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The Orientation of Point-Volumes Surrounding a Charge



The Orientation of Point-Volumes Surrounding a Charge

When you are inter­ested in physics you must read “Unbe­liev­able”!

When there is a charge in space the shown non-​orientation in fig­ure 2 of the point-​volumes will be influ­enced. Vac­uum is able to con­tain fields (field-​theory) like the elec­tro­sta­tic field pre­sented in vac­uum by the dielec­tric con­stant. The charge in vac­uum will ini­ti­ate dielec­tric dis­place­ment in the point-​volumes. The elec­tric field will influ­ence the ori­en­ta­tion of the point-​volumes. In fig­ure 3 we demon­strate that the energy of the charge influ­ences the point-​volumes.

The point-​volumes are respon­si­ble for trans­port of the elec­tric field accord­ing to the laws of physics. Dielec­tric dis­place­ment is achieved in the point-​volumes and dis­trib­uted over space. One can imag­ine that at the QD level space is not homo­ge­neous and quan­tifi­ca­tion is inevitable.

Fig­ure 3. The ori­en­ta­tion of point-​volumes around a charge

The ori­en­ta­tion of the point-​volumes around the charge will min­i­mize the energy level accord­ing to physics laws. The non-​orientation of fig­ure 2 has disappeared.

The reader can see that the space around charge +Q can­not be filled homo­ge­neous any­more with point-​volumes. The ori­en­ta­tion of the sketched 6 point-​volumes around the charge in fig­ure 3 is still com­pa­ra­ble with field free point-​volumes in fig­ure 2, but the cir­cle of 12 point-​volumes around +Q can­not be found in the field/​energy free vac­uum of fig­ure 2.

The ten­sion of the elec­tric field draws the point-​volumes towards +Q and at the same time ori­en­tates the point-​volumes or “ether” as far as pos­si­ble into a bulb shape orientation.

When you are interested in physics you must read “Unbelievable“!

When there is a charge in space the shown non-orientation in figure 2 of the point-volumes will be influenced. Vacuum is able to contain fields (field-theory) like the electrostatic field presented in vacuum by the dielectric constant. The charge in vacuum will initiate dielectric displacement in the point-volumes. The electric field will influence the orientation of the point-volumes. In figure 3 we demonstrate that the energy of the charge influences the point-volumes.

The point-volumes are responsible for transport of the electric field according to the laws of physics. Dielectric displacement is achieved in the point-volumes and distributed over space. One can imagine that at the QD level space is not homogeneous and quantification is inevitable.

Figure 3. The orientation of point-volumes around a charge

The orientation of the point-volumes around the charge will minimize the energy level according to physics laws. The non-orientation of figure 2 has disappeared.

The reader can see that the space around charge +Q cannot be filled homogeneous anymore with point-volumes. The orientation of the sketched 6 point-volumes around the charge in figure 3 is still comparable with field free point-volumes in figure 2, but the circle of 12 point-volumes around +Q cannot be found in the field/energy free vacuum of figure 2.

The tension of the electric field draws the point-volumes towards +Q and at the same time orientates the point-volumes or “ether” as far as possible into a bulb shape orientation.

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