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4.11 Resolution reasons for the paradoxical nature of modern electrodynamics

The article: "Modern electrodynamics and reasons for its paradoxical '- GV Nikolayev writes:

"Any theory, no matter how perfect it may be, will never exclude the possibility of its further improvement. The value of a physical theory is determined, above all, the scope of its practical applicability. With reference to the well-known theory of electromagnetism, in the framework of modern concepts in electrodynamics, the question of the applicability of the theory of general practice, of course, can not be doubted. However, despite the seemingly endless field of practical applicability of the modern theory of electromagnetism and the tremendous achievements of science and technology in these areas to date accumulated a significant amount of electrodynamics phenomena of electromagnetism that modern theory can not give a consistent and correct explanations. That is, in the long process of practical development of the laws of electromagnetism, which were identified as part of the well-known theory, humanity is faced with the phenomena of electromagnetism, which has clearly gone beyond the modern theory. The appearance of such paradoxical from the point of view of the existing phenomena of the theory of electromagnetism is completely natural and just proves, on the one hand, the limitations of the existing theory of electromagnetism, and on the other hand, the need for further improvement. Therefore, to understand the reasons for the paradoxical nature of modern electrodynamics, contact, first of all, to analyze the substance of the undeservedly forgotten paradoxical phenomena of electromagnetism which were already known in the times of Ampere and found now in many experimental observations. The number of such complementary observations already accumulated enough so that you can make them quite definite conclusions. In addition to the famous observations of "strange" magnetic interactions author posed a series of special experiments that reveal the actual physical nature of the so-called "paradoxical" effects of electromagnetism. Below is a description found in numerous experiments "strange" magnetic interaction forces, correct explanation that in the framework of the modern theory of electromagnetism can not be found. "so you can make them quite definite conclusions. In addition to the famous observations of "strange" magnetic interactions author posed a series of special experiments that reveal the actual physical nature of the so-called "paradoxical" effects of electromagnetism. Below is a description found in numerous experiments "strange" magnetic interaction forces, correct explanation that in the framework of the modern theory of electromagnetism can not be found. "so you can make them quite definite conclusions. In addition to the famous observations of "strange" magnetic interactions author posed a series of special experiments that reveal the actual physical nature of the so-called "paradoxical" effects of electromagnetism. Below is a description found in numerous experiments "strange" magnetic interaction forces, correct explanation that in the framework of the modern theory of electromagnetism can not be found. "Below is a description found in numerous experiments "strange" magnetic interaction forces, correct explanation that in the framework of the modern theory of electromagnetism can not be found. "Below is a description found in numerous experiments "strange" magnetic interaction forces, correct explanation that in the framework of the modern theory of electromagnetism can not be found. "

For a correct explanation of the physical nature of a series of "strange" results of the experiments, when passing current through conductors, consider the third experience of G.V. Nikolaeva, whose scheme is shown in Fig. 4.11.1.

Fig.4.11.1

We give description of the experience: "To demonstrate the feasibility of the laws of mechanics the interaction elements perpendicular rectilinear movable current conductor 1 is placed on the suspension at a distance of 2-4 mm from the remaining conductors of rectangular contour. The capacitance C is charged up to 10-20 kV. In the breakdown of the gaps between the movable conductor 1 and the movable conductor circuit conductors comes into translational motion along the direction of current stream therein in the direction acting on it longitudinal force F_║. The transverse force F _┴ reaction from the movable conductor 1 are attached to the side conductor circuit 3 '.

3.7 The study helps explain the observed in this experiment results. Indeed, as was found in a study on the conductor, during the passage of current thereto, a force directed in the direction of current movement.

Therefore, "the conductor comes into translational motion along the direction of current stream therein in the direction acting on it longitudinal force F _║ ». This explanation applies to the entire series of experimental observations in the interaction of current-carrying conductors.

For a correct explanation of the physical nature of a series of "strange" results of the experiments, the interaction of magnets, consider the 35-rd of experience G.V. Nikolaeva, whose scheme is shown in Fig. 4.11.2.

Fig.4.11.2

 

We give description of the experience: "Two are located on one plane of rectangular magnets with unlike poles are attracted to each other. When approaching the magnet force of attraction increases and reaches its maximum value at full convergence of adjacent sides. If one of the magnets above and below to make another 6-8 of the magnets, the force of attraction between a magnet and a single compound increases. However, the approach of the magnets of the magnetic attraction force between them first increases and then decreases and becomes a repulsive force. Calculations show that with a significant number of magnets in the two component magnets with magnetic fluxes in different directions (for a sufficiently long magnetic cores) magnetic force interaction between such magnets is now only the repulsive force, instead of the original attraction.

Analogous conclusions can also come in if the two considered sufficiently long magnetic rod with a similarly directed magnetic flux in them as two separate elements interacting toroids sufficiently large dimensions. Similar phenomena have magnetic interaction observed for equivalent sufficiently long solenoids with unidirectional magnetic flux therein. In the calculations must take into account the interaction of the currents of some circuits with other vector potential. " /doverchiv.narod.ru > Nikolaev ... electrodynamics.htm /

magnet 1 magnet 2

Fig. 4.11.3
magnet 1 magnet 2

А В

view А view В

Fig. 4.11.4

Research 3.6, 3.7 and 4.9 make it possible to justify observed in this experiment results. Consider first the model of interaction between the magnets, shown in Figure 4.11.3. The figure shows the structural components of the substance in the form of elongated magnets maxi- sources with the sign (-) and maximum effluent with the sign (+). total stream of ether also shows the emitted and absorbed by Maxi sources and maximum runoff. According to the study 4.9 maxi- sources vertically arranged magnets and maximum constitute vertically orienting drains chain. And, the greater the chain length, the faster the stream elliptic ether will pass through it, since the rates of the individual sources and maximum maxi- drains forming a chain, are folded together in an elliptic total flow. In cross-section the magnets having annular streams total ether whose speed is independent of the length of the magnets.

In Fig. 4.11.3 following notation for the total ether flow:

- vector elliptical total stream rate ether magnet 1 disposed between the magnets;

- vector sum elliptical magnet ether stream rate of 2 disposed between the magnets;

- vector sum elliptical ether magnet stream rate of 1 located on the left of one magnet;

- vector sum elliptical half current ether speed magnet 2 disposed on the left of one magnet;

- vector sum elliptical magnet ether stream rate of 2 to the right of the magnet 2;

- vector elliptical total stream rate ether magnet 1 disposed to the right of the magnet 2;

- vector ether total circumferential velocity of the magnet 1 disposed between the magnets;

- vector sum circular magnet ether stream rate of 2 disposed between the magnets;

- vector of total ether circular magnet stream rate of 1 located on the left of one magnet;

- vector sum circular magnet ether stream rate of 2 to the left of one magnet;

- vector sum circular magnet ether stream rate of 2 to the right of the magnet 2;

- vector ether total circumferential velocity of the magnet 1 to the right of the magnet 2.

Then, when:

- magnets will repel, as the pressure between the magnets is greater than the pressure on the left and right sides.

As rightly pointed G.V. Nikolaev - "in the calculation should take into account the interaction of the currents of some circuits with other vector potential." However, when a sufficiently long ring magnets influence of streams of one magnet to the other can be neglected. Which in any case should not be allowed in the interaction of relatively short magnets, as will be shown below.

Now consider the model of the interaction of the magnets shown in Figure 4.11.4. The figure shows two short magnets 1 and 2 as well as the total ether vectors fluxes acting on the magnet.

In Fig. 4.11.4 following notation for the total ether flow:

- vector elliptical total stream rate ether magnet 1 disposed between the magnets;

- vector sum circular magnet ether stream rate of 2 disposed between the magnets;

- vector elliptical total stream rate ether magnet 1 acting directly on the magnet 2;

- vector sum circular magnet ether stream rate 2 acting directly on the magnet 1;

- vector of total ether elliptical stream velocity of the magnet 1, the current right of the magnet 2;

- vector sum circular magnet ether stream rate 2 acting on the left of one magnet;

- vector ether total circumferential velocity of the magnet 1, the current right of the magnet 2;

- vector sum circular magnet ether stream rate 2 acting on the magnet 1 on the right;

- vector of total ether circular magnet stream rate of 1 acting on the left of one magnet;

- vector sum circular magnet ether stream rate 2 acting to the right of the magnet 2;

- vector of total ether circular magnet stream rate of 1, the current right of the magnet 1;

- vector sum circular magnet ether stream rate 2 acting on the left of magnet 2;

- vector elliptical total stream rate ether magnets 1 and 2, located between the magnets;

- vector sum elliptical ether magnet stream rate of 1 located on the left of one magnet;

- vector sum elliptical magnet ether stream rate to the right of the magnet 2.

According to the study 4.7 under the influence of the total velocity vector stream ether +, Maxi- sources drains and maximum turn of the magnet 1, as shown in view A and maxi- sources and drains maxi- magnet 2, under the influence of the total velocity vector stream ether +, fall down, as shown in view B .

Then, when: - magnets will be attracted because the pressure between the magnets is less than the pressure on the left and right sides of the magnets. This case corresponds to the magnets remote from each other.

If the magnets begin to converge, the elliptic stream of the sum of ether and will increase, at constant circular streams ether and . This convergence will lead to the fact that:

  
In this case, the magnets will repel as between the magnets the pressure will be greater than the pressure on the left and right sides of the magnets.

The results fully correspond to the experimental data obtained by GV Nikolaev, other researchers and can justify the mechanical nature of previously unexplained "paradoxical, strange phenomena of electromagnetism."