Zero Point Energy doc
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| ZP OWER C ORPORATION PAGE OF 352 Z ERO P OINT E NERGY however when halted in the flow, a resulting " Gravitational " field is felt by the mass. This can be referred to as Aether pressure. Fig. 1 From Fig 1 one can deduct that a " Gravitational Field " increases towards the surface of amass, decreases from the surface towards the center of said mass, and that no limitation need be placed upon the number of nodal lines depicting Aether pressure since said Aether pressure has no mass. If the force of gravity pulling down upon amass towards the center of another mass is an illusion produced by Aether pressure which is Aether flow in one direction, then tidal forces and rotation of cosmic bodies can be explained When the Aether flow forms a loop instead of a vector, a magnetic field is the result. The direction of the flow of the nodal lines of force of a magnetic field is also an illusion, produced by the Aether flowing in the opposite direction. See figure 2. [8] This theory fits the aether model, but remains to be proven. The following depiction of an electrostatic field is also subject to the same test. In an electron gravity, rotation, magnetic and static fields exist The same should hold true for the proton. The proton cannot be ignored in the mechanics of the Aether since it constitutes such a large part of the atom. Logically when one affects the electrons surrounding the nucleus of an atom, then the nucleus must also be affected. Figure 3 depicts the fields associated with an electron. If the poles are reversed fora proton, the equator becoming a high and the poles becoming a low, then the Aether flow is reversed, causing the proton to act as a sink for the static field and since the electron already acts as a source for the static field, an attraction results between the electron and proton. [9] See figure 4. Without becoming involved any further in the atomic structure of the atom, electron flow in a conductor will be reviewed since the object of this paper is to map the electromagnetic fields surrounding a conductor when a potential is applied. Referring to figure 5 When a potential c is placed at the ends of conductor a the electron b begins to accelerate. At this point voltage is almost zero, current is very high, power is almost zero, resistance is nearly zero and power propogation h in the form of heat is at the temperature of the rest of the conductor. A magnetic vorticity n forms f that is centripetal in nature, and the Aether g forms a centrifugal field. When the electron reaches the point of |