© Magnetic self-motion.2001.
The main property.
1) The main property of the neutral zone of a permanent magnet is the presence of a directed force of movement (magnetic self-motion) with a pronounced attraction in relation to any main pole of another magnet. (Fig.1).
2) When the neutral zone magnetic field moves parallel to the magnetization axis along the plane of the conducting circuit, an electric current is generated. (This statement is true: for the region between the opposite poles of a magnet, there is a resulting magnetic field.(Electromagnetic induction). The same is true for the neutral zone of a permanent magnet.(Magnetic self- motion)).(Fig 3)
Directed motion.
A property of the magnetic field of a permanent magnet's neutral zone is the presence of a directional force of motion (magnetic self-motion) with a pronounced attraction bordering on dipole repulsion relative to any primary pole of another magnet (a magnetized ferromagnet by the primary pole of a permanent magnet). When connecting unlike poles in series, we obtain a chain of motion in two directions.(Fig. 1).

A series circuit has a limited length, corresponding to the mechanism of magnetic self-propulsion. A circuit with unlimited length distributes magnetic properties as follows: magnetic self-propulsion occurs at the beginning and end of the circuit, while attraction occurs at the center of the circuit.
Magnetic self-propulsion interacts well with the (dipole) repulsion effect (resulting in a directional repulsion effect). (Fig. 2).

Interaction with magnetized iron.
By placing an axially magnetized magnetic disk on a freely rotating circular convex platform, we magnetize iron rods at a minimum distance from each other in a semicircle around the edge of the magnetic disk's primary pole. We apply a magnetic self-propelled chain to the semicircle to achieve directional motion (rotation) from the beginning to the end of the semicircle.
The emergence of an electric current.
When the magnetic field of the neutral zone moves parallel to the axis of magnetization along the plane of the conducting circuit, an electric current arises.
We insert a sharp iron core into the center of a copper coil. Perpendicular to the iron core, we touch the center of the neutral zone plane of an axially magnetized magnetic cube and perform a reciprocating motion without an air gap, approximately 1/10th of the way across the neutral zone plane (a doubly charged magnetic field with a dipole sequence). This generates a bidirectional electric current.
The same actions with the main pole of a permanent magnet - a single-charge magnetic field (electromagnetic induction) of current arises insignificantly.
We insert an iron core into the center of a copper coil. With its neutral zone plane parallel to the magnetization axis of a magnetic cube with axial magnetization, perpendicular to the iron core of the copper coil with a fixed air gap, we perform a linear motion with the magnetic cube approaching and receding relative to the iron core of the copper coil. Consider the pattern of current generation with iron permeability: we obtain the end-on approach and receding of the main opposite poles (an increasing and decreasing magnetic field)—currents in the same direction, approximately 30% of each for electromagnetic induction. (The direction of the current corresponds to the direction of motion). When moving in the region of magnetic self-motion, the current is 100% pulsating in the opposite direction.
The same actions without an iron core result in the same pattern of magnetic field physical properties. (Fig. 3).


Interaction with alternating current.
We insert an iron core into the center of a copper coil, pass an alternating electric current through the coil, and act on the core with the center of a magnetic self-motion circuit. Directional motion is absent (the electromagnetic field does not interact with the magnetic self-motion). With alternating current, reciprocating motion occurs.
To achieve directional motion, we magnetize the iron core with the primary pole of a permanent magnet and act on the core with a magnetic self-motion circuit. Directional motion occurs. We increase the air gap between the magnetic self-motion circuit and the iron core of the copper coil magnetized by the magnetic field until the directional motion ceases. We pass an alternating electric current through the coil. Directional motion occurs between the magnetic self-motion, the iron core magnetized by the magnetic field of the permanent magnet, and the electromagnetic field of the current-carrying coil. (When an iron core is magnetized by a magnetic field, the electromagnetic field of the coil with current enhances the interaction of the magnetic field with magnetic self-motion, increasing the traction force of the directed motion, while the direction of the current in the coil does not play a significant role).









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