Patent Description:
High-field magnets are often constructed from superconductors due to the capability of superconductors to carry a high current without resistance. Such magnets may, for instance, carry currents greater than <NUM> kA. <CIT> and <CIT> each disclose a magnet according to the precharacterizing portion of claim <NUM>.

According to the present invention, there is provided a magnet characterized according to claim <NUM>.

In the drawings, identical or nearly identical components illustrated in various figures may be represented by a like numeral.

A high-field superconducting magnet often comprises multiple electrically insulated turns of a superconductor grouped in a multi-layer arrangement. When the superconductor is cooled below its critical temperature (the temperature below which the electrical resistivity of the material drops to zero), current may pass through the superconducting path without losses that would normally occur due to electrical resistance.

A superconducting magnet and/or systems to which it is coupled may include current paths made from a non-superconducting conductor (also referred to as a "normal conductor"). For instance, an interface between the superconductor in the magnet and a power supply may comprise a normal conductor. In other cases, there may be connections between regions of superconductor within the magnet to facilitate construction of the magnet. An interconnection to and/or within a superconducting magnet is sometimes referred to as a "joint. " The joint may comprise a normal conductor as in the example above, but in other cases may be an interconnection between neighboring regions of superconductor.

In general, it is desirable that joints in a superconducting magnet have a number of properties. First, the electrical resistivity of the joints should be as low as possible, since current flowing through the joints will cause joule heating of the joints and a superconducting magnet is operated at low temperatures. Second, the joint should be mechanically robust. During operation, a superconducting magnet can produce large forces within its structure (e.g., Lorentz forces), which can result in the application of forces (e.g., compressive forces) onto the joints as well as onto other portions of the structure. For this reason, joints in a superconducting magnet may be thought of as being 'electromechanical' structures rather than mere electrical conductors. Third, it is preferable that joints in a superconducting magnet are easy to manufacture. Fourth, it is preferable that the joints take up a relatively small amount of space (and ideally minimal space) in the superconducting magnet so that more space is available for inclusion of a superconductor within the magnet.

Conventional superconducting magnet joints generally rely on special preparation of the superconductor so that superconducting coils can be joined together. As noted above, it is desirable that joints have a low electrical resistance, so directly connecting different regions of superconductor is one way to meet this goal. Such approaches can, however, be extremely complex and error-prone to fabricate. For instance, neighboring regions of superconductor must be measured and cut so that they can be in intimate contact with one another when joined, while having identical contact resistance to ensure uniform current distribution within the joint. These approaches may also produce fixed assemblies once constructed - that is, once the neighboring regions of superconductor have been mounted onto one another, it may be difficult or impossible to demount the joint without damaging or destroying it.

The inventors have recognized and appreciated joint designs that utilize normal conductors (i.e., non-superconductors). The joint design may be implemented in a modular component of a superconducting magnet, such as a plate that includes a spiral superconducting path, with the joints described herein providing electrically conductive connections between the superconducting paths of adjacent modular components (e.g., between adjacent plates in a stack of plates). A joint may be installed and coupled to the component (e.g., plate) after its fabrication, thereby providing freedom in design of both the joint and the component. In at least some cases, the joints may be arranged to be flush with a surface of the component after installation into the component so that neighboring instances of the components may be stacked flush with one another, thereby putting joints from the neighboring components into intimate contact with one another. Moreover, this design may allow the components to be fabricated to comprise the joints prior to the components being coupled to one another, thereby allowing a flexible, modular and convenient fabrication process.

<FIG> is a cross-section of a portion of an illustrative plate suitable for use in a stacked-plate superconducting magnet, according to some embodiments. In the example of <FIG>, plate <NUM> comprises a baseplate material <NUM> in which a conducting path <NUM> is formed (e.g., via traditional machining processes, via additive and/or subtractive processes, etc.). To produce a magnet, a superconductor may be inserted into the conducting path of the baseplate <NUM>. The conducting path <NUM> may comprise channels, grooves and/or any other space into or onto which a superconductor may be provided.

In the example of <FIG>, the conducting path may be a curved path with successive turns of the path lying within the previous turns, such as but not limited to a spiral path or a plurality of concentric circular paths. An outer part of the conducting path is coupled to a joint <NUM>, which comprises or consists of a normal conductor such as copper. The joint <NUM> comprises a conducting path <NUM>, which is an interior space (e.g., a channel) within the joint into which the superconductor that is to be inserted into the conducting path <NUM> may also be inserted. As such, when the joint <NUM> is installed, disposed, or otherwise provided in the baseplate <NUM>, the conducting path <NUM> and conducting path <NUM> may be arranged adjacent to one another to form a continuous path. The superconductor may thereby be arranged within the path formed by the combination of conducting paths <NUM> and <NUM>.

According to some embodiments, adjacent instances of the plate <NUM> (or instances of a similar plate, examples of which are described below) may be arranged so that joints <NUM> of the plates electrically couple to one another. As a result, a superconductor within the conducting path <NUM> may be arranged in a plurality of turns within one plate, with one end of the superconductor electrically coupled to (e.g., terminating with) the joint <NUM>, which couples to a joint of another plate, which is coupled to another superconductor in that plate, etc. In this manner, a stack of plates <NUM> may be arranged with a plurality of regions of a superconductor to form a continuous current path through the stack, with the joints providing the current path across neighboring plates. In some embodiments, this current path may comprise an alternating sequence of inward and outward spirals, with each plate being configured with the conducting path being either an inward spiral path or an outward spiral path. In this case, the joint <NUM> may be arranged at an interior of the spiral or at an exterior of the spiral. In some embodiments, the plate <NUM> may include a joint <NUM> at an exterior of the conducting path <NUM> and a second joint at an interior of the conducting path, with the two joints being arranged to be exposed on opposing faces of the plate, thereby facilitating connections to neighboring plates at the exterior of the conducting path on one side of the plate and at the interior of the conducting path on the other side of the plate.

According to some embodiments, the baseplate <NUM> may comprise, or may consist of, a high mechanical strength material such as but not limited to steel, Inconel®, Nitronic® <NUM>, Nitronic® <NUM>, Incoloy®, or combinations thereof. In some embodiments, the baseplate <NUM> may be plated with a metal such as nickel to facilitate adhesion of other components to the plate, including solder as described below.

In the example of <FIG>, the conducting path <NUM> is shown as being at a first surface of the baseplate <NUM> (here illustrated as an exterior bottom surface of the baseplate <NUM>), though it will be appreciated that the current path may be arranged at any suitable location within the plate, including within the interior of the plate, and/or on the exterior top surface of the plate <NUM>.

According to some embodiments, the joint <NUM> may comprise, or may consist of, copper. In some embodiments, the joint may be mechanically coupled to the baseplate <NUM> via bolts or other fasteners. In some embodiments, the bolts may provide some amount of electrical coupling between the baseplate and the joint. Additionally, or alternatively, the joint may be coupled to the baseplate <NUM> via other means, such as by attaching the joint to the baseplate with a solder, brazing or welding the joint to the plate. A solder arranged between the joint and the baseplate and mechanically coupling the two together may also provide electrical coupling between the two. As such, electrical continuity between the plates may be increased by the addition of electrically conducting material around the joints, for example by soldering the perimeter of the joints.

The geometry of the joint <NUM> may, according to some embodiments, allow the joint <NUM> to be inserted into the baseplate <NUM> subsequent to the plate being fabricated. In this case, it may be advantageous to mechanically couple (i.e., removably couple) the joint to the plate rather than fixedly couple (e.g., via brazing or welding) the joint to the plate. In some embodiments, subsequent to installation of the joint <NUM> in the baseplate <NUM>, a molten solder may be introduced into the plate to fill any gaps between the joint and the plate. In some cases, the molder solder process may also be introduced into the conducting path <NUM> to fill any gaps between the baseplate <NUM> and a superconductor introduced into the path.

According to some embodiments, prior to its installation in the plate <NUM>, some or all of the joint <NUM> (e.g., the interior of conducting channel <NUM> and/or the exterior of the joint that will contact the baseplate <NUM>) may be pre-tinned with a metal (e.g., a PbSn solder, plated with silver, etc.) to promote a good bond (e.g. a mechanical and/or electrical connection) between the joint and a subsequently-deposited solder. The joint may be inserted into (or otherwise provided in) the plate and optionally secured to the plate (e.g., fastened to the plate via one or more mechanical fasteners such as via bolts). A conductive material may then be deposited into the groove in which the joint was inserted (or otherwise provided) via a vacuum pressure impregnation (VPI) process. Such a process may comprise one or more of the following steps: cleaning the empty space within the plate using an acidic solution following by a water rinse; evacuating space from within the plate; purging the space with an inert gas; depositing flux into the space to coat the joint <NUM>; draining any excess flux from the plate; heating at least part of the plate to a temperature below, at, or above a temperature at which the alloy to be deposited will melt; and flowing a molten alloy (e.g., a PbSn solder) into the plate.

According to some embodiments, baseplate <NUM> may comprise one or more through holes (i.e., one or more holes extending from a first surface of the plate to a second, opposite surface of the plate - not shown in <FIG>) for attaching the plate to other plates and/or other structures. In some cases, the through holes may comprise an interior thread to facilitate insertion of threaded mechanical fasteners such as screws or bolts into or through the plate.

According to some embodiments, baseplate <NUM> may comprise one or more cooling channels for delivering coolant to a superconductor arranged within the conducting channel <NUM>. The cooling channels may be arranged adjacent to the conducting channel <NUM> and/or may be arranged anywhere else within the plate <NUM>. In some cases, the joint <NUM> may have a geometry such that an empty region remains between the joint and the baseplate <NUM> after the joint is inserted into the baseplate. Such an empty region may be used as a cooling channel. The joint design described herein may thereby allow for flexibility in coolant channel design within the plates.

According to some embodiments, joint <NUM> may be machined to have a smooth upper surface - that is, the exposed surface that will contact another joint within another plate. A smooth surface may decrease contact resistance (i.e., may decrease electrical resistance between two mechanical structures in contact with each other). In this instance a smooth surface may decrease contact resistance between the joint <NUM> and the joint within the other plate, thereby leading to less Joule heating of the joints and/or nearby materials.

The example of <FIG> depicts a plate that may be suitable for use in a non-insulated (NI) magnet design (also referred to as a no-insulation (NI) magnet), in which adjacent superconducting turns of the magnet are not insulated from one another but are instead separated by a normal conductor (i.e., not a superconductor). In this instance, the normal conductor is the baseplate <NUM>. When the magnet is operating below the superconductor's critical temperature, current flows through the superconductor and not across turns because the superconductor has zero resistance compared with the finite resistance of the conductor that lies between the turns.

During a quench, however, at least one or more portions of the superconductor may be in a "normal" (non-superconducting) state (i.e., at least one or more portions of the superconductor have a finite resistance rather than a zero resistance which is characteristic of a superconductor). The at least one or more portions of the superconductor having a normal resistance are sometimes referred to as "normal zones" of the superconductor. When normal zones appear, at least some zero resistance current pathways are no longer present, causing the current to flow through the normal zones and/or between the turns, with the balance of current flow between these pathways depending on their relative resistances. By diverting at least some current from the superconducting material when it is normal in this manner, therefore, NI magnets, and in particular non-insulated high temperature superconductor (NI-HTS) magnets (NI magnets that comprise HTS), can in principle be passively protected against quench damage without the need to continuously monitor quench events and/or to actively engage external quench protection mechanisms.

<FIG> is a cross-section of a portion of an illustrative plate suitable for use in a stacked-plate superconducting magnet with an alternate joint design, according to some embodiments. <FIG> illustrates a plate <NUM> comprising the same baseplate <NUM> as in the example of <FIG> (and which also includes the same conducting path <NUM>), but with a joint <NUM> which has a different geometry to the joint <NUM> shown in <FIG>. But for the different geometry on the upper surface of the joint <NUM>, all of the above comments with respect to <FIG> also apply to <FIG>, with the conducting path <NUM> being a path within the joint <NUM> that may be arranged adjacent to the conducting path <NUM> just as for the conducting path <NUM> in the example of <FIG>.

According to some embodiments, the upper surface of the joint <NUM> may not be arranged flush with the upper surface of the baseplate <NUM> but may include a notch or other feature designed to mate with a complementary feature in the joint of a neighboring plate. In the example of <FIG>, for instance, the joint <NUM> includes a section that protrudes above the upper surface of the baseplate <NUM>, with the remainder of the joint being flush with the upper surface of the baseplate. Another plate may be fabricated that includes a joint with a section that is recessed below the upper surface of the baseplate <NUM>, with the remainder of the joint being flush with the upper surface of the baseplate. As a result, these joints may mate together when the plates are arranged adjacent to one another. The approach of <FIG> may increase or simplify alignment of adjacent plates and/or may provide for a more robust electrical connection between the two joints by increasing the contact area between the two plates, compared with the example of <FIG>. In some embodiments, the height of the protrusion of the joint <NUM> may be less than <NUM> inches (e.g., <NUM> inches) above the face of the joint <NUM>. It should be appreciated that the protruding portion may be provided having any regular or irregular geometric shape. The shape of the protruding portion may be selected to suit the needs of a particular application.

<FIG> is a cross-section of a portion of an illustrative plate suitable for use in a stacked-plate superconducting magnet with a second alternate joint design, according to some embodiments. <FIG> illustrates a plate <NUM> comprising a baseplate <NUM> in which conducting path <NUM> is formed. The baseplate also includes a channel into which joint <NUM> is inserted. Joint <NUM> includes a conductive channel <NUM> and is mechanically coupled to the baseplate <NUM> via bolts <NUM>. The joint <NUM> thereby includes through holes for the bolts and the baseplate <NUM> includes holes aligned with the through holes in the joint for insertion of the bolts.

The above comments with respect to <FIG> may also apply to the example of <FIG> with respect to joint <NUM>, baseplate <NUM>, conducting path <NUM> and conducting path <NUM>; and joint <NUM>, baseplate <NUM>, conducting path <NUM> and conducting path <NUM>, respectively. In the example of <FIG> it may be noted, however, that the conducting paths <NUM> and <NUM> are arranged at the uppermost surface of the baseplate <NUM> and joint <NUM>, respectively. This positioning of the paths within the baseplate and the joint may simplify the insertion of superconductor into the paths compared with the examples of <FIG>, since in <FIG> the paths are exposed at the top of the plate after installation of the joint into the baseplate.

<FIG> is a cross-section of two illustrative plates in a stacked-plate superconducting magnet, according to some embodiments. The example of <FIG> depicts a magnet <NUM> comprising plate <NUM> shown in <FIG> in contact with a second plate <NUM>, which includes conducting path <NUM> within baseplate <NUM>, and joint <NUM> which comprises conducting path <NUM>. As with conducting paths <NUM> and <NUM> in the example of plate <NUM>, the conducting path <NUM> in joint <NUM> may be arranged to be adjacent to the conducting path <NUM>.

According to some embodiments, a first superconductor may be arranged within conducting paths <NUM> and <NUM>, and a second superconductor arranged within conducting paths <NUM> and <NUM>. As a result, during operation at temperatures where the superconductor is superconducting, a current path of the magnet <NUM> may flow along the first superconductor, through the joint <NUM> to the joint <NUM>, then along the second superconductor. The joints <NUM> and <NUM> may be arranged at an interior end or exterior end of the plates within the magnet and, as discussed above, additional joints may be arranged at the opposing end of the plates irrespective of whether the depicted joints in <FIG> are arranged at the exterior or interior end of the plates.

According to some embodiments, a metal layer may be arranged between the joints <NUM> and <NUM> to facilitate intimate electrical contact between the joints. The metal may for instance be a soft metal configured to be compressed and conform to the surfaces of the joints during assembly of the magnet. In some embodiments, the metal layer may comprise, or may consist of, indium.

<FIG> is a cross-section of neighboring joints in a stacked plate superconducting magnet, according to some embodiments. The example of <FIG> depicts an alternate design for the base plate and joint and includes clamps that fasten multiple plates together. Magnet <NUM> includes plate <NUM> and plate <NUM>. The plate <NUM> includes a baseplate <NUM> of which two portions are shown in the cross-section of <FIG>, and the plate <NUM> includes a baseplate <NUM> of which two portions are shown in the cross-section of <FIG>. Plate <NUM> includes a joint <NUM> in which a conducting channel <NUM> is arranged. Plate <NUM> includes a joint <NUM> in which a conducting channel <NUM> is arranged. The plates <NUM> and <NUM> also include clamps <NUM> and <NUM>, respectively, wherein bolts <NUM> and <NUM> pass through the clamps to attach the plates <NUM> and <NUM> to one another. As noted above, bolts may be fully or partially threaded to mate with threads provided in one or both of plates <NUM>,<NUM> or threaded to mate with a nut.

According to some embodiments, each plate of magnet <NUM> may be assembled by inserting the joint into the baseplate, and optionally mechanically attaching the joint to the baseplate (e.g., as in the example of <FIG> described above). Superconductor may subsequently be inserted into the conducting path of the baseplate (these paths are not shown in the example of <FIG>), and into the conducting path of each joint (e.g., path <NUM> or <NUM>). Optionally, solder may subsequently be deposited into the conducting paths of the baseplate and joint, such as with a VPI process as described above. A stack of plates formed through this method may then be arranged and the plates coupled to one another through the clamps arranged between adjacent pairs of plates (or between more than two plates). Optionally, a layer of a soft metal such as indium may be arranged between the joints of neighboring plates in the stack so that when force is applied across the joint-joint interfaces by the clamps, the metal conforms to the interface and provides a good electrical contact between the joints.

For purposes of illustration, <FIG> depicts the stacked plates shown in <FIG> with a superconductor provided within the conducting channels of the joints <NUM> and <NUM> (visible in <FIG>). In particular, in the conducting paths are arranged an HTS material <NUM>, a cap <NUM> and an intervening conductive material <NUM> which provides electrical and thermal contact between the HTS material <NUM> and cap <NUM>.

In the example of <FIG>, the HTS material is provided as a co-wound stack of HTS tape. According to some embodiments, the HTS <NUM> may comprise a rare earth barium copper oxide superconductor (REBCO), such as yttrium barium copper oxide (YBCO). In embodiments, the HTS tape may comprise a long, thin strand of HTS material. In embodiments, the strand of HTS material may be provided having cross-sectional dimensions in the range of about <NUM> to about <NUM> in thickness (or height) and a width in the range of about <NUM> to about <NUM> (and with a length that extends into and out of the page in the example of <FIG>). According to some embodiments, each strand of HTS tape may comprise an HTS material such as REBCO in addition to an electrically conductive material (referred to as a co-wind). In some embodiments, the electrically conductive material may be disposed on the REBCO. In some embodiments, the electrically conductive material may be a cladding material such as copper. In some embodiments, HTS tape may comprise a polycrystalline HTS and/or may have a high level of grain alignment.

According to some embodiments, cap <NUM> may comprise, or may consist of, copper. According to some embodiments, conductive material <NUM> may comprise a Pb and/or Sn solder. In some embodiments, conductive material <NUM> may comprise a metal having a melting point of less than <NUM>, wherein at least <NUM> wt% of the metal is Pb and/or Sn, and at least <NUM> wt% of the metal is Cu. In some embodiments, the conductive material <NUM> may be a solder introduced into the plates via a VPI process as discussed above.

<FIG> is a cross-section of neighboring joints in a superconducting magnet, according to some embodiments. <FIG> depicts an alternate design to that shown in <FIG> and <FIG> that includes cooling channels, joint mounting bolts and a chamfer and drain to aid in a VPI process that introduces solder into the plates.

Magnet <NUM> includes plate <NUM> and plate <NUM>. The plate <NUM> includes a baseplate <NUM> of which two portions are shown in the cross-section of <FIG>, and the plate <NUM> includes a baseplate <NUM> of which two portions are shown in the cross-section of <FIG>. Plates <NUM> and <NUM> include joints <NUM> and <NUM> respectively, in which a superconductor <NUM> is arranged within channels therein. The plates <NUM> and <NUM> also include clamps <NUM> and <NUM>, respectively, wherein bolts <NUM> and <NUM> pass through the clamps to attach the plates <NUM> and <NUM> to one another. A layer <NUM> of a soft metal such an indium is arranged between the joints. A soft metal layer between the joints may produce a high degree of contact between the joints (e.g., may fill in any imperfections in the surface of either or both joints to ensure the surfaces are flush), and may also allow for the joints to be disassembled and reassembled easily. In some embodiments, the thickness (e.g., vertical direction in <FIG>) of the combination of joint <NUM> and clamp <NUM> may be equal to, or approximately equal to, the thickness of baseplate <NUM>.

In the example of <FIG>, the joints <NUM> and <NUM> are configured so that cooling channels <NUM> are provided between the joints and their respective base plates (and in the case of plate <NUM>, additionally between the joint and the clamp <NUM>). As shown, the geometries of the baseplates and joints may be selected so as to leave a suitable channel for a coolant between those elements.

In the example of <FIG>, joint mounting bolts <NUM> and <NUM> are included which mount joint <NUM> to baseplate <NUM> and joint <NUM> to baseplate <NUM>, respectively. In the example of <FIG>, the joints <NUM> and <NUM> may have portions shaped to form or otherwise provide drain regions <NUM> and <NUM> respectively. In this example, joints <NUM>, <NUM> have a chamfer shape potion which define (or form) drain region <NUM>, <NUM>. Joints <NUM> and <NUM> may, of course, also be provided having other shapes (i.e., portions having shapes other than a chamfer shape) which may define drain regions <NUM>, <NUM>. In some embodiments, the drain region <NUM> may be arranged to catch excess solder and/or flux that may flow over the surface of a plate during a solder deposition process (e.g., the VPI process described above).

<FIG> and <FIG> depict top perspective views of a baseplate for a stacked-plate superconducting magnet, according to some embodiments. In the example of <FIG>, the baseplate only is shown, whereas in <FIG> the same baseplate with joints and a superconductor arranged within the baseplate is shown.

As shown in <FIG>, baseplate <NUM> includes grooves or pockets <NUM> and <NUM> into which joints may be inserted. The baseplate also includes mounting locations <NUM> and <NUM> for securing the joints to the baseplate (e.g., the mounting locations may comprise threaded or non-threaded holes for bolts).

<FIG> depicts the baseplate <NUM> subsequent to inserting joints <NUM> and <NUM> into the baseplate, in addition to superconductor <NUM>. In the example of <FIG>, the joint <NUM> is arranged to have an exposed upper conductive surface (e.g., as in the portion of the plate <NUM> shown in <FIG>), whereas the joint <NUM> is arranged to have an exposed lower conductive surface (e.g., as in the portion of the plate <NUM> shown in <FIG>). The joint <NUM>, as shown in <FIG>, includes bolts <NUM> that secure the joint to the baseplate <NUM>, holes <NUM> for a joint clamp to affix the plate to another plate in the magnet, and grooves or pockets <NUM> for clamps to be inserted to affix the plate to another plate.

<FIG> is a cross-section of a superconducting magnet comprising a plurality of plates each comprising joints at inner and outer sides, according to some embodiments. To further illustrate how the joint design described above may be implemented in a superconducting magnet, <FIG> depicts magnet <NUM> comprising a number of plates that each include an inner joint and an outer joint. In <FIG>, the uppermost and lowermost plates are cropped but it will be appreciated that the illustrated arrangement could be repeated for as many plates as desired or necessary. In magnet <NUM>, each plate includes four turns of a superconductor <NUM>, and each pair of adjacent plates are clamped together with clamps <NUM> at either the inner end or the outer end, with the position of the clamps alternating with each successive pair of plates as shown. A layer of insulating material <NUM> is arranged between adjacent plates except for the region where the joints contact one another (although it will be appreciated that such a layer of insulating material may not be a required feature, as the example of <FIG> for instance does not include such a layer). As shown in <FIG>, this insulating layer may be provided between adjacent clamps in each pair of clamps.

Since, in the example of <FIG>, the joint design recesses the clamps into the joint, the thickness of the joint plus the clamp is the same (or approximately the same) as the average thickness of a plate itself. As a result, all of the inner joints may be arranged over one another and all of the outer joints may be arranged over one another as shown in <FIG>. Consequently, the magnet <NUM> may be formed from only two unique plates (e.g., a so-called A plate and a B plate) where adjacent instances of these plates meet at an inner joint and at an outer joint. This arrangement can be repeated because the plates can nest together since, as noted above, the thickness of the joint plus clamp may be the same (or approximately the same) as the average thickness of a plate. Thus, the joint design techniques described herein enable one to make a magnet comprising a relatively small number of unique plates (in this example only two unique plates are required). The joint design described herein also enables one to make a magnet comprising relatively few total joint locations and thus a small (and ideally minimal) overall volume of the magnet is devoted to joint volume. Thus, the joint design described herein results in a magnet which is relatively simple to assemble (since there are relatively few unique plates) and has a relatively small volume taken up by the joints connecting the magnet plates.

<FIG> is a cross-section of a superconducting magnet comprising a plurality of plates mirrored around a central plane, according to some embodiments. In some cases, plates comprising joints as described above may be arranged in a stack that is mirrored around a midplane. Such a stack may include four types of plates, with two types of plates being arranged in an alternating fashion on either side of the midplane.

As shown in the example of <FIG>, a stack of plates <NUM> (also referred to as "winding pack") comprises a plurality of plates mechanically and electrically coupled to one another via the joint coupling techniques described above. As shown, each plate within stack <NUM> is coupled to adjacent plates via an inner joint and an outer joint. As shown in <FIG>, the stack <NUM> includes repeated alternating instances of plates <NUM> and <NUM> beneath the midplane, and repeated alternating instances of plates <NUM> and <NUM> above the midplane. In some embodiments, the plates <NUM> and <NUM> may be mirror images of plates <NUM> and <NUM>, respectively.

As with the example of <FIG>, in <FIG> the joint design recesses the clamps into the j oint, the thickness of the joint plus the clamp is the same (or approximately the same) as the average thickness of a plate itself. As a result, all of the inner joints may be arranged over one another and all of the outer joints may be arranged over one another. Also, as with <FIG>, the techniques illustrated in <FIG> allow one to make a winding pack comprising a relatively small number of unique plates (in this example only four unique plates are required). The joint design described herein also enables one to make a winding pack comprising relatively few total joint locations and thus a small (and ideally minimal) overall volume of the winding pack is devoted to joint volume. Thus, the joint design described herein results in a winding pack which is relatively simple to assemble (since there are relatively few unique plates) and has a relatively small volume taken up by the joints connecting the winding pack plates.

In the example of <FIG>, a malleable conductive metal (e.g., indium) may be disposed between the plates to provide good electrical connections between the plates in the winding pack. In this particular example, it is preferable that the malleable metal (e.g., the indium) be highly compressed. Suitable compression may be achieved via the joints described herein (e.g., via bolts to pull together clamps (e.g., steel clamps) around the indium).

<FIG> is a three-dimensional graphic of a fusion power plant with a cutaway portion illustrating various components of the power plant, according to some embodiments. A magnet within a fusion power plant may be formed from a superconductor arrangement as described above. <FIG> shows a cross-section through a power plant and includes a magnet coil <NUM>, which is fabricated from, or otherwise includes, a superconducting magnet comprising a stack of plates as discussed and described above, a neutron shield <NUM>, and a core region <NUM>. According to some embodiments, the magnet coil <NUM> may be, or may form part of, a toroidal field coil. Magnet coil <NUM> may be fabricated from, or otherwise includes, a superconducting magnet comprising a stack of plates as discussed and described above. According to some embodiments, the magnet coil <NUM> may be, or may form part of a central solenoid and/or other poloidal field solenoidal coils.

Persons having ordinary skill in the art may appreciate other embodiments of the concepts, results, and techniques disclosed herein. It is appreciated that superconducting coils configured according to the concepts and techniques described herein may be useful for a wide variety of applications, including any application in which superconducting material is wound into a coil to form a magnet. For instance, one such application is conducting nuclear magnetic resonance (NMR) research into, for example, solid state physics, physiology, or proteins, for which superconducting coils may be wound into a magnet. Another application is performing clinical magnetic resonance imaging (MRI) for medical scanning of an organism or a portion thereof, for which compact, high-field magnets are needed. Yet another application is high-field MRI, for which large bore solenoids are required. Still another application is for performing magnetic research in physics, chemistry, and materials science. Further applications are in magnets for particle accelerators for materials processing or interrogation; electrical power generators; medical accelerators for proton therapy, radiation therapy, and radiation generation generally; superconducting energy storage; magnetohydrodynamic (MHD) electrical generators; and material separation, such as mining, semiconductor fabrication, and recycling. It is appreciated that the above list of applications is not exhaustive, and there are further applications to which the concepts, processes, and techniques disclosed herein may be put without deviating from their scope.

As used herein, a "high temperature superconductor" or "HTS" refers to a material that has a critical temperature above <NUM>, wherein the critical temperature refers to the temperature below which the electrical resistivity of the material drops to zero.

Claim 1:
A magnet (<NUM>; <NUM>; <NUM>; <NUM>; <NUM>) comprising:
a plurality of plates arranged in a stack that includes a first plate (<NUM>; <NUM>; <NUM>; <NUM>; <NUM>) and a second plate (<NUM>; <NUM>; <NUM>), the first plate comprising:
a first conducting path (<NUM>), at least part of the first conducting path being a spiral path, the first conducting path comprising a high temperature superconductor, HTS, material; and
a first conductive joint (<NUM>; <NUM>; <NUM>; <NUM>) arranged interior to, or exterior to, the spiral path of the first conducting path, the first conductive joint being electrically coupled to the HTS material of the first conducting path, and
the second plate (<NUM>) being arranged next to the first plate in the stack and comprising:
a second conducting path (<NUM>) comprising the HTS material; and
a second conductive joint (<NUM>; <NUM>; <NUM>) arranged adjacent to and electrically coupled to the first conductive joint, the second conductive joint being electrically coupled to the HTS material of the second conducting path,
characterized in that the HTS material comprises a stack of HTS tapes (<NUM>).