A circuit with no length limit distributes magnet properties in the following way: in the beginning and end of the circuit – the mechanism of magnet self - motion; in the center of the circuit – attraction.
Magnet self – motion interacts with the effect of (dipole) repulsion rather well (there will be the directed effect of repulsion); (Figure 2).




















Series of split – level circuits with magnet self – motion and main poles of permanent magnet may act (directed motion) surpassing reaction thrust of the effect of repulsion and attraction of the main poles.

Interaction with magnetized iron

If we’ll place a magnet disc on a round, convex platform with free rotation, on the edge of the main pole of magnet disc and at the minimal mutual distance, in semi – ring and after that magnetize the iron bars – then while acting upon the semi – ring with the magnet self – motion circuit we’ll observe a directed motion (rotation) from the beginning to the end of the semi – ring.

Interaction with electric current

We’ll place an iron core into the center of copper coil, connect it to the power supply source, act upon the iron core with the center of magnet self – motion circuit and see that there is no directed motion at all.

In order to obtain the effect of magnet self – motion from the opposite side at the magnet circuit, towards to the iron core we’ll fix the main pole of permanent magnet and act upon the iron core with magnet self – motion circuit. That will cause directed motion. Having increased the air gap distance between magnet self – motion circuit and iron core of the copper coil (until the interaction of directed motion stops) and connected the coil to the power supply source - we’ll observe the directed interaction between the iron core magnetized by the main pole of permanent magnet and magnet self – motion circuit (while magnetizing the iron core with main pole of permanent magnet, the current in the magnet coil increases the capacity of magnet self – motion; at that, the direction of the current in the coil is not important).

Magnet self – motion is able to produce the work of directed pulling motion by interacting with the iron core of electric magnet which is magnetized by the main pole of permanent magnet, at that the current in the electromagnet coil increases the capacity of pulling force of magnet self – motion.

Obtaining of electrical current

We’ll place a sharp iron core into the center of copper coil. Having touched the edge of the iron core by the center of neutral zone (hereinafter referred to as: magnet self – motion) of a magnet cube of the dipole magnet and performed a back-and-forth motion without any gap distance, approximately by 1/10 part of the magnet self – motion area – we’ll obtain an electrical current. The same actions with using of magnet self – motion will produce very little electrical current.

Approaching and moving away of the main pole to the ore core of the copper coil – an electrical current occurs. The same actions with magnet self motion will produce very little electrical current.

We’ll place an iron core into the center of copper coil and will perform a linear motion with flat surface of magnet cube with magnet self – motion, perpendicularly to the iron core with fixed air gap distance. At that we’ll approach and move away the magnet cube.
(We’ll study the case of obtaining of electrical current under the conditions of permeability of iron).
Having done that we’ll get a butt approaching and moving away, if we deal with the main opposite poles – it will be electrical current of the same direction; and in the case of the surface with magnet self – motion – it will be electrical current of the opposite direction. (The same actions without any iron core will lead to the same situation with physical properties of magnet).
For comparison, we’ll obtain electrical current in the following way. We’ll place a rotating round platform with electric motor drive in front of copper coil with an iron core. And turn-based, we’ll compare the effect of both main pole and magnet self – motion by placing the magnet cube on the platform with fixed air gap distance between the magnet and iron core of the copper coil.
The magnet self – motion then will be characterized with a higher electric potential (voltage) and lower current.
The properties of magnet, given above, point out the possibility of creating of engine – generator where consumption of the current obtained will increase pulling effect of magnet self – motion.

For example: let’s magnetize iron cores of electric magnets with the main pole of permanent magnet, place them around (circumferentially), in semi – ring (that is in an incomplete ring) and at different levels complete the circle with using of other semi – rings (on a stator basis) where each of the semi – rings in a certain sequence will interact with magnet self – motion circuit: at split-level sequence of magnet circuit construction (on a rotor basis), for obtaining circular rotation,- and then during rotation electrical current is obtained finally. At that, the electrical current enforces the pulling force of magnet self – motion.
By moving away the magnet circuit from the semi – ring, we get the effect of attraction.
In order to decrease the reaction thrust of the effect of attraction we need some of the decreasing measures; in case, we speak about interaction of the generator with chemical source of the electrical current – we’ll have to use the collector.