EP0350264A1 - Eine supraleitende abschreckgesicherte Spule - Google Patents

Eine supraleitende abschreckgesicherte Spule Download PDF

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Publication number
EP0350264A1
EP0350264A1 EP89306784A EP89306784A EP0350264A1 EP 0350264 A1 EP0350264 A1 EP 0350264A1 EP 89306784 A EP89306784 A EP 89306784A EP 89306784 A EP89306784 A EP 89306784A EP 0350264 A1 EP0350264 A1 EP 0350264A1
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EP
European Patent Office
Prior art keywords
wire
coil
superconductive
coils
magnet
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Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
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Application number
EP89306784A
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English (en)
French (fr)
Inventor
Evangelos Trifon Laskaris
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General Electric Co
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General Electric Co
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Publication of EP0350264A1 publication Critical patent/EP0350264A1/de
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    • H—ELECTRICITY
    • H01—ELECTRIC ELEMENTS
    • H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F6/00—Superconducting magnets; Superconducting coils
    • H01F6/02—Quenching; Protection arrangements during quenching

Definitions

  • the present European patent application is one of seven related European patent applications which are identified by title and applicants' reference in the following list: RD-18070 - CERAMIC SUPERCONDUCTOR CRYOGENIC CURRENT LEAD. RD-18204 - SUPERCONDUCTIVE MAGNETIC RESONANCE MAGNET. RD-18483 - COUPLING CRYOGENIC COOLER TO A BODY TO BE COOLED. RD-18522 - HEAT CONDUCTIVE, ELECTRICALLY INSULATIVE JOINTS. RD-18896 - SUPERCONDUCTIVE QUENCH PROTECTED COIL. RD-18897 - CABLE SUSPENSION SYSTEM FOR CYLINDRICAL VESSELS. RD-18898 - SUPPORTING A RADIATION SHIELD IN A MAGNETIC RESONANCE MAGNET.
  • the present invention relates to a superconduct­ive quench protected coil.
  • the coil may be a magnet.
  • the invention relates to example to protecting supercon­ductive windings during a quench event particularly in magnets used in magnetic resonance spectroscopy.
  • the superconductor wire When a magnet is operating in the supercon­ducting mode, current is carried in the superconductor wire without any heat dissipation since the supercon­ducting wire offers no resistance to the current flow.
  • the superconductor filaments are typically embedded in a copper matrix with all the current flowing in the superconductor filaments, while the filaments are superconducting.
  • a quench loss of superconduct­ivity
  • a portion of the superconducting wire becomes resistive and begins to heat due to electrical resistance losses.
  • the entire stored magnet energy will begin to be dissipated at just the one site at which the quench began, destroying the superconductor wire. If the quench can be quickly spread to the other coils the heat dissipation of the stored magnet energy can be accomplished over a larger volume avoiding damaging the coils. The coils can then survive the quench and the magnet is used again.
  • the speed at which a quench spreads from its origin depends on many factors including the elemental composition of superconductors used, its cross sectional shape and the amount of copper in the copper matrix. For example, in a coil of niobium titanium superconductor having a rectangular cross section and closely wound together, the propagation velocity of a quench can be three to ten times than in a magnet having epoxy impregnated coils of round niobium tin wire.
  • An embodiment of the present invention provides a quench protected superconductive coil which when used in a magnet can quickly spread the quench to all the magnet coils avoiding damage to the superconductive wire.
  • a further embodiment of the present invention provides a quench protected superconductive coil that is epoxy impregnated and does not require a high packing factor of superconductor wire to assure good quench propagation.
  • a quench protected superconductive coil having a plurality of layers of superconductive wire.
  • a strip of electrically conductive foil is located between superimposed layers of wire which enclose the inner layer. The ends of the foil are joined together to form an electrically conductive loop.
  • a quench protected coil having a length of superconductive wire which has a copper matrix and a length of insulated current conductive stabilizer wire.
  • the superconductive and stabilizer wire are co-wound to form a winding plurality of layers.
  • the co-wound wires are joined together with electrically conductive joints at the beginning and at the end of the winding and preferably at a plurality of intervals in between.
  • the magnets are designed to operate using a high temperature superconductor, namely niobium tin (Nb3Sn) in the present embodiments.
  • Nb3Sn niobium tin
  • the magnets are directly cooled by a highly reliable two stage cryocooler, based on the Gifford Mcmahon cycle.
  • the magnet geometry is arranged for the lowest possible peak magnetic flux density within the superconductor. This requirement is dictated by the intrin­sic field versus current capability of Nb3Sn superconductor at elevated temperatures of 9K or above.
  • a cylindrical magnetic resonance magnet 11 having an integral epoxy impregnated winding 13 in a shielded vacuum vessel 15 is shown.
  • the six windings 17, 18, 19, 20, 21, and 22 are wound in slots symmetrically situated about the axial midplane of a cylin­drical fiber reinforced form which in the present embodiment is a fiberglass form 25.
  • the cylindrical fiberglass form 25 is fabricated as a uniform thickness shell and then machined to provide cutouts for copper connectors which have axially and circumfer­entially extending portions 31 and 27, respectively.
  • the circumferential sections extend only partway around the coil form.
  • the copper connectors are used to join the six windings in series.
  • the copper connectors are bonded to the fiberglass form 25 using epoxy.
  • the fiberglass form is again machined with the copper connectors in place to provide six circumferentially extending winding slots with the circumferential portions of the connectors situated on either side of the slots.
  • ledges 33 are formed in the circumferentially extending copper connectors 27 at the bottom of the slot on one side and near the top of the slot on the other.
  • a superconductor wire 35 which comprises niobium tin superconductors in a copper matrix and a strand of stabilizer 37, which comprises insulated copper wire in the present embodiment, are cowound in the slots.
  • the Nb3Sn and copper wires are soldered to the ledge on the copper connector in the bottom of the slot to begin the winding and wound in layers separated by woven glass cloth 41 as shown in Figure 4.
  • the superconductor wire and stabilizer are preferably soldered together at every layer of the winding.
  • the insulation is removed from the stabilizer prior to soldering and the connection reinsulated using tape, for example.
  • the glass cloth is also used to line the slot prior to winding the coil also shown in Figure 4.
  • the windings in the slot terminate in a solder connection to the ledge 33 copper connector on the opposite side of the slot.
  • every few layers is a closed loop of copper foil 43.
  • the copper foil is separated from the layer of windings above and below it by glass cloth insulation.
  • the foil is overlapped and soldered so that it surrounds the winding, forming an electrically conductive loop. A portion of the loop is narrowed allowing the two wires being cowound to extend alongside the loop to begin the next layer.
  • the number of closed loops of copper used in any winding is determined by several factors such as the amount of space available, the quench protection needed and cost.
  • Axially extending copper connectors 31 couple adjacent circumferential copper connectors 27.
  • Co-winding with an insulated copper wire 37 controls the peak field and provides improved quench propagation.
  • Filler pieces 45 situated above the copper connectors are bonded to the copper connectors by epoxy to provide a constant radius outer circumference diameter.
  • the filler pieces can com­prise G-10, for example.
  • the wound coils are overwrapped with stainless steel wire 47 to provide additional support against the Lorenz forces which act on the coils when the magnet is at full field.
  • a ring 51 of heat conductive material such as stainless steel is bolted to the ends of the coil form 25.
  • the ring has a circumferential groove 53 which is aligned with axial slots in the fiberglass coil form shown in Figure 4.
  • the axial slots 55 extend the length of the coil form and are interconnected by circumferential slots 56 situated between windings on the form.
  • a high heat conductivity nonmagnetic material such as copper is rolled around in the exterior of the coil form to form a shell 57 which can be seen in Figures 2 and 3.
  • the shell is attached by overlap­ping and soldering the ends of the sheet together and by using high heat conductivity epoxy to secure the edges of the shell to the stainless steel rings 51.
  • Electrolytic tough pitch (ETP) copper is preferred for use in the shell because of its high low-temperature thermal conductivity and a thermal contraction closely matching that of the fiber­glass form 25.
  • ETP Electrolytic tough pitch
  • the surface to be bonded to the fiberglass form is treated with a commer­cial chromate chemical-conversion coating, such as Alodine® 1200 S a trademark of Amchem Products, Inc. Ambler, PA, or similar process such as sodium dichromate-sulfuric acid method, or chromic acid-sulfuric acid method, or alcohol-­phosphoric acid method, or anodizing, to obtain good bonding to epoxy adhesives.
  • Surface roughening, such as sand blasting or knurling may also be employed to further enhance bonding.
  • the preferred method of surface treatment for a copper shell is Ebonol® "C" special black cubric oxide coating, a trademark of Enthone, Inc., New Haven, CT.
  • Alternate methods include, ammonium persulfate process, or ferric chloride process, or hydrochloric acid-ferric chloride process, or sodium dichromate-sulfuric acid pro­cess.
  • Bus bars 61 and 63 are joined to the circumferen­tial connectors 27 on either end of the coil form by solder­ing or using an indium pressure joint.
  • the bus bars extend toward the midplane of coil on an insulator 64.
  • the com­plete assembly of coils, coil form, rings and shell is vacuum impregnated with epoxy. The impregnation can take place with the assembly standing on end and the epoxy introduced at the lower end through a fitting in the ring 51 (not shown).
  • the circumferential groove 53 in the ring 51 helps distribute the epoxy to all the axial channels 55 in the form. Additional circumferential grooves 56 help assure a good distribution of the epoxy throughout the interior of the windings and between the form 25 and the shell 57.
  • the magnet assembly is mounted inside the vacuum housing 15 surrounded by a radiation shield 65 which can be fabricated of copper or aluminum.
  • the bus bars in addition to carrying current between the coils provide a thermal bridge between the coils carrying heat generated during a quench from the interior of the resin impregnated coil to the adjacent coils increasing the speed at which the quench spreads to the other coils.
  • the coil form 25 is suspended in the shielded vacuum housing 15 by a radial and an axial cable suspension system.
  • the radial suspension which prevents radial movement of the coil form relative to the evacuable housing, has four cables 67, 68, 69 and 70 and eight cable tensioners arranged in pairs 73a and b, 75a and b, 77a and b, and 79a and b.
  • the cable tensioners are affixed to the exterior of the housing 15. At each end of the evacuable housing, two pair of cable tensioners are used with each pair of cable tensioners located circumferentially spaced on either side of where an imaginary diametral line passing through the end rings 51 emerges through the evacuable housing.
  • Each cable is attached at one end to a respective one of the cable tensioners in each pair and each cable extends through an aperture in the housing, through shield 65 and more than half way around the ring in a respective one of the grooves 81 in the outer surface of the rings. Each cable then passes through an opening in the shield and the housing and is secured to the other cable tensioner in the pair.
  • the cables can comprise 1/4" stainless steel wire rope or a 1/4" aramid fiber cable.
  • the cables terminate in a threaded rod 83 which is secured to the cable by, for example, a swagged fitting.
  • the cable tensioners comprise machined steel cable anchor extension which are welded to the steel housing.
  • the cable anchor exterior has two openings for receiving a pair of threaded rods at a prede­termined angle.
  • Belleville washers 85 and nuts 87 secure the cable end and maintain tension on the cables during cooling of the cables.
  • a counterbored hole can be provided in the housing at an appropriate angle and the cable secured directly against the housing.
  • An airtight cover 91 is welded in place over each pair of tensioners after magnet assembly so that the housing 15 remains air-­tight.
  • FIG. 6 the axial coil form suspension is shown.
  • four cables 93, 94, 95 and 96 each having one end formed in a loop have their looped ends encircling a respective one of four trunnions 97.
  • the trunnions are located directly opposite one another with two trunnions on either side of the coil form.
  • the trunnions on each side are symmetrically spaced axially about the axial midplane of the coil form and secured to the form.
  • the trunnions are located close to the axial midplane to limit movement of the trunnions relative to the housing when the magnet is cooled and the coil form contracts.
  • the cable looped about each trunnion extends axially away towards the closest end of the vacuum housing 15.
  • one or both ends of the cable turn radially outward about a pulley 101 mounted to the housing rather than extend through the housing ends.
  • the cable extends radially through an aperture in the housing to securing means.
  • the securing means comprises a tensioning bolt 103 about which the cable is wrapped and a "U-shaped" bracket 105 supporting the bolt from the housing.
  • a nut and lock nut 107 are located on the tensioning bolt to prevent the bolt from turning relative to the bracket.
  • Shield 65 is supported from the coil form by nine spacers affixed to the coil form and extending radially from the form.
  • Six spacers 111 are arranged in two groups of three equally circumferentially spaced radially outwardly extending spacers.
  • the spacers 111 each comprise a thin wall G-10 cylinders with a disc shaped plug 113 on one end and a plug 114 having exposed threads on the other.
  • the plugs which also can be fabricated from G-10 provide rigidity.
  • Spacers 111 are situated in holes extending through the coil form 25 in heat conductive sleeves 115.
  • the sleeves have a flanged end which is secured to the copper shell 57 of the coil form.
  • the other end of the sleeve extends radially inward and has an inner threaded aperture to receive the threaded end of plug 114.
  • the threaded disc shaped plug 114 has a slot 116 which extends to the spacer interior which serves to vent the spacer during evacuation of the magnet and to provide a screw driver slot to adjust the spacer radially outwardly from the form so that the end of the spacer having plug 113 extends beyond the coil form.
  • Spacers 111 keep the radiation shield 65 surrounding the coil form spaced away and not directly touching any portion of the form or shell 57.
  • Spacers 117 comprise a thin wall G-10 cylinder with a disc shaped plug 119 inserted at one end and a ring of insulating material 120 surrounding the other end.
  • the ring 120 has threads on its outside diameter.
  • the spacers 117 are located in apertures in the coil form.
  • the shell end of apertures are threaded.
  • the spacers 117 are threaded in place protruding radially inwardly from the coil form.
  • spacers 121 In addition to the nine radial spacers, four spacers 121, two on each axial end of the coil form are positioned in apertures to keep the ends of the shield from contacting the coil form. All the spacers 111, 117 and 121 by being situated in apertures and not contacting the coil form except at an end which is situated in the aperture, have a length greater than the distance between the coil form and the adjacent shield making the effective thermal path of the spacer greater than the distance between the coil form and the shield
  • the vacuum pressure impregnated fiberglass coil form is placed inside the vacuum housing which has both ends removed.
  • the four cables of the axial suspension system are looped around the trunnions.
  • the radiation shield which comprises an inner and outer cylinder and two end rings has the outer cylinder slipped over the coil form which for assembly convenience can be standing on end inside the housing which is also on one end.
  • Spacers 111 which are initially retracted almost flush with the coil form exterior are extended outwards using adjustment slots accessible from the interior of the coil form to adjust the spacing between the coil form and the outer cylinder of the radiation shield.
  • Spacers 117 protrude a fixed distance radially inwards from the coil form are not adjustable after initial installation.
  • Spacers 121 protrude from the ends of the coil form a fixed distance.
  • Spacers 117 and 121 normal­ly do not contact the shields but rather are a short dis­tance away to ease assembly and reduce thermal conduction paths. If the magnet is jarred, such as during shipping, spacers 117 and 121 prevent contact between the shield and coil form. Typically peak shipping acceleration above gravity is 1g in all directions. Since the magnet will be shipped with the coils superconducting, direct contact between shield and coil form should be avoided. With the axial suspension cables extending through the shield the shield end rings are bolted in place. Once the cable suspension are put in place and properly tensioned the ends of the shield can be bolted or welded in place.
  • spacers 117 and 121 act as bumpers to limit shield deflection spacers 111, 117 and 121 all must be designed for minimum heat leak in case of plastic deforma­tion of the shield or out of roundness of the shield.
  • the heat leak down a .01" thickness by 5/8 inch diameter tube from 50K, the nominal shield operating temper­ature, to 10K is 6 mW.
  • the 11 supports thus represent a total heat load of .066 W, which corresponds to a negligible increase in magnet operating temperature of 0.03 K.
  • This heat leak must be carried to the cooler by the copper shell surrounding the coil form, so the outward radial supports are attached to a copper sleeve which carries their heat leak to the shell.
  • the inner radial supports are threaded into the outer diameter of the coil form, so their heat will pass directly into the shell.
  • the axial supports are threaded into the metallic end rings on the coil form, so their heat is also carried directly to the copper shell.
  • a cryocooler 123 is positioned in a low field region in the midplane of the cylindrical assembly in a vertical service stack 125 which penetrates the outer vacuum vessel 15 and the thermal radiation shield 65.
  • the second and first heat stations are in intimate contact with shell 57 and shield 65, to maintain the temper­ature below 10°K and 50°K, respectively, by direct thermal conduction cooling.
  • the bus bars are heat stationed to the second heat station. Permanently connected leads extend down the service stack and are heat stationed at both heat stations and electrically connected to the bus bars 61 and 63.
  • a cryocooler cold head interface receptacle such as the one shown in copending application, Serial No. (RD-18,483) can be used in the embodiment of Figure 1 and is hereby incorporated by reference.
  • Cryostat vacuum envelope 15 is shown designed as a passive magnetic shield to contain the fringe 5 Gauss field of a 0.5T magnet within a cylindrical surface of 3m radius and 8m length as typically required to install the magnet in a standard hospital room with a 12 foot high ceiling.
  • the coils in Fig. 1 are wound with a bare Nb3Sn wire having a 0.018 inch diameter and an insulated copper wire also having a diameter of 0.018 inch.
  • the interlayer glass cloth insulation is 0.004 inch and the current flowing in the conductors is 58 amperes.
  • the 5 gauss line is 2.9 m. in the radial direction measured from the center of the bore and 4.0 m. measured axially from the center of the bore.
  • the inhomogeneity on the surface of 50 cm. diame­ter spherical volume centered in the bore is 65 ppm. and 15 ppm. on a 40 cm. diameter spherical volume centered in the bore.
  • superconductive magnet 131 with individually wound coils is shown.
  • Three coil pairs 135 and 136, 137, 138, and 139 and 140 are co-wound with bare Nb3Sn wire and a strand of stabilizer which comprises insulated copper wire in the embodiment of Figure 10.
  • the Nb3Sn and copper wire are electrically connected at least at the beginning and end of each coil.
  • the indi­vidually constructed coil windings with layers of insulation such as fiberglass cloth between layers are vacuum epoxy impregnated and all of the coils are made to have the same outside diameter by adjusting the fiberglass overwrap thickness on the outside of each superconductor coil.
  • a closed loop of copper foil is used every few layers, every third or fourth, for example, to provide quench protection as described previously.
  • the coils are assembled with cylindrical shell fiberglass spacers 143 to form a cylindri­cal subassembly with the coil pairs symmetrically situated in the axial direction about the midpoint of the cylindrical shell.
  • the coil to coil lead connections are made in axially extending grooves (not shown) on the outside of the spacers using copper bus bars, for example.
  • the cylindrical subassembly is machined to obtain a smooth cylindrical outside surface.
  • the subassembly is adhesively bonded inside a high thermal conductivity thermal shell 145 fab­ricated from high thermal conductivity copper or aluminum which encloses the sides and inner diameter of the winding.
  • Leads 147 and 149 extend from the windings at nearly the same circumferential location.
  • the leads are electrically insulated from the high thermal conductivity shell.
  • the coil subassembly, enclosed by the high thermal conductivity shell is positioned in a thermal radiation shield 151 which is spaced away from the coil subassembly.
  • the coils in the thermal shell are suspended in a vacuum housing by a radial and axial cable suspension similar to the suspension used to support the coil form in Figure 1.
  • Stainless steel rings 153 with a single circumferential groove in the outside surface are bolted to the copper shell 145.
  • Four cables 155, 156, 157 and 158 and eight cable tensioners 161a and b, 163a and b, 165a and b, 167a and b are again used.
  • the cable tensioners are positioned as previously described, however, the cables are connected differently. There are still two cables used at each end but each cable is connected between one of each of the pairs of cable tensioners that are closest cir­cumferentially. Each cable extends less than halfway around the ring in the circumferential groove.
  • the axial support is the same as previously described.
  • the shield 151 is sup­ported from the coil assembly at discrete locations as previously discussed.
  • a two stage Gifford McMahon cryocooler 123 is positioned in a low field region in the midplane of the cylindrical assembly in a vertical service stack 125 which penetrates the outer vacuum vessel 171 and the thermal radiation shield 151.
  • the second stage of the cryocooler which operates at approximately 9K is in intimate contact with the high thermal conductivity shell.
  • the first stage of the cooler which operates at about 50°K is in intimate contact with the thermal radiation shield 151.
  • the current through the magnet windings is 50 amperes.
  • the superconductive coils comprise a bare Nb3Sn wire with a diameter of 0.043 cm. cowound with an insulated copper wire also having a diameter of 0.043 cm.
  • the bare Nb3Sn wire has a single core with 1500 filaments 5 microns in diameter.
  • the copper to matrix ratio is 1.5.
  • the wire can be obtained, for example, from Intermagnetics General Corp., Guilderland, New York.
  • the interlayer insulation has a thickness of 0.010 cm.
  • the magnet load line is shown in Fig. 12 for a Nb3Sn wire diame­ter of 0.043 cm.
  • the expected inhomogeneity is 29 ppm at the surface of a 50 cm. diameter spherical volume centered in the bore of the magnet and 4 ppm at the surface of a 40 cm. diameter spherical volume centered in the bore of the magnet.
  • a hybrid superconductive/resistive magnet 179 suitable for use in a magnetic resonance imaging system is shown in Figures 13, 14 and 15.
  • Two epoxy-impregnated superconducting coils 181 and 183 are each supported by aluminum rings 185 which are shrunk fit on the outside surface of the epoxy-impregnated coils.
  • the two coils are spaced apart from one another and lie in parallel planes with their centers being on a line extending perpendicularly to the planes.
  • the aluminum rings 185 in addition to surrounding the outside surface of the coils cover the surfaces of the coils which face one another.
  • the coils are spaced apart by four solid aluminum posts 187 which are secured between portions of the aluminum rings covering the facing surfaces of the coils.
  • the coils and posts are surrounded by a thermal shield 191 which surrounds each of the posts and coils individually.
  • the coils and thermal shield are supported inside a vacuum enclosure 193 by three suspension posts 194.
  • Each suspension post comprises two concentric G-10 thin wall tubes 195 and 197 to support the windings.
  • the exterior of the tubes can be covered with aluminized mylar to reduce emissivity.
  • One end of inner tube 195 is in contact with an aluminum bracket 201 affixed to the aluminum ring 185.
  • the other end of the inner tube is supported in an aluminum cup 203 having a central aper­ture 205.
  • the cup is also affixed to one end of the second concentric tube 197.
  • the other end of the second concentric tube is suspended from a ring 207 which is supported by a third concentric tube 211 which surrounds the two concentric tubes 195 and 197.
  • the third concentric tube 211 in addi­tion to supporting the second concentric tube 197 also supports the thermal shield 191.
  • the other end of the third concentric tube is affixed by a ring 213 to the vacuum housing 193 which also individually surrounds the three concentric tube supports.
  • the inner and third tubes 195 and 211, respectively, in the supports are in compression while the second tube 197 is in tension.
  • the suspension posts are sufficiently flexible to accommodate the radial thermal con­traction of the shield and windings relative to the vacuum enclosure during cool down.
  • the vacuum enclosure housing 193 and radiation shield 191 are each fabricated as transversely split toroids.
  • the radiation shields can have their exterior silver coated to reduce their thermal emissivity.
  • the halves of the radiation shield can be joined together by soldering or by thermally conductive epoxy.
  • the stainless steel housing has welded seams joining the halves to create an airtight enclosure.
  • the windings are cooled by a two-stage cryocooler 215 which is situated in an extension of the vacuum enve­lope.
  • the first stage of the cryocooler is thermally connected to the thermal shield 191 to maintain the thermal shield at 50K and the second stage is in thermal contact with the aluminum ring 185 of the winding to maintain the winding below 10K.
  • Low thermal resistance is established between the cryocooler temperature stations and those of the shield and windings, by high pressure contact through soft indium gaskets.
  • Inboard resistive coils 217 are situated approxi­mately in the same plane and concentric with each of the superconductive coils, respectively.
  • the inboard resistive coils carry sufficient low ampere-turns so that they can be wound with hollow water cooled copper conductors to operate at a current density of 500A/cm2.
  • the resistive coils are each supported from the vacuum envelope by four radially extending brackets 220.
  • the resistive coils and super­conductive coils are all connected in series and each carries current in the same circumferential direction. Current is provided to the superconductive coil by perma­nently connected heat stationed leads.
  • a 0.5T embodiment of the hybrid superconductive/­resistive magnet would have the following characteristics.
  • the superconducting and resistive coils would each carry 50 amperes, with 6074 and 135 turns respectively, and a coil current density of 11,400 and 500 amperes/cm2, respectively.
  • the superconductive coils each would have a radius of 59.4 cm. and the resistive coils would have a radius of 15.2 cm.
  • the superconductive coils are spaced apart axially by 51.4 cm while the resistive coils are spaced apart by 52.2 cm.
  • the cross section in height by width of the superconductive and resistive coils are 3.8 X 7 cm. and 3.7 X 3.7 cm., respectively.
  • the magnet has an inductance of 206 H and stored energy of 258 kilojoules.
  • the supercon­ductor wire is Nb3Sn wire and copper wire cowound.
  • the bare Nb3Sn wire and insulated copper wire each have a diameter of 0.043 cm. with a copper to superconductor ratio of 1.5.
  • the superconductor wire is superconducting at 10°K.
  • the magnet 222 has generally the same configuration as the magnet of Figure 13.
  • Two superconducting coils 221 and 223 are provided wrapped around a copper coil form 225 having a "U" shaped cross-section.
  • the coil form comprises three pieces, a band 227 formed by rolling and welding the ends of a copper strip and two circular flange pieces 229 having a central aperture which are joined at their inner diameter on either side of the band 227, such as by solder­ing.
  • the superconductor wire can comprise a 0.017 X 0.025" Nb3Sn superconductor with a copper to superconductor ratio of 0.5.
  • the wire is covered by a .0025" glass braid.
  • the wire is processed by the bronze method and is available from Oxford Airco.
  • the wire is soldered to a start­ing terminal 231 in the flange 229 which is insulated from the rest of the flange by insulating block 233.
  • the wire is wrapped with a tension of 3-5 ounces.
  • Each layer is sep­arated by fiberglass cloth insulation.
  • Every fourth or fifth layer is surrounded by a thin copper foil band approx­imately 0.010 inch thick.
  • the band surrounds the layer of wire in the coil form with the ends overlapping and sol­dered. The band allows the winding to pass through to the next layer as previously described.
  • the winding terminates at finishing terminal 235 to which it is soldered.
  • the winding is covered with fiberglass cloth and copper plates 237 are slid into slots formed in the flange pieces.
  • the slots extend to the periphery of the ring in one location to allow a plurality of copper plates to slide in and be positioned circumferentially about the perimeter of the winding.
  • an uninsulated stainless steel overwrapping 241 encloses the copper plates.
  • the overwrap­ping is covered with release material and covered with brass shims (not shown) held in place by wire (not shown) and both coils 221 and 223 are vacuum epoxy impregnated.
  • the wire and brass shims are removed together with any excess epoxy. After impregnation the plates are rigidly positioned in their slots. The copper plates transmit part of the radial­ly outward load created by the windings during magnet operation to the "U" shaped coil form.
  • the coils are surrounded by a 50K radiation shield 191 which in turn is surrounded by a vacuum enclosure housing 193. Both the shield and housing are fabricated as previously described, and supported in the cryostat by three supports 194 each having three concentric tubes 195, 197 and 211 also of the type previously described.
  • Four aluminum posts 187 support coil 221 above coil 223.
  • Clamping brack­ets 243 hold the coil form 225 and coils and are secured to supports and posts.
  • the resistive coils are supported as previously described by brackets. Leads are permanently attached to the cryocooler connecting the two superconduct­ing coils in series. The incoming leads are heat stationed to the two stages of the cryocooler.
  • Leads from the second stage heat station are coupled to the input terminal of winding 223 and the output terminal of winding 221.
  • the output and input terminal of windings 223 and 221, respec­tively, are coupled together.
  • the resistance coils are also connected in series with each other and the superconductor coils. All the currents in all the coils flow in the same circumferential direction.
  • FIG. 21 Another embodiment of an open magnet configuration is shown in Figure 21.
  • the magnet 244 has no resistive coils but rather has four superconducting resin impregnated coils, 251, 252, 253 and 254, two superconducting coils 251 and 252, and 253 and 254 in each of the two toroidal sections of the cryostat.
  • Coil 251 and 253 have the same diameter and number of turns both of which are greater than those of coils 252 and 254 which both have the same diameter and number of turns.
  • the superconductor coils in each of the toroidal sections is wound on a copper form 257.
  • the coil forms are spaced apart parallel to one another with their centers lying on the same line which is perpendicular to the plane in which each of the coils lie.
  • the coil forms are separated by aluminum posts as previously described with both coil forms supported by supports 194 each having three concentric tubes.
  • a radiation shield surrounds the coil forms and is in turn surrounded by a vacuum enclosure. During operation, all the coils are connected in series with the coils 251 and 253 each carry current in the same direc­tion while coils 252 and 254 carry current in the opposite circumferential direction.
  • the coils 251, 252, 253 and 154 can be wound on a fiberglass form having the shape of the metal coil form 257.
  • a conductive shell can surround the lower portion and sides of the coil form supporting coils 253 and 254.
  • the generally U-shaped shell fabricated of copper, for example, could be used as a pan in which the coils could be vacuum pressure impregnated.
  • the outer coils are spaced 65 cm. from one another and have a radius of 56.1 cm.
  • the outer coils carry 50 amperes in a Nb3, Sn wire having a diameter of .043 cm. which is cowound with an insulated copper wire having a diameter of 0.043 cm.
  • the coils have a cross section 2.6 cm. high by 14 cm. in width.
  • Superconductive coils 252 and 254 are spaced 51.8 cm. apart and have a radius of 40 cm.
  • the coils 252 and 254 are cowound with the same dimension copper and Nb3Sn wire and carry 50 amperes.
  • Coils 252 and 254 each have a cross section of 2 cm. high by 3.4 cm. wide.
  • the magnet has a clear bore diameter of 70 cm. with a transverse patient access of 40X70 cm.
  • the calculated homogeneity in a 25 cm. sphere is 13 ppm.
  • the configuration of the open magnet 179 provides a greater patient field of view than magnets having a series of coils on a closed cylindrical coil form.
  • the open magnets can be arranged with a patient 261 to be imaged standing or lying down.
  • the patient can remain stationary while the magnet moves in the vertical direction as needed.
  • FIG. 22 A typical refrigeration capacity of a Model 1020 Cryodyne® cryocooler from CTI-Cryogenics, Waltham, Massa­chusetts, operating from 60 Hz. power supply is shown in Fig. 22, which also shows the operating point of the cryo­cooler when used with the different embodiments super­conductive magnets.
  • the magnet cooling load is approximate­ly as follows: Nb3Sn Winding Radiation 0.110 Conduction 0.090 Current leads, copper 0.600 Cryocooler Second Stage Heat Load 0.800 Watts Radiation Shield Radiation 8.6 Conduction 2.0 Current leads, copper 4.8 Cryocooler First Stage Heat Load 15.4 Watts
  • cryocooler During start up the cryocooler is operating and a power supply ramps up gradually to a constant 50 amperes of current through the current leads. During ramp up, currents will be induced in the conductive loops in the layers of the coil. The currents, however, will not create a problem since the change of current is gradual. Once superconduct­ing operation is achieved the power supply can remain connected, although the coils are superconducting the copper bars connecting coils have resistive losses as well as the current leads. The losses, however, are not very great and the large inductance and small resistance of the magnet provides for a large time constant.
  • cowound stabilizer if soldered to the super­conductor every layer provides a low resistance in parallel with the portion of the superconductor wire undergoing the quench reducing the current carried by the quenched super-­conductor.
  • resistive metallic conductors such as copper are used in the lead section from the exterior of the cryostat, which is at an ambient temperature of 300°K, to the first stage of the cryocooler which has a temperature of 50°K during operation.
  • a resistive metallic conductor is also used in the lead section from the first stage of the cryocooler which is at 50°K to the second stage which is at 10°K.
  • the tempera­ture profile of the current leads with optimized aspect ratio for a 50 ampere current is shown in Fig. 25.
  • the slope of the temperature profile of the leads extending between the 10°K and 50°K heat station as it approaches the 50°K heat station is seen to be horizontal signifying that the resistive and conductive heat flows are balanced.
  • the slope of the temperature profile of the current leads between the 50°K heat station and ambient as the lead approaches ambient temperature is horizontal.
  • a high temperature ceramic superconductor is used in a lead section from the 50°K to 10°K heat station then the resistive heating in that lead section is zero and there is no optimum lead aspect ratio for that section.
  • the ceramic superconductor lead section is made sufficiently large to carry the required current, I, and the lead length is made sufficiently long to result in acceptable conduction heat transfer to the 10°K heat station.
  • the lead cross sectional area, A must be varied inversely with temperature so that with sufficient safety margin, (J c -J)/J c approximately 10 to 30 percent, where J is the actual current density in the ceramic lead and I is the current.
  • Figure 26 shows a cold end portion of a cryocooler sleeve in an evacuated housing 260.
  • Two straight ceramic leads 261 extending from the 50°K to 10°K stations 263 and 265, respectively, of a cryocooler sleeve with the leads tapered so that the lead has greater cross sectional area at the warmer end.
  • the ceramic leads are heat stationed at the 50°K and 10°K heat stations 263 and 265, respectively.
  • the high temperature section of the lead between the ambient (300°K) and the 50°K heat station comprises copper conduc­tors having an optimized L/A to minimize the heat trans­ferred to the 50°K station at the operating current.
  • the leads should be metallized with silver.
  • One method is sputtering another is using silver epoxy.
  • the ceramic leads 261 are coated with silver loaded epoxy in the region where current conductive junctions are to be made. During processing of the ceramic, the epoxy is vaporized leaving behind a silver coating to which copper leads can be soldered. Resistive metallic conductors are soldered to the ceramic leads at the 10°K heat station using low resistivity solder, such as indium solder. The copper leads extending from the ambient are soldered to the ceramic leads in the vicinity of the 50°K heat station. The ceramic leads can be heat stationed, for example, using beryllia or alumina metallized with copper or nickel on both sides and soldered between the metallized ceramic lead and the cryocooler sleeve heat station. See copending application RD 18522, incorporated herein by reference.
  • Figures 27 and 28 show two tapered spiral high temperature ceramic superconductors 271 and 273 which can be formed from a single cylindrical length of ceramic supercon­ductor such as yttrium barium copper oxide (YBa2Cu3O x ).
  • the ceramic leads extend from the 50°K to 10°K heat station 263 and 265, respectively, and are heat stationed at the 50°K and 10°K heat stations.
  • the ceramic leads are metallized with silver, such as by coating them with silver loaded epoxy which during heating leaves a coating of silver behind allowing the resistive metallic conductors to be soldered to the silver coated ceramic leads at the 10°K heat station.
  • a low resistance solder such as indium solder is preferably used.
  • the current leads each from ambient temperature are soldered to the ceramic leads in the vicinity of the 50°K heat station.
  • cryocooler in the sleeve which is thermally coupled to the magnet cryostat temperature stations at 10°K, and 50°K, will experience negligible heat load from the current leads at the 10°K station, when the optimized aspect ratio resistive metallic conductors or the ceramic superconductors are used.
  • the cooling capacity at the 10°K station is limited and the heat station receives negligible heat load from the current leads, while the lead thermal load at the 50°K heat station can be easily handled by the increased refrigeration capacity available at this temperature.
  • Power is supplied to the magnets in the present invention by permanently connected leads supplied from a stable power supply.
  • the power supply provides power lost due to the resistance in copper bus bars current leads and superconductor splices.
  • diodes are connected in the magnet to provide a continuous current path. During operation with the current leads connected and operating properly the voltage across the diodes is insufficient to cause them to conduct. If the leads current is interrupted, the voltage across the diode increases causing them to conduct.
  • niobium tin superconductor wire are nonsuperconductive but have a very low resistance. Using only superconductive wire and no copper bus bars, or perma­nently connected leads, the magnet resistance would be approximately 10 ⁇ 8 ohms. The inductance of the magnet depends on magnet strength varying from 160 to 1600 henries for the embodiments shown. Once a current is established in the superconducting coils, the long time constant of the magnet circuit (thousands of years) could provide virtually persistent operation and a stable field in the magnet.
  • the material G-10 referred to in the foregoing description is a laminated thermosetting material (comprising a continuous filament-type glass with an epoxy resin binder) identified in the ASTM specification D709-87.

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  • Engineering & Computer Science (AREA)
  • Power Engineering (AREA)
  • Magnetic Resonance Imaging Apparatus (AREA)
  • Containers, Films, And Cooling For Superconductive Devices (AREA)
EP89306784A 1988-07-05 1989-07-04 Eine supraleitende abschreckgesicherte Spule Withdrawn EP0350264A1 (de)

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US215479 1988-07-05

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Cited By (9)

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EP0468415A2 (de) * 1990-07-24 1992-01-29 Oxford Magnet Technology Limited Magnetanordnung
EP0826977A2 (de) * 1996-08-26 1998-03-04 General Electric Company Kompakter supraleitender MRI-Magnet
WO2008114184A2 (en) 2007-03-19 2008-09-25 Koninklijke Philips Electronics N.V. Superconductive magnet system for a magnetic resonance examination system
JP2013031658A (ja) * 2011-07-29 2013-02-14 General Electric Co <Ge> 超伝導マグネットシステム
GB2510410A (en) * 2013-02-04 2014-08-06 Siemens Plc Quench pressure reduction for superconducting magnet by reducing heat flux from coil to cryogen
GB2540623A (en) * 2015-07-24 2017-01-25 Tesla Eng Ltd Superconducting winding arrangements
CN108447644A (zh) * 2018-05-29 2018-08-24 潍坊新力超导磁电科技有限公司 一种用于肢端成像的核磁共振成像超导磁体
WO2020079238A1 (en) * 2018-10-19 2020-04-23 Koninklijke Philips N.V. Fast quench protection for low copper to superconducting wire coils
EP3920196A1 (de) * 2016-10-31 2021-12-08 Tokamak Energy Ltd Quenchschutz bei supraleitenden magneten

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CN102792396A (zh) * 2010-03-23 2012-11-21 日本超导体技术公司 超导磁体
JP5448988B2 (ja) * 2010-04-09 2014-03-19 ジャパンスーパーコンダクタテクノロジー株式会社 超電導マグネット
JP6091999B2 (ja) * 2012-06-01 2017-03-08 住友重機械工業株式会社 サイクロトロン

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US3869686A (en) * 1972-11-06 1975-03-04 Bbc Brown Boveri & Cie Super-conductive coils incorporating insulation between adjacent winding layers having a contraction rate matching that of the super-conductive material
US4218668A (en) * 1977-03-01 1980-08-19 Hitachi, Ltd. Superconductive magnet device
EP0014915A1 (de) * 1979-02-23 1980-09-03 Siemens Aktiengesellschaft Supraleitende Magnetwicklung mit mehreren Wicklungslagen
US4437080A (en) * 1983-02-14 1984-03-13 The United Of America As Represented By The Secretary Of Commerce And The Secretary Of The Air Force Method and apparatus utilizing crystalline compound superconducting elements having extended strain operating range capabilities without critical current degradation
US4499443A (en) * 1984-01-31 1985-02-12 The United States Of America As Represented By The United States Department Of Energy High-field double-pancake superconducting coils and a method of winding
US4727346A (en) * 1985-09-11 1988-02-23 Bruker Analytische Mebtechnik Gmbh Superconductor and normally conductive spaced parallel connected windings

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US3869686A (en) * 1972-11-06 1975-03-04 Bbc Brown Boveri & Cie Super-conductive coils incorporating insulation between adjacent winding layers having a contraction rate matching that of the super-conductive material
US4218668A (en) * 1977-03-01 1980-08-19 Hitachi, Ltd. Superconductive magnet device
EP0014915A1 (de) * 1979-02-23 1980-09-03 Siemens Aktiengesellschaft Supraleitende Magnetwicklung mit mehreren Wicklungslagen
US4437080A (en) * 1983-02-14 1984-03-13 The United Of America As Represented By The Secretary Of Commerce And The Secretary Of The Air Force Method and apparatus utilizing crystalline compound superconducting elements having extended strain operating range capabilities without critical current degradation
US4499443A (en) * 1984-01-31 1985-02-12 The United States Of America As Represented By The United States Department Of Energy High-field double-pancake superconducting coils and a method of winding
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Cited By (18)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0468415A2 (de) * 1990-07-24 1992-01-29 Oxford Magnet Technology Limited Magnetanordnung
EP0468415A3 (en) * 1990-07-24 1992-06-10 Oxford Magnet Technology Limited Magnet assembly
US5210512A (en) * 1990-07-24 1993-05-11 Oxford Magnet Technology Ltd. Magnet assembly
EP0826977A2 (de) * 1996-08-26 1998-03-04 General Electric Company Kompakter supraleitender MRI-Magnet
EP0826977A3 (de) * 1996-08-26 1998-10-14 General Electric Company Kompakter supraleitender MRI-Magnet
WO2008114184A2 (en) 2007-03-19 2008-09-25 Koninklijke Philips Electronics N.V. Superconductive magnet system for a magnetic resonance examination system
WO2008114184A3 (en) * 2007-03-19 2008-12-31 Koninkl Philips Electronics Nv Superconductive magnet system for a magnetic resonance examination system
US8072301B2 (en) 2007-03-19 2011-12-06 Koninklijke Philips Electronics N.V. Superconductive magnet system for a magnetic resonance examination system
JP2013031658A (ja) * 2011-07-29 2013-02-14 General Electric Co <Ge> 超伝導マグネットシステム
GB2510410A (en) * 2013-02-04 2014-08-06 Siemens Plc Quench pressure reduction for superconducting magnet by reducing heat flux from coil to cryogen
GB2510410B (en) * 2013-02-04 2016-03-09 Siemens Plc Quench pressure reduction for superconducting magnet
GB2540623A (en) * 2015-07-24 2017-01-25 Tesla Eng Ltd Superconducting winding arrangements
EP3920196A1 (de) * 2016-10-31 2021-12-08 Tokamak Energy Ltd Quenchschutz bei supraleitenden magneten
US11776721B2 (en) 2016-10-31 2023-10-03 Tokamak Energy Ltd Quench protection in high-temperature superconducting magnets
CN108447644A (zh) * 2018-05-29 2018-08-24 潍坊新力超导磁电科技有限公司 一种用于肢端成像的核磁共振成像超导磁体
CN108447644B (zh) * 2018-05-29 2024-01-26 潍坊新力超导磁电科技有限公司 一种用于肢端成像的核磁共振成像超导磁体
WO2020079238A1 (en) * 2018-10-19 2020-04-23 Koninklijke Philips N.V. Fast quench protection for low copper to superconducting wire coils
JP2021534924A (ja) * 2018-10-19 2021-12-16 コーニンクレッカ フィリップス エヌ ヴェKoninklijke Philips N.V. 低銅対超伝導ワイヤコイルのための高速クエンチ保護

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JPH0335818B2 (de) 1991-05-29
IL90667A0 (en) 1990-01-18

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