stable, though ill defined, an R^o_x, though blessed into Being by spontaneous generation, will decay;   its two ls, each drifting away, beyond the ability of any recovery into the field whence they once ago arose, only to drive their energy one more time around in this finite region of the Random Field, about which we study.

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