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1. Symmetrized-physical transition in mechanical phenomenon.

Geometry of a phenomenon and objects taking part it possess some degree of symmetry. In the present article utmost cylinder-like and sphere-like versions, characterized by conversion of an phenomenon (object) itself into itself at continuous turning around one ore two available axis of symmetry.

According to the facts, the utmost symmetry is more than variety of a geometric form. It shows itself as effectual side of a phenomenon being in continuous contact with physical properties of the participants and cause-and-effect relationships between them. Real change of the utmost geometric symmetry of any natural essence is accompanied by physical changes in it.

In the Table 1 an example of symmetrized-physical transition in the region of physical phenomena is represented.

Upon changing of symmetry of acting forces, the body acceleration is replaced by its deformation and instead of inertial property, another body’s property – its elasticity, becomes apparent.

The Newton’s cause-and-effect relation transferes into Hooker’s one.

2. Symmetrized-physical transition in magnetostatics.

2.1 Symmetrized aspect. By analogy with a mechanical example, transition of physical properties of the magnetic field (table 2) is expected upon changing of currents symmetry.

At sufficient distance from centrosymmetrical currents of charges geometric summing of vectors of tensity and magnetic potential in all cases as a result gives zero-vectors.

In natural phenomenon of symmetry, causes and effects can not be different, and that fact makes it possible to formulate the following judgment. Artificial transferring of the cause (current sauce) to more symmetrical one is followed by natural transition to the same symmetry in the effect (in magnetic field). Known electromagnetic fields, from the point of view of their geometric structure, have either closed or open field lines.

There are no any other versions in the electromagnetism. Therefore, in the region of zero—vector the result of geometric recapitulation of field vectors, substitution of the compensated initial circulating property of the magnetic field with cylinder – like symmetry for a potential property with ball symmetry, similar to that of the electric charge field, is supposed without any alternative.

2.2 Physical aspect. Everything known about lengthy structure of the fields is obtained from empiric facts about the results of their local influence on electric charges.

So, the supposed transition to another structure of magnetic field can be confirmed only by transition to another orientation of the magnetic forces in the frames of their relativistic nature.

For clear comprehension of the cause, and immediate vision of mechanism of such transition in subsequent representation, two, in point of fact, similar examples are given below, which combine both logic and evidence.

Black circles denote positive current charges moving in the current direction marked by the arrows. The light circles are negative ones moving in the opposite direction. Consideration is carried out in the system of rest of the trial charge. In such a case the inclined vectors of the summed speeds ∑V characterize both charges movement in the conductor and their approach with the resting trial charge. Relativistically “flattened” diagrams of field lines of the fields of the current charges are found to be inclined as well.

The essence of the Parsell’s idea is in an assertion, that thickening of the field lines strengthen influence of each current charge upon the trial one, and that rarefaction makes it weaker.

The general relativistic constituent of the force impact of unidirectional currents is clearly presented as cross-oriented one to the speed of the trial charge.

multiplier of the force impact becomes oriented along the speed of the trial charge movement.

Form and quantity of the relativistic effect in the field of each moving charge both in

unidirectional and centrosymmetric currents correspond to the special theory of relativity. Only symmetries of their imposition in the region of the trial charge tell the difference and that is the genuine cause of the existence of longitudinal and transversal directions of the magnetic force.

As an example of a practically realized mono-field source of a potential magnetic field is equal stretching in both directions of an elastic electrically charged thread causing forming of centrosymmetric currents of charges transferring.

2.3 Material aspect . After symmetrized transition the amount of magnetic energy in the space near the centralsymmetrical source of the field remains unchanged, because unidirectional and opposite sense current constituents equally do not interact with each other in neither force nor inductive ways. In both cases there are no reasons for converting even a part of magnetic energy into other forms upon conditional drawing together along the general straight line of the left and right current components from the infinity because along all its extension, the magnetic field is equal to zero.

Under the conditions of prohibition by principle of super position by the

centrosymmetrical currents with circulation property creation of general magnetic field to be a substitute in accordance with remaining magnetic energy, forming another magnetic property is inevitable. Positive one - without any alternative.

Zoro - a vector field situation which does not testify mutual compensation of imposing magnetic fields of current charges, but only initial circulating properties. In other case it would violate the principle of conservation of energy

- grad |A| = B (1)

2.4 Mathematical aspect. In mathematical models of nature phenomena to the real geometric symmetries of described objects, geometric symmetries of a tensor values correspond. The lower the rank of the tensor, the degree of its geometrical symmetry is higher.

Let us represent symmetrical-physical transition in local electric dynamics by means of the rank conversion. For this purpose let us multiply well known Maxwell’s equation by dimensionless 4-vector.

By transition of an equation with tensors of the first rank to an equation with tensors of the zero rank, rise of degree of symmetry of geometrical values is described. And, as a result, change of their physical fillings. The equality (2) describes relations between different symmetries of the same natural essence – between eddy and eddy-free electrodynamics.

Equating with zero the field sources, (in (2)) we obtain the description of the symmetrized-physical transition in field wave process in empty space.

and a new Gausslike differential equation for more symmetric local magnetostatics with potential

magnetic field

with non-directional (in general case – infinitesimal spherical) centrsymmetrical charge currents.

Experimental aspect. Alternating magnetic field with open field lines (cause) forms electric field of the same symmetry (effect). Reciprocating induction currents in the conductor are also open. During experiments there was registered induction heat of an aluminium bushing (D=1 cm, d=0.8 cm, ℓ=3 cm) longitudinally located in the region of forming zero-vectors, which came in on a symmetry line of a pair of alongside located in the same plane rectangular multiturn (n=300) frames with alternate (f=50Hz) opposite sence currents (i=0.55 A) in them.

To record the time of beginning of temperature changing of the aluminium bushing a Zener diode located inside of it was used. Presence of strong temperature-ohm tie (100 KΩ/grad in the opposite directions in the interval 0.8…1.9 mΩ) made it possible to register the required moment of time by beginning of reduction of ohmic resistance, uninterruptedly measured during the experiment by a digital ohmmeter DT890B.

The bushing with stabilitron was put into an alabaster casing (m=0.5 kg). Freely admitting electro-magnetic field, it detained for some time display of heating by Joulean heat generated by the currents in a pair of frames.

In the Fig. 3 scheme of location of technical means for the experiment and diagram of changing of ohmic resistance of the stabilitron during the experiment are shown.

In the zone I the medium horizontal line demonstrates invariability of the bushing temperature in time without current in the frames. In the zone II descending of the line indicates the beginning of the bushing induction heating 4…5 min after connecting of the frames to a source of current. In the zone III in 10…12 min prevailing heating of the bushing by Joulean heating becomes apparent.

In a cases of stationary currents in the frames, when the induction process was absent, bushing heating by Joulean heating became apparent after the same time - 10…12 minutes.

In a serious of 12 experiments it was determined that before heating of the bushing by Joulean heat became apparent, induction heating, passing ahead of the first one by 5…6 minutes, took place. At the same time, on the same line of symmetry (on the other side of the pair of frames) electromotive force (emf) was not induced. By two test results there were registered facts of forming in the zero-vector region of an induced irrotational electric field and absence of induced rotational one in it.

Besides registration of induction heating of the aluminium bushing, there were obtained positive results of experiments connected with cooling of a stabilitron semi-conducting crystal by a stationary potential magnetic field. During a number of experiments the stabilitron was placed into a steel bushing with thick walls (D=2.3 cm, d=1.4 cm, ℓ=6.5 cm).

It did not prohibit magnetic cooling. So, it confirms supposition about absence of interaction of the potential magnetic field with spin magnetic moments of a ferromagnetic material.

Similar results of experiments connected with heating of a bushing and cooling of crystal were observed during experiments with two versions of mono-field sources of a potential magnetic field (co-axial cable). An idea of a potential magnetic field is present in Dirakhypothesis about magnetic micro-mono-field. The question of interaction of a micro-particle magnetic charge with a circulating magnetic field remains to be unsolved till its experimental solution.

Therefore it is interesting to use potential magnetic field in the Wilson chamber. It would give a possibility to determine if an elementary particle has a magnetic charge.

It is expedient to use in experiments of search of Dirak mono-field magnetic traps, able to accumulate dissimilar magnetic charges.

Mathematically correct zero-vectors are irrational from the physical point of view.

Despite conservation of electro-magnetic energy, they testify compensation of polarized (transverse) and structural (rotational) characteristics of the general field.

As a matter of fact the situation is analogous to imposition of circulating magnetic fields (Fig. 2), caused by centrosymmetrical charges currents. Following the earlier used way of thinking an analogous conclusion is made about absence of alternative for transition result. Besides closed and open field lines, besides transverse and longitudinal wave processes in the nature nothing else is known. Therefore, rotational structure is supposed to be turning into irrotational one. Accordingly, transverse field-wave process turns into longitudinal.

Irrotational electric field of longitudinal EMW can not induce electromotive force in a closed conductor. Registration of this effect was provided with the device 2 – an introduced co-axial part with increased diameter relatively to the cable.

The increased waveguide value allowed to install in the mentioned device a multiturn closed electric conductor connected to a digital voltmeter 3. General EMW is radiated into open space by a dielectric rod antenna (Fig. 4a,) end (Fig. 4b, 4g).

In the Fig. 5 scheme of imposition of transverse electromagnetic waves in a recapitulative waveguide is represented.

4. Zero-vector photons. The light range does not overstep the limits of the idea of forming other properties by the same natural substance, changing its geometric symmetry. It is supposed that photons can amalgamate into zero-vector pairs like Cooper’s electron pairs. Theoretically, direct radiation of a zero-vector photon by an atom upon an electron transition between centrosymmetrical S – orbitals without inversion of pertaining to it spin mechanical moment.

The top-priority is the problem of registration of zero-vector photons during experiments. At the beginning, it is necessary to find and master photochemical or photoluminescent reactions activated by inverse process - absorption of electromagnetic energy by the atom. Throwing out by longitudinal photon of non-turning electron from one S-orbital to another one (higher) should make this atom chemically active in relevant aspect.

Literature.