ALIGNMENT OF HTS TAPES

Abstract

A cable for carrying electrical current in a coil of a magnet. The cable comprises a stack of tape assemblies. Each tape assembly has a length and a width, such that the length is much larger than the width, and each tape assembly comprises an HTS layer of anisotropic high temperature superconductor, HTS material, wherein a c-axis of the HTS layer is at a non-zero angle to a vector perpendicular to the plane of the HTS layer. The tape assemblies are stacked as a series of pairs, each pair comprising first and second HTS tape assemblies and a copper layer therebetween. The tape assemblies in each pair are arranged such that the c-axis of the HTS layer of the first HTS tape assembly of each pair have reflective symmetry to the c-axis of the HTS layer of the second HTS tape assembly of each pair about a plane which is parallel to and equidistant from each HTS layer.

Claims

1. A cable for carrying electrical current in a coil of a magnet, comprising: a stack of tape assemblies, each tape assembly having a length and a width, such that the length is much larger than the width and each tape assembly comprises an HTS layer of anisotropic high temperature superconductor, HTS material, wherein a c-axis of the HTS layer is at a non-zero angle to a vector perpendicular to the plane of the HTS layer; wherein the tape assemblies are stacked as a series of pairs, each pair comprising first and second HTS tape assemblies and a copper layer therebetween; wherein the tape assemblies in each pair are arranged such that the c-axis of the HTS layer of the first HTS tape assembly of each pair have reflective symmetry to the c-axis of the HTS layer of the second HTS tape assembly of each pair about a plane which is parallel to and equidistant from each HTS layer.

2. The cable according to claim 1, wherein the HTS material is one of: ReBCO; and BSCCO.

3. The cable according to claim 1, wherein each HTS tape assembly comprises a substrate.

4. The cable according to claim 3, wherein each pair is arranged such that the HTS layers of the HTS tape assemblies are arranged between the substrates of the HTS tape assemblies.

5. The cable according to claim 3, wherein each pair is arranged such that the substrates of the tape assemblies are arranged between the HTS layers of the HTS tape assemblies.

6. The cable according to claim 3, wherein each pair is arranged such that one HTS layer is arranged between the substrates of the HTS tape assemblies, and the other HTS layer is arranged outside the substrates of the HTS tape assemblies.

7. The cable according to claim 1, wherein each HTS tape assembly comprises exfoliated HTS tape.

8. The cable according to claim 1, wherein the thickness of the copper layer is between 10 microns and 400 microns.

9. A method of manufacturing a cable for carrying electric current in a coil of a magnet, the method comprising: providing first and second tape assemblies, each tape assembly comprising a high-strength metal substrate layer, and an HTS layer of anisotropic high temperature superconductor, HTS, material, wherein a c-axis of the HTS layer is at a non-zero angle to a vector perpendicular to the plane of the HTS layer; applying the first tape assembly to a copper layer; applying the second tape assembly to the copper layer, such that the HTS layer of the first tape and the HTS layer of the second tape are parallel and separated by the copper layer, and such that a c-axis of the second HTS tape assembly has reflective symmetry to the c-axis of the HTS layer of the second HTS tape assembly of each pair about a plane which is parallel to and equidistant from each HTS layer.

10. The method according to claim 9, wherein each HTS tape assembly comprises a substrate layer.

11. The method according to claim 10, wherein the first and second HTS tape assemblies are applied to the copper layer such that the respective HTS layer is between the respective substrate layer and the copper layer.

12. The method according to claim 10, wherein the first and second HTS tape assemblies are applied to the copper layer such that the respective substrate layer is between the respective HTS layer and the copper layer.

13. The method according to claim 10, wherein the first and second HTS tape assemblies are applied to the copper layer such that the HTS layer of the first HTS tape assembly is between the substrate layer of the first HTS tape assembly and the copper layer, and the substrate layer of the second HTS tape assembly is between the HTS layer of the second HTS tape assembly and the substrate layer.

14. The method according to claim 8, wherein each HTS tape assembly comprises exfoliated HTS tape.

15. The method according to claim 8, and comprising partially transferring a master HTS tape assembly from a first reel to a second reel, separating the portion of the master HTS tape assembly on the first reel from the portion of the master HTS tape assembly on the second reel, and applying the first HTS tape assembly from the first reel and the second HTS tape assembly from the second reel.

16. The method according to claim 8, wherein the first HTS tape assembly is applied in the opposite direction along the copper layer to the direction in which the second HTS tape assembly is applied.

17. The method according to claim 8, wherein the first and second HTS tape assemblies are formed by folding a master HTS tape assembly about an axis in the plane of the HTS layer and perpendicular to the length of the master HTS tape assembly, and removing a region of the master HTS tape assembly containing the fold.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

[0011] FIG. 1 is an illustration of the structure of ReBCO tape;

[0012] FIG. 2 is a diagram showing a coordinate system for describing ReBCO tape;

[0013] FIG. 3 is a pair of cross sections of a ReBCO tape, showing the principal axes of the ReBCO crystal;

[0014] FIG. 4 is a cross sections of a type 0 pair;

[0015] FIG. 5 is a cross sections of an exemplary type 0 pair;

[0016] FIGS. 6A, 6B, 6C, and 6D show the critical current variation with external magnetic field of the constructions of FIGS. 4A/B and 5A/B for different ReBCO tapes;

[0017] FIG. 7A shows the current ratio of ReBCO within a field coil constructed using the construction of FIG. 4;

[0018] FIG. 7B shows the current ratio of ReBCO within a field coil constructed using the construction of FIG. 5;

DETAILED DESCRIPTION

[0019] The invention describes a method of combining pairs of HTS tapes such that any variation in the angle at which peak critical current occurs along the tape is averaged out in the pair, leading to a more consistent behaviour.

[0020] FIG. 4 shows an exemplary type-0 pair of ReBCO tapes in a cross section perpendicular to the axis of the tape. A type-0 pair comprises two tapes 410, 420, oriented such that the ReBCO layers 411, 421 face each other, and with a copper lamination 430 between them. In the event of a flaw or “dropout” in critical current in one tape (such as a crack), this allows current to transfer between the ReBCO layers 411, 421 via the copper lamination, which has low resistivity. The resistance between pairs of ReBCO is lower in this orientation that the more common arrangement of simply stacking tapes with the HTS layers facing in the same direction (type-1 pairs).

[0021] Each tape has a c-axis 412, 422 at an angle a from the perpendicular to the plane of the ReBCO layer (i.e. the z-axis), and a peak Ic angle (i.e. the angle of applied magnetic field for which the critical current is greatest) which is perpendicular to the c-axis.

[0022] Conventionally, the type-0 pair would be constructed by first applying the tape 410 from a spool of ReBCO tape to the copper lamination 430 from one end to the other and then applying the tape 420 from the same spool of HTS tape in the same direction on the opposite side of the copper lamination. This results in the c-axis of the ReBCO 412, 422 and the a/b plane 413, 423 (i.e. the angle of applied magnetic field for which Ic is maximised) being oriented as shown in FIG. 4, with rotational symmetry about the y axis 401 of the type-0 pair.

[0023] As an alternative, the type-0 pair can be constructed as shown in FIG. 5, which is a cross section equivalent to FIG. 4 for an exemplary type-0 pair construction. The tapes 510, ReBCO layers 511 and copper lamination 530 are equivalent to the tape 410, ReCBO layer 511, and copper lamination 430 of FIG. 4. The tape 520 has been applied such that the ReBCO layer 421 faces the ReBCO layer 511 of the tape 510, and such that the c-axes 511, 521 and a/b planes 512, 522 of each tape 510, 520 have reflective symmetry about a plane 501 which is parallel to and equidistant from each tape of the type-0 pair.

[0024] The application of the tape to form the construction of FIG. 5 (i.e. a “flipped pair”) can be done by first applying the tape 510 from a spool of ReBCO tape in one direction), and then applying the tape 520 from the same roll of ReBCO tape in the opposite direction along the y-axis. Alternatively, the ReBCO tape may be unwound from the spool between application of the tape 510 and application of the tape 520, and rewound in the opposite direction, then the tape 520 is applied in the same direction as the application of the tape 510. As a further alternative, the tape 510 and the tape 520 may be applied in the same direction from different rolls, which have been wound in opposite senses, to produce the correct alignment of the c-axes.

[0025] If the tape does not need to be applied directly from a spool, the “flipped pair” orientation is most easily achieved by: [0026] 1. Spooling off two equal lengths of tape from a spool. [0027] 2. Turning over one tape about its y axis so that the HTS coated sides face each other. [0028] 3. Rotating one tape 180 degrees lengthways about the z-axis.

[0029] Alternatively, this can be achieved by spooling off one tape of greater than twice the required length, folding it in the middle about the x axis (i.e. end-to-end), and cutting off or otherwise removing a section containing the fold, to leave two tapes which are then arranged in a type-0 pair in a “flipped” orientation (or a type-2 pair if the tape is folded such that the substrates face each other).

[0030] FIGS. 6A to 6D show plots of the critical current vs angle of magnetic field for type-0 pairs constructed according to FIG. 4 (blue line) or FIG. 5 (red line), for tapes with an angle between the c-axis and the perpendicular of the tape of approximately 1 degree (FIG. 6A), 5 degrees (FIG. 6B), 10 degrees (FIG. 6C) and 35 degrees (FIG. 6D).

[0031] As can be seen from the figures, the use of the construction of FIG. 5 results in a lower peak critical current, but a range of relatively high critical currents across a broader range of angles. For a tape in which the c-axis is exactly aligned with the perpendicular to the tape (z-axis), the two constructions are equivalent.

[0032] For tapes with a small angle (<5 degrees) offset between the c-axis and z-axis, the flipped-pair arrangement has the beneficial effect of averaging out the impact of any changes in the angle at which peak critical current occurs at any position along the tape. This is because the peaks of the individual tapes in the pair are merge into one lower broader peak, as shown in FIG. 6A (red curve). Small variations in the angular offset along the tape will cause the peak to broaden or sharpen.

[0033] Furthermore, where the flipped pair is made from a single reel of tape, if the critical current at the start of the reel is lower or higher than at the end of the reel, as supplied, this will also be averaged out by the flipped type-0 orientation.

[0034] The net effect of flipped pair orientation is to average out production variations in peak critical current along the HTS tape. The advantages for translating a magnet design, which assumes uniform critical current along the tape, into a real working magnet are clear.

[0035] However, it should be noted that in some commercially available tapes, the c-axis 320 diverges by as much as 30-35 degrees from the perpendicular to the plane of the tape. The flipped pair orientation is less useful with these tapes, because the peak Ic becomes split into two peaks, both lower than the peak in the un-flipped arrangement of tape pairs. This is illustrated in FIG. 6D.

[0036] In addition, the use of the “flipped tape” construction results in a symmetrical distribution of current sharing within a magnet coil wound using the type-0 pairs and pushed close to critical current. FIG. 7A shows a chart of the ratio between current and critical current for a cross section of a pancake solenoid magnet coil constructed from a plurality of type-0 pairs according to the construction of FIG. 4, and FIG. 7B shows a chart of the ratio between current I and critical current Ic for a cross section of a magnet coil constructed from a plurality of type-0 pairs according to the construction of FIG. 5 (ie: the “flipped” orientation). Each coil is constructed from two spiral “pancake” windings of type-0 pairs, stacked on top of each other (i.e. one from z=0 to z=12, and one from z=0 to z=−12), with the x axis of all tapes being parallel to the axis of the magnet coil and the tape's z-axis oriented along the radius of the magnet coil. The ReBCO tape used has an angle between the c-axis and the perpendicular to the plane of the tape (z-axis) of 35 degrees. As can be seen from the Figures, the arrangement of FIG. 7B is symmetrical. This leads to symmetric heating due to current sharing, which is more desirable from the perspective of understanding coil performance.

[0037] While the above description has focussed on arrangements of type-0 pairs of HTS tapes, similar arrangements may be used for type-1 pairs (i.e. where the HTS layer of one tape faces the substrate layer of the other, such that one HTS layer is between the substrates and one is not) or type-2 pairs (i.e. where the substrate layers face each other, such that they are between the HTS layers), arranged such that the c-axes of the HTS tapes have reflective symmetry about a plane parallel to the HTS layers. Furthermore, the above disclosure may also be applied to cases where one or both tapes in a pair are “exfoliated” HTS tape, i.e. HTS tape without a substrate.