Device and method for winding and twisting fibre material in ring spinning or ring twisting frames

Abstract

A device and a method for winding and twisting fibrous material in ring spinning and ring twisting frames are disclosed. The device and method allow the operating speed of the frames to be substantially increased, achieve higher productivity during ring spinning, and reduce the outlay, in terms of time and material, for assembling and servicing the device. This is achieved in that at least two high-temperature superconducting stators, together with the thermally connected cooling devices thereof, are arranged in a contactless manner and in parallel with one another along the progression of the spindle row, and the magnetic field-generating rotors, oriented coaxially with respect to the spindle, are introduced in a magnetically levitating manner in the magnetic field of the continuous intermediate space, between the stators which are adjacent in each case.

Claims

1. A device for winding and twisting fiber material in ring spinning or ring twisting frames, comprising: at least two high-temperature superconducting stators (1), each stator (1) comprising at least one high-temperature superconducting material (4) and a stator cooling device; and annular, magnetic field-generating rotors (2), each of the rotors (2) being coaxially associated with a rotatable spindle which, together with a connected runner, serves for guiding and spooling a strand onto the spindle, wherein the at least two stators are arranged in a contactless manner and in parallel with one another along a progression of a spindle row, and wherein the magnetic field-generating rotors (2) are introduced in a magnetically levitating manner in a magnetic field of a continuous intermediate space between the stators (1).

2. The device according to claim 1, wherein the magnetic field-generating rotors (2) are provided with ferromagnetic magnetic flux collectors which serve to increase a field strength and to guide the magnetic field towards the superconducting material (4).

3. The device according to claim 1, wherein the at least two high-temperature superconducting stators (1) each comprise at least two bulk HTS elements which are designed so as to be separated from one another, in portions, and which are associated with respective magnetic field-generating rotors (2).

4. The device according to claim 1, wherein each of the at least two stators (1) consist of material that is joined together in a layered manner, and designed so as to be strip-like or cable-like in a longitudinal extension thereof

5. The device according to claim 1, wherein the at least two high-temperature superconducting stators are formed of a thermally insulated tube-in-tube configuration, in which during use an inner “cold” tube (8), connected to the stator (1), is cooled to a temperature below a superconducting critical temperature, and an outer tube (9) assumes a surrounding ambient temperature.

6. The device according to claim 5, wherein the outer tube (9) is made of a material which has a high electrical conductivity suitable for generating eddy currents, and thereby brings about additional magnetic stabilization during the rotational spinning and twisting operation.

7. The device according to claim 1, wherein each of the at least two stators (1) is formed of a YBaCuO crystal of the composition Y.sub.1Ba.sub.2Cu.sub.3O.sub.x (Y123) or a single crystal of the REBaCuO group of the composition RE.sub.1Ba.sub.2Cu.sub.3O.sub.x (RE—rare earth) and the superconducting material is of the bismuth family BiSrCaCuO.

8. The device according to claim 1, wherein each of the at least two stators (1) consists of a plurality of single crystals that are arranged side-by-side or are grown together.

9. The device according to claim 1, wherein, for the purpose of compensating their centrifugal forces, the magnetic field-generating rotors (2) each comprise an encompassing bandage (13) which consists of a material having a high tensile strength.

10. The device according to claim 1, wherein in the stator cooling device, for the purpose of additional stabilization, an electrodynamically assisted levitation is affected by a material with a high electrical conductivity and due to an eddy current generation in a metallic surface of the stator cooling device.

11. The device according to claim 5, wherein the inner tube (8) is cooled by supplying liquid nitrogen, and wherein thermal heat conduction between the inner tube (8) and the outer tube (9) is prevented by thermal vacuum insulation between the inner tube (8) and the outer tube (9) and by punctual rests (11; 12) of mechanical spacer assemblies (10) inserted between the inner tube (8) and the outer tube (9).

12. The device according to claim 5, wherein the inner tube (8) is cooled by a connection to a cryocooler.

13. A method for winding and twisting fiber material in ring spinning or ring twisting frames, in which permanent magnetic rings, which serve as the rotors, are mounted in high-temperature superconducting magnetic bearings, comprising: providing the device according to claim 1; mounting the rotors (2) which are associated in a coaxial manner with the spindles (3) in a magnetically levitating manner within a continuous intermediate space between the at least two stators (1); connecting the least two stators (1) to cryostats; wherein simultaneous cooling of the at least two stators (1) is carried out by the cryostats which are connected to the at least two stators (1) and which also extend along the spindle row.

14. The method according to claim 13, wherein the cooling of the at least two stators (1) is achieved by suppling liquid nitrogen via an inner tube (8), extending along the spindle row, of a tube-in-tube connection of the cryostat, a thermal insulation between the inner tube (8) and an outer tube (9) being achieved by vacuum insulation, the method further comprising: condensing, liquifiying, and supplying back to the cooling lines returned “cold” working gas N2 (14) by continuous mechanical re-cooling.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

[0020] FIG. 1 is a schematic comparative view of the prior and new magnetic bearing and rotors.

[0021] FIG. 2 is a perspective view of the magnetic bearing comprising three stators-

[0022] FIG. 3 is a cross-sectional view of the magnetic bearing comprising three stators.

[0023] FIG. 4 is a perspective view of the magnetic bearing comprising two stators.

[0024] FIG. 5 is a cross-sectional view of the magnetic bearing comprising two stators.

[0025] FIG. 6 shows the structural internal design of the stator.

[0026] FIG. 7 schematically shows the additional stabilization of the rotor.

[0027] FIG. 8 shows the enveloping bandage of the rotor, for the purpose of compensating the dynamic forces.

DETAILED DESCRIPTION

[0028] FIG. 1 schematically shows a comparison between the conventional ring single yarn twisting (a) and the HTS high-speed ring spinning method by means of a winding ring and runner construction suspended magnetically and in a frictionless manner (b). For this purpose, the spindles 3, together with the yarn spooled to form coils 5, are magnetically mounted between two high-temperature superconducting stators 1 that are arranged in parallel. In both arrangements, annular magnetically mounted magnetic field-generating rotors 2 are used. The yarn to be spooled is fed by the feeder system 16 of the machine. The difference between the two solutions consists in the design of the magnetic bearing, and the cooling system, required in each case, of the high-temperature superconductor. Typically, the HTS magnetic bearing is arranged so as to be coaxial to each spindle 3, and the cooling system is adapted in a complex manner to every individual bearing. In contrast, in the case of the magnetic bearing according to the disclosure, the magnetic bearing is achieved between two adjacent HTS stators extending along the spindle row. In this case, the required cooling system is designed so as to allow for simultaneous cooling of all the stators, in a simple manner.

[0029] The perspective view shown in FIG. 2 shows the superconducting magnetic bearing comprising three stators 1. The rotors 2 are designed as permanent magnetic rings having integrated runners (e.g. lugs). The stators 1 provided with high-temperature superconductors (HTS) extend in parallel with one another and along the spindle row. The rotors 2 are magnetically mounted in the intermediate space between two adjacent stators 1 in each case. It is furthermore possible, if required, to also arranged further stators 1 in parallel. A small tube 8, comprising HTS superconductors arranged thereon, is introduced in the interior of the stators 1 formed as tubes 9. Said superconducting materials 4 are applied, in portions, along the longitudinal extension of the tube 8 such that they achieve the intended position of the relevant rotor 2. The solution provided is adapted, in terms of structure and design, to the conventional ring spinning machines. On account of the linear structure, the innovation follows the traditional ring spinning frame design and eliminates the necessity for significant ring spinning frame changes if conventional ring runner devices are replaced by superconducting magnetic bearings (SMB). In this case, the system operates in a contactless manner and exhibits extremely low rotational friction.

[0030] The free suspension of the rotor combination above the HTS stator 1, and the rotation thereof at virtually the speed of the spindle, makes it possible for the frictional heat of the rotor 2 to be significantly eliminated, even when the rotor speed is further increased. In this case, in the dynamic process only a low friction force between the strand and runner is generated. The generated rotation of the rotor 2 significantly reduces the strand/runner frictional interaction, as a result of which the majority of the heat source is eliminated. In this case, the rotor 2 and the stator 1 are designed such that in each case a circular air gap is formed, so as to be axially spaced between the rotor 2 and the stator 1 and coaxial to the spindle 3. The strand is guided through the rotating runner, and can be wound onto the rotating coil body. In contrast to previous bearing solutions, in which adjacent spindles 3 run at ambient temperature conditions in the feed-through of a cryostat, in the new solution the spindles 3 do not have to be kept separate, and have clear space along the spindle row. This construction allows for combined LN2 cooling of a row of corresponding stators 1 having a large free space. Furthermore, in this way spindles 3 and coils can be serviced or replaced much more easily.

[0031] FIG. 3 shows the schematic cross-sectional structure of the magnetic bearing that is formed of three stators 1. The arrangement of the inner tubes 8 in the respective outer tubes 9 is visible. The rotors 2, together with the associated spindles 3 in each case, are magnetically suspended in the intermediate space between two adjacent stators 1 in each case. Between the tubes (8; 9), the simultaneous cooling of all the superconductors is performed by cooling by means of liquid nitrogen (LN2).

[0032] The illustration of FIG. 4 shows the perspective view of a magnetic bearing consisting of two stators 1. In this embodiment, too, the HTS superconductors 4 are applied to the inner tube 8, in portions along the longitudinal progression of the stators 1, and are positioned, in terms of location, such that they magnetically achieve the position of the spindles 3 that is to be assumed. Furthermore, the possibility is also provided of designing the HTS superconductors 4 so as to be strip-like or cable-like, which superconductor is applied to the inner tube 8, over the entire length of the stator 1, during assembly. At the magnetic bearing points of the rotor 2, provided in each case, the HTS superconductor, which is generally constructed in a layered manner, is already adapted to the magnetic strengths to be generated, during the prefabrication.

[0033] A cross-sectional view of the magnetic bearing formed of two stators 1 is visible in FIG. 5. In addition to the bearing of the rotors 2 already set out, the cooling lines 15 leading into and out of the interior of stators 1 can be seen in the schematic drawing.

[0034] The structural internal design of the stator 1 is visible from the illustration of FIG. 6. In this case, the square outer tube 9 constitutes the vacuum chamber for the likewise square inner tube 8. The HTS superconductor 4 is adhesively bonded to the inner cold tube 8. Liquid nitrogen, as a coolant, is introduced into the inner tube 8. The magnetic fixing of the inner tube 8, connected to the HTS superconductor 4, is achieved by means of spacer assemblies 10 consisting of glass fiber structures. These are designed such that they have a heat-conducting connection to the outer tube 9 only at the punctual rests 11, 12. As a result, a heat-conducting connection between the “cold” inner tube 8 and the outer tube 9, adjusted to the ambient temperature, is largely prevented. Since the bars can consist of a lightweight AL alloy, the design can be constructed in a very compact manner, and at a low weight. Furthermore, the AL alloy material of the cryostat achieves a high thermal connection between the inner tube 8 and the HTS superconductor 4. However, the high thermal expansion coefficient of the AL alloy at ambient temperature must be taken into account in the determination and fixing of the exact longitudinal position of the superconducting stators 1 in the 4-5 m long carrier elements.

[0035] The schematic view of an additional stabilization of the position of the rotor 2 is visible in FIG. 7. In addition to the levitation of the strand-guiding annular rotor 2, in an innovative manner additional stabilization is achieved by electrical eddy currents 17 which are induced in the cryostat and the stators 1. The inner and outer tube consist of an electrically conductive aluminium alloy. As a result, the rotating rotor 2 will levitate over a metal Al sheet. Two effects can thereby contribute to the stabilization of the rotating rotor 2. According to Lenz's law, the direction of every magnetic induction effect is such that it acts counter to the cause of the effect. As a result, the direction of the magnetic force on the moving magnet is counter to its movement. The induced current results in the current status quo being preserved, in that it counteracts the movement or a flux change. A lift, in the normal direction with respect to the conducting plane, and a resistance braking force counter to the direction of rotation, exist above the stators 1. Accordingly, both forces contribute to additional retention and stabilization of the rotating rotor 2 during winding and twisting. A further embodiment is the generated braking force, which, as a result of the change in the peripheral magnetisation of the annular rotor 2, brings about rapid braking of the rotating rotor 2. At a low speed, the resistance is proportional to the speed v=ω/r and greater than the lift, which is proportional to v.sup.2.

[0036] As the speed of the rotor 2 increases, the resistance achieves a maximum and reduces by 1/(v).sup.1/2. In contrast, the lift, which stabilises the rotor 2, increases, at a low speed, by v.sup.2, and overtakes the resistance as the speed increases. The ratio of lift to resistance is of significant practical importance, and results in f.sub.L/f.sub.D=v/v.sub.i, wherein v and v.sub.i are the speeds of the magnetic dipole above the conductive sheet and the corresponding positive and negative image which propagates downwards at the speed v.sub.i.

[0037] The graph of FIG. 8 shows the fundamental behavior of the rotors 2 in the case of high-speed ring spinning applications. In the case of the solution according to the disclosure for high speeds, the rotational friction and the dynamic effects of the magnetic bearing are particularly important. The essential advantages of superconducting bearings compared with conventional bearings are significant in this field. The superconducting passive magnetic bearings exhibit substantially lower friction than conventional rolling bearings, at least by a factor of forty. Even in comparison with pressurised air bearings, the friction of the passive magnetic HTS bearing is in the permille range, and is therefore surprisingly small. This extremely low friction is the physical basis for the innovative ring spinning technology, up to very high spindle rotational speeds.

[0038] The centrifugal forces are a further critical point of the ring rotor dynamics. The present disclosure focusses on rotational speeds of the permanent magnetic rotor 2 comprising the strand guide of up to 50,000 rpm. A rotor 2 of size 60 cm×40 cm×1 cm, which serves as a twisting and rotation element, is subject to extremely high centrifugal forces, which can destroy the operating ring. In a first approach, it is intended to consider the maximum tensile force or force density by way of the tangent vector at the inside radius r.sub.i.

σ.sub.t=ρv.sup.2=ρω.sup.2r.sup.2

[0039] When the annular rotor 2 rotates, different centrifugal forces result, which can destroy the rotor 2. The highest mechanical forces arise at the inside radius of a rotating ring. The value of the tensile stress of sintered NdFeB is approximately 80-90 MPa (12,000 psi). However, at a rotational speed of 50,000 rpm about the spindles, a PM ring made of NdFeB, of a size 60×40×10 is subjected to a maximum tangential force density of ˜185 MPa; more than a factor of two than the intrinsic material tensile stress. Accordingly, the dynamic forces have to be compensated by a corresponding enveloping bandage 18 in the peripheral direction of the rotor 2.

[0040] The bandage ring 18 should consist of materials having a high tensile stress, either metal, such as non-magnetic stainless steel, high-strength Al or Mg alloys, or a non-metal ring consisting of glass or carbon fiber compounds. In the best and optimum case, the safety ring reinforcement ensures pre-pressure on the rotor 2 even at a speed of zero, and then prevents any cracks or defects of the NdFeB magnetic ring below the nominal operating speeds. As a practical solution, a safety ring thickness of 3 mm Al alloy AL7075 was selected, and rigidly connected to the rotor 2 by means of thermal shrinkage.

[0041] While the present invention has been described with reference to exemplary embodiments, it will be readily apparent to those skilled in the art that the invention is not limited to the disclosed or illustrated embodiments but, on the contrary, is intended to cover numerous other modifications, substitutions, variations and broad equivalent arrangements that are included within the spirit and scope of the following claims.

LIST OF REFERENCE CHARACTERS

[0042] 1 stator

[0043] 2 rotor

[0044] 3 spindle

[0045] 4 HTS superconductor

[0046] 5 coil

[0047] 6 yarn

[0048] 7 runner

[0049] 8 inner tube

[0050] 9 outer tube

[0051] 10 spacer assembly

[0052] 11 punctual rest

[0053] 12 punctual rest

[0054] 13 bandage

[0055] 14 working gas N2

[0056] 15 cooling lines

[0057] 16 feeder system

[0058] 17 electrical eddy current

[0059] 18 bandage