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4.8 The attraction and repulsion of parallel conductors with current

"In 1820, Hans Christian Oersted discovered that a wire on which there is a current creates a magnetic field and causes a compass needle deviate. He noted that the magnetic field perpendicular to the current, rather than parallel to it, as one would expect. Amperes, inspired by a demonstration of the experience of Oersted, discovered that two parallel conductors through which current flows, attract or repel depending on whether one or opposite sides of it there is a current. Thus, not only the current produces a magnetic field but the magnetic field acts on the current. Within a week after the announcement of Oersted about her experience, amps offered an explanation: the conductor acts on the magnet, because the magnet current streams for a variety of small closed paths. ». /encyclopaedia.bid›

Wikipedia Ampere Power /

"The question is why two parallel electron beams repel each other, and the two parallel conductors through which currents stream in the same direction are attracted?

In the first case, there is an electrical interaction. Electron - negative particle. Similarly charged particles repel each other. Both electron beam a stream of moving negative electrons.

In the second case, the magnetic interaction occurs. Electric current - a directed stream of moving charged particles. Around the conductor there is a current magnetic field. The magnetic field of the first conductor with the Ampere force acts on the second current-carrying conductor, the magnetic field of the second conductor with a force acts on Ampere first current-carrying conductor. The direction of the Ampere force is determined by the rule of "Left Hand".

Remarkably, but somehow "around current-carrying conductor there is a magnetic field", and around exactly the same current (electron beam) but without the guide "around", no magnetic field? As a conductor, "adds" a magnetic field when current is only the movement of electrons in it? » / NanoWorld.org.ru›topic/701/page/7//
"To explain attraction and repulsion of parallel conductors with current possible that the electrical field around a magnetic field having its pole, probably at these conductors, they are different, this attraction is obtained. Just like a magnet, different poles attract and repel each other with the same name.

Obviously, it is very simple. Around any conductor with a current magnetic field is formed. If two parallel conductor and around each conductor appeared magnetic field become effective strength of the magnetic poles. Wires of opposite poles attract and repel each other with the same name. " /3.1Chem can be explained by the attraction of two parallel bolshoyvopros.ru ... > Questions ... ... provodnikov tokom.htm /

The case remains for small. Find out how current-carrying conductors are transformed into magnets.

In Fig. 4.8.1 is a sectional view of two current carrying wires. Displaying circular transverse direction ether flows. Paragraph 43. / Interaction with current conductors servomotors.ru > documentation / electrical 43.html ... 2 ... / current explanation is presented the physical nature of interaction with the current conductors:

- "If close to each other arranged conductors with current in one direction, the magnetic lines of these conductors, covering both conductors, having a longitudinal tensile properties and in order to cut, will cause the conductors to be attracted.

- Magnetic lines of two conductors with the currents of different directions in the space between the conductors in the same direction. Magnetic lines having the same direction, are mutually repelled. Therefore, the conductors with currents in opposite directions repel one another. "

Such an explanation does not match the reality. According to the concept of Faraday and Maxwell, and the results of this study around current-carrying conductors do arise streamline, i.e. circular transverse streams ether as shown in the figures and 4.8.1a 4.8.1b. The mechanical nature of the electric current in the conductors is considered in the study 3.7. Where the lines are thick current - ether stream rate will be greater, therefore, the pressure will be less than where current lines are less common. Therefore, in this case, the conductors depicted in Fig. 4.8.1a will be repelled rather than attracted. While depicted in Fig. 4.8.1b, will be attracted, not repelled. However, besides circular transverse currents exist ether longitudinal streams directed along the axes of the conductors with current. Figures 4.8.2 and 4.8.3 are presented mechanical interaction model with current conductors. Shows longitudinal and cross sections of conductors with current. In Fig. 4.8.2 sloping ether streams along the first conductor - and along the second conductor- directed in the same direction (unidirectional currents). A in Fig. 4.8.3 incident stream ether and in opposite directions (Note i -. hereinafter - denote the ordinal number of the handset participating in the interaction).

For convenience, the conductors are shown in the figures one above the other. In fact, the conductor 1 is disposed in front of the conductor 2 that correspond to the image presented in the section A-A.

The set angular velocity streams of small ether sources (electrons) conductor 1 - , it creates a directed stream of ether around the conductor 2 - . Where - angular tube ether unit stream rate of the conductor 1, and - linear velocity of the circular cross-flow mini ether source conductor 1.

Similarly, a plurality of angular velocities mini sources ether conductor 2 streams - it creates a directed ether stream around the conductor 1 - . Where - angular tube ether unit stream rate of the conductor 2, and - linear velocity of the circular cross-flow mini ether conductor source 2.

Mini sources are shown in the figures in small circles with the sign (-) and the solid arrow indicating the direction of rotation of mini-power.

Under the influence of the amount of perpendicular stream + Explorer 1, and under the influence of the amount of perpendicular stream + conductor 2, maxi- drains (protons) and maximum sources (antiprotons) that make up the substance of conductors in accordance with the study 4.7 turn the magnetic poles of the side into which streams ether stream into, as shown in Figures 4.8.2 and 4.8 .3. Maxi sources depict large circles with the sign (-), and Maxi drains depicted large circles with the sign (+). The solid arrows indicate the direction of rotation maxi- sources and maximum effluent. Mechanical model of electrons, protons and antiprotons are considered in studies 3.6 and 4.1.

In this case the angular rotation velocity streams ether maxi- sources and maximum runoff - will coincide with the direction of +. decomposed into two components: - disposed along the axis of the conductors and - disposed across the conductors. And   decomposed into two components: - disposed along the axis of the conductors and - disposed across the conductors. The angular rotation speed of ether streams depicted in the figures by white arrows.

The set angular velocity streams ether maxi- sources  and maximum runoff - conductor 1 creates a field of linear velocities circular cross stream around the conductor 1 ether - . A plurality of angular velocities ether streams maxi- sources - and maximum runoff - conductor 2 field linear velocities creates circular cross stream around the conductor ether 2 - . Applying the principle of superposition of velocity fields  and , we obtain mechanical interaction model circular cross stream ether parallel conductors with current, shown in Fig. 4.8.1. As stated previously, in this case, the conductors with unidirectional currents will be repelled, and with oppositely directed currents will be attracted.

Similarly, a plurality of angular velocities ether streams maxi- sources - and maximum runoff - conductor 1 creates a field of linear velocities of a longitudinal stream along the axis of the conductor ether 1. A plurality of angular velocities ether streams maxi- sources and maximum runoff - conductor 2 field linear velocities creates longitudinal stream of ether along the axis of the conductor 2 - . Where and - linear velocity field of longitudinal stream ether maxi- sources and maximum effluent conductors 1 and 2 respectively. Applying the principle of superposition of velocity fields and , we obtain mechanical interaction model ether longitudinal stream parallel conductors with current, shown in Fig. 4.8.2 and 4.8.3. Figures 4.8.2 and 4.8.3 in the cross sections A-A and between the conductors on both sides of them multidirectional circles show unit section tubes ether fluxes (magnetic field lines). Where circles () - indicate the removal of the ether streams from the observer, and circles () - indicate the approaching ether stream to the observer. In this case, the pressure between the wires with the same current direction as shown in Fig. 4.8.2, will be less than on either side of them as and between the conductors are added and subtracted from the outside. While the pressure between the conductors with oppositely directed currents, shown in Fig. 4.8.3 will be greater than outside, because  and between the conductors are deducted, and outside the fold.

Consequently, the parallel wires with the same current direction will be attracted, while as the opposite direction will be repelled.

We conclude that in the case of interaction with parallel conductors shock forces arising from the longitudinal ether stream prevail over the forces that arise from the transverse ether streams. These findings are confirmed by experiments with magnets Nikolaev having similar nature of physical interactions presented in the study, 4.11.

The present study provides substantiate mechanical nature of the physical phenomenon of interaction of parallel conductors with the currents.

Fig. 4.8.1

А


Conductor 1

Conductor 2

А

() А-А

Conductor 2 Conductor 1

Longitudinal ()

single tubes

Fig. 4.8.2

А Conductor 1

Conductor 2

А


() А-А ()

Conductor 2 Conductor 1

Longitudinal

single tubes

Fig. 4.8.3