Partial insulation superconducting magnet

Abstract

The present invention is a superconducting partial insulation magnet and a method for providing the same. The magnet includes a coil with a non-insulated superconducting wire winding wound around a bobbin. The coil has a first wire layer, a second wire layer substantially surrounding the first layer, and a first layer of insulating material disposed between the first wire layer and the second wire layer. Each wire layer comprises a plurality of turns, and the first layer of insulating material substantially insulates the second wire layer from the first wire layer.

Claims

1. A superconducting partial insulation magnet, comprising: a bobbin; and a coil comprising a non-insulated superconducting wire winding wound around the bobbin, comprising: a first wire layer; a second wire layer substantially adjacent to and substantially surrounding the first layer; and a layer of insulating material disposed between the first wire layer and the second wire layer, wherein each wire layer comprises a plurality of turns of the wire around the bobbin, and the layer of insulating material substantially insulates the second wire layer from the first wire layer.

2. The magnet of claim 1, wherein the superconducting wire winding comprises a core of superconducting material clad in a conducting stabilizing material.

3. The magnet of claim 2, wherein the stabilizing material comprises copper.

4. The magnet of claim 2, wherein the superconducting material comprises at least one of the group of NbTi, MgB2, and Nb3Sn.

5. The magnet of claim 1, wherein the first wire layer is substantially adjacent to the bobbin.

6. The magnet of claim 1, wherein the superconducting wire comprises NbTi wire.

7. The magnet of claim 6, wherein the NbTi wire comprises NbTi tape.

8. The magnet of claim 1, further comprising a third wire layer substantially surrounded by the first layer.

9. A method of forming a superconducting magnet comprising a plurality of partially insulated coils, comprising the steps of: winding a first wire layer comprising a first plurality of turns of a non-insulated wire around a bobbin; winding a second wire layer comprising a second plurality of turns of the non-insulated wire around the first wire layer, applying a layer of insulating material around the second wire layer; and winding a third wire layer comprising a third plurality of turns of the non-insulated wire around the layer of insulating material, wherein the first layer is substantially adjacent to the second layer, the second layer substantially surrounds the first layer, and the third layer substantially surrounds the second layer.

10. The method of claim 9, wherein the superconducting wire winding comprises a core of superconducting material clad in a conducting stabilizing material.

11. The method of claim 10, wherein the stabilizing material is selected from the group consisting of copper, brass, silver, Cu—Ni alloy, and aluminum.

12. The method of claim 10, wherein the superconducting material comprises at least one of the group of NbTi, MgB2, and Nb3Sn.

13. The method claim 9, further comprising the step of winding a fourth wire layer comprising a fourth plurality of turns of the non-insulated wire around the third wire layer, wherein the fourth layer is substantially adjacent to the third layer, and the fourth layer substantially surrounds the third layer.

14. A superconducting partial insulation magnet, comprising: a bobbin; and a non-insulated superconducting wire winding, wound around the bobbin, comprising: a first wire layer substantially adjacent to the bobbin; a second wire layer substantially adjacent to the first layer and substantially surrounding the first layer; a third wire layer substantially surrounding the second layer; and a first layer of insulating material disposed between the second wire layer and the third wire layer, wherein each wire layer comprises a plurality of turns, and the first layer of insulating material substantially insulates the third wire layer from the second wire layer.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

(1) The accompanying drawings are included to provide a further understanding of the invention, and are incorporated in and constitute a part of this specification. The drawings illustrate embodiments of the invention and, together with the description, serve to explain the principals of the invention.

(2) FIG. 1 is a schematic drawing of a prior art magnet detailing an m-turn by n-layer (m×n) NI winding.

(3) FIG. 2 is a schematic drawing of a cross section of coil of a first embodiment of a partial insulation magnet.

(4) FIG. 3 is a schematic drawing of a cross section of coil of a second embodiment of a partial insulation magnet.

(5) FIG. 4A and FIG. 4B are a pair of graphs comparing test results for magnets with NI coils and INS coils.

(6) FIG. 5 is a flowchart of an exemplary method for forming a partial insulation superconducting magnet of FIGS. 2 and 3.

DETAILED DESCRIPTION

(7) Reference will now be made in detail to embodiments of the present invention, examples of which are illustrated in the accompanying drawings. Wherever possible, the same reference numbers are used in the drawings and the description to refer to the same or like parts.

(8) The following definitions are useful for interpreting terms applied to features of the embodiments disclosed herein, and are meant only to define elements within the disclosure. No limitations on terms used within the claims are intended, or should be derived, thereby. Terms used within the appended claims should only be limited by their customary meaning within the applicable arts.

(9) As used within this disclosure, a bobbin refers to a substantially rigid structure formed of a non-conducting material for supporting a coil. Coils may be in several configurations, for example, but not limited to a solenoid (cylindrical), a racetrack, or a saddle for dipole or multi-pole coils. The bobbin may include a first rim protruding radially outward from a first end of the cylindrical structure, and a second rim protruding radially outward from a second end of the cylindrical structure, where the distance between the first rim and the second rim defines the width of the bobbin. The top rim and bottom rim generally serve to contain a wire coil wound around the cylindrical outer surface of the bobbin.

(10) As used within this disclosure, a turn refers to a single winding of a single wire around a bobbin.

(11) As used within this disclosure, a wire layer refers to a plurality of turns substantially spanning the width of the bobbin. While turns of a layer are generally adjacent, they may be irregular due to the winding process, as understood by a person having ordinary skill in the art.

(12) As used within this disclosure, a coil refers to a single wire wound around a bobbin in a plurality of turns and layers.

(13) As used within this disclosure, an insulating layer is an insulating material that electrically isolates adjacent layers of a coil, other than the electrical current flowing through the spiral path of the wire coil between the adjacent layers.

(14) As mentioned previously, there is a need to mitigate the adverse effects of the NI technique especially for large magnetic resonance (MR) magnets. Typically, “large” may indicate a magnet having a winding bobbin diameter of 60 cm or greater. This disclosure presents exemplary embodiments of partial insulation (PI) magnets according to the current invention.

(15) As shown in FIG. 2, a first embodiment of a magnet 200 with PI winding is similar to the prior art NI magnet 100 of FIG. 1, in that a PI coil 205 has an m-turn by n-layer (m×n) array of windings 120. The core 130 of each winding 120 is formed of a superconductor material surrounded by a stabilizing cladding 140. As depicted in FIG. 2, the first embodiment includes a first (innermost) layer 271 of windings 120 as shown on the left, and a sixth (outermost) layer 276 of windings 120 shown on the right. The first layer 271 is wound adjacent to a bobbin 290. A second layer 272, a third layer 273, a fourth layer 274, and a fifth layer 275 are between the first layer 271 and the sixth layer 276. A first turn 261 is depicted on the top, followed by a second turn 262, a third turn 264, and a fourth turn 264, which is depicted on the bottom. The first turn 261 and the fourth turn 264 are adjacent to rims of the bobbin 290. The bobbin 290 has generally C shaped profile. In alternative embodiments, the bobbin 290 may be rimless.

(16) While the magnet 200 of FIG. 2 is depicted with the coil 250 having six layers 271-276 and four turns 261-264 of windings 120, other configurations of the coil 205 are possible, for example, a coil 205 with two, three, four, five, seven or more layers, and two, three, five, or more turns of windings 120.

(17) The first embodiment 200 has no insulation between adjacent turns 261-264. Similarly, there is no insulation between the first layer 271 and the second layer 272, no insulation between the third layer 273 and the fourth layer 272, and no insulation between the fifth layer 275 and the sixth layer 276. However, unlike the NI windings 120 (FIG. 1) of the prior art, there is a first layer of insulation 281 between the second layer 272 and the third layer 273, and a second layer of insulation 282 between the fourth layer 274 and the fifth layer 275. The insulation layers 281 and 282 electrically insulate surface leakage between adjacent layers. Therefore, PI refers to a coil with at least two adjacent layers having no insulation between them, and at least two adjacent layers having insulation between them. In a PI magnet, a group of two or more adjacent layers without insulation between them is called a sub-winding. In FIG. 2, the first layer 271 and the second layer 272 form a first sub-winding. Similarly, the third layer 273 and the fourth layer 274 form a second sub-winding, and the fifth layer 275 and the sixth layer 276 form a third sub-winding.

(18) While adjacent sub-windings are depicted as physically separated by insulation, they are connected by a contiguous winding 120. For example, the first sub-winding is connected to the second sub-winding by a contiguous winding 120, namely the egress winding 120 of the second layer 272 and the first turn 261, marked with a “−”, and the ingress winding 120 of the third layer 273 and the first turn 261, marked with a “+”.

(19) The coil 205 is wound with a contiguous winding 120, starting with the first layer 271 and first turn 261, both adjacent to the bobbin 290. Upon completing the first winding, the second turn 262 of the first layer 271 is wound. The third turn 263 is wound around the bobbin 290, followed by the fourth turn 264, thereby completing the first layer 271. The winding continues with the fourth turn 264 of the second layer 272, so that the fourth turn 264 of the second layer 272 is substantially adjacent to both the bobbin 290 and the fourth turn 264 of the first layer 271. The winding of the second layer 272 proceeds by the winding of the third turn 263, the second turn 262, and the first turn 261 of the second layer 272, such that the first turn 261 of the second layer 272 is substantially adjacent to the first turn 261 of the first layer 271.

(20) As noted above, the first layer 271 and the second layer 272 make up the first sub-winding. The first layer of insulation 281 substantially surrounds the first sub-winding. After the first layer of insulation 281 is applied to the first sub-winding, the winding of the second sub-layer commences in substantially the same manner, such that the second sub-layer is applied around the first sub-layer, with the second sub-layer consisting of the third layer 273 and the fourth layer 274.

(21) The second layer of insulation 282 substantially surrounds the second sub-winding. After the second layer of insulation 282 is applied to the second sub-winding, the winding of the third sub-layer commences in substantially the same manner, such that the third sub-layer is applied around the second sub-layer, with the third sub-layer consisting of the fifth layer 275 and the sixth layer 276. In alternative embodiments, additional sub-layers, for example, a fourth sub-layer and a fifth sub-layer, etc., may be wound around the bobbin 290.

(22) FIG. 2 shows a PI winding with an insulation layer 281, 282 between every two layers (PI2). FIG. 3 shows a second embodiment having insulation 380 between every third layer (PI3). In the third embodiment, there is no insulation between a first layer 371 and a second layer 372, the second layer 372 and a third layer 373, a fourth layer 374 and a fifth layer 375, and the fifth layer 375 and a sixth layer 376. A layer of insulation 380 is disposed between the third layer 373 and the fourth layer 374. A first sub-winding includes layers 371-373, and a second sub-winding includes layers 374-376. While FIG. 3 shows two sub-windings, alternative embodiments may have three, four or more sub-windings, where each sub-winding has three adjacent layers with no insulation between them, and adjacent sub-windings are physically separated by insulation.

(23) While the first embodiment (PI2) and the second embodiment (PI3) have substantially uniform sub-windings, alternative embodiments may have non-uniform sub-windings, for example, where adjacent sub-windings have unequal numbers of layers. A sub-winding may have only a single layer, or may have two, three, four, or more layers.

(24) Each sub-winding, electrically separated by insulation, may be modeled as an independent NI winding. Similarly, the total PI winding may be modeled as a group of the NI windings electrically connected in series. As a result, the inter-coil resistance R.sub.c of a PI winding is larger than that of its NI counterpart. This reduced inter-coil resistance R.sub.c of a PI winding helps to speed up charging time and reduce the ohmic loss. Note that, in FIG. 3, the PI3 sub-windings have the ingress current and the egress current on different rows in the resistor matrix. In contrast, PI2 sub-windings (FIG. 2) have the egress current and the ingress current for a sub-winding on the same rows. The PI3 has an increased R.sub.c compared with PI2, and thus much reduced charging time and ohmic loss. These issues are further discussed below.

(25) Insulation material used for partial insulation coils may include organic material, for example, polyimide films such as Kapton®, aramid polymers such as Nomex®, thermoplastic resins such as Fomvar®, polyester films such as Mylar®, or non-conducting metal, for example stainless steel. Insulation layers may be added, for example, by wrapping organic insulation tape or sheet insulation around a sub-coil, applying a liquid molding compound such as epoxy around the sub-coil, and wrapping the winding in an electrically non-conductive tape or sheet such as stainless steel.

(26) NI magnets provide enhanced stability and reduced weight in comparison with fully insulated magnets. Without losing the benefits provided by NI magnets, the PI technique provides a low cost feasible solution to the major technical challenges of the NI technique discussed above, namely, at least slow charging rate and extra ohmic loss under a time-varying operation. While particular focus has been placed on whole-body MRI and large bore NMR magnets, PI magnets may provide a significant solution for minimizing premature quenches in NbTi magnets, not just limited to MRI and NMR. PI magnets provide reduction of magnet price as well as installation cost and lead to better clinical MRI services for an MRI patient and to less expensive NMR devices for many laboratories.

(27) PI coils may be used not only in NMR and MRI magnets, but also superconducting magnets in general. For example, PI coils may be used in laboratory superconducting magnets, such as an accelerator, power devices, such as a motor, generator, and/or transformer, environmental devices, such as magnetic separation devices, and biomedical devices, such as a drug delivery magnet.

(28) Tests comparing NI coils with insulated (INS) coils indicate the advantages of NI coils over INS coils. Two test coils having 30-mm winding diameter were wound with INS and NI NbTi wires, where the winding inner diameter, height, and number of turns of the NI coil were identical to those of the INS coil. A charge-discharge test results and field analysis using a circuit model to indicated that the NI field performance was essentially identical to that of the INS except a for charging delay, and coil terminal voltage measurements during critical current tests indicate that the NI coil has better thermal stability than its INS counterpart.

(29) In a NI coil, current can flow through turn-to-turn contact in radial and axial directions as well as through the intended spiral path in azimuthal direction. This anisotropy of an NI coil may be equivalently modeled with three components: L.sub.coil (self inductance of the test coil), R.sub.θ (azimuthal resistance including index loss and matrix resistance of NbTi wire), and R.sub.c (characteristic resistance of the NI coil which originates mostly from radial and axial contact resistances). In a normal operation below the critical current of the coil, R.sub.θ must be zero (superconducting). When coil current is increased over the critical current, R.sub.θ starts increasing. After a test coil was placed in a bath of LHe, it was charged up to 30 A at a 10 A/min rate, held at 30 A for 30 s, and then discharged down to 0 at a rate of □10 A/min. During the test, coil terminal voltage, power supply current, and center field were measured.

(30) The fields from the NI and INS coils are almost identical except for a small charging delay of the NI coil. However, stability testing indicated more divergent results. The NI test coil and the INS test coil were each charged at a 10 A/min rate up to its critical current, 46 A for the NI coil and 50 A for the INS coil, and their terminal voltage was measured simultaneously. The results are shown in FIG. 4A and FIG. 4B.

(31) The graph in FIG. 4A shows the NI coil terminal voltages, while the graph in FIG. 4B shows the INS coil terminal voltages. As seen in the graphs, the NI voltage is much quieter than the INS voltage under the same power supply and measurement system setup. More importantly, significantly less voltage spikes were observed from the NI coil than from the INS coil, where a time scale of the voltage spikes ranged 1-10 ms. This is a typical disturbance in LTS magnets by wire motion.

(32) Assuming that a single turn in the NI coil shares copper stabilizer of its neighbor turns, the respective enthalpy margins of the NI and INS coils are respectively calculated as 31 and 18 mJ/cm3 at the Iop/Ic of 0.1 and as 3.6 and 1.8 mJ/cm3 at the Iop/Ic of 0.7. The enthalpy margin of the NI coil is twice that of the INS coil, which may explain the more stable charging voltages of the NI coil. The quieter terminal voltages with a much smaller number of voltage spikes indicate that the NI coil is more stable than its INS counterpart.

(33) FIG. 5 is a flowchart of an exemplary method for forming a partial insulation superconducting magnet. It should be noted that any process descriptions or blocks in flowcharts should be understood as representing modules, segments, portions of code, or steps that include one or more instructions for implementing specific logical functions in the process, and alternative implementations are included within the scope of the present invention in which functions may be executed out of order from that shown or discussed, including substantially concurrently or in reverse order, depending on the functionality involved, as would be understood by those reasonably skilled in the art of the present invention.

(34) FIG. 5 is a flowchart of an exemplary method 500 of forming a superconducting magnet with a plurality of partially insulated coils. A first wire layer including a first plurality of turns of a non-insulated superconducting wire is wound around a bobbin, as shown by block 510. The superconducting wire winding has a core of superconducting material clad in a conducting stabilizing material. The core may be formed from one or a combination of two or more of several superconducting materials, for example, but not limited to, NbTi, MgB2, and Nb3 Sn. The stabilizing material may be, for example, but not limited to, copper or a copper alloy. A second wire layer including a second plurality of turns of the non-insulated wire is wound around the first wire layer, as shown by block 520. A layer of insulating material is applied around the second wire layer, as shown by block 530. A third wire layer including a third plurality of turns of the non-insulated wire is wound around the layer of insulating material, as shown by block 540. The first layer is substantially adjacent to the second layer, the second layer substantially surrounds the first layer, and the third layer substantially surrounds the second layer.

(35) In summary, PI coils may provide many of the advantages that NI coils have demonstrated over INS coils, while mitigating the delay charge and ohmic loss in the winding. It will be apparent to those skilled in the art that various modifications and variations can be made to the structure of the present invention without departing from the scope or spirit of the invention. In view of the foregoing, it is intended that the present invention cover modifications and variations of this invention provided they fall within the scope of the following claims and their equivalents.