Patent Grant
11094439
As is known in the art, existing approaches for fabrication of high-field superconducting magnetics include: (1) low temperature superconductor (LTS) cable-in-conduit conductor (CICC) designs, such as is being employed for ITER's toroidal field magnetics; and (2) high temperature superconductor (HTS) designs based upon HTS tapes wound directly into layer-wound coils or spiral-wound “pancake” coil assemblies. CICC-like approaches based upon HTS conductors are also being pursued.
In the CICC approach, a conduit is electrically insulated from a winding pack. Coolant is constrained to flow inside of a conduit. The shape of the winding pack and an external support shell define a shape of the electrical current pathway and coolant pathway. For the example of the ITER toroidal field coils, the winding pack and an external support shell are provided having a D-shape. The winding pack and external shell structures are primarily responsible for containing Lorentz forces generated by the high-field magnets (i.e. the winding pack and shell must support the Lorentz loads). In the case of a magnet quench event (which must be detected reliably and with enough lead time to mitigate damage via external protection systems), the stored magnetic energy is dumped into external resistors at the magnet terminals. Thus, current in the CICC bypasses normal zones in the superconductor, flowing instead into a copper stabilizer.
The need to have a copper stabilizer and a coolant channel in the conduit, combined with the need for high voltage electrical insulation, complicates the magnet design since these elements are structurally weak, yet they occupy significant volume in the winding pack. Additionally, the fabrication process for CICC-based magnetics is long and arduous involving many steps, including: cabling of the strands/tapes, jacketing these sub-elements together, and bending and inserting the CICC into a winding pack.
This Summary is provided to introduce a selection of concepts in simplified form that are further described below in the Detailed Description. This Summary is not intended to identify key or essential features or combinations of the claimed subject matter, nor is it intended to be used to limit the scope of the claimed subject matter.
Described herein are concepts, systems, structures and techniques which provide a means to construct robust high-field superconducting magnets using fabrication techniques which are relatively simple compared with prior art fabrication techniques and modular components that scale well toward commercialization. The resulting magnet assembly—which utilizes non-insulated, high temperature superconducting tapes (HTS) and provides for enhanced (and ideally, optimized) coolant pathways—is inherently strong structurally. This enables a high degree of utilization (and ideally, maximum utilization) of the high magnetic fields available with HTS tape technology. In addition, the concepts described herein provide for control of quench-induced current distributions within a tape stack and surrounding superstructure to safely dissipate quench energy, while at the same time obtaining acceptable magnet charge time. The net result is a structurally and thermally robust, high-field magnet assembly that is passively protected against quench fault conditions.
In embodiments, the concepts described may facilitate commercialization of high-field magnets for use in fusion power plants (e.g. compact fusion power plants) as well as in high-energy physics applications. However, after reading the description provided herein, one of ordinary skill in the art will readily appreciate that the disclosed concepts are generally applicable for use in a wide range of other applications (e.g. a wide range of industrial uses) which may make use of high-field magnets. Such applications include but are not limited to: applications in the medical and life sciences field (e.g. magnetic resonance imaging and spectroscopy); applications in the chemistry, biochemistry and biology fields (e.g. nuclear magnetic resonance (NMR), NMR spectroscopy, electron paramagnetic resonance (EPR), and Fourier-transform ion cyclotron resonance (FT-ICR)); applications in particle accelerators and detectors (e.g., for use in health care applications such as in instruments for radiotherapy); applications in devices for generation and control of hot hydrogen plasmas; applications in the area of transportation; applications in the area of power generation and conversion; applications in heavy industry; applications in weapons and defense; and applications in the area of high energy particle physics.
In accordance with one aspect of the concepts describe herein, a high-field magnet assembly includes a plurality of electrically conductive plates with each of the plurality of electrically conductive plates having spiral-grooves provided therein with said plurality of electrically conductive plates disposed (e.g. stacked) to form a monolithic pancake assembly having a first outermost surface and a second, opposing outermost surface. The high-field magnet assembly further includes a non-insulated (NI) HTS tape stack disposed in a channel formed by the grooves of said first and second electrically conductive plates. In embodiments, the HTS stack may include co-wind materials which may comprise one or a combination of non-insulated, insulated or semiconducting materials. In embodiments, the channel may be suitably sized to contain more than one stack, with separate structures placed between stacks that can optionally engage with the plates mechanically. The channel has a first opening on the first outermost surface of the pancake assembly and a second opening on the second, opposite outermost surface of the pancake assembly. The NI HTS tape (and co-wind stack, when included) is continuously disposed in the channel such that the NI HTS tape (and co-wind stack) forms a path from the first outer-most surface of the pancake assembly to the second, opposite outer-most surface of the pancake assembly.
In embodiments a pair of spiral-grooved plates (e.g. a top plate and a bottom plate) are stacked to form a monolithic double-pancake assembly.
In embodiments, two identical spiral-grooved plates are assembled back-to-back with an insulating material inserted or otherwise disposed therebetween. One or more HTS tape stacks with co-wind are disposed into the groove which executes an in-going spiral on the top plate, a helix down to the bottom plate, and an out-going spiral on the bottom plate.
In embodiments, the high-field magnet assembly can include co-wind materials and surface coatings selected to provide a desired (and ideally, an optimized) magnet quench behavior.
In embodiments, the high-field magnet assembly can include spiral-grooved plates provided from a composite of base materials and surface coatings (electrically insulating, electrically conducting and/or electrically semiconducting) selected to provide a desired (and ideally, an optimized) magnet quench behavior.
In embodiments, a bladder element can also be included in the tape stack to preload the stack prior to soldering or to eliminate the need for soldering.
In embodiments, a bladder element can be filled with a material that is liquid during assembly but is solid at magnet operating temperatures. The heat of fusion associated with this material can act a large thermal reservoir to protect the HTS during a quench event.
In embodiments, a copper spiral cap can be soldered or otherwise coupled or secured to the tape bundle to help facilitate heat removal to coolant channel plates, which are stacked on top of the spirals.
In embodiments, grooves can be cut in the copper spiral cap and top surface of the baseplate, along and/or across the path of the spiral winding, to facilitate coolant passageways.
In embodiments, a copper interconnection between in-going and out-going spiral-grooved pancakes may be used. This can be employed at both the inside diameter (ID) and outside diameter (OD) of each spiral-groove winding plate. In this case, a magnet assembly may be constructed by simply stacking a series of spiral-grooved, HTS-loaded plates against each other, interleaved with coolant channel plates and/or using coolant channel grooves cut into the surfaces of the plates as described above.
In embodiments, the HTS and co-wind stack is embedded in a matrix of copper or other high electrical conductance material at the point at which it enters and exits the spiral-grooved winding plate and at the point at which the stack transitions from one spiral-grooved winding plate to another. This serves to protect against overheating and damage of the HTS during magnet charging and magnet quench conditions.
In another aspect of the concepts described herein, a stacked-plate magnet assembly comprises a first plate, a second plate disposed over the first plate, an electrically insulating material disposed between the first and second plate, and one or more HTS tape stacks that each may include co-wind materials (electrically conducting, electrically insulating and/or semiconducting). The first plate is provided having at least one spiral-shaped groove provided therein. The second plate is also provided having at least one spiral groove provided therein such that when a first surface of the first plate is disposed over a first surface of the second plate, said grooves form a channel having an in-going spiral shape on the first plate, a helix down to the second (or bottom) plate, and an out-going spiral on the bottom plate. The electrically insulating material is disposed between the first and second plates. The HTS tape stack(s) with co-wind is disposed in the channel to this provide the winding having a spiral shape. It should be appreciated that while the winding will be generally spiral-shaped, the magnet core may be provided having a D-shape, a solenoid shape, a circular shape or any other shapes suitable for the application in which it will be used. Similarly, the helical channel can be deformed into the shape needed to facilitate a continuous channel that allows the HTS tape stack to pass from the first plate to the second plate. After reading the description provided herein, one of ordinary skill in the art will appreciate how to select a winding and magnet shapes appropriate for the needs of a particular application.
In an embodiment, the grooves in the first and second plates are substantially identical. The first and second plates can also have substantially identical spiral-shaped grooves and can be assembled back-to-back.
The channel forms an in-going spiral on the top plate, a helix down to the bottom plate, and an out-going spiral on the bottom plate. The HTS tape stack(s) that may include co-wind materials can be inserted into the grooved channel. The co-wind materials and surface coatings can be selected to optimize magnet quench behavior.
In embodiments, a bladder element can be included as a co-wind material in the HTS tape stack. The bladder element can be configured in the HTS tape stack to preload the HTS tape stack prior to soldering. In embodiments, the bladder element can also be configured in the HTS tape stack to eliminate the need for soldering. The bladder element can also be configured to pre-compress the HTS tape stack against a load-bearing sidewall of at least one spiral groove.
In embodiments, the bladder element can be filled with a material that is liquid during assembly but is solid at magnet operating temperatures. One such material includes, but is not limited to, gallium. The heat of fusion associated with this material can act a large thermal reservoir to limit the temperature rise of the HTS during a quench event.
In embodiments, the number, size and type of HTS tapes in the stacks with optional co-wind materials can be varied according to location along the spiral pathway, if desired, such as to save cost and/or to optimize magnet quench response.
The magnet can further comprise at least one coolant channel. In embodiments, at least one coolant channel may be provided in one or both of the first and second plates. In embodiments, the coolant channel can comprise one or more coolant pathways that run along the HTS tape stack. In other embodiments, at least one coolant channel can comprise one or more cooling channel plates interleaved with one or both of the first plate and second plate or interleaved in a stack of such plates that may comprise a magnet assembly. In such embodiments, the coolant channel path need not run along the HTS tape stack. In some embodiments, coolant channels are formed by cutting grooves in the surfaces of the plates, including a copper cap that is placed over the HTS tape stack. Such coolant channel grooves need not run along the HTS tape stack.
The magnet can also comprise an electrically conductive plate disposed between the first and second plates or interleaved in a stack of such plates that may comprise a magnet assembly. The electrically conductive plate may be provided from any electrically conductive material including, but not limited to, copper. The electrically conductive plate may also be provided from a thermally conductive material and may be configured to provide conduction cooling.
Additionally, the magnet can comprise one or more electrical interconnections between the first and second plates with such one or more electrical interconnections configured to establish and maintain a high electrical resistance in some areas in order to minimize the flow of bypass currents between each of the winding plates during magnet charging.
In another aspect, a method for constructing a high-field magnet comprises assembling a series of HTS-loaded spiral-grooved plates, stacked between coolant channel plates; and forming one or more inter-pancake electrical connections, each of the one or more inter-pancake connections having a low electrical resistance characteristic. Forming one or more inter-pancake connections can comprise forming one or more inter-pancake connections automatically.
The method can further comprise pre-loading HTS tape stacks in the spiral-grooved plates to eliminate a need for soldering.
In another aspect of the concepts described herein, a magnet assembly includes a first electrically conductive plate having a first surface with a plurality of grooves provided therein, the grooves defined by one or more walls with at least two grooves of the plurality of grooves having a different width and a non-insulated (NI) high temperature superconductor (HTS) tape stack having a length such that said NI HTS tape stack may be disposed in the plurality of grooves such that the NI HTS tape stack forms a continuous path between an outer-most groove in the first electrically conductive plate and an innermost groove of the first electrically conductive plate. In embodiments, the HTS tape is configured in each groove such that in response to generated forces, the HTS tape stack distributes forces into the first and second electrically conductive plates.
In embodiments, the magnet assembly further includes a second electrically conductive plate disposed over the first plate, such that when a first surface of the first plate is disposed over the first surface of the second plate, the grooves form a channel having an opening at a first end thereof and the HTS tape forms a continuous path between the first and second electrically conductive plates.
In embodiments, the HTS tape stack is disposed within one of the plurality of grooves of varying widths and is wound against itself to occupy the width of the groove.
In embodiments, the walls which define the grooves in the first electrically conductive plate are provided having a variable wall thickness such that a thickness of a first portion of a wall is different from a thickness of a second portion of the same wall.
In embodiments, the walls which define the grooves in the first electrically conductive plate are provided having different wall thickness.
In embodiments, a thickness of a first portion of a first wall in a first radial direction as measured from a center of the first electrically conductive plate differs from a thickness of a first portion of a second, different wall along the same first radial direction.
In embodiments, the first and second electrically conductive plates have substantially identical spiral-shaped grooves.
In embodiments, the NI HTS tape stack is comprised of two or more NI HTS tape stacks joined by a low resistance electrical connection.
In embodiments, the materials comprising the NI HTS tape stack in the first and second plates are continuous across the plates.
In embodiments, the NI HTS tape stack further comprises a co-wind material disposed in the groove such that the NI HTS tape and co-wind stack follows a path between a first outer-most groove of the first electrically conductive plate and an innermost groove of the first electrically conductive plate wherein the HTS tape and co-wind stack are configured in the grooves such that in response to generated forces, the HTS tape and co-wind stack distribute forces into the first and second electrically conductive plates.
In embodiments, the co-wind material is provided as one or more of: an electrically conducting material; an electrically insulating material and/or an electrically semiconducting material.
In embodiments, the co-wind materials are selected to optimize magnet quench behavior, or magnet charging behavior, or both.
In embodiments, the HTS tape and co-wind stack are embedded in a matrix of high electrical conductivity material at points where: the HTS tape and co-wind stack passes between stacked plates; the HTS tape and co-wind stack enters into and exit from the magnet assembly; and electrical interconnections are formed between windings.
In embodiments, the co-wind material varies in either composition or thickness along a length of the NI HTS tape stack.
In embodiments, an electrically insulating material is placed at selected areas between the stacked plates.
In embodiments, the NI HTS tape stack comprises one or more HTS tapes and the number, size and type of HTS tapes in said NI HTS tape stack varies along a length of said NI HTS tape stack.
In embodiments, the groove defines an in-going spiral on the first electrically conductive plate, the in-going spiral having a first end and a second end, and the first electrical plate has a helical opening provided therein, the helical opening having a first end and a second end with the first end of the helical opening coupled to the second end of the in-going spiral and a second end of the helical opening which leads to the to the second electrically conductive plate and coupled to a first end of an out-going spiral provided in said second electrically conductive plate.
In embodiments, a bladder element is included in the HTS tape stack. In embodiments, the bladder element is configured to pre-compress the HTS tape stack against a load-bearing sidewall of the at least one spiral groove. In embodiments, the bladder element contains a material that is liquid or gaseous during magnet assembly and solid or liquid or gaseous or evacuated during magnet operation. In embodiments, the bladder element contains a material that exhibits a phase change from solid to liquid and/or liquid to gas during magnet operation.
In embodiments, the first conductive plate has at least one coolant channel provided therein. In embodiments, the coolant channel comprises one or more coolant pathways disposed along said HTS tape stack. In embodiments, the at least one coolant channel comprises one or more cooling channel plates interleaved with one or both of the first plate and second electrically conductive plates. In embodiments, the at least one coolant channel comprises one or more coolant pathways disposed along a path that is different from that of the HTS tape stack.
In embodiments, a conducting plate may be inserted between the first and second electrically conductive plates.
In embodiments, high electrical conductivity coatings may be disposed on selected locations of at least one of the first and second electrically conductive plates.
In embodiments, the conducting plate comprises copper in whole or in part.
Some embodiments relate to an apparatus, comprising: an electrically conductive plate having a groove; and a high-temperature superconductor (HTS) tape stack disposed in the groove, the HTS tape stack having a spiral shape.
The groove may have a spiral shape.
The electrically conductive plate may comprise a metal or a metal alloy.
The apparatus may further comprise a coolant channel.
The coolant channel may be disposed in the groove.
The coolant channel may be disposed outside the groove.
The HTS tape stack may be a non-insulated HTS tape stack.
The HTS tape stack may comprise a plurality of turns, wherein the electrically conductive plate provides electrical connections between respective turns of the plurality of turns.
The apparatus may further comprise a shim or a bladder in the groove.
The electrically conductive plate may be a first electrically conductive plate, the groove may be a first groove, and the HTS tape stack may be a first HTS tape stack, and the apparatus may further comprise: a second electrically conductive plate having a second groove; and a second HTS tape stack disposed in the second groove, the second HTS tape stack having a spiral shape, wherein the first HTS tape stack is electrically coupled to the second HTS tape stack.
The first electrically conductive plate may be electrically insulated from the second electrically conductive plate.
The first and/or second electrically conductive plates have one or more alignment structures to align the first and second electrically conductive plates when the first and second electrically conductive plates are mated together.
The apparatus may further comprise a conductive connection between the first HTS tape stack and the second HTS tape stack.
The conductive connection may comprise a high temperature superconductor or a metal that is not a superconductor at a temperature above 30 degrees Kelvin.
The conductive connection may comprise copper.
The conductive connection may be formed between innermost turns of the first and second HTS tape stacks or between outermost turns of the first and second HTS tape stacks.
The first HTS tape stack and the second HTS tape stack may be a same HTS tape stack.
A transition between the first HTS tape stack and the second HTS tape stack may be formed by a helical portion of the same HTS tape stack.
The first groove may comprise at least first and second turns, wherein the first turn has a first width and the second turn has a second width, wherein the second width is greater than the first width.
The second turn of the groove may comprise a plurality of turns of the HTS tape stack.
The apparatus may comprise a magnet.
The HTS tape stack may comprise a rare-earth oxide.
The HTS tape stack may comprise comprises rare-earth barium copper oxide.
The apparatus may further comprise a conductive terminal block electrically coupled to the HTS tape stack.
Some embodiments relate to a fabrication method, comprising: forming an electrically conductive plate having a groove; and disposing a high-temperature superconductor (HTS) tape stack into the groove in a spiral shape.
The foregoing and other objects, features and advantages will be apparent from the following more particular description of the embodiments, as illustrated in the accompanying drawings in which like reference characters refer to the same parts throughout the different views. The drawings are not necessarily to scale, emphasis instead being placed upon illustrating the principles of the embodiments.
Described herein are concepts and techniques for providing a high-field magnet. Described herein are structures and techniques for the design and construction of high-field magnets having a relatively compact size and shape. The described concepts, structures and techniques provide a means to construct robust high field superconducting magnets using fabrication techniques which are relatively simple compared with prior art high-field magnet fabrication techniques. Furthermore, the described concepts, structures and techniques can utilize modular components that scale well toward commercialization. The described high-field magnet assemblies may utilize spiral-grooved stacked-plates and non-insulated, high temperature superconducting (HTS) tapes. Non-insulated tapes allow current to flow from turn to turn of the tape outside of the superconductor, and may be, but need not be, free of insulating material. Such an approach can result in magnet assemblies which are inherently strong structurally, which enables high (and ideally, maximum) utilization of the high magnetic fields available with HTS technology. Furthermore, the use of spiral-grooved stacked-plates and non-insulated, HTS tape stack(s) (or HTS tape and co-wind stack(s) with conducting, non-conducting and/or semiconducting materials) disposed within the spiral groove can allow for inclusion of coolant pathways, which in some cases may be optimized coolant pathways.
An HTS tape includes a HTS material. As used herein, the phrase “HTS materials” or “HTS superconductors” refers to superconducting materials having a critical temperature above 30 K at self field. Examples of HTS superconductors include rare-earth oxides, such rare-earth barium copper oxide (REBCO), but are not limited thereto.
An HTS self-wound pancake assembly is provided. The HTS tapes themselves (including an optional co-wind) in conjunction with the spiral grooved plate provide the mechanical strength needed to generate high magnetic fields. In embodiments, the spirals naturally favor a circular geometry. As a result of the HTS tapes themselves providing the requisite mechanical strength, such coils are easy to construct and are mechanically strong. For example, an 8 tesla double-pancake non-insulated (NI) HTS tape coil was designed, constructed and successfully operated in less than 6 months. In some embodiments, the NI HTS tape (and co-wind stack when used) forms a continuous path from the first outer-most surface of the pancake assembly to the second, opposite outer-most surface of the pancake assembly. It should, however, be appreciated that in some embodiments, the path of one material may be broken and not continuous. Thus, it should be appreciated that the grooved path is more or less continuous but the material disposed in the grooved path may not be.
The NI HTS pancakes are particularly interesting since they have a unique current sharing characteristic/phenomenon during magnet quench. Specifically, since the HTS tapes (or tape stacks) are not insulated or only partially insulated, joule heating may be distributed more or less uniformly throughout the winding. It is desirable to optimize and fully exploit this behavior by devising a robust, passively protected magnet design that can operate at high energy density. The spiral-grooved plate assembly configuration described herein can control the distribution quench-driven currents within the coil structure and reduce (and ideally, minimize) the magnitude and duration of current-sharing currents, and therefore joule heating and temperature rise, of the HTS tape stack itself. Furthermore, the current is electromagnetically coupled to the spiral-grooved plates and other surrounding structures which, by careful choice of magnet design, can further lead to uniform current distribution and reduced temperature rise due to joule heating since the magnetic field energy can be dissipated in a much larger volume of material compared with prior art techniques.
In addition, the described concepts, structures and techniques provide for control of quench-induced current distributions within an HTS tape stack and surrounding superstructure so as to safely dissipate quench energy, while at the same time obtaining acceptable magnet charge time. The net result is a structurally and thermally robust, high-field magnet assembly that is passively protected against quench fault conditions.
Although reference is sometimes made herein to the use of such high-field magnet assemblies in connection with fusion power plants (e.g. compact fusion power plants) and fusion research experiments (e.g. SPARC), such references are not intended to be, and should not be construed as, limiting. It is appreciated that high-field magnet assemblies provided in accordance with the concepts described herein find use in a wide variety of applications including, but not limited to applications in the area of high-energy physics, applications in the area of medical and life sciences, applications in the areas of chemistry, biochemistry and biology, applications in the areas of particle accelerators and detectors, applications in the area of devices for generation and control of hot hydrogen plasmas, applications in the area of transportation, applications in the area of power generation and conversion, applications in heavy industry, applications in weapons and defense, and applications in the area of high energy particle physics.
For example, in the medical and life sciences field, high-field magnets provided in accordance with the concepts described herein may find use in magnetic resonance imaging (MRI) and spectroscopy. In the chemistry, biochemistry and biology fields, high-field magnets provided in accordance with the concepts described herein may find use in nuclear magnetic resonance (NMR), NMR spectroscopy, electron paramagnetic resonance (EPR), and Fourier-transform ion cyclotron resonance (FT-ICR). In the area of particle accelerators and detectors, high-field magnets provided in accordance with the concepts described herein may find used in health care applications such as in instruments for radiotherapy and in charge particle beam delivery (e.g., from accelerator to target/patient). In the area of transportation, high-field magnets provided in accordance with the concepts described herein may find use in high power density motors, generators and MHD propulsion (e.g. electric aircraft, maglev trains, hyperloop concepts, railroad engines and transformers, marine propulsion and generators, and vehicles). In the area of utility and power applications, high-field magnets provided in accordance with the concepts described herein may find use in electromechanical machinery, power generation and power conversion systems (e.g. wind generators, transformers, synchronous condensers, utility generators such as those producing up to or greater than 300 MW, superconducting energy storage, and MHD energy generation). High-field magnets provided in accordance with the concepts described herein may find use in the area of heavy industrial applications (e.g., large industrial motors, magnetic separation, disposable mixing systems, induction heaters). In the area of weapons and defense applications, high-field magnets provided in accordance with the concepts described herein may find use in propulsion motors and generators, ElectroMagnetic Pulse (EMP) generation, directed energy weapon power supplies, and rail-guns/coil-guns.
Reference is sometimes made herein to one or more HTS tape stacks or HTS stack(s) and co-wind being disposed in a spiral groove or channel. It should be appreciated that as used herein, the term “HTS tape stack” includes a “stack” having multiple layers of HTS tape or only a single layer of HTS tape and possibly including one or more tapes made of non-HTS materials, which are herein referred to as being ‘co-wind’ tapes. The number, size and type of tape layers to use in any particular HTS tape stack are selected in accordance with the needs of a particular application. For example, in applications which only require a low current capability and can accept a high inductance characteristic, a single layer tape stack may be used. However, in high current/low inductance applications (e.g. compact fusion applications), an HTS tape stack provided from a single layer or a plurality of individual layers, up to many individual layers of HTS tape (e.g. in the range of 10-1000 layers, or more) may be used. In the case where are plurality of HTS tape layers are included in an HTS tape stack, the multiple layers of HTS tape are essentially coupled in parallel to provide a structure having an increased current carrying characteristic relative to a single HTS tape layer.
Referring now to
In general overview,
The co-wind materials and surface coatings can be chosen to provide a desired (and ideally, an optimized) magnet quench behavior. In embodiments, a bladder element can also be included in the tape stack to preload the stack prior to soldering or to eliminate the need for soldering. A copper (or other high thermal conductivity material) spiral cap (
The illustrative stacked-plate, double-pancake magnet assembly 100 (
Groove 125 is provided which may have at first a helical shape as it enters the plate and then a spiral shape within the plate. In this illustrative embodiment, the spiral is provided as a curved spiral (i.e. a winding in a substantially continuous and radially widening or tightening curve either around a central point on a flat plane or about an axis so as to form a column). It should, of course, be appreciated that in other embodiments a spiral-like shape may be used (i.e. a winding in a generally widening or tightening path either around a central point on a flat plane or about an axis). As used herein, the term “spiral shape” includes “spiral-like” shapes. For example, in some embodiments, it may be desirable or necessary to utilize a rectangular spiral-like shape. In still other embodiments it may be desirable or necessary to utilize a triangular spiral-like shape. In still other embodiments it may be desirable or necessary to utilize an oval spiral-like shape. Other spiral-like shapes including geometrically irregular shapes may also be used. After reading the disclosure provided herein, those of ordinary skill in the art will appreciate how to select the particular spiral or spiral-like geometry/shape to use in a particular application. It should also be appreciated that the spiral or spiral-Ike groove may be provided having a constant pitch (i.e. the same pitch) or may be provided having a variable pitch. A variable pitch can provide significant design flexibility, for example, providing space between windings to accommodate coolant passageways between pancake plates, and/or increasing the strength of the pancake in certain areas while reducing total magnet weight and/or providing more uniform quench energy deposition.
The first plate 105 includes optional interface apertures 120a-N which are included in this illustrative embodiment to aid in securing the first plate 105 to a second plate (e.g., the second plate 110 of
As will become apparent from the description herein below, groove 125 (
In embodiments, the HTS tape stack is fed or otherwise disposed into an end of spiral groove 130 (i.e. so-called in-going spiral groove 130).
In the embodiment shown here, alignment pins 115a-N are used to interface with a second plate (e.g., plate 110 of
Referring briefly to
The mating faces of the two spiral-grooved plates may be partially electrically insulated from each other by application of an insulating coating and/or an insulating plate 140 (also depicted as 440 in
The second plate 110 has formed or otherwise provided therein grooves 135 which define an in-going channel 136 having a generally spiral shape. As noted above in conjunction with groove 125, it should be appreciated that although groove 135 is here shown having a generally curved spiral shape, other spiral shapes including but not limited to square, rectangular, triangular or oval shapes map also be used. In the embodiment shown here, one end of groove 135 connects to a helical channel, 137, which passes between plates 105 and 110.
When grooves in respective plates are mated together they may form a channel, such as in-going spiral channel 136. The in-going spiral channel 136 receives the HTS tape and co-wind stack (e.g., the HTS tape and co-wind stack 150 of
In some embodiments, the material surrounding the helical channel is chosen to have high thermal and electrical conductivity, and may be copper, for example. It should be appreciated that the concept accommodates considerable flexibility in the choice of materials in this region and the specific way in which the geometry of the helical channel is formed and supported mechanically and electrically.
In some embodiments, the HTS tape and co-wind stack is embedded in copper or an otherwise suitable high electrical conductivity material over an extended region that includes the point at which the HTS tape and co-wind stack enter and exit the channels on each of the spiral-grooved plates and extends, uninterrupted, outside the spiral-grooved plates to current feeder connections. This serves to protect the HTS from overheating and damage during magnet charging and magnet quench events.
Referring now to
Referring now to
In embodiments, the first and second plates 105, 110 may include or be formed from superalloys including, but not limited to Inconel 718, Hastelloy C276, as well as a wide variety of structural materials including, but not limited to stainless steels such as 316, and dispersion hardened copper alloys such as GRCop-84. In embodiments, it may be desirable to coat or otherwise dispose a material layer within the channels 130, 135. Such materials may include, but not be limited to electrodeposited solder to aid fabrication, semiconductor coatings, copper plating/coatings and/or ceramic coatings of a variety of thicknesses to control quench current distributions.
In some embodiments, channels 130, 135 and/or the entire plate assembly, 105, 110, can be formed via additive manufacturing technologies such as three-dimensional (3-D) printing. Such technologies have already demonstrated ability to fabricate structures of the sizes and shapes needed using super alloys such as Inconel 718, Inconel 625, as well as a wide variety of structural materials such as 316 stainless steel and the dispersion hardened copper alloy GRCop-84. Suffice it to say that a wide variety of additive manufacturing technologies can be used for fabrication using a wide variety of different materials.
Significantly, in embodiments, the HTS tape stack and co-wind 150 can be un-insulated, partially insulated and/or contain semiconducting materials.
The HTS tape stack may be composed entirely of HTS tapes or may include ‘co-wind’ tapes, that is, tapes made entirely of non-superconducting materials, interleaved and/or stacked separately on top of a stack of HTS tapes. Co-wind materials can be conducting, insulating or a semi-conducting with electrical properties chosen to be advantageous for optimizing quench behavior. Co-wind tapes may also include a ‘bladder’ as described further below. In some embodiments, the HTS tape stack 150 may be formed outside of the channel and then disposed in the channels. In other embodiments, elements of the HTS tape stack 150, including but not limited to the co-wind material, may formed directly into the channels 130, 155, such as via 3D printing techniques.
In some embodiments, the cross-sectional shape of the grooves in the first and second plates are may be substantially identical. In other embodiments, the cross-sectional shapes of the grooves in the first and second plates may be different (e.g. so as to accommodate features, such as structural elements, that may be unique to the plates).
Also, in some embodiments, the first and second plates can also have substantially identical spiral-shaped grooves and can be assembled back-to-back. i.e., with the grooves on opposing surfaces such that when the plates are assembled, the grooves form channels. In other embodiments, the spiral shape in each plate may differ.
In embodiments, the channel forms an in-going spiral on the top plate, a helix down to the bottom plate, and an out-going spiral on the bottom plate. The HTS tape stack and co-wind can be inserted into the channel. The co-wind materials and surface coatings can be selected to safely distribute magnet quench energy within the volume of the structure.
In some applications (for example a toroidal field coil for the proposed SPARC experiment), it may be necessary to remove heat generated from volumetric sources in the region of the tape stack (e.g., neutron-induced heating, copper junctions) to maintain operating temperature. The spiral-grooved, stacked-plate approach can readily accommodate this in a number of ways.
In this illustrative embodiment, plate 205a has width 233 of about 15 mm. The channels 230 have a depth of about 11 mm into the plate 205a. The channels also have a length 234 of about 9 mm. Inserted or otherwise disposed within the channels 230 is an HTS tape stack 250 having a width 231 of about 6 mm and a length 232 of about 8.33 mm. A shim 235, here having a wedge shape, is inserted or otherwise arranged into the groove 230 such that the HTS tape stack 250 is pressed against a sidewall of the groove. In this illustrative embodiment, one of the channels is formed or otherwise provided a distance 239 of about 4.25 mm from a surface of plate 205a. However, these dimensions are merely by way of illustration, as the structures described herein may have any of a variety of suitable dimensions.
In embodiments, the magnet assembly can further comprise one or more coolant channels. In embodiments, the one or more coolant channels may be provided in one or both of the first and second plates. In embodiments, the one or more coolant channels can comprise one or more coolant pathways disposed proximate the HTS tape stack. In other embodiments, the one or more coolant channels can comprise one or more cooling channel plates interleaved or otherwise dispersed between a plurality of plates which make up the high-field magnet assembly.
A coolant channel 215 is provided proximate the HTS tape stack 250. In this illustrative embodiment, the coolant channel 215 is positioned on top of the HTS tape stack 250 and is formed or otherwise defined by a thermally conductive member 210 having a C-shape (e.g., a C-shaped channel member 210). In this illustrative embodiment, the coolant channel is provided having an area of about 30 mm2. However, this is merely by way of illustration, as any suitable coolant channel area may be used. The thermally conductive member 210 may comprise one or more of: copper, copper alloy, and a high thermal conductivity material. The coolant channel 215 is covered or otherwise closed (or capped) using a cap 220 that is secured (e.g. welded or otherwise secured) onto the plate 205a. The cap 220 is configured to seal the HTS tape stack 250 and the coolant channel 215 within the grooves 230. In an embodiment, a tape stack having a length of about 8 mm may be provided from about 190 HTS tapes, each 6 mm wide. In embodiments, a superalloy (e.g. Hastelloy) may be used as a co-wind material to achieve the 8 mm length with a reduced number of HTS tapes.
In embodiments, a plurality of spiral grooved plates may be used and a method for constructing a high-field magnet comprises assembling a series of HTS-loaded spiral-grooved plates, stacked between coolant channel plates includes forming one or more inter-pancake electrical connections, each of the one or more inter-pancake connections having a low electrical resistance characteristic, such that the resultant joule heating can be accommodated by the coolant scheme. In embodiments, forming one or more inter-pancake connections can comprise forming one or more other inter-pancake connections automatically.
In the examples illustrated by
As noted above,
This ‘coolant channel plate’ concept provides significant flexibility for improvement of (and ideally, optimization of) coolant pathways. This may be a useful feature in some applications such as the SPARC toroidal field coil. Alternatively, a conduction-cooled plate can be used in place of the coolant channel plate or eliminated altogether, accommodating designs and applications that have low levels of internal volumetric heating.
In order to control quench dynamics and to help mitigate temperature rise of HTS tapes during a quench, conducting plates (e.g. copper) may be inserted between the double pancakes; one observation is that quench-induced eddy currents would be preferentially excited in these structures, localizing the magnetic stored energy deposition to regions that are thermally and electrically disconnected from the HTS tapes. Such structures are naturally accommodated by the spiral-grooved, stacked-plate design concept; they may be incorporated directly into the coolant channel plate design, which is electrically isolated from the pancakes and in good thermal contact with the coolant.
In order to control quench dynamics and to help mitigate temperature rise of HTS tapes during a quench, high electrical conductivity coatings (e.g. copper) and/or insulating coatings (e.g. alumina) may be applied to selected areas of the spiral-grooved plates, including but not limited to, the grooved side of the plate and the non-grooved side of the plate; one observation is that the quench-induced current density, distribution and resultant joule heating can be controlled by tailoring the resistance of key electrical pathways in the magnet structure.
This stacked-plate geometry also naturally accommodates copper interconnections between pancakes, if desired, as shown in
It may be advantageous to preload the tape stack in the groove prior to soldering or to employ a preloading mechanism that eliminates the need for soldering altogether.
In an embodiment in which the coolant assembly 340 is a coolant channel between plates 330, 335, the coolant path established by the channel is not constrained to flow along the HTS stack and can therefore be optimized for heat removal. For example, short radial pathways across the HTS stacks can be used, spreading heat more effectively across turns. This can be useful for applications in which high levels of internal volumetric heating of the magnet windings may occur (e.g. toroidal field magnet for SPARC). In addition, multiple coolant loops can be employed, reducing coolant velocity and drive pressure requirements. Finally, coolant passageways can have variable size and may be implemented only where they are needed, setting aside more volume in the winding pack for structural elements. In embodiments that have lower levels of internal volumetric heating, a conduction-cooling approach may be adequate. In this case, the coolant channel plate can be replaced with a conduction-cooled plate or even eliminated.
To control quench dynamics and to help mitigate temperature rise of the HTS tape stack 305 during a quench, conducting plates (e.g. copper) may be inserted between the plates 330, 335 in the coolant channel region 340. Accordingly, quench-induced eddy currents would be preferentially excited in the conducting plates, localizing magnetic stored energy dissipation to regions that are thermally and electrically disconnected from the HTS tape 305.
Spiral grooves 420 are provided in the plates 430, 435. An HTS tape stack which may include co-wind materials 405 is inserted into the grooves 420 and a cap assembly 410 (which may be provided, for example, as a copper cap assembly) is disposed on top of the HTS tape stack and co-wind 405.
A bladder element 415 (or more simply bladder 415) is disposed in the groove (or channel) to compresses the stack 405 against a sidewall 411 of the groove 420. In embodiments, the bladder 415 can be a hydraulic bladder in which hydraulic fluid can be applied to provide the compression. In some embodiments, the bladder 415 is positioned such that the tape stack 405 is compressed against the primary load-bearing sidewall. In this example, tape stack is provided having a width 412 of about 4 mm a length 413 of about 4.5 mm and the direction of primary load (i.e. the primary Lorentz force (l×B) load) in
In embodiments, a bladder element can be included as a co-wind element in the HTS tape stack (i.e. as part of the HTS tape stack). The bladder element can be configured in the HTS tape stack to preload the HTS tape stack prior to soldering so as to facilitate the soldering process by securing the HTS tape stack in a desired position. In embodiments, the bladder element can also be configured in the HTS tape stack to eliminate the need for soldering. The bladder element can also be configured to pre-compress the HTS tape stack against a load-bearing sidewall of the at least one spiral groove.
In some examples, after the HTS tape stack 405 is soldered, the hydraulic fluid can be removed and can further be replaced with an inert gas. In cases in which the bladder 415 is empty, the bladder acts as a spring to accommodate differential thermal shrinkage of the soldered HTS stack 405 relative to the grooved plates 430, 435 during magnet cool-down and warm-up periods to reduce a risk of HTS stack and co-wind delamination damage.
In other examples, if hydraulic fluid is retained, a compressive force on the HTS tape stack 405 may be maintained such that it is fully immobilized. The hydraulic fluid can be selected such that it will freeze at a magnet operating temperature, eliminating a need to actively maintain hydraulic pressure.
In some cases, the bladder element can contain (e.g. be filled with or otherwise have disposed therein) a material that is liquid during assembly but is solid at magnet operating temperatures. One such material includes, but is not limited to, gallium. The heat of fusion associated with this material can act a large thermal reservoir to limit the temperature rise of the tape stack 405 during a quench event, i.e., limit an HTS stack temperature to be no greater than a melt temperature of 29.8 degrees C. in the case of gallium.
In all of these embodiments, a choice of materials, coatings, conductors, semiconductors, and insulators in the assembly can be used to improve (and ideally, optimize) current sharing and eddy current pathways in response to a magnet quench event, safely distributing the magnet quench energy over a large volume.
Referring now to
The rate of volumetric heat generation in the spiral grooved plate due to quench currents can be quantified as θj2, where j is the current-sharing current density and η is the electrical resistivity of the material in which it flows. In
In overview,
In this embodiment, current flows into and out of each double pancake 605 at the top of
In this embodiment, feeders, generally denoted 620, are configured to send and receive coolant into the coolant channel plates 622a-622f that are located in the middle of the double pancake assemblies.
The first plate 705a includes an access 715a that is configured to receive an HTS tape stack 710a. The HTS tape stack 710a is fed into groove channels (e.g., grooves or channels 130 of
In some embodiments, the HTS tape and co-wind stack is embedded in copper or an otherwise suitable high electrical conductivity material over an extended region that includes the point at which the HTS tape and co-wind stack enter 715a and exit 715b the channels on each of the spiral-grooved plates and extends, uninterrupted, outside the spiral-grooved plates to current feeder connections. This serves to protect the HTS from overheating and damage during magnet charging and magnet quench events.
In some embodiments, more than one HTS tape stack may be disposed in the grooved channel with separate structures and/or co-wind materials disposed between tape stacks; the dimensions of the channel groove are appropriately modified to accommodate these materials and/or to engage them mechanically, such as via secondary spiral grooves. In some embodiments, some or all of the co-wind materials may be disposed to engage with the plate mechanically, such as via spiral grooves.
It should be noted that an internal electrical interconnect, perhaps taking the shape of a circular ring in this example case, could also be used on the outermost turns to connect between double-pancake assemblies.
It should be noted that if the double pancake embodiment of
It should be understood that coolant pathways shown in
In overview,
It is appreciated that the use of variable-width spiral grooves has several advantages. By varying the width of the grooves, an HTS stack (and co-wind) may be wound directly on itself a given number of times in each radial groove. Doing so allows fine control over the current density distribution in the winding, which can used to reduce magnetic field strength variation and concentration in the HTS tape due to self-fields. Under the assumption that the magnetic field will decrease in magnitude with increasing distance from the center of the assembly 800, it is appreciated that the HTS stack will be able to withstand a greater number of self-winds in each groove with increasing radial distance from the center of the assembly.
Moreover, the use of variable-width spiral grooves eliminates the need to cut (or otherwise form or provide) a “narrow groove” in the plate for the entire length of the HTS tape stack. For purposes of this disclosure, a groove is considered “narrow” when its depth is more than two times its width. Thus, using a plate having variable-width spiral grooves provided therein allows use of narrow HTS tape stacks without a need to use narrow grooves. The design also allows the coil and its structure to be optimized separately with respect to magnetic field generation, self-field experienced by HTS tapes, and mechanical loads, i.e. structural stiffness, locations for welds and fasteners, locations for coolant channels including channels between plates.
Referring now to
It is appreciated that the number of grooves (hence, the number of walls) in a variable-width spiral-grooved, stacked-plate, double-pancake magnet assembly may vary according to an intended use. It is also appreciated that the number of winds of HTS tape stack and/or co-wind within each groove likewise may vary according to the intended use. Thus,
Each wall 810, 812, 814, 816, and 818 may include cooling means as described above, or provide structural support against magnetic forces experienced by the HTS tape stack 806, or both.
Each of the walls 810, 812, 814, 816, and 818 may wind substantially around the magnet assembly 800 one or more times (or portions thereof). Furthermore, as may be most clearly seen in
The total width of a given wall along a given cross-section may be calculated as the sum of the radial extents of each of its portions appearing in the cross-section. This total width may or may not be equal for different walls in different embodiments, and the total width of a given wall may vary as a function of the angular position of the respective cross-section.
With reference now to
With reference to
A layer of the HTS tape stack 806 is indicated between the portion 812a and the portion 812b of the wall 812. As indicated above, the wall 812 wraps around the magnet assembly 800 more than once, and thus two portions 812a and 812b thereof appear in the particular cross-section A-A. The channel between these portions 812a and 812b is provided to permit a contiguous winding of a single HTS tape stack 806 between the large groove defined by walls 810 and 812a, and the large groove defined by walls 812b and 814a. Thus, it is appreciated that embodiments of the magnet assembly 800 may include a single, narrow stack but nevertheless enable a high inductance winding.
Following the above-described pattern, the portion 812b of the wall 812 abuts a layer 806d of the HTS tape stack 806. Six layers of the stack are wound against each other in the groove defined by the portion 812b and a portion 814a of the wall 814. A channel is provided between the portion 814a and a portion 814b of the same wall 814, through which is wound a layer of the HTS tape stack 806, appearing on the other side of the wall 814 as the layer 806e. Three layers of the stack are wound against each other in the groove defined by the portion 814b of the wall 814 and a portion 816a of the wall 816. A channel is provided between the portion 816a and a portion 816b of the same wall 816, through which is wound a layer of the HTS tape stack 806, appearing on the other side of the wall 816 as the layer 806f. Three layers of the stack are wound against each other in the groove defined by the portion 816b of the wall 816 and a portion 818a of the wall 818. A channel is provided between the portion 818a and a portion 818b of the same wall 818, through which is wound a layer of the HTS tape stack 806.
The innermost portion of the magnet assembly 800 may be occupied by a second, optional copper terminal block 820, as indicated in
Of particular note is that the portion 812a as shown in
Having an invariant total thickness may be advantageous in some embodiments; for example, to the extent that each portion 812a and 812b provides some structural support onto which magnetic forces are shunted, this structural support is uniform and does not vary according to the angular direction. However as explained above, in some embodiments the total thickness of the wall 812 may vary with the angular direction. Moreover, in some embodiments, the width of the tape stack may vary with distance along the stack, requiring the wall thicknesses to be adjusted accordingly.
Continuing radially inward with the description of
Three layers of the stack are wound against each other in the groove defined by the portion 814b of the wall 814 and a portion 816a of the wall 816. A channel is provided between the portion 816a and a portion 816b of the same wall 816, through which is wound a layer of the HTS tape stack 806, appearing on the other side of the wall 816 as the layer 806f. The portion 816a is thicker in
Three layers of the stack are wound against each other in the groove defined by the portion 816b of the wall 816 and a portion 818a of the wall 818. A channel is provided between the portion 818a and the copper terminal block 820, through which is wound a layer of the HTS tape stack 806. Note that the terminal block 820 may extend completely through the plate 802 to provide an external point of electrical contact. Of further note is that the wall 818 contains only a single portion 818a in the cross-section B-B illustrated in
Next are shown four layers of HTS tape stack 806 in the groove between the wall 810 and the outer portion 812a of the wall 812, including layers 806b and 806c. Below that is shown the layer of stack in the channel between the portions 812a and 812b of the wall 812.
Note that the portion 812a as shown in
Continuing radially inward (i.e. downward) with the description of
Three layers of the stack are wound against each other in the groove defined by the portion 814b of the wall 814 and a portion 816a of the wall 816. A channel is provided between the portion 816a and a portion 816b of the same wall 816, through which is wound a layer of the HTS tape stack 806, appearing on the other side of the wall 816 as the layer 806f. The portion 816a is thicker in
Three layers of the stack are wound against each other in the groove defined by the portion 816b of the wall 816 and a portion 818a of the wall 818. An inlay channel is provided between the portion 818a and the copper terminal block 820 (by material removed from the copper terminal block 820), through which is wound a layer of the HTS tape stack 806. Note that the terminal block 820 may extend completely through the plate 802 to provide an external point of electrical contact. Of further note is that the wall 818 contains only a single portion 818a in the cross-section C-C illustrated in
The inlaid conductive strip or plate 804 provides, among other things, a large contact area between the conductive terminals and the relatively low-conductance material that comprises the back plate 802, and between the HTS tape stack 806 and the conductive terminals. In embodiments, the conductive terminals are provided as copper terminals and the inlaid conductive strip 804 is provided as an inlaid copper strip 804. Use of such a conductive strip facilitates the attainment of a low joint resistance between HTS stack tape 806 and copper terminals.
This feature can be useful when the magnet is being charged and during off-normal events. The contact area is chosen to be large enough so as to ensure that the current density at the interface between copper and backplate material 802 is within acceptable limits (e.g. acceptable joule heating), both for the materials themselves and for the contact resistances between materials. This includes design consideration of potential damage from overheating during off-normal events and consideration of the joule heating distribution in the back plate 802 during charging and its impact on cooling requirements.
The copper plate 804 is deeper than the stack depth or height, to accept the stack and provide additional surface area along which to distribute local heating effects. Thus, for example, in
It should be understood that various embodiments of the concepts disclosed herein are described with reference to the related drawings. Alternative embodiments can be devised without departing from the scope of the broad concepts described herein. It is noted that various connections and positional relationships (e.g., over, below, adjacent, etc.) are set forth between elements in the following description and in the drawings. These connections and/or positional relationships, unless specified otherwise, can be direct or indirect, and the present invention is not intended to be limiting in this respect. Accordingly, a coupling of entities can refer to either a direct or an indirect coupling, and a positional relationship between entities can be a direct or indirect positional relationship. As an example of an indirect positional relationship, references in the present description to disposing a layer or element “A” over a layer or element “B” include situations in which one or more intermediate layers or elements (e.g., layer or element “C”) is between layer/element “A” and layer/element “B” as long as the relevant characteristics and functionalities of layer/element “A” and layer/element “B” are not substantially changed by the intermediate layer(s).
The following definitions and abbreviations are to be used for the interpretation of the claims and the specification. As used herein, the terms “comprises,” “comprising,” “includes,” “including,” “has,” “having,” “contains” or “containing,” or any other variation thereof, are intended to cover a non-exclusive inclusion. For example, a composition, a mixture, process, method, article, or apparatus that comprises a list of elements is not necessarily limited to only those elements but can include other elements not expressly listed or inherent to such composition, mixture, process, method, article, or apparatus.
Additionally, the term “exemplary” is used herein to mean “serving as an example, instance, or illustration.” Any embodiment or design described herein as “exemplary” is not necessarily to be construed as preferred or advantageous over other embodiments or designs. The terms “one or more” and “one or more” are understood to include any integer number greater than or equal to one, i.e. one, two, three, four, etc. The terms “a plurality” are understood to include any integer number greater than or equal to two, i.e. two, three, four, five, etc. The term “connection” can include an indirect “connection” and a direct “connection”.
References in the specification to “one embodiment,” “an embodiment,” “an example embodiment,” etc., indicate that the embodiment described can include a particular feature, structure, or characteristic, but every embodiment can include the particular feature, structure, or characteristic. Moreover, such phrases are not necessarily referring to the same embodiment. Further, when a particular feature, structure, or characteristic is described in connection with an embodiment, it is submitted that it is within the knowledge of one skilled in the art to affect such feature, structure, or characteristic in connection with other embodiments whether or not explicitly described.
For purposes of the description provided herein, the terms “upper,” “lower,” “right,” “left,” “vertical,” “horizontal,” “top,” “bottom,” and derivatives thereof shall relate to the described structures and methods, as oriented in the drawing figures. The terms “overlying,” “atop,” “on top,” “positioned on” or “positioned atop” mean that a first element, such as a first structure, is present on a second element, such as a second structure, where intervening elements such as an interface structure can be present between the first element and the second element. The term “direct contact” means that a first element, such as a first structure, and a second element, such as a second structure, are connected without any intermediary conducting, insulating or semiconductor layers at the interface of the two elements.
One skilled in the art will realize the concepts, structures, devices, and techniques described herein may be embodied in other specific forms without departing from the spirit or essential concepts or characteristics thereof. The foregoing embodiments are therefore to be considered in all respects illustrative rather than limiting of the broad concepts sought to be protected. The scope of the concepts is thus indicated by the appended claims, rather than by the foregoing description, and all changes that come within the meaning and range of equivalency of the claims are therefore intended to be embraced therein.
This application is a U.S. National Stage of International Application PCT/US2019/068332 filed in the English language on Dec. 23, 2019 and entitled “GROOVED, STACKED-PLATE SUPERCONDUCTING MAGNETS AND ELECTRICALLY CONDUCTIVE TERMINAL BLOCKS AND RELATED CONSTRUCTION TECHNIQUES,” and is a continuation-in-part of U.S. application Ser. No. 16/233,410 filed Dec. 27, 2018, and is a continuation of U.S. application Ser. No. 16/416,781 filed May 20, 2019, which is a continuation-in-part of U.S. application Ser. No. 16/233,410 filed Dec. 27, 2018. The contents of the above-referenced applications are hereby incorporated by reference as if fully set forth herein.
| Filing Document | Filing Date | Country | Kind |
|---|---|---|---|
| PCT/US2019/068332 | 12/23/2019 | WO | 00 |
| Publishing Document | Publishing Date | Country | Kind |
|---|---|---|---|
| WO2020/139832 | 7/2/2020 | WO | A |
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| Number | Date | Country | |
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| 20200402693 A1 | Dec 2020 | US |
| Number | Date | Country | |
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| Parent | 16416781 | May 2019 | US |
| Child | 16233410 | US |
| Number | Date | Country | |
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| Parent | 16233410 | Dec 2018 | US |
| Child | 16959600 | US | |
| Parent | 16233410 | Dec 2018 | US |
| Child | 16416781 | US |
