WO2002059917A1 - Liquid cryogen-free superconducting magnet system - Google Patents

Liquid cryogen-free superconducting magnet system Download PDF

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Publication number
WO2002059917A1
WO2002059917A1 PCT/US2001/041829 US0141829W WO02059917A1 WO 2002059917 A1 WO2002059917 A1 WO 2002059917A1 US 0141829 W US0141829 W US 0141829W WO 02059917 A1 WO02059917 A1 WO 02059917A1
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Prior art keywords
magnet
coils
magnet coils
superconducting
cool
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PCT/US2001/041829
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French (fr)
Inventor
Leong Ying
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Everson Electric Company
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Publication of WO2002059917A1 publication Critical patent/WO2002059917A1/en

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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
    • H01F6/04—Cooling
    • H—ELECTRICITY
    • H01—ELECTRIC ELEMENTS
    • H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F6/00—Superconducting magnets; Superconducting coils
    • Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y10—TECHNICAL SUBJECTS COVERED BY FORMER USPC
    • Y10S—TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y10S505/00—Superconductor technology: apparatus, material, process
    • Y10S505/825—Apparatus per se, device per se, or process of making or operating same
    • Y10S505/888—Refrigeration
    • Y10S505/892—Magnetic device cooling

Definitions

  • the present invention pertains to a superconducting magnet having two separate magnet coils.
  • Superconductivity is a phenomena whereby certain materials lose all electrical resistance when the temperature of the material is lowered below a certain critical point.
  • superconducting alloys such as niobium titanium (Nb Ti) in the early days of the decade of the 1960's that the superconductivity effect was put to practical use, particularly in the production of very high-field superconducting magnets.
  • Low temperature superconductors require refrigeration at temperatures close to absolute zero (0°K or -273 °C) before the critical superconducting limits are reached. At these low temperatures, the only refrigerant medium that can be used is helium. The normal boiling point of liquid helium at one atmosphere is 4.2°K.
  • high temperature superconductors In the 1980's, high temperature superconductors (HTS) were discovered. Unlike the low temperature superconducting materials which tend to be metallic alloys and compounds, the new high temperature superconducting materials are ceramic based. Because of the brittle nature of these ceramic-like materials, high temperature superconductors are currently confined mainly for use as straight sectioned current leads.
  • U.S. Patent No. 5,442,928 discloses and claims a compact conduction-cooled superconducting magnet wherein the magnet is cooled by liquid helium with the evaporating liquid helium re-condensed by a closed cycle refrigerator. All of the main coils are wired in series and powered together.
  • U.S. Patent No. 5,448,214 discloses and claims an actively-shielded open MRI high-temperature niobium tin superconducting magnet, conduction cooled by a high- temperature cryo cooler.
  • the niobium-tin superconductor is cooled to 10°K using a closed cycle refrigerator to cool both halves of the magnet coil.
  • the second coil is conduction cooled to the first coil which is then, in turn, conduction cooled by the closed cycle refrigerator.
  • U.S. Patent No. 5,412,363 discloses and claims an open MRI superconducting magnet cooled by a single closed cycle refrigerator.
  • the coils of the magnet according to patentee are energized in series and powered up to produce a homogenous high central feel.
  • the liquid helium returns to the closed cycle refrigerator for recondensing.
  • the first magnet coil is cooled by first circulating liquid helium around the heat exchange circuit associated with the first magnet coil. After circulating around the first heat exchange circuit, the helium is returned to the refrigerator for re- cooling before it passes around the heat exchanger associated with the second magnet coil.
  • the MRI superconducting magnet is operated in persistence mode where the current is perpetually circuited internally, separate from the power supply.
  • U.S. Patent No. 5,517,169 discloses and claims an invention relating to provision of a superconducting magnet with improved magnetic shielding.
  • the improved magnetic shielding is an external iron shield.
  • U.S. Patent No. 5,934,082 discloses indirect cooling of a magnetic device in order to reduce vibration by using low-vibration thermal coupling. Patentees describe using a 10 °K (high-temperature) cryo cooler with no cooling system described in detail. SUMMARY OF THE INVENTION
  • the present invention pertains to a superconducting magnet having at least two magnet coils separated from one another.
  • the magnetic coils are so constructed and arranged to provide a central magnetic field that is accessible along an X, Y, and Z axis with the axis generation point being at the center of the magnetic field.
  • the magnet according to the invention has full open access to the central magnetic field.
  • each of the magnet coils is contained in a separate vacuum jacket with an intermediate radiation shield disposed between the magnet and the vacuum jacket.
  • a two stage closed cycle cryogenic refrigerator is directly coupled to the magnet coil and the radiation shield. The first stage of the cryogenic refrigerator is in direct thermal contact with the radiation shield and the second or colder stage of the closed cycle refrigerator is in direct thermal contact with the magnet.
  • the magnet can be cooled to cryogenic temperatures utilizing only the closed cycle refrigerator. Inclusion of a coil of conductive tubular material around each magnet coil through which a liquid cryogen (e.g. liquid nitrogen or liquid helium) can be circulated can significantly reduce the cool-down time for the magnet coil. By circulating the liquid cryogen through the tubing, more rapid cool-down of the magnet coils can be effected.
  • a liquid cryogen e.g. liquid nitrogen or liquid helium
  • the present invention is a superconducting magnet assembly comprising, in combination, two separate generally toroidally shaped magnet coils positioned in spaced apart relationship to define access to a magnetic field along X, Y, and Z axes originally from the center of the magnetic field; each of the magnetic coils contain within, and spaced apart from an outer vacuum jacket, at least one radiation shield disposed within each of the vacuum jackets between each of the magnet coils and its vacuum jacket, and a separate two stage closed cycle refrigerator adapted to cool each of the magnets to a temperature of about 4°K and each of the radiation shields to a temperature of about 50 °K.
  • the present invention is a superconducting magnet assembly comprising, in combination, two separate generally toroidally shaped magnet coils positioned in spaced apart relationship to define access to a magnetic field along X, Y, and Z axes originally from the center of the magnetic field; each of the magnetic coils contain within, and spaced apart from an outer vacuum jacket, at least one radiation shield disposed within each of the vacuum jackets between each of the magnet coils and its vacuum jacket, a separate two stage closed cycle refrigerator adapted to cool each of the magnets to a temperature of about 4°K and each of the radiation shields to a temperature of about 50 °K, and auxiliary means to cool the magnet coils by circulating a liquid cryogen around the magnet coils.
  • Figure 1 is a top view of the magnet assembly according to the present invention.
  • Figure 2 is a right side view of the magnet assembly of Figure 1.
  • Figure 3 is a front view of the magnet assembly of Figure 1.
  • Figure 4 is a schematic representation of the magnet assembly of the invention illustrating cooling of the magnet.
  • Figure 5 is an enlarged front view partially in section of the individual magnet coil assemblies of a magnet according to the present invention.
  • Figure 6 is a view taken along lines 6-6 of Figure 5.
  • cryogenic refrigerators With the advent of improved two stage closed cycle cryogenic refrigerators, one type many refer to as a Gifford-McMahon refrigerator, permit cooling of superconducting magnets by direct thermal connection to the refrigerator by mechanical means. This can supplant traditional cooling of superconducting magnets by immersion in a bath of liquid helium.
  • the superconducting magnet system or assembly is shown generally as 10.
  • the system includes a first magnet coil assembly 12 and a second magnet coil assembly 14 spaced apart from one another to define a central magnetic field point that is accessible along an X, Y, or Z axis generated from the central point which is shown as 16 in Figures 1, 2, and 3.
  • Each of the magnetic coil assemblies 12, 14 is enclosed in an outer vacuum tight housing 18, 20.
  • Each magnet coil assembly 12, 14 is supported by vertical stands or supports 22, 24, 26, and 28, respectively, which can be of any height, depending upon the use to which the superconducting magnet assembly is placed, and cross members 30,
  • Each magnet coil assembly 12, 14 has associated with it a closed cycle two stage refrigerator 34, 36 generally referred to as a Gifford-McMahon (cycle) refrigerator.
  • Each of the cryogenic refrigerators 34, 36 is a refrigerator adapted to produce a first stage temperature of about 50°K and a second stage temperature of about 4°K.
  • One particular refrigerator useful in the present invention is manufactured and sold by Leybold Cryogenic North America of Hudson, New Hampshire, under the designation 4.2 GM.
  • each of the magnet coil assemblies 12, 14 has an outer vacuum housing 18, 20.
  • Housing 18 contains the magnet coil 38
  • housing 20 contains the magnet coil 40.
  • Disposed between the magnet coil 38 and the housing 18 is a radiation shield 42
  • between the magnet coil 40 and the housing 20 is a radiation shield 44.
  • a first two stage closed cycle cryogenic refrigerator 34 is disposed on the housing 18 of magnet assembly 12.
  • the first stage 46 of refrigerator 34 is thermally connected directly to radiation shield 42 and the second stage 48 of refrigerator 34 is thermally connected directly to the magnet coil 38.
  • the first stage 50 of refrigerator 36 is thermally connected directly to the radiation shield 44 and a second stage 52 of refrigerator 36 is thermally connected directly to the magnet coil 40.
  • the first stage refrigeration is adapted to cool the heat shields 42, 44 to a temperature of about 50 °K and the second stage refrigeration is adapted to cool the magnet coils 38, 40 to a temperature of about 4°K.
  • the magnet can be cooled to a temperature at which superconductivity takes place.
  • magnet assemblies 12 and 14 can contain several turns of a conductive tubing wrapped around the magnet coils 38 and 40 respectively.
  • a liquid cryogen e.g. , liquid nitrogen or liquid helium
  • the position of the conductive coils 54, 56 is shown in more detail in the view of Figure 6.
  • the tubing can be of any conductive metal, copper being preferred.
  • the copper tubing can be connected to low thermal conductivity stainless steel fittings 58, 60, 62, 64 which penetrate the vacuum housings or vacuum jackets 18, 20 to permit introduction of liquid cryogen into the coiled tubing 54, 56 to rapidly cool the magnet coils 38, 40.
  • the stainless steel tubing used in conjunction with the copper tubing has an intermediate thermal anchor point (shown at 66, 68, 70, and 72 respectively in Figure 5), attached to the intermediate radiation shields 42, 44 in the magnet coil assembly housings 18, 20.
  • Each magnet coil 38, 40 is fabricated by winding composite wires having a nominal outer diameter of 1 mm containing niobium titanium superconducting filaments onto an aluminum mandrel. The completed coil with the multiple turns is then vacuum impregnated to produce a structure with good mechanical and electrical properties. By pumping electrical currents through the multiple turns, very high magnetic fields can be generated. Because the electrical currents flow through a superconducting medium with no electrical resistance, there is no electrical Joules heating generated by the superconducting circuit.
  • mechanical two-stage closed cycle refrigerators are used to cool a superconducting coil and thereby eliminate the necessity to use liquid cryogen in normal operation.
  • each superconducting coil is housed in a vacuum jacket or a vacuum dewar and independently conduction-cooled by a two stage Gifford-McMahon cryogenic cooler of the type identified above.
  • One of the unique features of the magnet assembly results from the provision of two separate individually cooled magnet coils that are liquid cryogen-free and are incorporated into a single system where there is complete open access between the central room temperature gap and the middle of both halves.
  • the housings, vacuum dewars, or vacuum jackets for the superconducting coils are supported by horizontal fiber glass reinforced plastic supports and vertical stainless steel supports. These structures are used to support the coils gravitationally and against the large electro-magnetic forces.
  • the housing in each instance is evacuated and maintained at a pressure below 10 "5 torr.
  • One of the major external heat loads from outside the vacuum dewars is conductive heating through the magnetic current leads.
  • Traditional systems use normal resistive leads fabricated from materials such as copper or brass. However, these resistive leads generate high heat loads through conduction and Joules heating when high- current are run through them to energize the superconducting coils. The heating generated from these resistive metal aides is too excessive for the two stage cryogenic refrigerators to handle.
  • the use of high-temperature superconductor leads reduces the heat source to a level where two stage cryogenic refrigerators can operate effectively. Because the high temperature superconducting materials are ceramic, the conductive heat loads are much lower when compared to the normal metallic resistive leads.
  • the high temperature superconductor leads can also maintain the superconducting properties at temperatures above 80 °K, which eliminates localized Joules heating at the connection to the cold superconducting coils.
  • An energized superconducting coil and an external iron yoke are used by the system of the present invention to produce the magnetic field.
  • the iron yoke is fabricated from standard magnetic grade steel and is used to both enhance and shape the field. Due to saturation in the iron, this method is only viable for generated fields of the order of 2 Tesla (20,000 Gauss).
  • One of the unique features of the superconducting magnet system according to the present invention is the use of two opposing independently operated liquid cryogen-free superconducting magnet units to generate a central high magnetic field within the gap separating the two units. This room temperature gap provides for a complete access from the vertical and horizontal planes for user interfaces.
  • each coil half can be energized independently of the other half. With both coils energized with the same current polarity, a high homogenous high-magnetic field is generated between the central gap separating the two units. With the two coils energized with opposing current polarity, a zero field can be generated at the center with a large magnetic field gradient extending outwardly.
  • the superconducting magnet system of the present invention utilizes two opposing liquid cryogen-free superconducting magnet units to provide complete vertical and horizontal central room temperature access.
  • the present invention also features use of separate liquid nitrogen, liquid helium heat exchangers to aid in rapid cool-down of the magnets.
  • Another feature of the present invention is that, while the magnet coils can be cooled to approximately 4°K, they can also be cooled to the higher temperature normally associated with the cooling of the intermediate radiation shield if the magnet coils are fabricated from a high temperature super conducting material.
  • a magnet system awaiting to the present invention was constructed and had the following performance characteristics: a) 1.7 Tesla (17,000 Gauss) central magnetic field. b) +3 % field inhomogeneity over the central working volume. c) 1.5° field divergence angle over the central working volume.
  • a coil mass of 100 Kg (220 lbs.) it required approximately 100 hours to cool using only the two stage closed cycle refrigerators. By circulating liquid helium through the heat exchanger coil, cool- down time was reduced to approximately 10 hours.
  • Another feature of the present invention is the fact that cooling by liquid cryogen circulating through the coils and cooling by the closed cycle refrigerators can take place simultaneously.
  • two stage cryogenic refrigerators or cryo-coolers such as two stage pulsed tube refrigerators, can be used in place of the Gifford-McMahon refrigerators.

Abstract

A superconducting magnet assembly having two individual magnetic coils contained in separate vacuum jackets with a radiation shield between each magnet and its respective vacuum jacket. Each magnet coil is cooled to superconducting temperature by direct coupling to the second stage of a separate two stage closed cycle refrigerator. A first stage of each refrigerator cools an associated radiation shield.

Description

LIQUID CRYOGEN-FREE SUPERCONDUCTING MAGNET SYSTEM
BACKGROUND OF THE INVENTION
The present invention pertains to a superconducting magnet having two separate magnet coils.
Superconductivity is a phenomena whereby certain materials lose all electrical resistance when the temperature of the material is lowered below a certain critical point. Although superconductivity was discovered at the turn of the last century, it was not until the advent of superconducting alloys such as niobium titanium (Nb Ti) in the early days of the decade of the 1960's that the superconductivity effect was put to practical use, particularly in the production of very high-field superconducting magnets. Low temperature superconductors require refrigeration at temperatures close to absolute zero (0°K or -273 °C) before the critical superconducting limits are reached. At these low temperatures, the only refrigerant medium that can be used is helium. The normal boiling point of liquid helium at one atmosphere is 4.2°K.
In the 1980's, high temperature superconductors (HTS) were discovered. Unlike the low temperature superconducting materials which tend to be metallic alloys and compounds, the new high temperature superconducting materials are ceramic based. Because of the brittle nature of these ceramic-like materials, high temperature superconductors are currently confined mainly for use as straight sectioned current leads.
U.S. Patent No. 5,442,928 discloses and claims a compact conduction-cooled superconducting magnet wherein the magnet is cooled by liquid helium with the evaporating liquid helium re-condensed by a closed cycle refrigerator. All of the main coils are wired in series and powered together.
U.S. Patent No. 5,448,214 discloses and claims an actively-shielded open MRI high-temperature niobium tin superconducting magnet, conduction cooled by a high- temperature cryo cooler. The niobium-tin superconductor is cooled to 10°K using a closed cycle refrigerator to cool both halves of the magnet coil. The second coil is conduction cooled to the first coil which is then, in turn, conduction cooled by the closed cycle refrigerator.
U.S. Patent No. 5,412,363 discloses and claims an open MRI superconducting magnet cooled by a single closed cycle refrigerator. The coils of the magnet according to patentee are energized in series and powered up to produce a homogenous high central feel. The liquid helium returns to the closed cycle refrigerator for recondensing. According to patentees, the first magnet coil is cooled by first circulating liquid helium around the heat exchange circuit associated with the first magnet coil. After circulating around the first heat exchange circuit, the helium is returned to the refrigerator for re- cooling before it passes around the heat exchanger associated with the second magnet coil. The MRI superconducting magnet is operated in persistence mode where the current is perpetually circuited internally, separate from the power supply.
U.S. Patent No. 5,517,169 discloses and claims an invention relating to provision of a superconducting magnet with improved magnetic shielding. The improved magnetic shielding is an external iron shield.
U.S. Patent No. 5,934,082 discloses indirect cooling of a magnetic device in order to reduce vibration by using low-vibration thermal coupling. Patentees describe using a 10 °K (high-temperature) cryo cooler with no cooling system described in detail. SUMMARY OF THE INVENTION
The present invention pertains to a superconducting magnet having at least two magnet coils separated from one another. The magnetic coils are so constructed and arranged to provide a central magnetic field that is accessible along an X, Y, and Z axis with the axis generation point being at the center of the magnetic field. The magnet according to the invention has full open access to the central magnetic field.
According to the present invention, each of the magnet coils is contained in a separate vacuum jacket with an intermediate radiation shield disposed between the magnet and the vacuum jacket. A two stage closed cycle cryogenic refrigerator is directly coupled to the magnet coil and the radiation shield. The first stage of the cryogenic refrigerator is in direct thermal contact with the radiation shield and the second or colder stage of the closed cycle refrigerator is in direct thermal contact with the magnet. With a system according to the present invention, the magnet can be cooled to cryogenic temperatures utilizing only the closed cycle refrigerator. Inclusion of a coil of conductive tubular material around each magnet coil through which a liquid cryogen (e.g. liquid nitrogen or liquid helium) can be circulated can significantly reduce the cool-down time for the magnet coil. By circulating the liquid cryogen through the tubing, more rapid cool-down of the magnet coils can be effected.
Therefore, in one aspect, the present invention is a superconducting magnet assembly comprising, in combination, two separate generally toroidally shaped magnet coils positioned in spaced apart relationship to define access to a magnetic field along X, Y, and Z axes originally from the center of the magnetic field; each of the magnetic coils contain within, and spaced apart from an outer vacuum jacket, at least one radiation shield disposed within each of the vacuum jackets between each of the magnet coils and its vacuum jacket, and a separate two stage closed cycle refrigerator adapted to cool each of the magnets to a temperature of about 4°K and each of the radiation shields to a temperature of about 50 °K.
In another aspect, the present invention is a superconducting magnet assembly comprising, in combination, two separate generally toroidally shaped magnet coils positioned in spaced apart relationship to define access to a magnetic field along X, Y, and Z axes originally from the center of the magnetic field; each of the magnetic coils contain within, and spaced apart from an outer vacuum jacket, at least one radiation shield disposed within each of the vacuum jackets between each of the magnet coils and its vacuum jacket, a separate two stage closed cycle refrigerator adapted to cool each of the magnets to a temperature of about 4°K and each of the radiation shields to a temperature of about 50 °K, and auxiliary means to cool the magnet coils by circulating a liquid cryogen around the magnet coils.
BRIEF DESCRIPTION OF THE DRAWINGS
Figure 1 is a top view of the magnet assembly according to the present invention.
Figure 2 is a right side view of the magnet assembly of Figure 1. Figure 3 is a front view of the magnet assembly of Figure 1.
Figure 4 is a schematic representation of the magnet assembly of the invention illustrating cooling of the magnet.
Figure 5 is an enlarged front view partially in section of the individual magnet coil assemblies of a magnet according to the present invention. Figure 6 is a view taken along lines 6-6 of Figure 5. DETAILED DESCRIPTION OF THE INVENTION
With the advent of improved two stage closed cycle cryogenic refrigerators, one type many refer to as a Gifford-McMahon refrigerator, permit cooling of superconducting magnets by direct thermal connection to the refrigerator by mechanical means. This can supplant traditional cooling of superconducting magnets by immersion in a bath of liquid helium.
However, it has been discovered that while the improved two stage cryogenic refrigerators can achieve the same base temperature as liquid helium for cooling superconducting magnets, they still lack sufficient cooling capacity to allow the use of traditional vapor-cool resistive current leads. Using high temperature superconductors as current leads eliminates the final hurdle to achieving a complete liquid cryogen-free superconducting magnet system.
Referring to Figures 1, 2, and 3, the superconducting magnet system or assembly according to the present invention is shown generally as 10. The system includes a first magnet coil assembly 12 and a second magnet coil assembly 14 spaced apart from one another to define a central magnetic field point that is accessible along an X, Y, or Z axis generated from the central point which is shown as 16 in Figures 1, 2, and 3.
Each of the magnetic coil assemblies 12, 14 is enclosed in an outer vacuum tight housing 18, 20. Each magnet coil assembly 12, 14 is supported by vertical stands or supports 22, 24, 26, and 28, respectively, which can be of any height, depending upon the use to which the superconducting magnet assembly is placed, and cross members 30,
32.
Each magnet coil assembly 12, 14 has associated with it a closed cycle two stage refrigerator 34, 36 generally referred to as a Gifford-McMahon (cycle) refrigerator. Each of the cryogenic refrigerators 34, 36 is a refrigerator adapted to produce a first stage temperature of about 50°K and a second stage temperature of about 4°K. One particular refrigerator useful in the present invention is manufactured and sold by Leybold Cryogenic North America of Hudson, New Hampshire, under the designation 4.2 GM.
Referring to Figure 4, each of the magnet coil assemblies 12, 14 has an outer vacuum housing 18, 20. Housing 18 contains the magnet coil 38, while housing 20 contains the magnet coil 40. Disposed between the magnet coil 38 and the housing 18 is a radiation shield 42, and between the magnet coil 40 and the housing 20 is a radiation shield 44. A first two stage closed cycle cryogenic refrigerator 34 is disposed on the housing 18 of magnet assembly 12. The first stage 46 of refrigerator 34 is thermally connected directly to radiation shield 42 and the second stage 48 of refrigerator 34 is thermally connected directly to the magnet coil 38. In a like manner, the first stage 50 of refrigerator 36 is thermally connected directly to the radiation shield 44 and a second stage 52 of refrigerator 36 is thermally connected directly to the magnet coil 40. With a two stage cryogenic refrigerator of the type identified above the first stage refrigeration is adapted to cool the heat shields 42, 44 to a temperature of about 50 °K and the second stage refrigeration is adapted to cool the magnet coils 38, 40 to a temperature of about 4°K. Thus, the magnet can be cooled to a temperature at which superconductivity takes place.
As shown in Figures 5 and 6, magnet assemblies 12 and 14 can contain several turns of a conductive tubing wrapped around the magnet coils 38 and 40 respectively. A liquid cryogen, (e.g. , liquid nitrogen or liquid helium), can be circulated through the tubular coils 54, 56 to effect a rapid cool-down of the magnet coils 38, 40 and the magnet 10. The position of the conductive coils 54, 56 is shown in more detail in the view of Figure 6.
The tubing can be of any conductive metal, copper being preferred. The copper tubing can be connected to low thermal conductivity stainless steel fittings 58, 60, 62, 64 which penetrate the vacuum housings or vacuum jackets 18, 20 to permit introduction of liquid cryogen into the coiled tubing 54, 56 to rapidly cool the magnet coils 38, 40. To further reduce conductive heat loads on the inner mass of the magnet 10, the stainless steel tubing used in conjunction with the copper tubing has an intermediate thermal anchor point (shown at 66, 68, 70, and 72 respectively in Figure 5), attached to the intermediate radiation shields 42, 44 in the magnet coil assembly housings 18, 20.
Each magnet coil 38, 40 is fabricated by winding composite wires having a nominal outer diameter of 1 mm containing niobium titanium superconducting filaments onto an aluminum mandrel. The completed coil with the multiple turns is then vacuum impregnated to produce a structure with good mechanical and electrical properties. By pumping electrical currents through the multiple turns, very high magnetic fields can be generated. Because the electrical currents flow through a superconducting medium with no electrical resistance, there is no electrical Joules heating generated by the superconducting circuit.
According to the invention, mechanical two-stage closed cycle refrigerators are used to cool a superconducting coil and thereby eliminate the necessity to use liquid cryogen in normal operation.
As set forth above, each superconducting coil is housed in a vacuum jacket or a vacuum dewar and independently conduction-cooled by a two stage Gifford-McMahon cryogenic cooler of the type identified above.
One of the unique features of the magnet assembly, according to the present invention, results from the provision of two separate individually cooled magnet coils that are liquid cryogen-free and are incorporated into a single system where there is complete open access between the central room temperature gap and the middle of both halves.
The housings, vacuum dewars, or vacuum jackets for the superconducting coils are supported by horizontal fiber glass reinforced plastic supports and vertical stainless steel supports. These structures are used to support the coils gravitationally and against the large electro-magnetic forces. The housing in each instance is evacuated and maintained at a pressure below 10"5 torr.
One of the major external heat loads from outside the vacuum dewars is conductive heating through the magnetic current leads. Traditional systems use normal resistive leads fabricated from materials such as copper or brass. However, these resistive leads generate high heat loads through conduction and Joules heating when high- current are run through them to energize the superconducting coils. The heating generated from these resistive metal aides is too excessive for the two stage cryogenic refrigerators to handle. The use of high-temperature superconductor leads reduces the heat source to a level where two stage cryogenic refrigerators can operate effectively. Because the high temperature superconducting materials are ceramic, the conductive heat loads are much lower when compared to the normal metallic resistive leads. The high temperature superconductor leads can also maintain the superconducting properties at temperatures above 80 °K, which eliminates localized Joules heating at the connection to the cold superconducting coils. An energized superconducting coil and an external iron yoke are used by the system of the present invention to produce the magnetic field. The iron yoke is fabricated from standard magnetic grade steel and is used to both enhance and shape the field. Due to saturation in the iron, this method is only viable for generated fields of the order of 2 Tesla (20,000 Gauss).
One of the unique features of the superconducting magnet system according to the present invention is the use of two opposing independently operated liquid cryogen-free superconducting magnet units to generate a central high magnetic field within the gap separating the two units. This room temperature gap provides for a complete access from the vertical and horizontal planes for user interfaces.
According to the present invention, each coil half can be energized independently of the other half. With both coils energized with the same current polarity, a high homogenous high-magnetic field is generated between the central gap separating the two units. With the two coils energized with opposing current polarity, a zero field can be generated at the center with a large magnetic field gradient extending outwardly.
Thus, the superconducting magnet system of the present invention utilizes two opposing liquid cryogen-free superconducting magnet units to provide complete vertical and horizontal central room temperature access. The present invention also features use of separate liquid nitrogen, liquid helium heat exchangers to aid in rapid cool-down of the magnets.
Another feature of the present invention is that, while the magnet coils can be cooled to approximately 4°K, they can also be cooled to the higher temperature normally associated with the cooling of the intermediate radiation shield if the magnet coils are fabricated from a high temperature super conducting material. A magnet system awaiting to the present invention was constructed and had the following performance characteristics: a) 1.7 Tesla (17,000 Gauss) central magnetic field. b) +3 % field inhomogeneity over the central working volume. c) 1.5° field divergence angle over the central working volume. With the system according to the present invention with a coil mass of 100 Kg (220 lbs.) it required approximately 100 hours to cool using only the two stage closed cycle refrigerators. By circulating liquid helium through the heat exchanger coil, cool- down time was reduced to approximately 10 hours. Another feature of the present invention is the fact that cooling by liquid cryogen circulating through the coils and cooling by the closed cycle refrigerators can take place simultaneously.
Other types of two stage cryogenic refrigerators or cryo-coolers, such as two stage pulsed tube refrigerators, can be used in place of the Gifford-McMahon refrigerators.
Having thus described my invention what is desired to be secured by Letters Patent of the United States is set forth in the appended claims, which should be read without limitation.

Claims

What is Claimed: 1. A superconducting magnet assembly comprising in combination: two separate toroidally shaped superconducting magnet coils positioned in spaced apart relationship to define access to a magnetic field along an X, Y, and Z axis originating from the center of the magnetic field, each of said magnet coils contained within and spaced apart from an outer vacuum jacket; at least one radiation shield disposed within each of said vacuum jackets between each of said magnet coils and its vacuum jacket; and a separate two stage closed cycle refrigerator with a second stage of each of said refrigerators directly thermally connected to a respective magnet coil to cool each of said magnet coils to a temperature at which superconductivity takes place, and a first stage of each of said refrigerators directly thermally connected to a respective radiation shield to cool each of said radiation shields to a temperature above said temperature at which superconductivity takes place.
2. A superconducting magnet assembly according to claim 1 including auxiliary means to cool said magnet coils by circulating a liquid cryogen around said coils.
3. An assembly according to claim 2 wherein said means includes individual cooling coils fabricated from a tubular conductive metal wrapped around each of said magnet coils, each of said cooling coils having an inlet and outlet penetrating each of said respective vacuum jackets.
4. An assembly according to claim 3 including means to circulate a liquid cryogen through each of said cooling coils.
5. An assembly according to claim 4 wherein said liquid cryogen is selected from the group consisting of nitrogen and helium.
6. A superconducting magnet assembly according to claim 1 including means to separately energize each of said magnet coils.
7. A superconducting magnet assembly according to claim 1 including means to generate opposing magnetic fields in said magnet coils.
8. A superconducting magnet assembly according to claim 1 wherein each of said magnet coils consists of multiple turns of niobium titanium superconducting filaments wound onto an aluminum mandrel and vacuum impregnated to produce a coil structure.
9. A superconducting magnet assembly according to claim 8 wherein each magnetic coil includes an external iron yoke.
10. A method for cooling a superconducting magnet having two separate toroidally shaped superconducting magnet coils positioned in spaced apart relationship to define access to a magnetic field along an X, Y, and Z axis originating from the center of the magnetic field, each of said magnet coils contained within and spaced apart from an outer vacuum jacket; at least one radiation shield disposed within each of said vacuum jackets between each of said magnet coils and its vacuum jacket; a separate two stage closed cycle refrigerator to cool each of said magnet coils to a temperature at which said magnet coils exhibit superconductivity and each of said radiation shields to a temperature above said temperature to which said magnet coils are cooled, and individual cooling coils fabricated from a tubular conductive metal wrapped around each of said magnet coils, each of said cooling coils having an inlet and outlet penetrating each of said respective vacuum jackets; comprising the steps of energizing said refrigerators to cool said magnet coils and said radiation shields and circulating a liquid cryogen through each of said cooling coils.
11. A method according to claim 10 including the step of selecting said liquid cryogen from the group consisting of liquid nitrogen, and liquid helium.
12. A method according to claim 10 including the step of separately energizing each of said magnet coils.
13. A method according to claim 10 including the step of generating opposing magnetic fields in said magnet coils.
14. A method according to claim 10 including the step of delaying energizing of said refrigerators for a period of time while circulating liquid cryogen through said cooling coils.
15. A method according to claim 10 including the steps of first introducing liquid nitrogen into said cooling coils for a set period of time to pre-cool said magnet coils, followed by introducing liquid helium into said cooling coils to cool said magnet coils to a desired operating temperature.
PCT/US2001/041829 2000-08-25 2001-08-22 Liquid cryogen-free superconducting magnet system WO2002059917A1 (en)

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Families Citing this family (19)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP3698099B2 (en) * 2001-12-14 2005-09-21 株式会社日立製作所 Magnet for magnetic resonance imaging equipment
DE10201322B4 (en) * 2002-01-15 2004-05-06 Siemens Ag Switching device of superconductivity technology
US20050144971A1 (en) * 2003-07-21 2005-07-07 Zabtcioglu Fikret M. Super energy efficient refrigeration system with refrigerant of nitrogen gas and a closed cycle turbo fan air chilling
JP4288130B2 (en) * 2003-09-30 2009-07-01 東京エレクトロン株式会社 Electrical joining member and plasma processing apparatus
US20080209919A1 (en) * 2007-03-01 2008-09-04 Philips Medical Systems Mr, Inc. System including a heat exchanger with different cryogenic fluids therein and method of using the same
EP1970935B1 (en) * 2007-03-14 2011-01-12 ICT, Integrated Circuit Testing Gesellschaft für Halbleiterprüftechnik mbH Lens coil cooling of a magnetic lens
CN101889213A (en) 2007-12-10 2010-11-17 皇家飞利浦电子股份有限公司 Superconducting magnet system with cooling system
EP2310768B1 (en) * 2008-05-21 2018-12-26 Brooks Automation, Inc. Linear drive cryogenic refrigerator
JP2012523946A (en) * 2009-04-20 2012-10-11 タイム メディカル ホールディングス カンパニー リミテッド Cryogenically cooled superconducting RF head coil array and head-only magnetic resonance imaging (MRI) system using the same
EP2519786B1 (en) 2009-12-28 2019-03-27 Koninklijke Philips N.V. Cryo-cooling system with a tubular thermal switch
US8610434B2 (en) 2011-07-21 2013-12-17 ColdEdge Technologies, Inc. Cryogen-free cooling system for electron paramagnetic resonance system
US11099247B2 (en) 2012-01-27 2021-08-24 Bruker Biospin Corporation Ultra-low vibration cryogen-free cryostat for an electron paramagnetic resonance system
US9714992B2 (en) * 2014-01-23 2017-07-25 Shahin Pourrahimi Versatile superconducting magnet for extremities magnetic resonance imaging
EP2972443B1 (en) * 2013-03-06 2018-01-17 Shahin Pourrahimi Versatile superconducting magnet for extremities magnetic resonance imaging
WO2015071795A1 (en) 2013-11-13 2015-05-21 Koninklijke Philips N.V. Superconducting magnet system including thermally efficient ride-through system and method of cooling superconducting magnet system
US9190197B2 (en) * 2014-02-26 2015-11-17 Shahin Pourrahimi Superconducting magnet operating in occasional idling mode
CN112038033B (en) * 2020-08-13 2022-05-31 中国科学院合肥物质科学研究院 2T conduction cooling superconducting magnet for magnetic resonance imaging
CN114597618A (en) * 2020-12-07 2022-06-07 中国科学院理化技术研究所 Low-temperature system of high-temperature superconducting filter
JP2022161154A (en) * 2021-04-08 2022-10-21 住友重機械工業株式会社 Superconducting magnet device and cyclotron

Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4689591A (en) * 1985-01-04 1987-08-25 Oxford Magnet Technology Limited Magnet assemblies for use in magnetic resonance imaging
US5412363A (en) * 1991-12-20 1995-05-02 Applied Superconetics, Inc. Open access superconducting MRI magnet
EP0937953A1 (en) * 1998-02-19 1999-08-25 Oxford Instruments (Uk) Limited Refrigerator
EP0971240A2 (en) * 1998-07-09 2000-01-12 General Electric Company Helium vessel for open architecture magnetic resonance imaging superconducting magnet

Family Cites Families (21)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4924198A (en) 1988-07-05 1990-05-08 General Electric Company Superconductive magnetic resonance magnet without cryogens
US5103647A (en) 1991-02-19 1992-04-14 General Electric Company Dynamically balanced Gifford-McMahon refrigerator cold head
JP3123126B2 (en) 1991-07-15 2001-01-09 株式会社日立製作所 Vacuum container with cooler
US5301507A (en) 1992-08-03 1994-04-12 General Electric Company Superconducting magnetic energy storage device
US5394129A (en) 1992-09-03 1995-02-28 General Electric Company Superconducting switch thermal interface for a cryogenless superconducting magnet
US5489848A (en) * 1992-09-08 1996-02-06 Kabushiki Kaisha Toshiba Magnetic resonance imaging apparatus
JP3347870B2 (en) 1994-04-15 2002-11-20 三菱電機株式会社 Superconducting magnet and regenerative refrigerator for the magnet
US5448214A (en) 1994-06-15 1995-09-05 General Electric Company Open MRI magnet with superconductive shielding
US5442928A (en) 1994-08-05 1995-08-22 General Electric Hybrid cooling system for a superconducting magnet
US5517169A (en) 1994-10-17 1996-05-14 General Electric Company Superconducting magnet with magnetic shielding
JP3265139B2 (en) * 1994-10-28 2002-03-11 株式会社東芝 Cryogenic equipment
US5757243A (en) 1995-05-25 1998-05-26 Matsushita Electric Industrial Co., Ltd. High frequency system including a superconductive device and temperature controlling apparatus
DE19533555A1 (en) 1995-09-11 1997-03-13 Siemens Ag Device for indirect cooling of an electrical device
US5563566A (en) 1995-11-13 1996-10-08 General Electric Company Cryogen-cooled open MRI superconductive magnet
DE19547030A1 (en) * 1995-12-15 1997-06-19 Leybold Ag Low-temperature refrigerator with a cold head and process for optimizing the cold head for a desired temperature range
JP3654463B2 (en) * 1996-03-29 2005-06-02 株式会社日立メディコ Magnetic resonance imaging system
US5651256A (en) 1996-05-31 1997-07-29 General Electric Company Superconductive magnet having a thermal shield
US5939962A (en) * 1996-08-07 1999-08-17 Mitsubishi Denki Kabushiki Kaisha Split type magnetic field generating apparatus for MRI
US5932096A (en) * 1996-09-18 1999-08-03 Hitachi, Ltd. Magnetic purifying apparatus for purifying a fluid
JP3702063B2 (en) * 1997-02-25 2005-10-05 株式会社東芝 Thermal insulation container, thermal insulation device, and thermal insulation method
JPH10282200A (en) 1997-04-09 1998-10-23 Aisin Seiki Co Ltd Cooler for superconducting magnet system

Patent Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4689591A (en) * 1985-01-04 1987-08-25 Oxford Magnet Technology Limited Magnet assemblies for use in magnetic resonance imaging
US5412363A (en) * 1991-12-20 1995-05-02 Applied Superconetics, Inc. Open access superconducting MRI magnet
EP0937953A1 (en) * 1998-02-19 1999-08-25 Oxford Instruments (Uk) Limited Refrigerator
EP0971240A2 (en) * 1998-07-09 2000-01-12 General Electric Company Helium vessel for open architecture magnetic resonance imaging superconducting magnet

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