• 专利附录
  • 专利说明
  • 权利要求
  • 类似技术
  • 同族专利
  • 引用文献
  • 法律状态
  • 优先权
    • 专利摘要:
    The invention relates to a device (1) for demagnetizing a ferromagnetic, long-shaped component (2) of any length with a uniform profile, which on one side along its length an accessible surface (6). The device (1) comprises a rod-shaped, ferromagnetic core (7) with a circumferential lateral surface (8), which is closed by a front end face (9) and a rear end face (10), said end faces (9, 10) facing away from each other are aligned. At least one coil (12) is wound around the lateral surface (8) and is connected to a current source (15) which can generate an alternating current (AC), whereby a magnetic alternating flux (18) is induced in the ferromagnetic core (7). which at the two end faces (9, 10) enters and exits. According to the invention, a coil (12, 13) is wound around the lateral surface (8) of the ferromagnetic core (7), which is connected to a current source (15, 16) which can generate a direct current (DC) for superimposing the alternating magnetic flux (18 ) With a uniform magnetic flux (19) induced thereby by the ferromagnetic core (7), the responce at the two end faces (9, 10) resp. exit. In the method according to the invention for demagnetizing such a component (2), the ferromagnetic core (7) moves the component at a constant distance a, while the alternating magnetic flux (18) and the magnetic direct flux (19) are kept constant.
    公开号:CH714207A2
    申请号:CH01090/18
    申请日:2018-09-14
    公开日:2019-03-29
    发明作者:Sc Tech Urs B Meyer Dr；Maurer Albert
    申请人:Maurer Albert；
    IPC主号:
    专利说明:

    description
    Technical Field The present invention relates to an apparatus for demagnetizing a ferromagnetic long-length member of any length having a uniform profile with a longitudinal axis having an accessible surface along its length, the apparatus comprising a rod-shaped ferromagnetic core having a circumferential surface which is terminated by a front end surface and a rear end surface, these end faces are aligned facing away from each other and wherein at least one coil is wound around the lateral surface, which is connected at its ends to a power source which can generate an alternating current (AC), whereby a magnetic alternating flux is induced in the ferromagnetic core, which enters and exits at the two end faces and in the non-rewound region of the lateral surface. The invention also relates to a method for demagnetizing such components.
    Background Art Various devices are known for demagnetizing ferromagnetic bodies. As a rule, these bodies are exposed to a strong alternating magnetic flux. This exceeds the coercive force of the magnetized body, so that all magnetic dipoles in the body, which are aligned by the magnetization, are set in reversing motion. One speaks then of a charged up to the saturation flux density ferromagnetic body. When this alternating flux subsides, this movement eventually subsides until the electromagnets "freeze" in a disordered state. Alternatively, the body can be heated too much, which is often not possible. At the same time, a homogeneous domain structure is formed.
    The magnetic alternating flux is usually induced by a coil which is acted upon by a strong alternating current (AC). For demagnetizing the body is brought through the coil and then removed from it.
    Since the current for demagnetization must be very large, it is the desire to be able to demagnetize large components with smaller devices that can not be completely passed through a device.
    Thus, a magnetic alternating flux can be induced by a coil around an iron core forming a U-shape. The magnetic field lines then pass through the iron core and finally exit at the open ends. Thus, a component that is larger than the inner area of the coil, push in this open area or can rotate in this area. Such devices are particularly suitable for hard disks whose data should be permanently deleted.
    Another problem of demagnetization is the residual magnetism that remains in a component during the "freezing". This happens because at the time of solidification, a residual magnetic flux always acts on the component, caused for example by the geomagnetic field. In order to eliminate this residual magnetic flux, as shown in EP 2 851 911 A1, a protective cover can be arranged around the component, which shields an external magnetic field until the alternating magnetic flux has completely decayed.
    However, this requires that the component is completely in the shield during the entire demagnetization. For very large components, this is expensive, impossible with infinitely long stretched components.
    It turns out now that the known devices are not suitable to completely demagnetize ferromagnetic, long-configured, especially rigid and / or permanently installed components of any length. The most important example here are permanently laid tram or railroad tracks. These magnetize over time, on the one hand by the earth's magnetic field, on the other hand also by the magnetic rail brakes of the trains, which induce magnetic fields of 10 mT in the air gap to the rail even when switched off.
    The rails are separated at their joints by insulation layers from each other so that a monitoring system of a catenary center can determine whether a rail section is occupied or occupied by a train. Due to the magnetization of the rails, metal chips, nails, washers and so on accumulate gradually on the bumps because the magnetic flux escapes there until finally conductor bridges are created which bypass the insulation. This means that in the catenary no reliable information about the positions of the trains is obtained, which can lead to serious signal interference and ultimately to accidents.
    Other application examples are permanently installed carrier, but also long iron tubes that are too large to immerse in their entire circumference in a demagnetizing magnetic flux loop. A device for it would be very large and the enormous power consumption would bring further problems. In addition, the residual magnetization created by the environment can not be eliminated or with very great effort.
    DESCRIPTION OF THE INVENTION It is now the object of the present invention to describe a device which can achieve demagnetization of a ferromagnetic, elongated component of any length described above, the residual magnetization being smaller than a predetermined tolerance value. In particular, the device should be applicable to laid tram or rail tracks as well as other, only one-sided access, built-in profiles, installed cables and suspension cables and large metal pipes.
    Another object is to describe a self-sufficient device for the purpose mentioned. In addition, a method is to be described, which can achieve the desired demagnetization.
    The objects are achieved by the features of the independent claims of the respective categories. Further advantageous embodiments are specified in the subclaims.
    According to the invention, a coil is wound around the lateral surface of the ferromagnetic core, which is connected at its ends to a current source which can generate a direct current (DC), for superimposing the alternating magnetic flux with a thereby induced, in an apparatus for demagnetizing mentioned above, uniform magnetic flux through the ferromagnetic core, the responce at the two end faces. exit. The coil may be the same coil that is charged with alternating current or a coil that is different from it. All coil windings are parallel to each other. This is also true when two coils are used. The flux lines of the alternating magnetic flux and the magnetic direct flux overlap in parallel, that is, they do not intersect. In operation, the front end face facing the component and arranged close to the surface, the rear end face facing away from the component. The core is wider than the width of the component. The planes in which the coil windings are located run parallel to the two end faces of the core. They generate magnetic field lines which penetrate almost vertically into the component and extend in both directions of its longitudinal axis in this, until they finally, distributed over a relatively long distance, exit again from the component and enter the rear end face of the core.
    In a preferred embodiment, the device comprises a Nahtransporteinrichtung which on the one hand during operation ensures a distance between the front end face and the surface of the demagnetizing component, which remains within a predetermined range also in the magnetic forces occurring during operation, and on the other hand a translational Relative movement between the ferromagnetic core and the component along its entire length allows.
    In the inventive method for demagnetizing a ferromagnetic, long designed component, such a device is used with a Nahtransportvorrichtung. In this method, a constant alternating current is generated in the coil, which induces a magnetic flux change in the ferromagnetic core, which enters and exits at the two end faces. At the same time, a constant direct current is generated in a coil, which induces a magnetic alternating flux superimposed, uniform magnetic flux in the ferromagnetic core, the responce at the two end faces. exit. The coil may be the same or another coil. The Nahtransporteinrichtung always ensures a distance between the front face and the surface of the component within a predetermined range and causes a translational relative movement between the ferromagnetic core and the component along its entire length, while AC and DC are kept constant.
    The alternating current should be so strong that the zone lying under the front face of the component is completely saturated by the induced magnetic alternating flux. The DC current is adjusted in each case to the induced magnetization polarity of the component. After a demagnetizing crossing, the residual magnetism remaining on the component is measured and the method is repeated for as long as possible with corrected direct current intensities until this residual magnetism has fallen below a predetermined tolerance value.
    During the demagnetization of a tube causes the Nahtransporteinrichtung during demagnetization and a relative movement about the longitudinal axis of the component, which is carried out in addition to the translational relative movement between the ferromagnetic core and the component along its entire length.
    BRIEF DESCRIPTION OF THE DRAWINGS In the following, the invention will be explained in more detail with reference to the drawings. It shows:
    Fig. 1 is a schematic representation of an apparatus for demagnetizing a wire rope according to the prior art;
    Figure 2 is a schematic representation of a device in the form of a yoke, for demagnetizing a long component according to the prior art.
    3 is a schematic representation of a device according to the invention for demagnetizing a long component;
    Fig. 4 is a schematic perspective view of an alternative device according to the invention;
    5 shows a component in the form of a railroad rail in cross section with a part of the core and a coil;
    6 shows a component in the form of a railroad track in a perspective view with a core of the device;
    Fig. 7 A component in the form of a laid in the ground tram track in cross-section with a core and a
    Kitchen sink;
    8 is a side view of a device according to the invention with a Nahtransporteinrichtung and a component in the form of a rail in use.
    9 shows a schematic illustration of an apparatus according to the invention for demagnetizing a long component in the form of a tube;
    10 is a cross-sectional view of an inventive device with a Nahtransporteinrichtung and a component in the form of a tube in use.
    Means for Carrying out the Invention A solution known from the steel industry according to FIG. 1 consists in multiple wrapping of the component 2, here in the form of a bar material, with a flexible cable. This cable is thus wound into a coil 12, which is fed with an AC power source 15 and the rod material is continuously removed, as indicated by an arrow. In the wound zone of the coil 12, a magnetic flux corresponding to the flux lines 18, which magnetically flow through the component 2, is produced.
    The magnetic flux of the magnetic field acting in the wider environment of the earth 20 is collected in the ferromagnetic material of the component 2 and occurs there as a proportion of internal magnetism 21 in appearance. This inner magnetic flux 21 is composed of the permanent magnetic magnetism contained in the material (remanence) and a proportion which is caused by the prevailing magnetic field in the environment.
    The alternating magnetic flux 18 generated by the alternating current in the coil 12 decreases with the passage and removal of the material with demagnetizing effect. However, such a method is not practical, because the multiple looping of the component 2 is expensive, because the component 2 must be accessible on all sides, and finally, because the course of the alternating magnetic flux does not allow complete demagnetization.
    In Fig. 2, a solution is described which manages with a one-sided access to the component 2. The alternating current supplied by the current source 15 flows through a pair of coils 12, 13 which is mounted on the magnetic poles near the end faces 9, 10 of a yoke-shaped ferromagnetic core 7. The end faces 9, 10 are thus both aligned in the same direction and both facing the component 2. The resulting in the component 2 magnetic magnetic alternating flux 18 essentially follows the flux lines through the ferromagnetic core 7 and through the two end faces 9, 10, resp. through the magnetic poles. Such an arrangement is used in practice for magnetizing a rope in the magnetic inductive rope test, wherein current source 15 and coil 12, 13 can be replaced by permanent magnets in the magnetic poles near the end faces 9, 10. Again, the component 2 moves relative to the core 7 continuously, as shown by an arrow in Fig. 2.
    This arrangement can by means of alternating current in the coil 12, 13 generate a magnetic alternating flux 18. Such a method allows, as experiments have shown, a demagnetization, but the externally induced magnetic fields can be compensated only very limited.
    The device 1 according to the invention can therefore be described as follows with reference to FIGS. 3 and 4. It is suitable for demagnetizing a ferromagnetic, long-shaped component 2 of any length 4 with a uniform profile 3 with a longitudinal axis 5. The profile 3 has on one side along its length 4 an accessible surface 6. The device 1 comprises a rod-shaped, ferromagnetic core 7 with a circumferential jacket surface 8, which is closed off by a front end face 9 and a rear end face 10. The front end face 9 is facing the component 2 in use. These end faces 9, 10 are aligned facing away from each other. Their surface normals point in opposite directions. At least one coil 12 is wound around the lateral surface 8, which is connected at its ends 14 to a current source 15, which can generate an alternating current (AC). In use, this alternating current induces a magnetic alternating flux 18 in the ferromagnetic core 7, which enters and leaves at the two end faces 9, 10 and in the non-rewound region of the lateral surface 8. According to the invention, a coil 13 is wound around the lateral surface 8 of the ferromagnetic core 7, which is connected at its ends 14 to a current source 16 which can generate a direct current (DC) to superimpose the alternating magnetic flux 18 with a uniform magnetic flux 19 induced by the direct current through the ferromagnetic core 7, the responce at the two end faces 9, 10 resp. exit. Depending on the width of the coils, the flux lines generated by them also enter and leave the non-rewound area of the lateral surface 8.
    As shown in Fig. 3, the at least one coil 12 may be an AC coil 12 and the coil 13 for applying DC a different from the AC coil 12 DC coil 13. Preferably, the AC coil 12 is arranged closer to the front end surface 9 than In any case, however, the windings of the two coils 12, 13 parallel to each other, they do not intersect orthogonal. As a result, the field lines of the alternating magnetic flux 18 and of the magnetic direct current 19 generated by them also run parallel to one another at each point, and they also do not intersect orthogonally. This is also apparent from Fig. 3.
    Alternatively, as shown in Fig. 4, by adding a suitable circuit construction 17, the distributed to two coils 12, 13 and two power sources 15, 16 function for inducing a magnetic alternating field 18 superimposed by a magnetic field of reference 19, also with a single power source 15 or 16 and with a single coil 12 or 13 meet. Through this coil flows thus superimposed with a DC offset alternating current.
    In carrying out the method of the one or two coils 12, 13 wrapped ferromagnetic core 7 acts with its front end surface 9 on the demagnetizing component 2. The coil 12 is flowing through a serving of demagnetizing alternating current flowing from the Source 15 is fed. The alternating current is kept constant and ensures that the area of the component 2 lying under the front end face 9 of the ferromagnetic core 7 is completely magnetically saturated. The coil 12, 13 is traversed by a DC compensating the remaining magnetism, which is fed from the source 15, 16. This direct current is variable and is adjusted according to the residual magnetism remaining before demagnetization, but then kept constant during the process. The component 2 moves relative to the device 1 continuously at a speed Vt, as shown by an arrow in Fig. 3.
    The component 2 facing away from the rear end face 10 of the ferromagnetic core 7 protrudes from the covered by the coils 12 and 13 portion of the core 7 out. In this non-wound by any coil 12, 13 rear portion 11 of the core 7, the magnetic fluxes 18, 19 accumulate, as can be seen schematically from the flux lines 18, 19. In this rear region 11, the ferromagnetic core 7 may have a larger cross-sectional area Qh than the cross-sectional area Qs in a region wrapped by one of the coils 12, 13 in order to influence the course and the distribution of the alternating magnetic flux 18. This enlargement can, as shown in FIG. 4, be designed symmetrically. Alternatively, the rear cross-sectional area Qh can also be designed to be enlarged in one direction only, preferably counter to the direction of movement.
    5 and 6 show a component 2 with a cross-section 3 in the form of a schematic rail track in cross-section respectively. in perspective, over which the ferromagnetic core 7 of the device 1 according to the invention is arranged at a distance a and moves in the direction of the arrow relative to the component 2 during demagnetization at the speed vt. The cross-sectional area Qv of the ferromagnetic core 7 in the region of the front end face 9 is preferably greater than the cross-sectional area QB of the component 2 at the point at which magnetization is to be effected.
    In addition, it is proposed that the width BK of the ferromagnetic core 7 on the end face 9, which is aligned transversely to the longitudinal axis 5 of the component 2 in operation, is wider than the corresponding entire width Bb of the component 2, extending below the accessible Surface 6 extends.
    As already mentioned, the component 2 may be a tram rail, as shown in Fig. 7.
    In a particularly preferred embodiment, shown in Fig. 8, the device 1 comprises a Nahtransporteinrichtung 22, which ensures the one hand in operation the preferred distance a between the front end face 9 of the ferromagnetic core 7 and the surface 6 of the demagnetizing member 2 which remains within a predetermined range a-ι <a <a2 even in the case of the magnetic forces induced during operation, and on the other hand permits a translational relative movement vt between the device 1 and the component 2 along its entire length 4.
    This distance a should be smaller than the root of the cross-sectional area QB of the component 2, as shown in Fig. 5. In addition, this distance a should be greater than expected unevenness of the surface 6 of the component 2, over its entire length 4. In particular, curvatures of the component 2 can have a large effect on the distance a when the Nahtransporteinrichtung 22 moves on the component 2. Touches between the core 7 and the component should be avoided so that no grinding and sticking of the core 7 takes place on the component 2.
    When the component 2, as shown in Fig. 8, a rail, the Nahtransporteinrichtung 22 is preferably designed as a rail car 23 with a trailer hitch 24. A traction vehicle, coupled to this trailer coupling 24, the rail car 23 along the rails in pull the desired speed evenly. The ferromagnetic core 7 is then firmly attached to the rail car 23, so that the distance a to the component 2, therefore to the rail, is maintained. The Nahtransporteinrichtung 22 may in particular have no ferromagnetic components in the magnetic region of action between the ferromagnetic core 7 and the component 2. If steel wheels are used as the rolling stock of the Nahtransporteinrichtung 22, they should be spaced from the core 7 duly.
    In addition, one or more current sources 15, 16, which comprise, for example, a generator, can be arranged on this Nahtransporteinrichtung 22. Other components, such as the circuitry 17, not shown in FIG. 8, may be added if the device 1 is to be operated with a single coil 12.
    In an alternative embodiment according to FIG. 9 or 10, the device 1 comprises a Nahtransporteinrichtung 22, which in addition to the longitudinal movement vt also allows a rotational relative movement vr between the ferromagnetic core 7 and the component 2 about the longitudinal axis 5 of the component 2. In this embodiment, the component 2 is a tube to be demagnetized. The Nahtransporteinrichtung 22 is preferably fixedly mounted and also fixes the component 2, for example, four or more designated rollers 25, at a predetermined distance a to the ferromagnetic core 7. The component 2 is based on these rollers 25 of the Nahtransporteinrichtung 22 and becomes spiral moved on. The rollers 25 can thus be driven to rotate the component 2 on the one hand about its own longitudinal axis 5 and at the same time to achieve an offset by approximately the width Bl of the ferromagnetic core 7 in the direction of the longitudinal axis 5 with each rotation. Additional, not shown bearings, supports or suspensions can additionally stabilize the component 2. Alternatively, the Nahtransporteinrichtung 22 may not be stationary, but leave the component 2 along its length 4, while the component 2 in turn is rotated uniformly. It is important that the predetermined distance a between the component 2 and the ferromagnetic core 7 is always maintained. For this purpose, it is also possible to use gliders with or without rollers made of non-ferromagnetic material which ensure this distance a. These can also be arranged directly between the component 2 and the core 7.
    Preferably, the profile 3 of the front end face 9 of the ferromagnetic core 7 is the profile 3 of the accessible surface 6 of the component 2, here the curvature of the tube 2 adapted, as shown in FIG. By adjusting the profiles 3, the distance a between the component 2 and the core 7 can be kept in an optimum range, which can improve the penetration of the magnetic flux 18, 19. The width Bb of the rotating object 2, which is determined here by its diameter, must be narrower than the width BK of the ferromagnetic core 7. This is also shown in Fig. 10 so. Fig. 9 is more schematically understood in this regard.
    In the inventive method for demagnetizing a ferromagnetic, long-shaped component 2 of any length 4 with a longitudinal axis 5, which has an accessible surface 6 at least on one side along its length 4, a device 1 described above with a Nahtransporteinrichtung 22 is used. For this purpose, first of all a constant alternating current AC is generated, which induces a magnetic alternating flux 18 through the ferromagnetic core 7, which enters and leaves at the two end faces 9, 10 and a constant direct current DC, which comprises a uniform magnetic direct current 19 superimposed on the alternating magnetic flux 18 ferromagnetic core 7 induced, which also at the two end faces 9, 10 resp. exit. The Nahtransporteinrichtung 22 always ensures a distance a between the front end face 9 and the surface 6 of the demagnetizing member 2 within a predetermined range between a-ι and a2 and causes a translational relative movement vt between the ferromagnetic core 7 and the component 2 along its entire Length 4, while the AC and DC are kept constant. The translatory relative movement vt is, depending on the frequency of the alternating current, approximately between 1-3 m / s.
    The magnetic field can also be switched on on the component 2 itself. Preferably, however, prior to the induction of the magnetic fluxes 18, 19, the device 1 is brought into a distance of the component 2 in which the subsequent magnetic effect on the component 2 is smaller than an external field 20 prevailing in the environment. Subsequently, the alternating current AC and the DC current DC applied to generate the magnetic fluxes 18, 19. Only then is the device 1 brought into the vicinity of the component 2. The Nahtransporteinrichtung 22 now always ensures a distance a between the front end face 9 and the surface 6 of the demagnetizing component 2 within a predetermined range between a-ι and a2. In addition, the Nahtransporteinrichtung 22 causes a translational relative movement vt between the ferromagnetic core 7 and the component 2 along its entire length. 4
    In a preferred application, after the demagnetization has been carried out to the end of the component 2, the device 1 is brought into a distance of the component 2, in which the magnetic effect on the component 2 is smaller than an extraneous field prevailing in the environment 20, for example, the earth's magnetic field. Subsequently, the alternating and direct currents are switched off by the coils 12, 13 so that no further magnetic fluxes 18, 18 are induced. This ensures that even in the last stretch of the component 2 no residual magnetization remains.
    In an extended preferred method, a device 1 is used, the Nahtransporteinrichtung 22 additionally allows a rotational relative movement vr between the ferromagnetic core 7 and the component 2 about the longitudinal axis 5 of the component 2. In this method, the component 2 rotates helically relative to the device 1 in that the Nahtransporteinrichtung 22 in addition to the translational relative movement vt between the ferromagnetic core 7 and the component 2 along its entire length 4 also causes a rotational relative motion vr about the longitudinal axis 5 of the component 2 , The spiral thus traversed has a rise height which corresponds approximately to the width BL of the ferromagnetic core 7 in the direction of the longitudinal axis 5 in the region of the front end face 9. The vehicle speed vt in this case is approximately similar to the case described earlier and depends on the AC frequency.
    During demagnetization, the applied alternating magnetic field 18 with the correction field, which is caused by the magnetic DC field 19, distances itself from a demagnetized point. As a result, the flux density at this point decreases and approaches zero, while the external field 20 and in particular the internal magnetic flux 21, as described in Fig. 1, remains constant. Since the decay, because of the applied DC current, is asymmetrical, there is always a "push" in one direction, preferably against the external field 20. The stronger the internal magnetic flux 21 through this external field 20, the higher the DC current be adjusted so that the counter-shock compensates as possible during the "freezing" forced by the external panel 21 alignment of the electromagnets. In this way, it is possible to reduce the residual magnetization to a small, tolerable value, although the component is not protected by a shield from the external field during freezing and thus an internal magnetic flux 21 is formed.
    After demagnetization, the residual magnetism remaining on the component 2 is measured. If this is higher than a specified tolerance value, the process is repeated with appropriately corrected DC current strengths until this residual magnetism has fallen below this predetermined tolerance value.
    The Nahtransporteinrichtung 22 may also be a fixed device such as a robot arm, a machine tool or a portal.
    It has been found in studies of the present invention that during demagnetization of magnetized bodies, such as railroad tracks, a slow decay of the two applied magnetic fields 18, 19 is of great importance. The magnetic field lines, as they arise in Fig. 1, are suitable in principle because the field lines 18 gradually decrease with the distance to the coil 12. Unfortunately, this device is only suitable for rewindable objects.
    In the apparatus of Fig. 2, this is not the case. The field lines 18 all run from the object 2 into the end faces 9, 10, which are both facing the object. The density of the field lines concentrates on a narrow range and then decreases very rapidly. Outside the yoke hardly any are measurable. Therefore, yokes are not suitable for solving the problem underlying this invention. These do a good job of magnetizing in the area within the two poles because the field lines are very strong there.
    The advantage of the present embodiment is therefore in particular that a rod choke is used, as shown in Fig. 3, comprising a rod-shaped ferromagnetic core 7, which is wound on its lateral surface 8 with one or two coils 12, 13. The magnetic field lines 18, 19 generated thereby are very concentrated in the direction opposite to the direction of travel in the area close to the core 7, which is important for the ferromagnetic body to be charged up to the saturation flux density. After that, the field strength decreases continuously but slowly, so that the dipoles freeze again in disordered states. To enhance this effect, the core 7 is like. Fig. 4 on the rear end face 10 enlarged designed, at least on the side facing away in the direction of travel vt, as already described.
    LIST OF REFERENCES 1 device 2 component 3 profile 4 length 5 longitudinal axis 6 surface, accessible surface 7 core, ferromagnetic core 8 lateral surface 9 front end surface 10 rear end surface 11 rear region of the core 12 coil, AC coil 13 coil, DC coil 14 end of a coil 15th Current source, current source for generating alternating current 16 Current source for generating direct current 17 Circuit design 18 Magnetic alternating flux 19 Magnetic direct flux 20 Magnetic flux of an external magnetic field (Earth's magnetic field) 21 Internal magnetic flux 22 Nahtransporteinrichtung 23 Rail car 24 Trailer coupling 25 Pulley AC AC DC DC a Distance component core a1. ..a2 range in which a is allowed (a-ι <a <a2) vt translational relative movement between the ferromagnetic core and the component along its entire length vr rotational relative movement between the ferromagnetic core and the component about its longitudinal axis
    Qh cross-sectional area of the core in the rear area
    Qs cross-sectional area of the core in the area of a coil
    Qv cross-sectional area of the core in the area of the front face
    Qb Cross-sectional area of the component BK Width of the ferromagnetic core transverse to the longitudinal axis BL Width of the ferromagnetic core along the longitudinal axis
    Bb Width of the component under the accessible surface
    权利要求:
    Claims (17)
    [1]
    claims
    1. Device (1) for demagnetizing a ferromagnetic, long-shaped component (2) of any length (4) with a uniform profile (3) having a longitudinal axis (5) on one side along its length (4) has an accessible surface (6) wherein the device (1) comprises a rod-shaped, ferromagnetic core (7) with a circumferential lateral surface (8) which is closed off by a front end face (9) and a rear end face (10), these end faces (9, 10) At least one coil (12) is wound around the lateral surface (8) and is connected at its ends (14) to a current source (15) which can generate an alternating current (AC), whereby a magnetic alternating flux ( 18) is induced in the ferromagnetic core (7), which at the two end faces (9,10) and in the non-spooled area of the lateral surface (8) enters and exits, characterized in that a coil (12, 13) to di e) is wound on the lateral surface (8) of the ferromagnetic core (7) which is connected at its ends (14) to a current source (15, 16) capable of generating a direct current (DC) for superimposing the alternating magnetic flux (18) on a characterized uniform magnetic flux (19) induced by the ferromagnetic core (7), the responce respectively at the two end faces (9, 10). exit.
    [2]
    2. Device (1) according to claim 1, characterized in that the AC source with the at least one coil (12) comprises a circuit construction (17), which makes it possible to apply the same coil (12) simultaneously with a DC current to the Magnetic alternating flux (18) with the desired magnetic flux (19) to be superimposed.
    [3]
    3. Device (1) according to claim 1, characterized in that the at least one coil (12) is an AC coil (12) and that the coil (13) for applying to DC one of the AC coil (12) different DC coil (13) is.
    [4]
    4. Device (1) according to claim 3, characterized in that the AC coil (12) is arranged closer to the front end face (9) than the DC coil (13).
    [5]
    5. Device (1) according to one of the preceding claims, characterized in that the ferromagnetic core (7) near the rear end face (10) has a rear portion (11) which is not wound by any coil (12, 13) to to collect the magnetic flux (18, 19).
    [6]
    6. Device (1) according to claim 5, characterized in that the ferromagnetic core (7) in the rear region (11) has a larger cross-section than in an area which is wound by a coil (12, 13).
    [7]
    7. Device (1) according to one of the preceding claims, characterized in that the cross-sectional area (Qv) of the ferromagnetic core (7) in the region of the front end face (9) is greater than the cross-sectional area (Qb) of the component (7).
    [8]
    8. Device (1) according to one of the preceding claims, characterized in that the width of the ferromagnetic core (BK), which is aligned in operation transversely to the longitudinal axis (5) of the component (2), is wider than the width (Bb) of the component extending below the accessible surface (6).
    [9]
    9. Device (1) according to any one of the preceding claims, characterized in that a profile (3) of the front end face (9) is adapted to the profile (3) of the accessible surface (6).
    [10]
    10. Device (1) according to one of the preceding claims, characterized in that the device (1) comprises a Nahtransporteinrichtung (22) which on the one hand in operation a distance (a) between the front end face (9) and the surface (6). ensures the component to be demagnetized (2), which remains within a predetermined range (al <a <a2) even in the induced magnetic forces in operation, and on the other hand, a translational relative movement (vt) between the ferromagnetic core (7) and the component (2 ) along its entire length (4).
    [11]
    11. Device (1) according to claim 10, characterized in that the distance (a) is smaller than the root of the cross-sectional area (Qb) of the component.
    [12]
    12. Device (1) according to any one of claims 10 or 11, characterized in that the Nahtransporteinrichtung (22) in addition, a rotary relative movement (vr) between the ferromagnetic core (7) and the component (2) about the longitudinal axis (5) of the component (2).
    [13]
    13. A method for demagnetizing a ferromagnetic, long-shaped component (2) of any length (4) having a longitudinal axis (5) at least on one side along its length (4) has an accessible surface (6), using a device (1) according to one of claims 10 to 12, characterized in that a) that on the one hand a constant alternating current (AC) is generated, which induces a magnetic alternating flux (18) through the ferromagnetic core (7), at the two end faces (9, 10) a and b) and on the other hand a constant direct current (DC) is generated which induces a uniform magnetic flux (19) overlying the alternating magnetic flux (18) through the ferromagnetic core (7) which is connected to the two end surfaces (9, 10). one resp. c) that the Nahtransporteinrichtung (22) always a distance (a) between the front end surface (9) and the surface (6) of the demagnetizing component (2) within a predetermined range (al <a <a2) ensures, and d) that the Nahtransporteinrichtung (22) causes a relative translational movement (vt) between the ferromagnetic core (7) and the component (2) along its entire length (4), while the alternating current and the DC are kept constant.
    [14]
    14. The method according to claim 13, characterized in that a) that before the induction of the magnetic fluxes (18,19), the device (1) is brought into a distance of the component (2), in which the magnetic effect of the magnetic fluxes (18,19 ) on the component (2) is smaller than that of a magnetic flux of a prevailing magnetic field field (20), b) then the steps a) and b) are carried out, c) then the device (1) in the vicinity of the component ( 2) is brought, and d) then the steps c) and d) are carried out.
    [15]
    15. The method according to claim 13 or 14, characterized in that a) that after step d) the device (1) is brought into a distance of the component (2), in which the magnetic effect by the magnetic fluxes (18, 19) the component (2) is smaller than that of a magnetic flux of a magnetic field field (20) prevailing in the environment, and b) the alternating current and the direct current through the coils (12, 13) are subsequently switched off.
    [16]
    16. The method according to any one of claims 13 to 15 using a device (1) according to claim 12, characterized in that the Nahtransporteinrichtung (22) in step d) in addition to the translational relative movement (vt) between the ferromagnetic core (7) and the Component (2) along its entire length (4) also causes a relative rotational movement (vr) about the longitudinal axis (5) of the component (2).
    [17]
    17. The method according to any one of claims 13 to 16, characterized in that after the demagnetization of the remaining residual magnetism on the component (2) is measured and the method is repeated as long with corrected at most DC magnitudes until this residual magnetism has fallen below a predetermined tolerance value.
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    同族专利:
    公开号 | 公开日
    CN109545500A|2019-03-29|
    CN109545500B|2022-03-04|
    DE102018007179A1|2019-03-28|
    US20190096559A1|2019-03-28|
    US11127519B2|2021-09-21|
    引用文献:
    公开号 | 申请日 | 公开日 | 申请人 | 专利标题
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    JPS5814056B2|1980-05-28|1983-03-17|Nippon Jidosha Buhin Sogo Kenkyusho Kk|
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    CN101083447B|2006-06-01|2012-07-25|田景华|Generalized force application magnet and conductor rail magnetic suspension vehicle or train using the same|
    CH707443A2|2013-01-14|2014-07-15|Albert Maurer|Demagnetizing.|
    CH708509A2|2013-09-06|2015-03-13|Albert Maurer|Eliminating anhysteretischem magnetism in ferromagnetic bodies.|CN112530659A|2020-11-30|2021-03-19|北京航空航天大学|A simulation demagnetization current generating device for magnetism shielding section of thick bamboo demagnetization|
    法律状态:
    2020-10-15| PFA| Name/firm changed|Owner name: ALBERT MAURER, CH Free format text: FORMER OWNER: ALBERT MAURER, CH |
    优先权:
    申请号 | 申请日 | 专利标题
    CH11682017|2017-09-22|
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