The twin phenomena of Pair Production and Pair Annihilation lead us to the natural hypothesis of a space filled with positive and negative Dipole Particles. The organization of a Sea is less likely to be independent Dipole Particles that associate like oxygen atoms bonded together, and more likely like salt crystals, with every positive and negative particle bonded to 4 charges in a face centered cubic bonding.
This crystalline lattice structure assembles to form the equilibrium point between the forces of the magnetic poles and electrical charges of the positive and negative DPs that compose the lattice. The electrical poles will impose an alternating plus/minus/plus sequence to the lattice.
The magnetic poles will likewise attract and repel based on the North/South orientation of each magnetic particle. The magnetic pole alignment in a 2 dimensional array of magnets has as its lowest energy configuration: two single columns of North/South particles aligned next to oppositely aligned columns.
But, the Dipole Sea is a 3 dimensional array of infinitely spherically orientable magnetic poles. Thus, the point of lowest energy for such a system is the organization of magnetic poles with the greatest randomness of pole orientation. Every DP will be attracted and repelled electrically, and attracted and repelled magnetically. Thus, the magnetic orientations of the DP Sea will reflect this spherically oriented randomness in the direction pointed by each of the DPs.
To justify this hypothesis of the structure of the Dipole Sea as a lattice of alternating positive and negative DPs, and magnetic poles oriented randomly, we must examine our assumptions about the nature of the electric and magnetic forces emitted by each DP. This gives us a validation of our assumption for the steady state, rest-orientation of the DP Sea.
Having come to a conclusion about the nature of the steady state DP Sea based on the rules that such particles use to attract and repel, we may then proceed to understand how the DP Sea responds to the dynamic pressures of mass and waves transiting through this space.
Dipole Sea Electrical Force Interaction: Regarding the Electrical Attraction: Opposite charges attract. Without an opposing force, a pair of positive and negative DPs would move together as close as possible, collapsing and superimposing upon each other. Thus the requirement for the particles that make up all of space to have a mutual attraction to maintain cohesion, but also a countervailing force that prevents these particles from collapsing into a singularity.
The opposing forces acting on the electron-positron pairs that prevent their collapse into superimposition are the electrons and positrons that surround them in the crystalline lattice of the Dipole Sea.
Each electron is surrounded by 6 other positrons which are pulling the electron away from its bonding with any one positron.
The same is true of the positron, which is prevented from collapsing into any one electron by the 6 electrons that surround it closely.
Electrical Repulsion: The electrical forces orient in two strong geometric manners to act to oppose the collapse of the Dipole Sea. 1) The 8 DPs around each corner are repulsive of the DP in the center of the cube. 2) The pull of the DP on the other side of the cubic face opposite charge opposes the collapse of the positive and negative DP.
Both of these forces give stiffness to the system, and prevent a runaway collapse, but they are not sufficient by themselves to keep the DP Se particles from creeping inward. To prevent collapse, the DPs need the addition of the repulsive force of the magnetic field. This addiction creates a standalone system where every volume of the system is stable.
Magnetic Attraction: A single line of positive and negative DPs will line up head to tail in a North/South/North/South sequence to form a column of magnetically aligned particles.
The column of positive-negative DPs aligned in a head to tail orientation creates an overall North-South pole from this collection of individual poles.
A two-column assembly of magnets will form a stable system with one column up and one column down.
A three dimensional assembly will form a stable assembly when all pole are oriented randomnly.
Magnetic Repulsion: A North-South column of magnetic dipoles will not align next to another North-South column unless it is restrained from movement.
A North-South column pointing up will emit a magnetic field from its side also. The field on the side of the column will form from the individual fields emitted by each magnetic particle. The superimposition of the many fields from the individual particles on the long portion of the column, along its sides, will superimpose to create a magnetic field pointing down.
Thus, side by side columns will magnetically orient themselves in anti-alignment; with one column pointing up (North-South), and the other pointing down (South-North).
???Each North-South column will have around it four closely-positioned columns, each of which will point in South-North anti-alignment. This opposing magnetic alignment reflects the mutually attractive low energy configuration associated with reinforcing the magnetic fields at 90° from the poles.
The North-South columns will be surrounded by 4 South-North columns, just as each South-North column will be surrounded by 4 North-South columns.
Why do Magnetic Poles Attract, Repel, or Rotate Other Magnetic Poles?
As an analogous pattern of action, let us first review the method by which an external E field acts on a charged particle to produce force, acceleration, velocity, and displacement:
Negative E fields (e.g. generated by negative DPs, or electrons) exert an attractive force on particles with positive charges, and a repulsive force on negative charges.
Positive external E fields (e.g. fields generated by positive DPs or positrons) exert an attractive force on particles with negative charge, and repulsive forces on particles with positive charge.
As mentioned above, this system is explained in terms of conscious particles, which move according to rules and agreement rather than by a mechanical force. Having again emphasized that, we shall now return to the more conventional understanding of the B and E field as attracting or repelling a charge or pole with force.
Each charged particle processes the direction and strength of the fields coming from the particles and fields in its environment at each moment. Each DP responds with a proper response (according to its programming) to the E&B fields of such a magnitude and direction.
The charged particle then moves to an appropriate distance in the next moment.
In other words, a field force exerted on a particle changes its velocity, which is another name for acceleration, and is a hallmark of force.
The equation F = ma is the macroscopic relationship between the force exerted on a mass and the acceleration produced by that force.
Both the E and B field cause orientation, attraction, and repulsion of other DPs. All this movement is by conscious choice, and programmed rules.
Magnetic Influence: The magnetic particle’s response to a magnetic field includes:
Rotating the North-South poles of two magnetic particles to align head to tail, North to South with each other, thus creating a (N/S)(N/S) sequence of pole alignment.
The appearance of an attractive force between two DPs if their magnetic fields align.
And, the appearance of a repulsive force between two DPs if their magnetic fields anti-align.
The presence of an external B field can produce a rotational force and a repulsive or attractive force on a magnetic particle if the fields do not align exactly. When the DPs have rotated to align magnetic fields North to South, the two particles attract with maximum force.
An external B field produces a rotational torque on a magnetic particle to align the particle’s poles with the external B field.
Note: every particle emits a magnetic field, and that field is an “external field” to every other particle.
In the case of two magnetic particles, each emitting a magnetic field, both magnetic particles will rotate in response to the B field emitted by the other.
The charge polarity of a particle is unrelated to the magnetic dipole generated by the particle. A positive charge will generate exactly the same magnetic dipole as a negative charge.
When two particles align N/S magnetically, they generate an attractive magnetic force between the two particles.
If the two particles are of the same charge polarity the repulsive electric force of the charges will oppose the magnetic attraction.
If an electron and positron come into close proximity, their electrical charges will attract, and their magnetic poles will align to produce attraction. This strong force of attraction will produce Pair Annihilation, and result in the production of two ã rays in its place.
Magnetic dipoles will align head to tail, N-S, along their pole axis, if their poles are free to rotate (that is unconstrained by other forces).
If the poles have an angle è between them, then a rotational force acts on the two particles, which results in an angular displacement of the poles toward alignment.
When two particles interact, they respond to the sum of the forces in their space. These forces include: 1) rotation of magnetic poles, 2) attraction or repulsion due to E Fields, 3) attraction or repulsion due to B field. The steady state condition occurs when the forces of attraction, repulsion, and rotation balance.
Consider the case when Particle 1 has its pole pointed in the direction of the Z axis. Naturally the equator of Particle 1 will be on the xy plane, which we will call 0°.
Now, constrain this single magnetic particle to a particular position and magnetic orientation, to prevent it from rotating and translating.
Next: Constrain magnetic particle 2 at the equator of Particle 1, but allow the magnetic pole of Particle 2 to rotate.
With these constraints in place, Particle 2’s pole will rotate to point in the direction opposite to the pole of Particle 1.
The poles point in opposite directions because the B field generated by Particle 1 points downward at its equator, at the 0° position.
By analysis of the field line patterns emanating from a column of magnetic particles, we can hypothesize that the B field emitted by a single magnetic particle is a spherical emanation, with a B field vector that changes its direction at every angle from +90° to -90°.
At the equator of Particle 1, the magnetic field emitted by Particle 1 points downward toward -90°. Therefore, the free spinning magnetic pole of Particle 2 points downward to align with the external B field generated by Particle 1.
Magnetic particles respond to an external B field with an attractive or repulsive force depending upon the orientation of the magnetic particle’s pole compared to the external B field.
We shall define the direction of the external magnetic field as the direction that the North Pole of a magnet will point when in that field.
We shall define è as the angle between the direction pointed by the North pole of the particle and the direction of the magnetic field.
When è = 0°, the magnetic particle aligns with an external B field exactly, and will experience no rotational force. At è = 0°, the magnetic particle will experience only the force of moving in the direction of attraction.
When è is > 0° and < 90°, then there will be a combination of rotational and attractive forces exerted on the magnetic particle.
When è = 90°, there is only a rotational force exerted on the magnetic particle.
When è is >90° and <180°, then there will be a combination of rotational and repulsive forces exerted on the magnetic particle.
Rotational forces between two poles always exert a force to align poles according to the polarity of the rotational forces will never exert a force to create dis-alignment.
Note: when the rotational force has moved è from >90° to <90° that the translational force on the Particle 2 will turn from repulsive to attractive.
When è = 180°, the magnetic particle will respond only with repulsion.
