US3835242A

US3835242A - Multi-filament composite superconductor with transposition of filaments

Info

Publication number: US3835242A
Application number: US00286625A
Authority: US
Inventors: B Zeitlin; P Critchlow
Original assignee: Individual
Current assignee: Individual
Priority date: 1972-09-06
Filing date: 1972-09-06
Publication date: 1974-09-10
Anticipated expiration: 1991-09-10
Also published as: GB1401936A

Abstract

A multi-filament superconducting composite composed of a plurality of segments that is intrinsically stable. The individual segments are multi-filament composites that have been twisted after assembly and mechanical working and thereafter subsequently deformed. The deformed segments can be triangular or rectangular and are assembled into a second composite. After assembly the second composite is once again twisted. This second twisting transposes the filaments within the segments, thereby producing a superconductor that is resistant to flux jumps induced by self-field losses.

Description

United States Patent Critchlow et a1. I

[ MULTI-FILAMENT COMPOSITE SUPERCONDUCTOR WITH TRANSPOSITION OF FILAMENTS Inventors: Philip R. Critchlow, 1843 Edgewood, St. Bruno, Quebec, Canada; Bruce A. Zeitlin, 234 Henry Ct., North Plainfield, NJ. 07060 Filed: Sept. 6, 1972 Appl. N0.: 286,625

US. Cl. 174/126 CP, l74/DIG. 6, 174/114 S, 174/128 Int. Cl. H01v 11/08 Field of Search ..l74/l28, 126 CP, 114 S, 174/129, DIG. 6

References Cited UNITED STATES PATENTS 4/1933 Milliken l/l937 Gilbert 11/1971 Morton 4/1972 Woolcock..

174/128 X 174/128 X l74/DIG. 6 l74/DIG. 6

[ Sept. 10,1974

3,699,647 10/1972 Bidault l74/DIG. 6

3,702,373 11/1972 Ecomard 174/DIG. 6 FOREIGN PATENTS OR APPLICATIONS 708,162 4/1931 France 174/114 S Primary Examiner-E. A. Goldberg Attorney, Agent, or Firm-Larry R. Cassett; I-l.

Hume Mathews [57] ABSTRACT A multi-filament superconducting composite composed of a plurality of segments that is intrinsically stable. The individual segments are multi-filament composites that have been twisted after assembly and mechanical working and thereafter subsequently deformed. The deformed segments can be triangular or rectangular and are assembled into a second composite. After assembly the second composite is once again twisted. This second twisting transposes the filaments within the segments, thereby producing a superconductor that is resistant to flux jumps induced by selffield losses.

9 Claims, 9 Drawing Figures MULTI-FILAMENT COMPOSITE SUPERCONDUCTOR WITH TRANSPOSITION OF FILAMENTS BACKGROUND OF THE INVENTION 1. Field of the Invention This invention relates generally to superconductors and more specifically to multi-filamentary superconductor composites that are intrinsically very stable.

2. Prior Art A significant factor in the development of superconductors and superconducting devices is the attainment of adiabatic stability. This is essential in order to attian reliable performance in superconducting devices. Excellent superconducting properties have been attained in laboratory testing of short samples. However, when superconducting devices were fabricated fromlong superconductor wire, performance comparable to short sample testing was not attained.

Failure to'obtain short sample performance in superconducting devices has been attributed, in part, to flux jumps. Flux jumps cause degradation in superconducting devices by creating sudden local releases of energy resulting in a premature transition to the normal state and thereby preventing reliable attainment of high current densities.

, It is theorized that flux jumps occur when an external field is applied to asuperconducting device inducing loops of current at the critical current density which are unstable and may suddenly decay rapidly with a release of energy. This sudden release of energy causes a transition in the superconducting device fromthe superconducting state to the normal or resistive state thereby causing degradation of the superconductor. This sudden reversal can result in serious physical damage to the superconducting device.

Various techniques have been developed to improve the stability of superconductors by minimizing degradation caused by flux jumping. In the paper, Multifilamentary Superconducting Composites, by P. R. Critchlow, E. Gregory and B. Zeitlin, published in Cryogenics, February 1971, pp. 3-10, recent developments that have contributed to the production of stable superconducting composites are discussed. One such development is the production of superconductors from composites having 50l',000 superconducting filaments in a matrix of high purity copper. However, the apparent advantages offered by miltifilamentary composites were not fully realized because these wires behaved in some respects essentiallyv the same as an equivalent solid single core conductor and the occurrence of flux jumping was unchanged.

This paper points out a technique whereby flux jumps induced by an external field can be reduced and the full advantages of multifilamentary composites attained. If the composite is twisted, the wire is effectively cut into lengths equal to half the twist pitch. The twisted wire should, therefore, behave as a collection of isolated filaments and consequently be more stable than acomparable untwisted multifilament composite.

Critchlow et al disclose that a twisted composite is still susceptible to degradation and loss from self-field effects. The self-field of the wire is produced by the transport current flowing in it. This results in an unequal current distribution in which the outer filaments carry'more current than the inner ones. A flux jump I thereby afl'ecting the size of the may occur thereby producing more uniform current distribution with a concomitant transition to the normal state.

Twisting alone will not eliminate self-field effects because the filaments never change their radial position. Transposition will arrange the individual filaments so that they occupy successively every position of the cross-section. The filaments in an individual wire cannot be transposed. However, by winding a number of these wires into a braid or cable, a transposed conductor can be constructed.

By forming abraid. or cable insures that the inner wires get to the outside of the conductor cross-section. These techniques, however, are not entirely satisfactory because rigidity and high packing factor cannot be attained. Rigidity of wires in a'superconducting device is necessary to prevent objectionable wire motion. The shape of braided or cabled super-conducting wire does not produce a high packing factor. This restricts the amount of wire'than can be contained in a magnet magnet. Accordingly, thepresent invention provides a novel superconductor composite comprised of a plurality of segments and method of making same that utilizes superconducting filaments embedded in a normal matrix. The segments are twisted so as to obviate eddy current type losses resulting from external magnetic fields and the individual filaments are also transposed so that they occupy the same relative radial position within the superconductor cross-section, thereby also avoiding or eliminating self-field losses.

SUMMARY OF THE INVENTION An object of this invention is to provide an intrinsically stable milti-filament superconductor.

A further object of this invention is to provide an intrinsically stable milti-filament superconductor composed of a plurality of segmented composites.

Still a further object of this invention is to provide a superconductor that is free from degradation resulting from self-field losses.

Still a further object of this invention is to provide a method for producing intrinsically stable multifilament super-conductors.

A further object of this invention method for producing filament superconductors segmented composites.

These and other objects are obtained by assembling a first composite composed of a plurality of superconducting rods in a norrnal'matrix. This first'assembly is then mechanically worked until the superconductor rods are reduced to a filament of a diameter approximating the desired final diameter. The mechanically reduced composite is then twisted and segmented. As used herein, the term segmented means to alter mechanically the cross-section of the superconductor composite from round to triangular or rectangular by passingthe composite through a forming device. A second composite of rectangular or circular cross-section is made by assembling a plurality of the previously formed segments. This second composite is then mechanically worked until the diameter of the filaments is reduced to approximately 0.3 to 0.4 mil. The mechanically worked composite is then twisted a second time.

is to provide a intrinsically stable multicomposed of a plurality of The individual segments constitute composites composed of a suitable number of superconducting filaments in a matrix of normal material having a twist of the necessary pitch. The segments are resistant to flux jumping induced by an external magnetic field and are thereby stabilized against this form of degradation.- However, the filamentary strands within eachindividual segment will not vary in their radial location from the center of such segment and the segment will not avoid instability resulting from generated self-fields. The individual segments are combined to form a second composite. The second composite is then mechanically worked and twisted to a predetermined pitch. The convoluted filaments containedwithin each segment of this second composite assume a path of varying radial position along their lengths from the center of the final conductor. Such varying distribution of the individual filaments produces a more uniform sharing of each filament of the cross-section of the composite conductor so that each filament shares substantially equally'inthe conducting current. Thus the tendency towards instability resulting from self-generated fields is avoided.

The advantages of the superconductor of this invention will be apparent from the following drawings and detailed descriptions in which:

BRIEF DESCRIPTION OF THE SEVERAL VIEWS FIG. 1 is a diagrammatic transverse schematic of a first composite of this invention consisting of superconductor rods in a normal matrix.

FIG. 2 is a diagrammatic longitudinal schematic of a first composite of this invention showing the position of an outside filament after twisting.

FIG. 3 is a diagrammatictransverse schematic of a first composite after segmenting.

FIG. 4 is a diagrammatic transverse schematic of another embodiment of a first composite after segment- FIG. 5 is a diagrammatic transverse schematic of a second composite consisting of a plurality of triangular segments.

FIG. 6 is a diagrammatic longitudinal schematic of a second composite showing the position of a filament within the composite. I

FIG. 7 is a diagrammatic transverse schematic of another embodiment showing a second composite consisting'of a plurality of rectangular segments.

FIG. 8 is a diagrammatic transverse schematic of a second composite after twisting;

FIG. 9 is a diagrammatic longitudinal schematic of a second composite showing the position of a transposed filament within a segment after twisting.

DETAILED DESCRIPTION OF THE PREFERRED I EMBODIMENT Referring to FIG. 1, there is shown a superconducting composite 10 consisting of a normal 'matrix 12 4 v properties. In this instance composite 10 is reduced to a diameter approximating the desired final diameter.

After fabrication, composite 10 is twisted. As shown in FIG. 2, after twisting representative filament 14a follows path 16. The pitch or rate of twist is dependent upon the rate at which the superconducting device will be charged. For most applications at pitch of A to 5 twists per inch is acceptable. The intermediate diameter must be of such a magnitude so that reduction to the final diameter will not remove the original twist by I elongating the wire. Generally speaking, this intermediate diameter must not be more than twice the final desired diameter.

FIGS.'3 and 4 show two different embodiments, 10a and 10b, of segmented composite 10. After composites 10a or 10b are mechanically worked to an intermediate diameter and twisted, they are then segmented by mechanical shaping. Shaping to the desired cross-section may be performed by using dies, grooved rolls or a Turks-head. A Turks-head consists of 4-hardened steel rolls set in planes at right angles to each other. The narrow face of the rolls, as set in the framework, is adjustable on the same plane so that the assembly of the overlapping roll edges facing each other will project a contour of the opening so formed, into the desired shape of the cross-section of the product to be made.

Preferably the angle 0 in FIG. 3 should be a subdivision of 360, ie. 10, 12, 15, 20, 24, 30, 45, 60, 72, 90, 120, etc., so that the triangular orrectangular segments 10a or 10b so produced by the Turks-head can be assembled to form a second composite 22 or 30 as shown in FIGS. 5' and 7, respectively. After mechanically forming segments 10a or 10b, the segments can be further treated in order to facilitate assembly of composformed by ultra-sonically welding the segments together.

FIG. 5 shows a second composite 22 composed of

triangular segements

20a, 20b, 20c, 20d, 20e, 20f, 20g and 20h. The angle 0 formed during drawing first composite 10 through the forming dies in 45. As shown in FIG. 6, representative filament 24in segment 20a is transposed along the path 26.

FIG. 7 shows another embodiment of a second composite 30 composed of

rectangular segments

32a, 32b, 32c and 32d.

As shown in FIGS. 5 and 7, after assembly the mating segments have a common junction point, 28 and 34, which is located at the center of the second composite. This places some of the filaments which were formerly situated at the outside of the original composite on the inside or near junction point '28 or 34 of the second composite. These filaments were originally twisted and theywill retain their position in the interior of the segment cross-section after assembly of the second composite. Furthermore, filaments originally located near the center of the segments, such as filament 24, will now be located near the outside of the second composite. When the second composite is twisted after assemrate of twist is represented by numerical 36 in FIG. 8.

The segmented composite is now stabilized against selfinduced flux jumps. Representative filament 24 in segment a is transposed along the path 27.

Superconducting wire produced by the novel method of this invention has several distinct advantages over superconducting wireproduced by conventional prior four segments and was approximately 20 mil square. The individual segments each contained 360 filaments approximately 0.3 0.4 mil in diameter.

From the foregoing, it is apparent that by the present invention there has been provided a particularly advantageous method for producing a novel intrinsically stable superconducting wire. The invention has been deart methods. Some of the more apparent advantages include:

A solid superconducting wire of equivalent diameter and equal superconductor alloy to nonnal material ratio will exhibit more losses that a segmented superconductor composite produced by the invention disclosed herein. The windings of superconducting devices, such as magnets, will be more rigid with less wire motion when wound with this novel segmented wire as compared to other intrinsically stable superconducting wires, such as braid or cable. Furthermore, the shape of this wire produces a higher packing factor than braid or cable, resulting in more wire per superconducting device. Still further, a composite with a like number of small diameter filaments merely twisted and not transposed will not be stable against self-induced losses and the advantages of small diameter filaments will not be fully realized.

. SPECIFIC EXAMPLE First Composite A first composite was assembled by inserting 360 rods of a Nb-Ti alloy (Containing 55 percent by weight Nb) into an 8 inch diameter copper billet. This composite was then mechanically worked until the diameter of the composite was approximately 11 mil.

The mechanically worked composite was then twisted. The rate of twist was from about turns to 5 turns per linear inch Segmenting First Composite The 11 mil composite was then passed through a Turks-head. The rolls of theTurks-head were adjusted to produce a square wire approximately 10 mil square.

Second Composite The square segment was then passed through a bath of silver-tin solder (3 percent Ag, 97 percent Sn). A second composite was formed by paying out four solder-coated segments from four bobbins. This composite 30 is shown in FIG. 7. The payed out segments were passed through a series of closely-spaced aligning dies. The properly aligned segments then passed through a tapered die wherein a square composite was formed. At some convenient location heat was applied to the composite, melting the solder and bonding the segments together. The formed composite was twisted at a rate from about A turns to about 5 turns per linear inch.

The finished intrinsicially stable composite contained scribed with reference to a presently preferred embodiment, however, it' is intended to cover such modifications as fall within the spirit and the scope of the invention as hereinafter claimed.

We claim:

1. A superconductor comprising:

a plurality of initially twisted mated segments twisted together to form an assembly wherein each said segment consists of a matrix of normal material and a plurality of super-conducting filaments in twisted array the filaments within each segment occupy positions near the surface and interior of said matrix cross-section and are also disposed in a path of varing radial position in the longitudinal direction of said superconductor.

2. A superconductor as recited in claim 1 wherein said mated segments have a common juncture at the center of said super-conductor.

3. An intrinsically stable superconductor composite that is resistant to flux jumps induced by self-field losses comprising:

a plurality of initially twisted mated segments wherein each said segment further comprises a matrix of normal material and superconductor filaments embedded in said matrix, said segments further containing a helical twist of a pitch from about /2 to about 5 convolutions per linear inch.

4. A superconductor as recited in claim 3 wherein said mated segments are generally triangular in crosssection.

5. A superconductor as recited in claim 3 wherein said mated segments are generally rectangular in crosssection.

6. An intrinsically stable superconductor composite that is resistant to flux jumps induced by self-field losses comprising:

a matrix of normal material; and a plurality of filaments of a superconducting alloy embedded in said matrix wherein the individual filaments occupy positions near the surface and interior of said matrix cross-section and are also disposed in a path of varying radial position in the longitudinal direction of said composite.

7. A superconductor as recited in claim 6 wherein said normal material is copper.

8. A superconductor as recited in claim 7 wherein said superconductor alloy is a Nb-Ti alloy.

9. A superconductor comprising:

an assembly of initially twisted mated segments wherein each segment comprises a matrix of normal material and a plurality of filaments embedded in matrix, wherein the filaments within each segment occupy positions near the surface and interior of said matrix cross-section and are also disposed in a path of varing radial position in the longitudinal direction of said superconductor.

Claims

1. A superconductor comprising: a plurality of initially twisted mated segments twisted together to form an assembly wherein each said segment consists of a matrix of normal material and a plurality of super-conducting filaments in twisted array the filaments within each segment occupy positions near the surface and interior of said matrix cross-section and are also disposed in a path of varing radial position in the longitudinal direction of said superconductor.

3. An intrinsically stable superconductor composite that is resistant to flux jumps induced by self-field losses comprising: a plurality of initially twisted mated segments wherein each said segment further comprises a matrix of normal material and superconductor filaments embedded in said matrix, said segments further containing a helical twist of a pitch from about 1/2 to about 5 convolutions per linear inch.

4. A superconductor as recited in claim 3 wherein said mated segments are generally triangular in cross-section.

5. A superconductor as recited in claim 3 wherein said mated segments are generally rectangular in cross-section.

6. An intrinsically stable superconductor composite that is resistant to flux jumps induced by self-field losses comprising: a matrix of normal material; and a plurality of filaments of a superconducting alloy embedded in said matrix wherein the individual filaments occupy positions near the surface and interior of said matriX cross-section and are also disposed in a path of varying radial position in the longitudinal direction of said composite.

9. A superconductor comprising: an assembly of initially twisted mated segments wherein each segment comprises a matrix of normal material and a plurality of filaments embedded in matrix, wherein the filaments within each segment occupy positions near the surface and interior of said matrix cross-section and are also disposed in a path of varing radial position in the longitudinal direction of said superconductor.