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NEW INVENTIONS AND MODELS. ALTERNATIVE ENERGY || NEW INVENTIONS And MODELS. ALTERNATIVE ENERGY

PRINCIPLES OF EXTRACTION OF MAGNETIC ENERGY FROM CONSTANT MAGNETS
AND TRANSFORMATION OF IT TO OTHER TYPES OF ENERGY

Dudyshev Valery Dmitrievich, Russia, Samara
Samara Technical University
Valery Dmitrievich Dudyshev

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SEGMENTAL MAGNETIC ENGINES WITH MAGNETIC FLUX SWITCHING

For magnetic machines, the general principle of reversibility of their operating modes is also valid. Any workable magnetic machine on the PM can work both in the generator (generating electricity in the presence of an inductive winding), and in the driving regimes. In addition, in such a segmental magnetic converter-machine, a combined motor-generator operating mode is also possible, which is a fundamental difference from the known electromagnetic machines. The generator mode of the segmented magnetic converter is described above.

As experiments with annular magnets cut into segmented parts show, these segments are spontaneously pushed out of the ring magnet, and a splash (commutation) of the magnetic field is obtained.

The principle of operation of the simplest segmented magnetic motor

 The principle of operation of the simplest segmented magnetic motor consists in commutation - the interruption of the magnetic flux of the annular magnet by cyclic movement (sliding in and out) of the mobile magnetic segment of the ring ( Fig . 1 ).

Let us explain the principle of operation of such a segmented magnetic motor.

In such an unusual MD, the effect of spontaneous ejection of the magnetic segment from the annular permanent magnet is used. To do this, we make a ring magnet with one or several segments cut out in advance, places a ring with the same cut out segment above it. Since the ring is magnetized by a magnet, we get a system of two magnets one above the other in parallel planes (the ring is designated) from the first part. For such a system, Fig. 4 ( Fe ) there are two stable positions B and D and two unstable A and C from which the magnet rotor tends to turn to position D or B. As can be seen from Fig. 3 The iron ring on top of the magnet is cut into segments. The algorithm for controlling the commutation of the magnetic field in such a Md is sufficiently simple.

As the magnet rotates from the unstable position to the stable one, on the approach to the stable position, we pull out the next segment (if we look in the direction of rotation and we pull the pulled back in ( Figure 3 shows such a cyclogram.) Thus, the magnet again turns out to be unstable and accelerates To the next stable point.For continuous rotation of the main magnet, this process must be repeated cyclically, ie alternately switch segments of the MD (pull-insert segments of the magnet) in the course of rotation by special mechanical devices.Let us now explain the construction of this MD in more detail.

As the magnet rotates from an unstable position to a stable

Magnet 1 is preliminarily cut into four identical segments ( Figure 2 ), we place the ring assembled from the segments above the semi-ring magnet. As a result, in addition to the mutual attraction of the segmented metal ring to the permanent semi-ring magnet (there will be no turning-the system is symmetrical-the metal ring of the segments is one-segmented-the segments are shifted to each other), we obtain a second force: since the permanent magnet faces the ring with one side and the polarity, Then all segments magnetized by a single polarity will repel each other and if only one segment is allowed to become free, it will now simply be pushed out by the induced magnetic monopole from the circle ( Fig. 3 ). The arrows indicate the vectors of the monopole opposition forces.

Now, when one segment is pushed out by the induced field of a semicircular magnet, the symmetry of the ring is broken and it is due to the opening of the common magnetic line of the ring by the air gaps A and B in Fig. 3 - converted into a linear, bent magnet, and it has a maximum field strength at the edges - in the gaps A and B and the minimum of the stress at point C in Fig. 3 , that is now the system: the magnet - the split ring is not symmetrical and the magnet on the bearing of the cooler will entrust, having spent its energy - up to the equilibrium point of the system, the magnet will try to put its sine of the field strength along the magnet body into the cosine of the magnetic field induced on the split ring.

Now consider the cyclogram of the magnetic force interactions of these two magnets with the segments ( Figure 4 ) per revolution of the magnet 1 .

Now consider the cyclogram of the magnetic force interactions of these two magnets with the segments (Figure 4) per revolution of the magnet 1.

If we place above the magnetic semicircle - a metal semicircle - composed of two 45 degree segments, then there will be four equilibrium positions of the system ( Figure 4 ): two - stable B and D , and two unstable - hill tops - A and C , That the system will prefer sustainable options. According to the principle of La Chatelier, any energy system in nature in general by all means strives to become stable - with minimal energy of the state. If the magnet poses. And Fig. 4 , push it from the magnetic roller, then, trying to establish itself in a position of stable equilibrium, it will do the work, turning for example to position B of Fig. 4 , etc., that is - by manipulating segments with the integrity of a metal ring - we force the magnet to work when it is reinstalled and if the segments in Fig. 3 position 1 and 2 in turn put in place, thus pushing each other out, the point of stable angular equilibrium of the magnet will change from C to D in Fig. 3 , and so on provoking the magnet to work for us. - spinning in a circle. Now the problem is reduced to how - how less to spend your energy, forcing segments 1 and 2 of Fig. 3 to take turns to place in the ring, causing indirectly, through a change in the positioning of the induced magnetic field, to cause the magnet to work in this system.

Let us consider the main driving and opposing forces in this MD construction ( Figure 3 ) - in gaps A and B. Thus, in summary, in the gaps A and B of Fig. 3, the main induced magnetic field is concentrated on the repulsion, then to insert the segment 2 of Fig. 3 , and due to this, push out segment 1 of Fig. 3 - it is necessary to expend the same energy as the magnet gives, minus the friction loss, etc. Then where is the energy gain?

The cycle of the segments is as follows

 The cycle diagram of the segments is as follows (according to Fig. 5 ). Let's make the segments 1 and 2 of Fig. 5 , then segment 2 - with all the force is attracted to the semi-ring, and segment 1 - hovered at a balance of field forces, resulting in an unbalanced magnetic system - a magnetic trigger, but if the active segments are connected by lever 3 in Fig. 5 , then a complete damping of the system requires a damper-a pulse accumulator such as an intermediate spring 4A and 4B in Fig. 5 with a nonlinear quadratic compression characteristic, we now compensated for the nonlinear characteristic of the gap magnetic field by the reciprocal compression characteristic of springs 4A and 4B ( Figure 5 ), so that in the sum of the energy costs for segment switching we obtain a linear balanced and countercompensated segment management system and Turn extremely low-cost control of the force magnetic field of a permanent semi-ring magnet with the help of for example a solenoid - output speed setpoint pos. 5 fig. 5 . As a result, we provide an extremely long rotation of the magnet due to its internal potential energy.
An easier way to manage segments is shown, for example, in Fig. 6 . Here is a view from the side where:
1 - semi-ring magnet;
2 - active segments;
3 - the lever from a spring wire - that is it the lever-spring-accumulator of a control impulse;
4 - thrust coils of the control solenoid,
5 - a reference axis of a swing of the lever.

It is possible and simple to provide control of segments due to the crank-connecting mechanism installed on the main shaft.

In this embodiment of the switching device of the MD segments, the return springs need not be compensated so that a slightly trigger effect remains, i.e., the segments must reverse the position abruptly. Practice shows that the traction magnet of the rotor should ideally have a trapezoid shape, the plane of its faces coinciding with the lines of the radius of the magnetic ring. For experiments, the use of a magnet having the form of a parallelepiped is permissible.

An easier way to manage segments

LITERATURE

  1. Dudyshev V.D. The phenomenon of direct conversion of the energy of magnetic fields of permanent magnets to other types of energies - "New Energy", 3/2004.

  2. Dudyshev V.D. New methods for extracting and converting the latent potential energy of the electric field into kinetic energy and electricity - "New Energy", No. 4 // 2003

  3. Barkhausen magnetic effect-A great encyclopaedic dictionary, M. "SE", 1991, vol.1, p.108

  4. Electromagnetic induction-A large encyclopedic dictionary, M. "SE", 1991, vol.2, p.688, 690

  5. Curie thermomagnetic effect - Large Encyclopedic Dictionary, M. "SE", 1991, vol.1, p..680

  6. Dudyshev V.D. The new electric fire technology of environmentally friendly combustion - "New Energy" No. 1.2003g.

  7. Dudyshev V.D. Electro-fire utilization of oil sludge - "Ecology and Industry of Russia" May, 2002.

  8. Dudyshev V.D. The new electric field technology of extinguishing and preventing fires- "Ecology and Industry of Russia" December, 2003.

  9. Dudyshev V.D. Fuel economy and reduction of toxicity of gasoline engines- "Ecology and Industry of Russia" May, 2003.

  10. Dudyshev V.D. "New effect of cold evaporation and dissociation of liquids on the basis of the capillary electroosmotic effect" - "New Energy" "No. 1/2003.

  11. Magneto-electric generator based on an annular permanent magnet
    Http://WWW.SHRAM.KIEV.UA/invention/invention2/24.shtml

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Author: Valery Dudyshev
PS The material is protected.
Date of publication 03.01.2005гг