KR20030007703A - Magnetic controlled current or voltage regulator and transformer - Google Patents

Abstract

The invention relates to a magnetically influenced current or voltage regulator comprising a body (1) which is composed of a magnetisable material and provides a closed, magnetic circuit, at least one first electrical conductor (8) wound about the body of a first main winding (2) and at least one second electrical conductor (9) wound about the body of a second main winding (4). The winding axis (A2) for the main winding (2) is at right angles to the winding axis (A4) for the control winding (4) with the object of providing orthogonal magnetic fields (H1, B1 and H2, B2 respectively) in the body (1) and thereby controlling the behaviour of the magnetisable material relative to the field (H1, B1) in the main winding (2) by means of the field (H2, B2) in the control winding (4).

Description

Magnetically controlled current or voltage regulator and transformer

Typically, variable speed engine control is based on two devices. I.e., AC-DC-AC with a) direct electronic frequency-regulated converter and b) pulse-width modulation, and extended use of semiconductors such as thyristors and IGBTs. It is a converter. The AC-DC-AC converter represents a technology widely used in industrial applications and is also used on boards such as locomotives.

Speed control has recently been introduced in motors in the underwater environment, the main goal being the packing and operation of the systems described above. In this specification, operations include service, maintenance, and the like. In general, complex electronic systems must be operated in a controlled environment for temperature and pressure. The marine version of the system must be encapsulated in a container filled with nitrogen that maintains a pressure of atm. Due to the heat generation due to the heat loss of the electronic components, a considerable amount of heat is generated, which requires forced air cooling. This is usually solved by using a pan, which is known as a component that significantly reduces the operating life of the system and represents a very unsuitable solution.

In addition, electronic components and electronic power semiconductors are very sensitive and require protection circuits, but this complicates the system and increases the cost.

At large depths (above 300 meters) the protective containers of the above systems become very heavy, which accounts for a significant proportion of the total weight of the system. In addition, since maintenance of a simpler system is difficult to perform with a Remotely Operated Vehicle (ROV), it will be frequently required to elevate the entire frequency converter for maintenance of the system.

FIELD OF THE INVENTION The present invention relates to magnetically controlled current or voltage regulators and transformers and, more particularly, to control the connection / disconnection by means of the distribution of electrical energy as introduced in the appended claims. The present invention relates to an electrically controlled current or voltage regulator and a converter.

1 and 2 show the basic theory of the first embodiment according to the present invention.

3 is a wiring diagram showing one embodiment of the device according to the invention.

4 shows regions of different magnetic flux forming part of the device according to the invention.

5 shows a first balanced circuit of a device according to the invention.

6 is a schematic block diagram of an apparatus according to the invention.

7 is a graph showing current versus magnetic flux.

8 and 9 show magnetic curves and regions for magnetic materials of the device according to the invention.

10 is a graph showing the magnetic flux density for the main winding and the control winding.

11 is a view showing a second embodiment of the present invention.

12 is the same view as in the second embodiment of the present invention.

13 and 14 are sectional views of the second embodiment.

15 to 18 are views showing different embodiments of magnetic field connectors in the second embodiment of the present invention.

19 to 32 are views showing different embodiments of the pipe-like bodies in the second embodiment of the present invention.

33 to 38 are views showing different embodiments of magnetic field connectors used in the second embodiment of the present invention.

39 is a view showing the assembled device according to the second embodiment of the present invention.

40 and 41 are cross sectional and perspective views of a third embodiment of the present invention.

42 to 44 are diagrams showing other embodiments of magnetic field connectors used in the third embodiment of the present invention.

45 shows a third embodiment of the invention adopted for use as a transformer.

46 and 47 are cross-sectional and perspective views showing a fourth embodiment of the present invention used as a reluctance control, flux-connected transformer.

48 and 49 illustrate a fourth embodiment of the present invention without a magnetic field connector by applying a powder-based magnetic material.

50 and 51 are cross-sectional views taken along the lines VI-VI and V-V in FIG. 48.

52 and 53 are diagrams showing cores without magnetic field connectors by applying a powder-based magnetic material.

54 is a perspective view ("X-ray picture") according to a modification of the fourth embodiment of the present invention.

55 shows a second variant of the device according to the invention with the theory of eliminating the possibility of transformer connection.

56 is a diagram for suggesting an electrical wiring symbol for a voltage connector according to the present invention.

57 shows a block diagram wiring symbol for a voltage connector.

58 is a diagram illustrating a magnetic circuit that does not include the control winding and the control magnetic flux.

59 and 60 are diagrams suggesting electrical wiring symbols of a voltage connector according to the present invention.

Fig. 61 shows the use of the present invention in an alternating current circuit.

62 illustrates the use of the present invention in a three phase system.

FIG. 63 shows use as a variable choke of a DC-DC converter. FIG.

64 shows use as a variable choke of a filter with a condenser.

65 is a schematic reluctance model for a device according to the invention and a schematic electrical balance diagram for a connector according to the invention.

Fig. 66 shows a connection for a magnetic switch.

67 shows examples of three phases used in the present invention.

Fig. 68 is a diagram showing an apparatus used as a switch.

69 is a circuit diagram including six devices according to the present invention.

70 shows the use of the device according to the invention as a DC-AC converter.

71 shows the use of the device according to the invention as an AC-AC converter.

It is therefore an object of the device according to the invention to provide a frequency converter suitable for underwater pumping operations, with particular emphasis on reliability, stability and minimal maintenance requirements of operation. The requirement for this operation would be about 25 years at a depth of 3000 meters.

Standard frequency converters based on semiconductor technology convert AC power with a given frequency to AC power of another selected frequency without any intermediate DC connection. The conversion is performed by forming a connection between given input and output terminals for a controlled time interval. An output voltage curve with an output frequency FO is produced by sequentially connecting segments of the voltage curve selected on an AC input source having an input frequency F1 to the terminals. These frequency converters are in the form of standard symmetrical cycloconverters for powering three-phase motors in three-phase networks. Since the standard frequency converter module consists of a dual converter in each motor phase, it is common practice to employ three ideally and essentially independent double motors that provide a three phase output.

Other types of known frequency converters consist of three quadrant 12 pulse center converters with respective output phases. All three transducers share a common second winding on the input transformer. Neutral conductors can be omitted to balance the three phases loaded on the Y-coupled motor.

Another frequency converter based on semiconductor technology is a so-called symmetrical 12-pulse bridge circuit, which is equipped with three quadrangular 12 pulse bridge converters each having an output phase. Input terminals on each of the six six-pulse transducers are conveyed from a second winding separated on the input transformer. It should be noted that since each 12-pulse converter requires two fully insulated transformer second windings, the same second winding should not be used for more than one transducer.

Therefore, another essential object of the present invention is to avoid the main semiconductor components of the frequency converter which must be located at a large depth (deep sea), and for this purpose the present invention is a novel magnetic converter which is not entirely based on conventional concepts. ) Suggest technology.

The present invention includes a magnetically influenced current or voltage regulator, wherein the current or voltage regulator according to the first embodiment of the present invention is made of a magnetisable material and is a closed magnetic circuit. A body provided with; At least one first electrical conductor wound around the body along at least a portion of the closed circuit for at least one turn to form a first main winding; And at least one second electrical conductor wound around the body along at least a portion of the closed circuit for at least one rotation to form a second main winding or control winding, wherein the rotation or rotation of the main winding The winding axis for the wheel is preferably perpendicular to the winding axis for the rotation or turns of the control winding. The purpose of this is to provide an orthogonal magnetic field to the body to control the action of the magnetizing material in proportion to the magnetic field of the main winding by the magnetic field of the control winding. In a first preferred embodiment, the axis for rotation (s) of the main winding is parallel or coincident with the vertical direction of the body, and the rotation (s) of the control winding extends gradually along the magnetization body, so that the control The axis of winding is right angle with the vertical direction of the body. Another variation of the first embodiment is that the axis for rotation (s) of the control winding is parallel or coincident with the vertical direction of the body, and the rotation (s) of the main winding gradually extend along the magnetization body, The axis of the main winding is to be perpendicular to the vertical direction of the body.

This first embodiment of the device can be employed as a transformer by having a third electrical conductor wound around the body along at least a portion of the closed circuit for at least one rotation to form a third main winding. 3 The winding axis for the rotation or the rotations of the main winding is coincident with or parallel to the winding axis for the rotation or the rotations of the first main winding, such that when electricity is applied to at least one winding, the first main winding and the first It is desirable to provide a transformer effect between the three main windings. Another variant, in which the first embodiment of the present invention can be applied as a transformer, is provided with a third electrical conductor wound around the body along at least a portion of the closed circuit for at least one rotation to form a third main winding, The winding axis for the rotation or rotations of the third main winding is coincident with or parallel to the winding axis for the rotation or rotations of the control winding, so that if at least one winding is energized, a transformer between the third main winding and the control winding It is desirable to provide action.

A second embodiment of the present invention includes a magnetically affected current or voltage regulator, the current or voltage regulator comprising: a first body each made of a magnetizing material and provided with a closed magnetic circuit and adjacent to each other; Second body; At least one first electrical conductor wound along at least a portion of the closed circuit for at least one rotation to form a first main winding; And a second electrical conductor wound around at least a portion of the first body and / or the second body for at least one rotation to form a second main winding or control winding, the winding for rotation or rotations of the main winding. The axis is preferably perpendicular to the winding axis for the rotation or the turns of the control winding. Its purpose is to provide an orthogonal magnetic field to the body to control the action of the magnetizing material proportional to the magnetic field of the main winding by the magnetic field of the control winding. Of course, since the main winding and the control winding are interchangeable, at least one first electrical winding around at least a portion of the first body and / or the second body for at least one rotation to form a first main winding. conductor; And a second electrical conductor wound along at least a portion of the closed circuit for at least one rotation to form a second main winding or a control winding, wherein the second electrical conductor provides an orthogonal magnetic field to the body by the magnetic field of the control winding. Magnetically influencing, characterized in that the winding axis for the rotation or the rotations of the main winding is perpendicular to the winding axis for the rotation or the rotations of the control winding for the purpose of providing the action of the magnetizing material in proportion to the magnetic field of the main winding. A current or voltage regulator can be provided.

A preferred variant of the second embodiment includes first magnetic field connectors and second magnetic field connectors forming the closed magnetic circuit together with the bodies.

In addition, the second embodiment of the device can be employed as a transformer by having a third electrical conductor wound around one revolution to form a third main winding, wherein the winding axis for the rotation or turns of the third main winding Coincident with or parallel to the winding axis A2 for the rotation or rotations of the first main winding or the control winding, between the third main winding and the first main winding or the control winding when electricity is applied to at least one winding. It is desirable to provide a transformer action.

In the second preferred embodiment of the present invention, the first body and the second body are tubular, so that the first conductor or the second conductor extends through the first body and the second body. Can be. The magnetic field connectors preferably comprise apertures for the conductors. In addition, in a preferred embodiment of the present invention, each magnetic field connector includes a gap to facilitate the insertion of the first or second conductor. In a preferred embodiment, the device is provided with an insulating film located between the cross sections of the pipes and the magnetic field connectors, by short-circuiting the film layer by isolating connecting surfaces. It is possible to prevent the generation of induced eddy currents on the connecting surfaces. However, an insulation film would not be needed for cores made of iron or compressed powder. In addition, in the second embodiment, each pipe includes two or more core parts, and an insulating layer is provided between the core parts. In addition, the pipes according to the second embodiment of the present invention may have a cross section of a circle, a square, a rectangle, a triangle, or a hexagon.

A third embodiment of the invention relates to a current or voltage regulator which is magnetically affected, wherein the current or voltage regulator is made of a magnetic material, is provided with a closed magnetic circuit and is concentric with each other. A first external tubular body and a second internal tubular body; At least one first electrical conductor wound around the pipe-like bodies for at least one rotation to form a first main winding; And at least one second electrical conductor provided in the space between the bodies and wound around a common axis of the bodies for at least one rotation to form a second main winding or a control winding. The winding axis for the rotation or the turns of the winding is preferably perpendicular to the winding axis for the rotation or the turns of the control winding. In other words, the purpose is to provide an orthogonal magnetic field to the bodies to control the action of the magnetizing material which is proportional to the magnetic field of the main winding by the magnetic field of the control winding. In addition, in the third embodiment of the present invention, since the main winding and the control winding may be interchanged with each other, the main winding and the control winding may be interchanged with each other. At least one first electrical conductor forming; And at least one second electrical conductor wound around the pipe-like body for at least one rotation to form a second main winding or control winding, wherein the winding axis for the rotation or rotations of the main winding is a rotation of the control winding. Or a magnetically influenced current or voltage regulator characterized in that it is perpendicular to the winding axis for the rotations.

A preferred variant of the third embodiment of the present invention comprises first and second magnetic field connectors which together with the bodies form a closed magnetic circuit.

In addition, the third embodiment of the device may be employed as a transformer by being provided with a device having a third electrical conductor which is wound for at least one revolution to form a third main winding. In this case, the winding axis for the rotation or the rotations of the third main winding is coincident with or parallel to the winding axis for the rotation or the rotations of the first main winding and when the electricity is applied to at least one winding. Providing a transformer action between the third main windings or applying electricity to at least one winding in which the winding axis for the rotation or rotations of the third main winding is coincident with or parallel to the winding axis for the rotation or the rotations of the control winding Preferably provides a transformer action between the third main winding and the control winding.

The fourth embodiment of the present invention for a magnetically influenced current or voltage regulator is the same as the third embodiment of the present invention, wherein the current or voltage regulator is a closed magnetic circuit each made of a magnetizing material and closed. Or a first outer pipe-like body and a second inner pipe-like body forming an internal core. The apparatus further includes an additional tubular body having an outer core coupled to the outside of the first outer piped body and having a shared axis concentric with the body; At least one first electrical conductor wound around the pipe-like body for at least one rotation to form a first main winding; And at least one second electrical conductor provided in a space between the first and second bodies and wound on a shared axis of the bodies for at least one rotation to form a second main winding or a control winding. The winding axis for the rotation or the turns of the winding is preferably perpendicular to the winding axis for the rotation or the turns of the control winding. In other words, the purpose is to provide an orthogonal magnetic field to the bodies to control the action of the magnetizing material which is proportional to the magnetic field of the main winding by the magnetic field of the control winding. In the same manner as the second embodiment of the present invention, provided in the space between the first and second bodies and wound on a shared axis of the bodies for at least one rotation to form a second main winding or control winding. At least one first electrical conductor; It is possible to provide an apparatus comprising at least one second electrical conductor wound around the pipe-like bodies for at least one rotation to form a second main winding or control winding.

A preferred variant of the fourth embodiment of the present invention comprises first and second magnetic field connectors which together with the bodies form a closed magnetic circuit.

Further, the fourth embodiment of the device can be employed as a transformer by having a third electrical conductor wound around the outer core for one rotation to form a third main winding. In this case, there will be two ways. That is, firstly, the winding axis for the rotation or the rotations of the third main winding is coincident with or parallel to the winding axis for the rotation or the rotations of the first main winding, so that when the electricity is applied to at least one winding, the first and Providing a transformer action between the third main windings, and secondly, the winding axis for the rotation or the rotations of the third main winding is coincident with or parallel to the winding axis for the rotation or the rotations of the control winding. When electricity is applied it is to provide a transformer action between the third main winding and the control winding.

Of course, the fourth embodiment of the present invention described above is coupled to the outside of the pipe-like body forming the outer core, the two pipe-like bodies forming the inner core, providing the inner core to one pipe-like body and the outer It may also be constructed in such a way that the core is provided in two pipe-like bodies.

In a preferred variant of the fourth embodiment of the present invention, the device is such that the outer core is made up of several annular parts, and the first and / or third main windings have individual windings on each annular part. It is characterized by forming. In another variant, the control winding and / or the third main winding may form individual windings on each ring.

The fourth embodiment is theoretically preferred.

The apparatus according to the invention may have many interesting applications, only some of which are mentioned below. That is, the device according to the invention is a) a component of a frequency converter for converting an input frequency into an output frequency which is arbitrarily selected for operation of an asynchronous motor, preferably in a frequency converter connection, b) operation of an asynchronous motor. A connector of a frequency converter for converting an input frequency into an arbitrarily selected output frequency for the summation of the phase voltage components generated in the phase of each motor in a 6 or 12 pulse transformer and c) an output of arbitrarily selected DC voltage / current A DC / AC converter that converts frequency to AC voltage / current, d) variable inductance voltage converters interconnected to produce a three-phase voltage with an arbitrarily selected output frequency coupled to the asynchronous device. As a DC / AC converter, e) to convert industrial AC voltage to DC voltage in the future, A reluctance-controlled variable transformer in which the output voltage is proportional to the reluctance change of the core magnetically connected in parallel or in series with an external or internal core with a separate second winding. A device in which at least three said reluctance control transformers are connected to conventional three-phase rectifier connections for a six or twelve pulse rectifier connection of a diode output stage. For use in a rectifier for conversion to a voltage transformer, which forms voltage connectors used as variable inductances in series with the first windings on conventional transformer connectors, wherein the three or more transformers are 6 or 12 pulse rectifier connectors in the diode output stage. Device connected to three-phase rectifier connectors for the purpose of: g) switched power supply ( In order to reduce the size of the magnetic voltage converter in AC / DC or DC / AC converters used in switched power supply applications, isolation is preferably achieved by forming variable inductance by filters with inductance. A device for forming a reluctance control variable transformer in which the output voltage is proportional to the reluctance change of a core magnetically connected in parallel or in series with an external or internal core having a second winding. linear) A configuration of a controllable voltage compensator that forms a variable inductance, i) being connected to conventional filter circuits consisting of at least one capacitor to produce a linear variable inductance, the capacitance or inductance of which is automatically connected Compensator conne is adjusted to the extent required to compensate for reactive power a reactive reactive power compensator in the form of a reluctance control transformer, which is adopted as the construction of a function, j) in a system for reluctance control that directly converts an AC voltage into a DC voltage, k) DC It can be applied in a system for reluctance control that converts a voltage directly into an AC voltage.

The voltage connector has no movable part to absorb the electrical voltage between the generator and the load. The function of the connector is to control the voltage between the generator and the load by 0-100% with low control current. It can also be used as a pure voltage switch or a current regulator, and can form and convert voltage curves.

The new technique according to the invention could be used to upgrade the current diode rectifiers required for regulation. By connecting to a 12-pulse or 24-pulse rectifier system, it may be possible to have diode rectification that can adjust the voltage of the system in a simple manner and control it from 0-100%.

The current or voltage regulator according to the invention can be configured in the form of a magnetic connector without a moving part and can be used for connection, thus transferring electrical energy between the generator and the load. The function of the magnetic connector is to close and open the electrical circuit. Thus, the connector will work in a different way than the transducers where transformer theory is adopted to saturate the core. The connector of the present invention controls the operating voltage by in / out of the main core with the main winding to saturation through the control winding. The connector does not have any transitive or inductive connection between the control winding and the main winding (as opposed to the transducer). That is, no significant common flux is generated in the control winding and the main winding.

This new magnetically controlled connector technology could replace semiconductors such as MOSFETs or IGBTs in GTO and other applications in high power applications, which is a stray current generated by the magnetization of the main winding. It is not limited to applications that can withstand. As mentioned above, the new converter will be particularly suitable for realizing a frequency converter which converts AC power with a given frequency into AC power with different selected output frequencies. In this case, no intermediate DC connection will be needed.

As mentioned at the outset, the device according to the invention has a frequency such as converters based on frequency converter theory, frequency converters based on 12 pulse bridge converters or frequency converters which directly convert DC voltage to AC voltage of variable frequency. It can be adopted in connection with the transducers.

The theory of the device according to the invention that employs variable reluctance in the magnetizing body or main core is that the magnetization current of the main winding wound on the main core is dependent on flux resistance according to Faraday's Law. It is based on the fact that it is limited by The magnetic flux that is formed to produce a counter-induced voltage depends on the magnetic flux resistance of the magnetic core. The amount of magnetic current is determined by the amount of magnetic flux that is formed to adjust the voltage applied.

The magnetic flux resistance of the coil in which the core is in air is 1000 to 900,000 times greater than the magnetic flux resistance of the winding wound on the core of ferromagnetic material. In the case of a low magnetic flux resistance (iron core), almost no current is required to form the magnetic flux needed to generate a bucking voltage to the voltage applied according to the Faraday law. In the case of a high magnetic flux resistance (air core), a large amount of current is required to form the magnetic flux required to generate the same induced reverse voltage.

By controlling the magnetic flux resistance, the magnetic current or load current can be controlled. In accordance with the present invention, the saturation of the main core is determined by a control flux perpendicular to the magnetic flux generated by the main winding to control the flux resistance. As already mentioned, the above-mentioned theory forms the basis of the present invention and relates to magnetically affected current or voltage regulators (connectors) and magnetically affected converter devices.

The connector and transducer can be manufactured by a manufacturing facility suitable for toroidal cores. From a technical point of view, the transducer can be made of a magnetic material, such as electroplating, wound around a suitably designed cylindrical core, and can be used at higher frequencies with compressed powder or ferrite. Of course, there is an advantage in that it is possible to manufacture ferrite cores or compressed powder cores according to the instructions of the application.

Hereinafter, exemplary embodiments of the present invention will be described in detail with reference to the accompanying drawings.

1A and 1B are diagrams for explaining the theory (principle) of the present invention.

Arrows associated with the magnetic field and magnetic flux in this figure indicate the direction in the magnetic material and are drawn on the outside for clarity.

1a shows a device comprising a body 1 made of magnetizing material forming a closed magnetic circuit. The magnetizing body or core 1 may be annular or other suitable form. A first main winding 2 is wound around the rounded body 1, and the direction of the magnetic field H1 (which coincides with the direction of the magnetic flux density B1) generated when electricity is applied to the main winding 2 is the magnetic circuit. Flows along. The main winding 2 is the same as the winding of a conventional transformer. In one embodiment, the device is a second main winding which extends along the body 1 (ie H1, B1 are parallel) in the same way as the main winding 2 is wound on the magnetizing body 1. It includes (3). The device comprises in the preferred embodiment of the invention a third main winding 4 extending inward along the magnetic body 1. The magnetic field H2 (magnetic flux density B2) generated when electricity is applied to the third main winding 4 has a direction perpendicular to the magnetic field directions H1 and B1 of the first and second main windings. The invention may also comprise a fourth main winding 5 wound around the leg of the body 1. When electricity is applied to the fourth main winding 5, a magnetic field having a direction perpendicular to the magnetic fields of the first main winding H1, the second and third main windings H2 is generated (see FIG. 3). . This naturally requires the use of a closed magnetic circuit for the magnetic field produced by the fourth main winding. The above circuit is not shown since the figure only shows the relative position of the windings.

However, in the phase which is preferably considered herein, the turns of the main winding occur in the direction of the magnetic field from the control magnetic field, and the rotations of the control winding occur in the direction of the magnetic field of the main magnetic field.

1b to 1g show the axes defined and the directions of the different windings and the magnetic body. For these windings, it is referred to as an axis perpendicular to the plane constrained by each rotation. The main windings 2, 3 have an axis A2, an axis A3, and the control winding 4 has an axis A4.

In the magnetizing body, the vertical direction may have various shapes. If the body is extended, the vertical direction A1 will coincide with the vertical axis of the body. If the magnetic body is a quadrangle as shown in Fig. 1A, the vertical direction A1 may be defined as each leg of the quadrangle. If the body is piped the vertical direction A1 will be the pipe axis and if it is annular the vertical direction A1 will follow the circumference of the ring.

The invention is based on the possibility of changing the properties of the magnetizing body 1 proportional to the first magnetic field by changing a second magnetic field perpendicular to the first magnetic field. Therefore, as an example, if the magnetic field H1 is defined as a working field, the characteristics of the body 1 (action of the working magnetic field H1) may be controlled by the magnetic field H2 (hereinafter referred to as the control magnetic field H2). This will be explained in more detail below.

The magnetization current of an electrical conductor surrounded by ferromagnetic material is limited by reluctance in accordance with Faraday's law. The magnetic flux formed to produce a countererinduced voltage depends on the reluctance of the magnetic material, including the conductor.

The range of the magnetic current is determined by the amount of magnetic flux formed to adjust the applied voltage.

In general, the steady-state equation below applies a sinusoidal voltage:

1) flux

(E = applied voltage, ω = angular frequency, N = number of revolutions for winding)

Here, the magnetic flux? Passing through the magnetic material is determined by the voltage E, and the current required to form the required magnetic flux is determined by the following equation.

2) current

3) Reluctance (magnetic flux resistance)

(l _j = flux path length μ _r = relative transmission, μ ₀ = vacuum transmission, A _j = cross sectional area of the flux path)

Here, if there is a low reluctance (iron enclosure) according to Equation 2 above, little current will be required to form the required magnetic flux, and the applied voltage will be overlaid on the connector. On the other hand, in the case of high reluctance (air), much current will be required to form the required magnetic flux. In this case, the current will be limited by the voltage on the load and the voltage induced in the connector. The difference between the reluctance in air and the reluctance of the magnetic material may be about 1,000 to 900,000.

Magnetic induction or magnetic flux density of a magnetic material is determined by the relative permeability of the material and the intensity of the magnetic field. The strength of the magnetic field is generated through the windings or the material being arranged.

In these systems the following equations can be applied to obtain the values:

Field intensity:

( = Strength of magnetic field, s = integral path, I = current of winding, N = number of windings)

Magnetic flux density or induction:

Since the ratio between magnetic induction and magnetic field strength is non-linear, when the strength of the magnetic field increases beyond a certain range, the magnetic domain of ferromagnetic materials is saturated due to saturation phenomenon. Due to the fact that it is in a state, the magnetic flux density does not increase. Therefore, it is desirable to provide a control magnetic field H2 perpendicular to the working magnetic field H1 of the magnetic material to control the saturation of the magnetizing material, and avoid the transitional or inductive connection by avoiding the magnetic connection between the two magnetic fields. A transformative connection is a connection in which two windings "share" one magnetic field, so that a change in the magnetic field from one winding results in a change in the magnetic field of the other winding.

The way to get rid of the magnetic field H, which increases in saturation by transitional connections, is to have the magnetic fluxes have a common path and add them together. For example, a control that provides the magnetic material to a tube to position the main winding or windings carrying the operating current in the pipe, winding it in the longitudinal direction (vertical) of the pipe, and carrying a control current. By winding the winding or winding around the circumference of the pipe, the desired action can be achieved. Depending on the pipe area, a small area for the control flux and a large area for the working flux may be provided.

In the above embodiment, the working magnetic flux travels circumferentially along the circumference of the pipe and has a closed magnetic circuit. On the other hand, the control magnetic flux is moved by the first pipe disposed around the second pipe or two pipes which are moved in the longitudinal direction of the pipe and are arranged in parallel with each other and are provided with a magnetic material connecting the control magnetic flux therebetween. By being connected with a closed magnetic circuit, the control winding is located between the two pipes and the cross sections of the pipes are magnetically interconnected to obtain a closed path for the control flux. These methods will be described in more detail later.

In the following, the components providing the magnetic connection between the pipes or the core parts are called magnetic field connectors or magnetic field couplings.

The total flux of the material is given by

4)

The magnetic flux density B consists of the sum of the vectors B1 and B2 (see FIG. 4D), where B1 is generated by the current I1 of the first main winding 2 and has a tangential direction with the conductors of the main winding 2. . The main winding 2 has a rotational speed of N1 and is wound around the magnetization body 1. B2 is generated by the current I2 of the control winding 4 with the number of revolutions of N2, which is wound around the body 1. B2 has a tangential direction to the conductors of the control winding 4.

Since the windings 2, 4 are arranged at 90 ° to each other, B1 and B2 are orthogonally positioned. In the magnetizing body 1 B1 is directed transversely (horizontally), and B2 is oriented endwise (vertically). In this connection, reference is made especially to those shown in FIGS. 1 to 4.

5)

It should be taken into account that the relative transmittance is higher in the direction of the operating magnetic field H1 than in the direction of the control magnetic field H2, ie the magnetic material of the magnetizing body 1 is anisotropic. Of course, this does not limit the scope of the invention.

The vector sum of the magnetic fields H1 and H2 determines the condition of the body 1 for the total magnetic field and saturation of the body 1, and the magnetic current divided between the connector and the load connected to the main winding 2. And the voltage will be determined. Since the sources of B1 and B2 are orthogonal to each other, no magnetic field can resolve to each other. This means that B1 cannot be a function of B2 and vice versa. However, the vector sum of B1 and B2, B, is affected by their respective amounts.

B1 is a vector generated by the control current. Cross section A2 for the B2 vector is a cross section of the magnetic body 1 as compared to FIG. 4C. This may be a small area, in the case of an annular body, limited by the thickness of the magnetic body 1 given by the surface sector between the inner and outer diameters of the body 1. On the other hand, the cross section A1 (see FIGS. 4A and 4B) for the B1 magnetic field is determined by the length of the magnetic core and the applied voltage ratio. Such a surface may be 5 to 10 times larger than the surface of the control magnetic flux density B2 without limiting the scope of the present invention.

If B2 is at the saturation level, a change in B1 will not result in a change in B. In other words, this makes it possible to control which level of B1 gives the saturation of the material, thereby controlling the reluctance of B.

The inductance of the control winding 4 at rotational speed N2 can be set to a small value suitable for pulse control of the regulator. That is, it can provide a rapid reaction of approximately milliseconds.

6)

(N2 = rotation speed for control winding, A2 = area of control flux density B2, l2 = length of flux path of control flux)

In the following a general mathematical description of the invention and its applications will be made based on Maxwell's equations.

Maxwell's equations, a simple calculation of the magnetic field in electrical power engineering, use an integral form.

In a device of the type to be analyzed here (to some extent of the invention), the magnetic field has a low frequency.

Therefore, the displacement current may be independent of the current density.

Maxwell's equation, 7)

Can be simplified to

8)

The integral form can be obtained from Toke's theorem:

9)

In other words, this represents a solution for the system of FIG. 4, where the main winding 2 forms a magnetic field H1. Here, the calculations are performed with the winding centered to focus on the theory, and may not be an accurate calculation.

The integration path coincides with the magnetic field direction and the length l 1 of the average magnetic field is selected in the magnetization body 1. Thus, the solution of the integral equation is as follows:

11)

This is also known as magnetomotive force MMK.

12)

The control winding 4 will form the corresponding MMK generated by the current I2:

13)

14)

The magnetic material affected by the magnetic field H generated from the source windings 2, 4 is represented by the magnetic flux density B. That is, for the main winding 2:

15)

For control winding (4):

16)

to be. The transmissivity in the transverse direction is about 10 to 20 lower than the transmissivity in the longitudinal direction (vertical or vertical). The transmittance in vacuum is:

17)

Here, the capacity for conducting a magnetic field in iron is called μ _r , and the size of μ is 1000 to 100,000 in iron and rises to 900,000 in Mattglas material.

Combining equations 11) and 15) for the main winding (2):

18)

The magnetic flux of the magnetizing body 1 at the main winding 2 is given by the following equation:

19)

Assuming the flux is constant for the core cross section:

20)

Here, expressing the magnetic flux resistance R _m or reluctance as given in equation 3):

21)

22)

In the same way, the flux and reluctance for the control winding 4 can be found:

23)

24)

The present invention is based on the physical fact that the derivative of the magnetic field strength with the source of current in the conductor is expressed as "curl" in the magnetic field H. H vs. "curl" means the change or derivative of the magnetic field H relative to the direction of the magnetic field of H. Here, the magnetic field is calculated based on the vertical plane of the differential magnetic field loop having the same direction as the current. This also means that the magnetic fields from current-carrying conductors forming windings perpendicular to each other are orthogonal. The fact that the magnetic fields are orthogonal to each other is important for the orientation of the paths in the material.

Before examining this more closely, let us introduce self-inductance, which plays a very important role in the application of the magnetically controlled power configurations of the present invention.

According to the Maxwell's equation, a time-varying magnetic field induces a time-varying electric field, which is expressed as

25)

The left side of the integral represents the integral equation of the potential equation. The source of the variable magnetic field may be the voltage from the generator, and referring to FIG. 5, the Faraday law may be applied when the winding has a rotational speed of N and all the magnetic flux passes through all the rotations.

Here, lambda (Wb) represents the sum of the number of magnetic flux rotations and the magnetic flux through each rotation. If the circuit technique considers generator G of Figure 5, which breaks after the magnetic field is formed, the source of the magnetic field variable would be the current of the circuit (see Figure 5):

27)

From equation 21 we get:

28)

If L is a constant, then a combination of equations 26 and 27:

29)

Solving Eq 29):

30)

Substituting C = 0 from (28): 31)

This represents the self-inductance for winding N or main winding 2. The self-inductance is equal to the ratio between the magnetic flux rotations formed by the current in the winding (coil).

If the magnetizing body or the core is not saturated, the self-inductance of the winding is approximately linear. However, the present invention will change the self-inductance through changing the transmittance of the material of the magnetizing body by changing the magnetic path in the transverse direction by the control magnetic field (ie, the magnetic field H2 formed by the control winding).

Combining equations 21 and 31, we get:

32)

In an electrical circuit with self-inductance, the AC resistance or reactance is as follows:

33)

By applying magnetic force to the paths of the magnetizing body in the transverse direction, longitudinal reluctance will be changed. Here, a detailed description of what happens to the paths under the influence of different magnetic fields will not be given. In addition, we have considered conventional commercial electroplating with a silicon content of about 3%, and while we do not describe the phenomenon for matte glass materials herein, of course, magnetic materials having an amorphous structure are of the present invention. As this may play an important role in some applications, this is not a limitation of the scope of the present invention.

In transformers, the present invention employs closed cores with high transmission, where energy is accumulated in a magnetic leakage field and traces are accumulated in the core, but the accumulated energy does not occupy a direct part in the energy conversion. Thus, no energy conversion takes place in terms of what happens to the electromechanical system where electrical energy is converted into mechanical energy, but energy can be transferred by magnetic flux through the transformer. In a choke with an inductance coil or air gap, the reluctance of the air gap is as high as approximately all the energy accumulated in the air gap compared to the reluctance of the core.

In the device according to the invention a "virtual" air gap is created through the saturation of the paths. In this case, the energy accumulation will occur in a distributed air gap that encompasses the entire core. Considering a practical magnetic energy storage system without losses, no losses will be exhibited by the external components.

The description of energy used in the present invention is based on the theory of energy conservation.

The first law of thermodynamics applied to an electromagnetic system without loss (see FIG. 6) is:

34)

(dWelin = differential of electrical energy supply, dWfld = differential change of magnetically accumulated energy)

From equation 26 we obtain:

35)

Now, the inductance can be varied through the orthogonal or control magnetic field H2, substituting 31) into equation 26):

35)

The action in the system is

36)

Thus, we get

37)

In a system equipped with a core whose reluctance can vary and which has only a main winding, substituting equation 35) into equation 37):

38)

In the device according to the invention, L can be varied as μ _r , a function of the relative transmission of the magnetizing body or core 1 and vice versa, I 2, a function of the control current of the control winding 4.

If L is a constant, i.e. when I2 is a constant, dL = 0, so i × dL can be ignored, so the magnetic field energy is:

39)

When L is varied by I2, the magnetic field energy changes due to the changed L value. Therefore, the current I will also change because the current I is linked with the magnetic field value through the magnetic flux rotation λ. Since i and λ are variable and nonlinear functions of each other, mathematical calculations outside the scope of the present invention are included and no further solution is found here.

However, the present invention can conclude that magnetic field energy and energy distribution can be controlled by μ _r and affect how the energy accumulated in the magnetic field increases / decreases. That is, when the magnetic field energy is reduced, the surplus portion becomes a generator, or is the same as the extra winding in the same winding window as the first main winding 2 (e.g. winding 3 in FIG. 1). With a winding axis, it is possible to provide a transfer of energy from the first main winding 2 to the second main winding 3.

This results in an energy change in the magnetic field Wflt, where the change of λ is originally Wflt (λ ₀ , i ₀ ), as shown in FIG. Here, the variable assumes that i is small enough to be approximately constant while λ is changing. Likewise, a change in i can lead to a change in λ. Thus, the variable inductance of the present invention can be described as follows:

8 and 9 show what happens to the material.

8 shows magnetization curves for the entire material of the magnetizing body 1, the path of which changes under the influence of the magnetic field H1 from the main winding 2.

9 shows the magnetic curves for the entire material of the magnetizing body 1, the path of which is changed by the influence of the magnetic field H2 in the direction in the control winding 4.

10A and 10B show the magnetic flux densities B1 (magnetic field H1 formed by the operating current) and B2 (consistent with the control current). The dotted line represents the limit of saturation for magnetic field B, which will cause the material of magnetizing body 1 to saturate when magnetic field B reaches the limit. The dashed axes are the length of the magnetic field and the transmission of two magnetic fields B1 (H1) and B2 (H2) on the core material of the magnetizing body 1.

In FIG. 10, by having the axes represented by the MMK distribution or the magnetic field H distribution, it is possible to represent the magnetic force at two currents I1, I2.

8 and 9, by partial magnetization of the paths by the control magnetic field B2 (H2), the additional magnetic field B1 (H1) in the main winding 2 is vector to the control magnetic field B2 (H2). By incorporating and energizing the paths, the inductance of the main winding 2 will be initiated in a basis given the state of the paths under the influence of the control magnetic field B2 (H2).

Thus, the magnetic path, inductance L and alternating current (AC) resistance XL will vary linearly as a function of control magnetic field B2.

DETAILED DESCRIPTION Various embodiments of an apparatus according to the present invention will now be described with reference to the accompanying drawings.

11 is a view showing a second embodiment of the present invention.

12 is the same embodiment of a magnetically affected connector according to the present invention, in which FIG. 12A shows the assembled connector and FIG. 12B shows the connector as an end.

FIG. 13 is a cross-sectional view taken along the line II in FIG. 12B.

As shown in the figures, the magnetization body 1 consists of two parallel pipes 6, 7 made of magnetization material. The electrically insulated conductors 8 are successively passed N times (N = 1, ... r) in a path through the first pipe 6 and the second pipe 7 (see FIGS. 12A, 13). The main winding 2 is formed and the conductor 8 extends in the opposite direction through the two pipes 6, 7 as clearly shown in FIG. 13. Although the conductor 8 extends through the first pipe 6 and the second pipe 7 twice, the conductor 8 may be changed one or several times (the winding number N may vary from 1 to r). It is self-evident that it can extend through each of the pipes), so that when electricity is applied to the conductor, a magnetic field H1 can be generated on the parallel pipes 6, 7. The combined control windings 4 and the magnetic windings 4 'form a conductor 9 and are wound around the first pipe 6 and the second pipe 7, as indicated by the arrows of the magnetic field H2 in FIG. 11. When electricity is applied to the windings 4, the direction of the magnetic field H2 generated in the pipes is reversed. Magnetic field connectors 10, 11 are coupled to the ends of the respective pipes 6, 7 to interconnect the pipes in the form of a loop. Conductor 8 may be accompanied by a load current I1. The length and diameter of the pipes 6, 7 will be determined based on the power and voltage to which they are connected. The rotation speed N1 of the main winding 2 is determined by the reverse blocking ability with respect to the voltage and the cross sectional area which is the magnitude of the operating magnetic flux Φ2. The rotational speed N2 of the control winding 4 is determined by the magnetic field required for saturation of the magnetizing body 1 comprising the pipes 6, 7 and the magnetic field connectors 10, 11.

14 shows a special design of the main winding 2 of the device according to the invention. In practice, the solution of FIG. 14 differs from that shown in FIGS. 12 and 13, in which instead of a single insulated conductor 8 passing through the pipes 6, 7, the first conductor is two separate opposite conductors. By adopting 8 and the second conductor 8 ', it is possible to perform the function of a voltage converter for a magnetically affected device according to the present invention. We will now discuss this in more detail. The above schematic is basically similar to that shown in FIGS. 11 to 13, wherein the magnetization body 1 comprises two pipes 6, 7. The electrically insulated first conductor 8 is continuously passed N1 (N1 = 1, ... r) in a path through the first pipe 6 and the second pipe 7, and the first conductor 8 is It extends in the opposite direction to the direction through the two pipes 6, 7. An electrically insulated second conductor 8 'is continuously passed N1' (N1 '= 1, ... r) in a path through the first pipe 6 and the second pipe 7, and the second conductor 8 'extends in the opposite direction to the first conductor 8 passing through the two pipes 6, 7; At least one combined control and magnetic winding 4, 4 ′ is wound around the first pipe 6 and the second pipe 7, respectively, so that the direction of the magnetic field generated on the pipe is reversed. As in the embodiment according to FIGS. 12 to 14, the magnetic field connectors 10, 11 are coupled with the ends of the respective pipes 6, 7 to interconnect the pipes 6, 7 in a loop, and magnetize. The body 1 is formed. For simplicity, the first and second conductors 8 and 8 'are shown only once through the pipes 6 and 7, but the first and second conductors 8 and 8' It will be clear that the pipes 6, 7 can pass N1 and N1 ′ respectively. The length and diameter of the pipes 6, 7 are determined based on the power and voltage to be converted. In a transformer with a conversion ratio N1: N1 'of 10: 1, in theory ten conductors will be used as the first conductor 8 and only one conductor will be used as the second conductor 8'.

15 shows an embodiment of magnetic field connectors 10 and / or 11. The magnetic field connectors 10, 11 are made of a magnetically conductive material, preferably two circular grooves 12 for the conductor 8 of the main winding 2 of the connectors 10, 11. It is formed outside the magnetic material (see, eg, FIG. 13). In addition, a gap 13 is provided which obstructs the magnetic field path of the connector 8. The cross section 14 is the connecting surface for the magnetic field H2 in the control winding 4 consisting of the conductors 9, 9 ′ in FIG. 13.

FIG. 16 shows a thin insulating film 15 formed between the cross sections of the pipes 6, 7 and the magnetic field connectors 10, 11 in a preferred embodiment of the invention.

17 and 18 show other embodiments of magnetic field connectors 10, 11.

Figures 19 to 32 are cores forming the main part of the pipes 6, 7 forming the magnetizing body 1 together with the magnetic field connectors 10, 11, in the embodiment shown in Figures 12-14. Various embodiments of (16) are shown.

19 shows a cylindrical core portion 16 which is vertically divided and has one or more layers of insulating material 17 formed between two core halves 16 ', 16 ".

FIG. 20 shows a rectangular core portion 16 and FIG. 21 shows an embodiment of the core portion 16 which is divided into two partial sections at its side. In the embodiment shown in FIG. 21, one or more layers of insulating material 17 are provided between the core halves 16, 16 ′. 22 shows the modification which the said part part is arrange | positioned at each corner.

23 to 25 show a rectangular shape. 26 to 28 show a triangular shape, FIGS. 29 and 30 show an elliptical modification, and FIGS. 31 and 32 show a hexagon. In FIG. 31 the hexagon consists of the same six faces 18, and in FIG. 30 the hexagon consists of two parts 16 ′, 16 ″. Reference numeral 17 denotes a thin insulating film.

33 and 34 show magnetic field connectors 10, 11 that can be used as control magnetic field connectors between the square and square main cores 16 shown in FIGS. 20, 21 and 23-25, respectively. This magnetic field connector comprises three parts 10 ', 10 ", 19.

34 shows one embodiment of a core or main core 16 whose cross section 14 or connecting surface for the control magnetic flux is perpendicular to the core 16 axis.

FIG. 35 shows a second embodiment of the core portion 16 where the connecting surface for the control magnetic flux is on an angle with the axis of the core portion 16.

36 to 38 show various designs of the magnetic field connectors 10, 11, wherein the connecting surfaces 14 ′ of the magnetic field connectors 10, 11 have the same angle as the cross-sections 14 of the core portion 16. It is based on the fact that it is located in.

FIG. 36 shows magnetic field connectors 10, 11 showing different hole shapes 12 in the main winding 2 based on the shape of the core portion 16 (round, square, etc.).

In FIG. 37 the magnetic field connectors 10 and 11 are planar. In other words, the core portions 16 having right angled cross sections 14 may be employed.

In FIG. 38, α 'angles are shown for the magnetic field connectors 10 and 11, and the α angle is applied to the core portion (FIG. 35) so that the cross section 14 and the connecting surface 14' coincide.

39 shows an embodiment of the present invention combining the magnetic field connectors 10 and 11 and the core portions 16. 39B is a side view of the embodiment.

Although only individual combinations of magnetic field connectors and core portions are shown to illustrate the invention, it will be apparent to those skilled in the art that other combinations may be possible entirely within the scope of the invention.

In addition, the positions of the control winding and the main winding may be changed.

40 and 41 are cross sectional and perspective views respectively showing a third embodiment of the magnetically affected voltage connector device. The device comprises a magnetizing body 1 consisting of an outer pipe 20 and an inner pipe 21 (or core parts 16, 16 ′), the pipes being concentric with each other and the inner surface and inner pipe of the outer pipe 20. It is made of a magnetization material having a gap 22 between the outer surfaces of 21. Magnetic field connectors 10, 11 between pipes 20, 21 are coupled to the respective cross sections (FIG. 40A). A spacer 23 is formed in the gap 22 to hold the pipes 20, 21 concentrically (FIG. 40A). A combined control and magnetic winding 4 consisting of a conductor 9 is wound around the inner pipe 21 and located in the gap 22. Thus, the winding axis A2 for the control winding coincides with the axis A1 of the pipes 20, 21. An electrical current transport or main winding 2 consisting of a current conductor 8 passes through the inner pipe 21 N1 (N1 = 1, ... r) along the outer surface of the outer pipe 20. Magnetically affected voltage connectors with the combined control and magnetic windings 4 interlocked with the main windings 2 or the current carrying conductors 8 can be configured efficiently and easily. This embodiment of the device can be modified in such a way that the pipes 20, 21 have a cross section of square, square, triangle, etc., rather than a circular cross section.

In addition, the main winding may be wound around the inner pipe 21, in which case the axis A2 of the main winding coincides with the axis A1 of the pipes, and the control winding is formed on the inner surface of the inner pipe 21 and the outer pipe ( Wound on said pipes on the outer surface of 20).

42 through 44 illustrate various embodiments of magnetic field connectors 10 and 11 that may be applied to future designs of the present invention as described in FIGS. 40 and 41.

FIG. 42A is a cross sectional view and FIG. 42B is a top view showing the magnetic field connectors 10, 11 having a connecting surface 14 ′ on the axis of the pipes 20, 21. It is also clear that the inner pipe 21 and the outer pipe 20 can be in phase with the connecting surface 14.

43 and 44 show other variants of the magnetic field connectors 10, 11, wherein the connecting surfaces 14 ′ of the control magnetic field H2 (B2) are the main part of the cores 16 or the pipes 20, 21. Perpendicular to the axis. FIG. 43 shows a semi-toroidal magnetic field connector 10, 11 with a hollow semi-circular cross section, and FIG. 44 shows an annular magnetic field connector with a square cross section.

A modification of the apparatus shown in FIGS. 40 and 41 is shown in FIG. 45. That is, FIG. 45A is a side view of the apparatus, and FIG. 45B is a top view. The only difference in the voltage connectors of FIGS. 40 and 41 is that the second main winding 3 is wound in the same path as the main winding 2. A voltage converter magnetically affected by these devices can be obtained easily and efficiently.

46 and 47 are a sectional view and a perspective view showing a fourth embodiment of a voltage connector with concentric pipes.

That is, FIGS. 46 and 47 show voltage connectors acting as voltage converters with coupled cores. An internal reluctance-controlled core 24 is located in the outer core 25 which is wound on the main winding 2. The internal reluctance control core 24 has the same configuration as described above in FIGS. 40 and 41, but the only difference is that there is no main winding 2 wound around the core 24. That is, it has only a control winding 4 located in the gap 22 between the inner surface 21 and the outer surface portions forming the inner reluctance control core 24. Thus, the reluctance can be controlled magnetically by the influence of the control magnetic field H2 (B2) from the current of the control winding 4.

The main winding 2 of FIGS. 46 and 47 is a winding surrounding the core 24 and the core 25.

Now, the operation mode of the reluctance controlled voltage connector or converter according to the present invention mentioned in FIGS. 46 and 47 will be described.

Referring to Fig. 55 showing the principle of connection, Fig. 65 is an approximate equilibrium diagram of the reluctance model, where Rmk is a variable reluctance controlling the flux between the windings 2, 3, and Fig. 65b shows the connection. Equation for balanced electrical circuit, Lk is variable inductance.

Changing the voltage V1 relative to the winding 2 will form a magnetic current I1 in the winding 2. This is generated by the magnetic flux phi 1 + phi 1 'of the cores 24 and 25 necessary to form, thus providing the reverse voltage generated in the winding 2 according to the Faraday law. If there is no control current in the reluctance control core 24, the magnetic flux will be divided between the cores 24, 25 based on the reluctance of each core 24, 25.

In order to transfer energy from one winding to another, a control current I2 is applied to the internal inductance control core 24.

By applying the control current I2 during the (+) half period of the AC voltage V1 of the main winding 2, it is possible to obtain the half cycle voltage for the winding 2. Since energy is transferred by the flux arrangement between the reluctance control core 24 and the second outer core 25, the reluctance control core 24 is essentially driven by the control current I 2 during the period controlled to be saturated. Will be affected, and the working magnetic flux will travel to the second outer core 25 and interact with the first winding 2 during the energy transfer.

When the reluctance control core 24 is out of saturation by resetting the control magnetic flux B2 (H2) orthogonal to the operating magnetic flux B1 (H1), the magnetic flux from one side is again divided between the cores 24, 25, Since low reluctance appears only at the load connected to the second winding 3, a high inductance may appear without a connection between the first voltage V1 and the second voltage V3. A voltage is generated on the second winding 3, but because of the magnitude of Lk compared to the magnetic impedance Lm, most of the voltage from the first winding 2 will overlay Lk. The magnetic flux in the first winding 2 inevitably travels to where the minimum reluctance is and the magnetic flux path is shortest (FIG. 65B).

It is also contemplated that the outer core 25 may be controlled and may have a fourth main winding wound around the inner control core 24. This means that the voltage between the cores 24, 25 can be controlled as required.

FIG. 48 shows another variant of the fourth embodiment of the magnetically affected voltage connector or voltage converter according to the invention, wherein the magnetization body 1 has a control flux B2 (H2) through the main core 16. It is designed to be connected directly without a separate magnetic field connector.

That is, FIG. 48 is a side view of the annular voltage connector. The voltage connector comprises two core parts 16, 16 ′, a main winding 2 and a control winding 4.

FIG. 49 shows a voltage connector according to the invention which is provided with an additional main winding 3 which gives the possibility to convert voltage.

FIG. 50 is a cross-sectional view illustrating the device of FIG. 48 taken along line VI-VI of FIG. 48, and FIG. 51 is a cross-sectional view taken along line V-V. In FIG. 50 the circular groove 12 is shown as located in the control winding 4.

51 shows an additional aperture 26 through the windings.

52 and 53 show the structure of the core 16 without windings, the core 16 is designed such that no additional magnetic field connector for the control magnetic field is required. The core 16 has two core portions 16, 16 ′ and a groove 12 for the control winding 4. This design is for use where the magnetic material is sintered or compressed powder molded material. In this case, since topologically closed magnetic field paths can be interpolated, previously separated connectors required for the foil wound core can form an actual core to form the structure. have. 52 and 53 are diagrams showing the body 1 applied to the first embodiment of the present invention, which forms a closed magnetic circuit without separation of magnetic field connectors (dotted lines in FIGS. 1 and 2). It can be used in all embodiments of the present invention, including).

54 shows a magnetically affected voltage converter device, which has an inner control core 24 consisting of an outer pipe 20 and an inner pipe 21, the pipes being concentric and the outer pipe 20. ) And a magnetization material having a gap 22 between the inner surface of the inner shell and the outer surface of the inner pipe 21. The spacers 23 are coupled to the gap between the inner surface of the outer pipe 20 and the outer surface of the inner pipe 21. Magnetic field connectors 10, 11 are coupled at their ends between the respective pipes 20, 21. The combined control and magnetic windings 4 are wound on the inner pipe 21 and located in the gap 22. The apparatus also comprises ring-shaped core coils 25 ', 25 ", 25"', etc., consisting of an outer second core 25 with windings, which are arranged on the outer surface of the control core 24. Each Ring core coils 25 ', 25 ", 25 "', etc., are made of a ring of magnetized material wound around each second main winding or second winding 3 (only one is shown for clarity). The first main winding or the first winding 2 passes the inner pipe 21 of the control core 24 along the outer surface of the outer core 25 N1 times (N1 = 1, ... r).

Also, a second core located within the control core 24 can be considered, in which case the first winding 2 passes through the ring-shaped core 25 along the outer surface of the control core 24.

FIG. 55 shows a second embodiment of a magnetically influenced voltage regulator according to the invention, having a first reluctance control core 24 and a second core 25, each made of a magnetizing material Designed in the form of a closed magnetic circuit, the cores are in parallel. At least one first electrical conductor 8 is wound around the main winding 2 with respect to the transverse side of the first and second cores along at least part of the closed circuit. In addition, at least one second electrical conductor 9 can be coupled as a winding 4 to the reluctance control core 24 in a form consistent with the closed circuit. And at least one third electrical conductor 27 is wound around the cross-section of the second core 25 along at least a portion of the closed circuit. In the winding 2 of the first conductor 8 and the winding of the second conductor 9 the direction of the magnetic field is orthogonal. By this solution, the first conductor 8 and the third conductor 27 form a first winding 2 and a second winding 3, respectively.

Fig. 56 shows a proposal of an electrical schematic symbol for a voltage connector according to the present invention. 57 is a block diagram symbol proposal for the voltage connector.

58 shows a magnetic circuit without the control winding 4 and the control flux B2 (H2).

59 and 60 propose an electrochemical component symbol for the voltage connector, in which the reluctance of the control core 240 is the first core 25 with fixed reluctance and the second core 24 with variable reluctance. The magnetic flux between the two is moved (see, for example, FIG. 55).

Of course, there is no limitation to having two cores with variable reluctance. By adopting the fact that the magnetic flux can move between two windings within the same winding, it is possible to make a magnetic switch capable of turning the voltage on and off independently of the magnetic path of the main core. This means that you have a switch that functions like the GTO, except that you can select the desired switching time.

The apparatus according to the invention can be used in many different connections, examples of which are particularly suitable will be described below.

FIG. 61 illustrates controlling the voltage with a load RL, which may be a light source, a heat source or other load, using the present invention in an alternating current circuit.

FIG. 62 illustrates the use of the present invention in a three phase system wherein voltage connectors in each phase may be connected to a diode bridge and used for linear regulation of the output voltage of the diode bridge.

63 illustrates use as a variable choke of DC-DC converters.

64 shows use as a variable choke of a filter with condensers. Here, although only series and parallel filters (FIGS. 64A and 64B, respectively) are shown, variable inductance can be used for many filter topologies.

Another application of the invention, in particular referred to in FIGS. 14 and 45, is to propose a configuration symbol shown in FIG. In this application, the voltage connector has the function of a voltage converter to which a second winding is added. Also shown is an application as a voltage regulator, and the magnetic current and leakage reactance of the transformer connection can be controlled by the control winding 4. The feature of this system is that the magnetic current can be controlled by varying μ _r while applying the transformer equation. Thus, in this case the characteristics of the transformer can be adjusted to some extent. When a DC voltage is applied to one winding 2, the energy transferred through the transformer can be obtained by varying μ _r , so that the magnetic flux of the reluctance control core can be changed instead of varying the voltage excitation. . Thus, in theory, it is possible to generate an AC voltage through the DC voltage by the fact that the change in the magnetic current from the DC generator can be transferred to the winding on the other side.

46 and 47 illustrate another application of the present invention, in which the variable reluctance as the control core is surrounded by one or more separate cores with separate windings, and in FIG. 55 the first reluctance control core and The two cores are designed as closed magnetic circuits and the cores are in parallel. 65 shows a balanced electrical circuit.

55 shows how the magnetic flux of the present invention travels in the cores. The magnetic flux of the control core is connected to the magnetic flux of the working core by windings comprising two cores. In such a system, the transfer of electrical energy can be controlled by magnetic flux that is connected / disconnected with the control core and the operating core. Since the fluxes between the cores are interconnected through Faraday's law of induction, the functional dependence of one side equation and the other equation will be controlled by the connection between the magnetic fluxes. In a linear application, one can control the transition of voltage and current between the first and second windings by changing the reluctance of the control core. Thus, a reluctance-controlled transformer can be introduced here. Reluctance control switches may be introduced for the switched embodiments.

The magnetic flux connection between the first main winding 2 and the second main winding 3 will now be described. A winding 2 comprising a reluctance control control core 24 and a main core 25 forms magnetic flux in the cores. Self-inductance L1 indicates how much flux or flux turns are produced in the cores when current I1 passes through winding 2. Mutual inductance between the first winding 2 and the second winding 3 is such that the magnetic flux rotations formed by the winding 2 and the current I1 are at the first winding 2 and the second winding 3. It shows how much is rotated.

Of course, a reluctance-controlled main core 25 can be considered, but for simplicity we refer to a system having a main core 25 with a constant reluctance and a control core 24 with variable reluctance.

Magnetic flux lines flow along a path that gives the highest transmission (highest transmission), ie the least reluctance,

In Figures 55 and 65 the leakage field of the main windings 2, 3 is not taken into account. FIG. 55 shows that the first windings 2 and the second windings 3 are each wound on a transformer leg, preferably on the same transformer leg, in the case of the present invention the main core 25. The outer ring core is wound on a second winding 3 which is distributed along the entire core 25. Similarly, a first winding 2 is wound around the main core 25 and a control core 24 located concentrically within the main core.

65 shows an approximate reluctance model of the device according to the invention.

65B shows an approximate electrical balance in accordance with the present invention, where reluctances are replaced with inductances.

The current in the winding 2 creates magnetic flux in the cores 24, 25:

40)

Where Φ _p = the total magnetic flux formed by the current in the winding 2, Φ _k = the total magnetic flux traveling through the control core 24, Φ ₁ = the total magnetic flux moving through the main core 25. .

Since the leaking magnetic flux of the main core 24 and the control core 25 can be ignored,

41)

_K can be ignored by the controlled leakage flux.

Based on FIG. 65, an extremely coarse electrical balance for the magnetic circuit shown in FIG. 65B can be formulated.

Thus, Fig. 65B shows the principle of the connector controlled by the reluctance, and the inductance L _k absorbs the voltage from one side.

42)

Since this inductance can be controlled through the variable reluctance of the control core 24, the connection or voltage division for the steady state voltage, which is the sinusoidal curve applied to the first winding, is the ratio between the inductances of the respective cores as shown in equation 43. Will match about.

43)

If the control core 24 is saturated, L _k is very small compared to L _m and the voltage division will depend on the ratio of revolutions N1 / N3. When the control core is off, L _k is large and will block voltage transitions to the other side in the same range.

The magnetism of the cores with respect to the applied voltage and frequency is the rate at which the main core 25 and the control core 24 separately absorb and absorb the voltage integration over the entire time without saturation. In the present invention, the area of iron on the control and operating cores is the same without departing from the scope of the present invention.

Since the control core 24 does not become saturated due to the main winding 2, the control core 24 can be reset irrespective of the operating magnetic flux B1 (H1). Thus, it is possible to achieve the object of the present invention to realize a magnetic switch with the devices of the present invention. If necessary, the main core 25 may be reset after a pulse or half cycle by the required MMF to return to the next half cycle to compensate for the distortion of the magnetic current.

In switched applications, the first and second windings (when the switch is off, ie when the magnetic flux of the first winding 2 is distributed between the control core 24 and the operating core 25), The magnetic flux connection between 2 and 3 is fine, so that little energy transfer occurs between the first and second windings 2 and 3.

When the switch is on, i.e. when the reluctance of the control core 24 is very low (μ _r = 10-50) and close to the reluctance of the air coil, the first winding and the second winding It has a very good flux connection and energy transfer between (2, 3).

An important application of the present invention is a frequency converter with reluctance controlled switches and a DC-AC or AC-DC converter, which may employ a reluctance controlled switch in conventional frequency converter connections and rectifier connections.

A variant of the frequency converter can be realized by adding bits of sinus voltage from each phase of a three phase system, each phase being connected to a separate reluctance control core, the additional cores and the reluctance It is alternately connected with one or more additional cores magnetically connected to the reluctance control cores through a common winding through the control cores. Part of the sine voltage may be connected from the reluctance control cores to a voltage having a different frequency from the additional core.

The DC-AC converter can be implemented by connecting a DC voltage to a main winding comprising an operating core, wherein the operating core is wound around a second winding to change the magnetic flux connection between the operating core and the control core to a sinusoidal curve. By doing so, a sine voltage can be obtained.

66 shows a connection for a magnetic switch. Of course, this can act as an adjustable transformer.

67 and 67A show an example of a three phase design, all other kinds of three phase rectifier connectors may be possible. By connecting a diode bridge or individual diodes to each outlet of the 12-pulse connector, a regulating rectifier can be obtained.

In an application as a regulating transformer, the size of the reluctance control core is determined by the regulating range (0-100% or 80-100%) of the voltage required for the transformer.

Fig. 67b shows the use of the device according to the invention as a connector of a frequency converter, which converts an input frequency into an arbitrarily selected output frequency for operation of an asynchronous motor, which is produced in a 6 or 12 pulse transformer. Phase voltage portions are added to each motor phase (FIG. 67B).

68 shows an apparatus used as a switch of unrestricted frequency changer with forced commutation (UFC).

Figure 69 shows a circuit comprising six devices 28 to 33 according to the present invention. The devices 28 to 33 are frequency converters in which the period of the generated voltage is configured as part of the fundamental frequency. This acts to "letting through" a part of the half or half of the sine voltage, creating a new (+) half period at the new sine voltage, and then passing through a part of the (-) half or (-) half period to Generate a negative half period for the sine voltage. In this way, the sine voltage is generated at a frequency of 10% to 100% of the fundamental frequency. The converter also acts as a soft start because the output voltage can be adjusted by the reluctance control of the connection between the first and second windings.

In FIG. 69, when the first half cycle passes through the connector 28 or the main winding 2, the current through the second main winding 3 in the same connector is the second main winding 3 of the connector 28, 29, or the like. Direction changes to

70 shows the use of the device according to the invention as a DC-AC converter. Here, DC voltage U1 is applied to the main winding 2 of the connector to form the magnetic field H1 (B1) in the control core 24 and the main core 25 (not shown). The rotational speeds N1, N2, N3 and the area of iron are designed so that no cores saturate at steady state. In the process of applying the control signal to the control core 24, that is, the voltage of the control winding 4, the magnetic flux B2 (H2) is transferred to the main core 25 and the magnetic flux B1 (H1) of the core 25. Derives the voltage of the second main winding 3. By having a sinusoidal control current I2, a sinusoidal voltage can be generated on the second main winding 3 side having the same frequency as the control voltage U1.

70B illustrates the use of the present invention as a transducer with a change in reluctance.

71 shows the use of the device according to the invention as an AC-DC converter. Here, the same control principle as that described above for the frequency converter of FIG. 69 is used. 71B is a graph showing input and output voltage over time of the device.

As mentioned above, the voltage connector according to the invention has no moving parts for the absorption of the electrical voltage between the generator and the load. The function of the connector is to control the voltage between the generator and the load from 0% to 100% with a small amount of control current. Also, the connector can be used as a voltage switch and can transition by forming a voltage curve.

The novel technique according to the present invention described above can be used to upgrade existing diode rectifiers required for regulation. In a 12 or 24 pulse rectifier system, the voltage of the system can be adjusted in a simplified form with a controlled rectification of 0-100%.

Magnetic materials included in the present invention are selected based on a cost / benefit function. The cost is related to several factors such as marketability, productivity for the various solutions chosen and price. The gain function is based on the electroelectronics function required by the material, including the shape and magnetic properties of the material. Magnetic properties are considered important including hysteresis loss, saturation flux level, transmittance, magnetization capacity and magnetostriction in the two main directions of the material. Electricity integrates frequency, voltage and power into energy sources, and users in connection with the present invention will choose a material. Suitable materials include:

a) Iron-silicon steel: made of strips about 0.1 mm to 0.3 mm thick and 10 mm to 1100 mm wide and wound on coils. Due to the price, it is most desirable for large cores, and manufacturing technology is already developed Used at low frequencies.

b) Iron-nickel alloys (permalloy) and / or iron-cobalt alloys (permendur): made of pieces and wound on coils. Alloys with special magnetic properties equipped with subgroups with very special properties.

c) Amorphous alloys, Mattglas: made of pieces of about 20 to 50 µm thick and 4 to 200 mm wide and wound on coils. Very high transmission with almost zero magnetism, very low loss. There are countless variations, including iron-based and cobalt-based. Good property but expensive.

d) soft ferrites: developed in the converter industry and sintered in special forms. Used at high frequencies due to low losses. Low magnetic flux density. Low loss. There is a limit to the size that can be physically realized.

e) Compressed Powder Core: A specially shaped compressed iron powder alloy developed for special applications. Low transmittance, up to about 400-600 per day. Low loss but high magnetic flux density. Can be manufactured in very complex forms.

All sintered and compression molded cores can be composed of topologies associated with the present invention without the need for special magnetic field connectors because their practical shape is that closed magnetic field paths are suitable for magnetic fields.

If the cores are formed based on a wound metal plate, one or more magnetic field connectors will have to be added.

In line with the well-known energy converter technology, the present invention is particularly suitable as a voltage connector, current regulator or voltage converter which is several elements in the power electronics field. A feature of the present invention is that the transformative or inductive connection between control winding and main winding is approximately zero, and the inductance of the main winding is such that the control winding Is controlled through the current of the control winding, and the magnetic connection between the first and second windings of the transformer configuration can be adjusted via the current of the control winding.

For example, in the field of rectification, the present invention can be employed for high voltage input regulation of large rectifiers, which has the advantage of using diode rectifiers over the entire voltage range. In an asynchronous motor, the present invention can be used in connection with a soft start of a high voltage motor. The invention is also suitable for use in the field of power distribution in connection with voltage regulation of power lines and may be used for the compensation of power with reactance continuously controlled on a network.

Although not confined to the use of such a device, the present invention may be part of a frequency converter for converting an input frequency into an arbitrarily selected output frequency, which frequency converter is preferably for operation of an asynchronous motor. . The input side of the frequency converter is supplied in three phases and the input is transferred to at least one transformer for three phase output of the converter by a phase conductor, the outputs of the transformer being one of the three phase outputs. It may be connected by voltage connectors, each of which may be selectively controlled to form a, or voltage connectors additionally coupled with the transformer.

The device can be applied as a direct converter in which the frequency of the AC voltage can be continuously adjusted and directly converts the DC voltage to an AC voltage.

Especially using this type of frequency converter at large depths will require high capacity pumps with variable speeds. Pumping in the peripheral system will perform the work of elevating from an underwater location to a location above the surface of the water and injecting water from the underwater point into the reservoir.

Claims (40)

A body 1 made of magnetized material and having a closed magnetic circuit; At least one first electrical conductor (8) wound around the body (1) along at least a portion of the closed circuit for at least one rotation to form a first main winding (2); And At least one second electrical conductor (9) wound around the body (1) along at least a portion of the closed circuit for at least one rotation to form a second main winding or control winding (4); It includes, by providing the orthogonal magnetic field (H1, B1 and H2, B2) to the body (1) by the magnetic field (H2, B2) of the control winding (4) of the magnetic field (H1,) For the purpose of controlling the action of the magnetizing material in proportion to B1), the winding axis A2 for the rotation or the rotations of the main winding 2 is a winding axis for the rotation or the rotations of the control winding 4. A magnetically controlled current or voltage regulator characterized in that it is perpendicular to A4). The shaft A2 according to claim 1, wherein the axis A2 for rotation (s) of the main winding 2 is parallel or coincident with the vertical direction A1 of the body 1, and the rotation of the control winding 4 ( Is gradually extended along the magnetizing body 1, so that the axis A4 of the control winding 4 is perpendicular to the vertical direction A1 of the body 1; Controlled current or voltage regulator. The shaft A4 according to claim 1, wherein the axis A4 for the rotation (s) of the control winding 4 is parallel or coincident with the vertical direction A1 of the body 1, and the rotation of the main winding 2 ( Is gradually extended along the magnetizing body 1, so that the axis A2 of the main winding 2 is perpendicular to the vertical direction A1 of the body 1; Controlled current or voltage regulator. A third electrical device as claimed in claim 1, wherein the device is wound around the body 1 along at least a portion of the closed circuit for at least one rotation to form a third main winding 3. A conductor 27, the winding axis A3 for rotation or rotations of the third main winding 3 coinciding with the winding axis A2 for rotation or rotations of the first main winding 2, or In parallel with said magnetically controlled current or voltage regulator, characterized in that a transformer action is provided between said first main winding (2) and said third main winding (3) when electricity is applied to at least one winding. A third electrical device as claimed in claim 1, wherein the device is wound around the body 1 along at least a portion of the closed circuit for at least one rotation to form a third main winding 3. And a winding axis A3 for rotation or rotations of the third main winding 3 coincides with a winding axis A4 for rotation or rotations of the first control winding 4 or In parallel with said magnetically controlled current or voltage regulator, characterized in that when electricity is applied to at least one winding, a transformer action is provided between said third main winding and said control winding. A first body 6 and a second body 7 each made of a magnetizing material, provided with a magnetic circuit, and adjacent to each other; At least one first electrical conductor (8) wound along at least a portion of the closed circuit for at least one rotation to form a first main winding (2); And A second electrical conductor wound around at least a portion of the first body 6 and / or the second body 7 for at least one rotation to form a second main winding 4 ′ or a control winding 4 ″ ( 9); It includes, by providing the orthogonal magnetic field (H1, B1 and H2, B2) to the body (1) by the magnetic field (H2, B2) of the control winding (4) of the magnetic field (H1,) For the purpose of controlling the action of the magnetizing material proportional to B1), the winding axis A2 for the rotation or turns of the main winding 2 is the winding axis A4 for the rotation or turns of the control winding 4. Magnetically controlled current or voltage regulator, characterized in that it is perpendicular to. A first body (6) and a second body (7), each of which consists of a magnetizing material, a first magnetic field connector (10) and a second magnetic field connector (11), which are provided with closed magnetic circuits and are adjacent to each other; At least one first electrical conductor (8) wound along at least a portion of the first body (6) and / or the second body (7) for at least one rotation to form a first main winding (2); And A second electrical conductor (9) wound around at least a portion of the closed circuit for at least one rotation to form a second main winding or control winding (4); It includes, by providing the orthogonal magnetic field (H1, B1 and H2, B2) to the body (1) by the magnetic field (H2, B2) of the control winding (4) of the magnetic field (H1,) of the main winding (2) For the purpose of controlling the action of the magnetizing material proportional to B1), the winding axis A2 for the rotation or turns of the main winding 2 is the winding axis A4 for the rotation or turns of the control winding 4. Magnetically controlled current or voltage regulator, characterized in that it is perpendicular to. 8. The magnetically controlled current or voltage regulator as claimed in claim 6 or 7, wherein the device comprises magnetic field connectors (10, 11) which together with the bodies form the magnetic circuit. The device according to claim 6, wherein the device comprises a third electrical conductor 27 which is wound for at least one revolution to form a third main winding 3. The winding axis A3 for rotation or turns of (3) is coincident with or parallel to the winding axis A2 for rotation or turns of the first main winding 2 so that when electricity is applied to at least one winding Said magnetically controlled current or voltage regulator characterized by providing a transformer action between said first main winding (2) and said third main winding (3). The device according to claim 6, wherein the device comprises a third electrical conductor 27 which is wound for at least one revolution to form a third main winding 3. The winding axis A3 for the rotation or the turns of (3) is coincident with or parallel to the winding axis A4 for the rotation or the turns of the control winding 4 such that when electricity is applied to at least one winding, 3 said magnetically controlled current or voltage regulator characterized by providing a transformer action between the main winding (3) and the control winding (4). The method according to any one of claims 6 to 10, wherein the first body (6) and the second body (7) are pipe-shaped so that the first conductor (8) or the second conductor (9) is of the first type. It can extend through the first body 6 and the second body 7, characterized in that the magnetic field connectors 10, 11 comprise grooves 12 for the conductors 8, 9. Said magnetically controlled current or voltage regulator. 12. The magnetic field connectors (10, 11) of claim 11 facilitate the insertion of the first conductor (8) or the second conductor (9), respectively, and the magnetic field H1 (B1) at the conductors (8, 9). Said magnetically controlled current or voltage regulator comprising a gap (13) for obstructing a magnetic field path of said circuit. 12. The magnetically controlled current or voltage according to claim 11, wherein an insulating film (15) is provided between the cross sections of the pipes (6, 7) and the magnetic field connectors (10, 11). regulator. 12. The magnetically controlled current or voltage regulator as claimed in claim 11, wherein each pipe (6, 7) comprises at least two core portions (16, 16 ', 16 "). 15. The magnetically controlled current or voltage regulator as claimed in claim 14, wherein said device comprises an insulating layer (17) disposed between said core portions (16, 16 ', 16 "). 16. The magnetically controlled current or voltage regulator as claimed in claim 6, wherein the pipes (6, 7) have a circular, square, square, triangular or hexagonal cross section. A first outer piped body 20 and a second inner piped body 21 each made of a magnetizing material and provided with a magnetic circuit and concentric with each other; At least one first electrical conductor (8) wound around the pipe-like bodies (20, 21) for at least one rotation to form a first main winding (2); And At least one second electrical conductor 9 provided in the gap 22 between the bodies and wound around the shared shaft A1 of the body for at least one rotation to form a second main winding or control winding 4 ); It includes, by providing the orthogonal magnetic field (H1, B1 and H2, B2) to the body (1) by the magnetic field (H2, B2) of the control winding (4) of the magnetic field (H1,) of the main winding (2) For the purpose of controlling the action of the magnetizing material in proportion to B1), the winding axis A2 for the rotation or turns of the main winding 2 is the winding axis A4 for the rotation or turns of the control winding 4. Magnetically controlled current or voltage regulator, characterized in that it is perpendicular to. A first outer pipe-like body each made of a magnetizing material having a first magnetic field connector 10 and a second magnetic field connector 11, provided with a closed magnetic circuit, and having a common axis A1 concentric with each other ( 20) and second inner piped body 21; At least one first electrical conductor (8) wound around the shared shaft (A1) of the body for at least one rotation to form a first main winding (2); And At least one second electrical conductor (9) wound around the pipe-like bodies (20, 21) for at least one rotation to form a second main winding or control winding (4); It includes, by providing the orthogonal magnetic field (H1, B1 and H2, B2) to the body (1) by the magnetic field (H2, B2) of the control winding (4) of the magnetic field (H1,) For the purpose of controlling the action of the magnetizing material in proportion to B1), the winding axis A2 for the rotation or turns of the main winding 2 is the winding axis A4 for the rotation or turns of the control winding 4. Magnetically controlled current or voltage regulator, characterized in that it is perpendicular to. 19. The device according to claim 17 or 18, characterized in that the device comprises a first magnetic field connector (10) and a second magnetic field connector (11) for providing a closed magnetic circuit together with the bodies (20, 21). Said magnetically controlled current or voltage regulator. 20. The device according to any one of claims 17 to 19, wherein the device comprises a third electrical conductor 27 wound around one turn to form a third main winding 3, The winding axis A3 for rotation or turns of 3) coincides or is parallel with the winding axis A2 for rotation or turns of the first main winding 2 so that when electricity is applied to at least one winding Said magnetically controlled current or voltage regulator, characterized in that it provides a transformer action between the first main winding (2) and the third main winding (3). 20. The device according to any one of claims 17 to 19, wherein the device comprises a third electrical conductor 27 wound around at least one revolution to form a third main winding 3 The winding axis A3 for the rotation or the turns of (3) is coincident with or parallel to the winding axis A4 for the rotation or the turns of the control winding 4 such that when electricity is applied to at least one winding, 3 said magnetically controlled current or voltage regulator characterized by providing a transformer action between the main winding (3) and the control winding (4). A first outer piped body 20 and a second inner piped body 21 each of which is made of a magnetic material with a closed magnetic circuit or inner core 24; An additional pipe type body having an outer core 25 coupled to an outer surface of the first outer pipe type body 20 and having a shared shaft A1 concentric with the bodies 20, 21 and 25; At least one first electrical conductor (8) wound around the pipe-like bodies (20, 21, 25) for at least one rotation to form a first main winding (2); And It is coupled to the gap 22 between the first body 20 and the second body 21 and is wound around the shared shaft A1 of the bodies for at least one rotation to form a second main winding or control winding 4. Forming at least one second electrical conductor 9; It includes, by providing the orthogonal magnetic field (H1, B1 and H2, B2) to the body (1) by the magnetic field (H2, B2) of the control winding (4) of the magnetic field (H1,) For the purpose of controlling the action of the magnetizing material in proportion to B1), a winding axis A2 for the rotation or rotations of the main winding 2 has a winding axis A4 for the rotation or rotations of the control winding 4. Magnetically controlled current or voltage regulator, characterized in that it is perpendicular to. A first outer piped body 20 and a second inner piped body 21 each made of a magnetic material forming a closed magnetic circuit or inner core 24; An additional pipe type body having an outer core 25 coupled to an outer surface of the first outer pipe type body 20 and having a shared shaft A1 concentric with the bodies 20, 21 and 25; It is coupled to the gap 22 between the first body 20 and the second body 21 and is wound around the shared shaft A1 of the bodies for at least one rotation to form a second main winding or control winding 4. At least one first electrical conductor 8; And At least one second electrical conductor (9) wound around the pipe-like bodies (20, 21) for at least one rotation to form a second main winding or control winding (4); It includes, by providing the orthogonal magnetic field (H1, B1 and H2, B2) to the body (1) by the magnetic field (H2, B2) of the control winding (4) of the magnetic field (H1,) of the main winding (2) For the purpose of controlling the action of the magnetizing material in proportion to B1), a winding axis A2 for the rotation or rotations of the main winding 2 has a winding axis A4 for the rotation or rotations of the control winding 4. Magnetically controlled current or voltage regulator, characterized in that it is perpendicular to. 24. Device according to claim 22 or 23, characterized in that the device comprises a first magnetic field connector (10) and a second magnetic field connector (11) for providing a closed magnetic circuit together with the bodies (20, 21). Said magnetically controlled current or voltage regulator. 25. The device according to any one of claims 22 to 24, wherein the device comprises a third electrical conductor 27 wound on the outer core 25 for one rotation to form a third main winding 3; , The winding axis A3 for the rotation or rotations of the third main winding 3 is coincident with or parallel to the winding axis A2 for the rotation or rotations of the first main winding 2, so that at least one winding The magnetically controlled current or voltage regulator, characterized in that it provides a transformer action between the first main winding (2) and the third main winding (3) when electricity is applied. 25. The device according to any one of claims 22 to 24, wherein the device comprises a third electrical conductor 27 wound on the outer core 25 for one rotation to form a third main winding 3; The winding axis A3 for the rotation or rotations of the third main winding 3 is coincident with or parallel to the winding axis A4 for the rotation or the rotations of the control winding 4 so as to be electrically connected to at least one winding. Said magnetically controlled current or voltage regulator characterized by providing a transformer action between said third main winding (3) and a control winding (4) when is applied. 27. The outer core 25 is comprised of a plurality of annulus 25 ', 25 ", and the first main winding 2 and / or the third main. The magnetically controlled current or voltage regulator, characterized in that the windings (3) form individual windings on each ring. 27. The outer core 25 is comprised of a plurality of annulus 25 ', 25 ", wherein the first control winding 4 and / or the third main. The magnetically controlled current or voltage regulator, characterized in that the windings (3) form individual windings on each ring. 29. A device according to any one of the preceding claims, wherein the device can be used in the construction of a frequency converter for converting an input frequency into an arbitrarily selected output frequency for operation of an asynchronous motor with a frequency converter connection. Said magnetically controlled current or voltage regulator. 29. An output according to any one of claims 1 to 28, wherein said device comprises an output of which the input frequency is arbitrarily selected to add to each motor phase the operation of an asynchronous motor and a portion of the phase voltage generated in a 6 or 12 pulse transformer. Said magnetically controlled current or voltage regulator which can be used as a connector of a frequency converter for converting to frequency. 29. A device as claimed in any preceding claim, wherein the device can be used as a DC-AC converter for converting DC voltage / current into an AC voltage / current of an arbitrarily selected output frequency, The magnetic energy accumulated in the inductance of the winding 2 or the first winding 2 is varied by the orthogonal control magnetic fields B2 and H2 affecting the inductance, so that the voltage is at the same frequency as the flux variable / inductance variable frequency. Said magnetically controlled current or voltage regulator, characterized in that it is capable of generating an AC voltage at the third main winding (3) or the second winding of the connector. 32. The magnetically controlled current or voltage regulator as claimed in claim 31, wherein the three variable inductance voltage converters are interconnected to generate a three phase voltage having an arbitrarily selected output frequency and to be connected to the asynchronous machine. . 29. A device according to any one of the preceding claims, wherein the device is used to convert an AC voltage to a DC voltage and is used as a reluctance controlled variable transformer, the output voltage of which has an external second winding. Or in proportion to the reluctance change of the core magnetically connected in parallel or in series with the inner core, wherein at least three said reluctance control transformers are connected with three phase rectifier connections for 6 or 12 pulse rectifier connections at the diode output stage. Said magnetically controlled current or voltage regulator. 29. A device as claimed in any preceding claim, wherein the device is used in a rectifier for converting an AC voltage to a DC voltage, which device is used as a variable inductance in series with the first windings on conventional transformer connections. And the three or more said transformers are connected with three-phase rectifier connections for 6 or 12 pulse rectifier connections at a diode output stage. 29. The apparatus according to any one of claims 1 to 28, wherein the device is used as an AC / DC or DC / AC converter used in the field of switched power supplies, in order to reduce the size of the magnetic voltage converter. Wherein the output voltage is proportional to the change in reluctance of a core that is magnetically connected in parallel or in series with an external or internal core having a separate second winding. Current or voltage regulator. 36. The magnetically controlled current or voltage regulator as claimed in claim 35, wherein the filters, the inductance of which is formed in part, are provided with variable inductance. 29. The magnetically controlled current or voltage of any of claims 1 to 28 wherein the device is used as a configuration of an adjustable voltage compensator in a high voltage divider network and generates a linear variable inductance. regulator. 29. A device according to any one of the preceding claims, wherein the device is used as a configuration of a power compensator (variable compensator) with adjustable reactance and is connected with conventional filter circuits in which at least one capacitor is included in the configuration. Generating a linear variable inductance, the compensator connection of which capacitance or inductance is automatically coupled and scaled to the size necessary to compensate for the reactive power, which is adopted in the form of a reluctance control transformer. Controlled current or voltage regulator. 29. The magnetically controlled current or voltage regulator as claimed in claim 1, wherein the device is used in a system for direct conversion of an AC voltage to a DC voltage which is reluctance controlled. 29. The magnetically controlled current or voltage regulator as claimed in claim 1, wherein the apparatus is used in a system for direct conversion of a DC voltage to an AC voltage which is reluctance controlled.