US20060021355A1 - Cryostat configuration - Google Patents
Cryostat configuration Download PDFInfo
- Publication number
- US20060021355A1 US20060021355A1 US11/183,941 US18394105A US2006021355A1 US 20060021355 A1 US20060021355 A1 US 20060021355A1 US 18394105 A US18394105 A US 18394105A US 2006021355 A1 US2006021355 A1 US 2006021355A1
- Authority
- US
- United States
- Prior art keywords
- cryostat configuration
- neck tube
- helium
- cold
- cryocooler
- Prior art date
- 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.)
- Abandoned
Links
- 239000001307 helium Substances 0.000 claims abstract description 65
- 229910052734 helium Inorganic materials 0.000 claims abstract description 65
- SWQJXJOGLNCZEY-UHFFFAOYSA-N helium atom Chemical compound [He] SWQJXJOGLNCZEY-UHFFFAOYSA-N 0.000 claims abstract description 65
- 239000000725 suspension Substances 0.000 claims abstract description 44
- 239000007789 gas Substances 0.000 claims abstract description 35
- 230000005855 radiation Effects 0.000 claims abstract description 16
- 239000007788 liquid Substances 0.000 claims abstract description 11
- IJGRMHOSHXDMSA-UHFFFAOYSA-N Atomic nitrogen Chemical compound N#N IJGRMHOSHXDMSA-UHFFFAOYSA-N 0.000 claims description 36
- 229910052757 nitrogen Inorganic materials 0.000 claims description 17
- 238000005481 NMR spectroscopy Methods 0.000 claims description 10
- 238000009413 insulation Methods 0.000 claims description 9
- 238000002595 magnetic resonance imaging Methods 0.000 claims description 3
- 239000000463 material Substances 0.000 claims description 3
- 238000001816 cooling Methods 0.000 description 15
- 238000001704 evaporation Methods 0.000 description 4
- 230000005540 biological transmission Effects 0.000 description 2
- 230000007423 decrease Effects 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 238000000034 method Methods 0.000 description 2
- 238000009833 condensation Methods 0.000 description 1
- 230000008020 evaporation Effects 0.000 description 1
- 230000002349 favourable effect Effects 0.000 description 1
- 238000009434 installation Methods 0.000 description 1
- 238000012423 maintenance Methods 0.000 description 1
- 230000007704 transition Effects 0.000 description 1
Images
Classifications
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- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F25—REFRIGERATION OR COOLING; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS; MANUFACTURE OR STORAGE OF ICE; LIQUEFACTION SOLIDIFICATION OF GASES
- F25D—REFRIGERATORS; COLD ROOMS; ICE-BOXES; COOLING OR FREEZING APPARATUS NOT OTHERWISE PROVIDED FOR
- F25D19/00—Arrangement or mounting of refrigeration units with respect to devices or objects to be refrigerated, e.g. infrared detectors
-
- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F25—REFRIGERATION OR COOLING; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS; MANUFACTURE OR STORAGE OF ICE; LIQUEFACTION SOLIDIFICATION OF GASES
- F25B—REFRIGERATION MACHINES, PLANTS OR SYSTEMS; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS
- F25B9/00—Compression machines, plants or systems, in which the refrigerant is air or other gas of low boiling point
- F25B9/14—Compression machines, plants or systems, in which the refrigerant is air or other gas of low boiling point characterised by the cycle used, e.g. Stirling cycle
- F25B9/145—Compression machines, plants or systems, in which the refrigerant is air or other gas of low boiling point characterised by the cycle used, e.g. Stirling cycle pulse-tube cycle
-
- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F25—REFRIGERATION OR COOLING; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS; MANUFACTURE OR STORAGE OF ICE; LIQUEFACTION SOLIDIFICATION OF GASES
- F25B—REFRIGERATION MACHINES, PLANTS OR SYSTEMS; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS
- F25B2309/00—Gas cycle refrigeration machines
- F25B2309/14—Compression machines, plants or systems characterised by the cycle used
- F25B2309/1408—Pulse-tube cycles with pulse tube having U-turn or L-turn type geometrical arrangements
-
- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F25—REFRIGERATION OR COOLING; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS; MANUFACTURE OR STORAGE OF ICE; LIQUEFACTION SOLIDIFICATION OF GASES
- F25B—REFRIGERATION MACHINES, PLANTS OR SYSTEMS; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS
- F25B2400/00—General features or devices for refrigeration machines, plants or systems, combined heating and refrigeration systems or heat-pump systems, i.e. not limited to a particular subgroup of F25B
- F25B2400/17—Re-condensers
-
- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F25—REFRIGERATION OR COOLING; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS; MANUFACTURE OR STORAGE OF ICE; LIQUEFACTION SOLIDIFICATION OF GASES
- F25B—REFRIGERATION MACHINES, PLANTS OR SYSTEMS; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS
- F25B9/00—Compression machines, plants or systems, in which the refrigerant is air or other gas of low boiling point
- F25B9/10—Compression machines, plants or systems, in which the refrigerant is air or other gas of low boiling point with several cooling stages
-
- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F25—REFRIGERATION OR COOLING; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS; MANUFACTURE OR STORAGE OF ICE; LIQUEFACTION SOLIDIFICATION OF GASES
- F25D—REFRIGERATORS; COLD ROOMS; ICE-BOXES; COOLING OR FREEZING APPARATUS NOT OTHERWISE PROVIDED FOR
- F25D19/00—Arrangement or mounting of refrigeration units with respect to devices or objects to be refrigerated, e.g. infrared detectors
- F25D19/006—Thermal coupling structure or interface
Definitions
- the invention concerns a cryostat configuration for keeping liquid helium, comprising an outer jacket and a helium container installed therein, wherein the helium container is connected to the outer jacket via at least two suspension tubes, wherein the helium container also contains a neck tube whose upper warm end is connected to the jacket and whose lower cold end is connected to the helium container, the neck tube containing a multi-stage cold head of a cryocooler, wherein the outer jacket, the helium container, the suspension tubes and the neck tube delimit an evacuated space, and wherein the helium container is surrounded by at least one radiation shield which is connected in a heat-conducting fashion to the suspension tubes and to the neck tube of the helium container.
- the e.g. two-stage cryocooler cold head is usually installed into a separate vacuum chamber (as described e.g. in U.S. Pat. No. 5,613,367) or directly in the vacuum chamber of the cryostat (as described e.g. in U.S. Pat. No. 5,563,566) such that the first cold stage of the cold head is rigidly connected to a radiation shield and the second cold stage is connected to the helium container in a heat-conducting fashion, either directly or via a fixed, rigid or flexible thermal bridge.
- the overall heat input into the helium container can be compensated for by re-condensation of the helium, which is evaporated due to external heat input, on the cold contact surface in the helium container to obtain loss-free operation of the system.
- the connection between the second cold stage and the helium container has a thermal resistance.
- One possibility to avoid this thermal resistance is to insert the cold head into a neck tube which connects the external vacuum shell (outer jacket) of the cryostat to the helium container and is correspondingly filled with helium gas, as is described e.g. in US2002/0002830.
- the first cold stage of the two-stage cold head is in fixed heat-conducting contact with a radiation shield and the second cold stage is freely suspended in the helium atmosphere to directly liquefy evaporated helium.
- the cold head is surrounded by helium gas and since there is a temperature difference between the cold head and the neck tube wall or further structural elements of the neck tube, a considerable amount of heat may be transferred between the tube wall and the cold head due to thermal conduction in the gas as well as convection currents.
- WO03036207 and WO03036190 therefore propose insulating the cold head tubes. Heat conduction in the helium gas column and in the neck tube wall from the top to the bottom produces further heat input into the helium container.
- US2002/0002830 therefore proposes installation of a separating sleeve around the cold head, which is open at the top and at the bottom to guide a gas flow such that the gas rises on the neck tube wall thereby absorbing the heat conducted in the tube and being heated.
- the gas is deflected on the upper warm end and flows downwardly along the tubes of the cold head, thereby being cooled and finally being re-liquefied at the cold end of the cold head.
- the cryocooler thereby loses some cooling power as is e.g. disclosed in the publication “Helium liquefaction with a 4 K pulse tube cryocooler” (Cryogenics 41 (2001) 491-496).
- the helium container is usually connected to the outer vacuum jacket at at least two thin-walled suspension tubes.
- the helium container housing the superconducting magnet is thereby mechanically fixed and the suspension tubes simultaneously provide access to the magnet as is required e.g. for charging and also for refilling liquid helium.
- the boil-off gas is additionally discharged via the suspension tubes thereby cooling the suspension tubes and, in the ideal case, completely compensating the heat input via the tube wall.
- This object is achieved in accordance with the invention in that there is a direct connection between the warm ends of the suspension tubes and the neck tube through which the helium gas can flow.
- a gas flow occurs automatically which is excited and maintained by a suction-effect at the cold end of the cold head.
- the evaporating gas thereby cools the wall of the suspension tubes, in the ideal case, such that the heat input into the helium container through the suspension tubes is eliminated.
- the gas is thereby heated, exits the suspension tubes at approximately room temperature, and re-enters into the neck tube at the room temperature flange of the cold head.
- the gas from the different suspension tubes is advantageously combined in one line and then guided to the neck tube.
- the gas Due to the downward flow in the neck tube, the gas is cooled on the tubes of the cold head or on the neck tube, and is finally liquefied at the second cold stage of the cold head, thereby closing the cycle.
- the suction which maintains the flow, is generated i.a. through the phase transition from gaseous to liquid in the region of the second cold stage.
- the overall power of the cryocooler slightly decreases but the gain due to the reduced heat input is larger than the cooling power loss. Especially for systems with more massive suspension tubes, use of a less powerful cryocooler is therefore possible compared to the case without a circulating flow.
- the cold head of the cryocooler has several cooling stages. Therefore very low temperatures, in particular, temperatures in a range of 4K or less are possible.
- the cryocooler advantageously is a pulse tube cooler, since pulse tube coolers can be operated with extremely low vibration. Pulse tube coolers are also very reliable and require little maintenance. In principle, other cryocoolers such as e.g. Gifford-McMahon coolers can also be used.
- helium can be liquefied at a temperature of 4.2 K or less at the coldest cold stage of the cold head to provide a plurality of different applications in the region of very low temperatures.
- the helium which is evaporated within the cryostat is liquefied at the cold stage which is freely suspended in the neck tube, and drips back into the helium container. This reduces helium loss and the number of refilling processes or permits no-loss operation if the cooling power of the cooler is sufficiently large.
- the tubes of the cold head above the first cold stage and possibly also in the region of further cold stages are surrounded by a thermal insulation to eliminate or at least reduce undesired heat input from the neck tube into the tubes of the cold head.
- the tubes above the first cold stage of the cold head have temperatures between room temperature and the temperature of the first cold stage.
- a gap or channel is provided between the heat insulation and the neck tube wall, through which the gas can flow to provide sufficiently good thermal contact between the gas and the tube wall.
- the neck tube has no mechanical support function.
- the neck tube may have a thin wall and/or be designed like a bellows and be made from a material having poor thermal conductivity. In this manner, the heat input into the helium container is only small and at the same time, the transmission of vibrations via the neck tube is minimized.
- a preferably electric heater is provided in the helium container or in contact therewith to keep the pressure in the helium container at a constant value above the surrounding pressure in case of surplus cooling capacity of the cryocooler. It is, however, also feasible to control the power of the cooler via its operating frequency and/or the amount of the working gas (i.e. the gas pressure) in the cooler.
- one or more cold stages of the cold head are connected to one or more radiation shield(s) in a heat-conducting manner.
- the radiation shield(s) can then be directly cooled by the cold head.
- the or one of the radiation shield(s) include(s) a container with liquid nitrogen to which the cold head is connected in a heat-conducting manner, wherein the cold head of the cryocooler at least partially re-liquefies the nitrogen after evaporation.
- the nitrogen is liquefied through thermal connection between the radiation shield and the cold head of the cryocooler.
- the radiation shield is not cooled directly by the cooler but indirectly via the evaporating nitrogen.
- a preferably electric heater is provided in the nitrogen container or in contact therewith to keep the pressure in the nitrogen container at a constant level above the surrounding pressure in case of surplus cooling capacity of the cryocooler.
- the connecting line between suspension tubes and neck tube has a valve to control the gas flow.
- the gas flow can be reduced if required, e.g. if the suction effect on the cold head is so large that the gas flow exceeds that which would be sufficient for optimum cooling of the suspension tubes.
- a controllable circulating pump is provided in the connecting line between the suspension tubes and the neck tube for actively controlling the cooling flow.
- cryostat configuration contains a superconducting magnet arrangement, in particular, if the superconducting magnet arrangement is part of a magnetic resonance apparatus, in particular, magnetic resonance imaging (MRI) or nuclear magnetic resonance spectroscopy (NMR).
- MRI magnetic resonance imaging
- NMR nuclear magnetic resonance spectroscopy
- FIG. 1 shows a schematic view of an inventive cryostat configuration
- FIG. 2 shows a schematic view of an inventive cryostat configuration with insulated cold head tubes
- FIG. 3 shows a schematic view of an inventive cryostat configuration with a nitrogen tank
- FIG. 4 shows a schematic section of an inventive cryostat configuration with a valve which is integrated in the connecting line
- FIG. 5 shows a schematic section of an inventive cryostat configuration with a pump which is integrated in the connecting line.
- FIG. 1 shows a schematic view of an inventive cryostat configuration with a helium container 1 which is connected to the outer jacket 3 via at least two suspension tubes 2 .
- the helium container 1 is surrounded by a radiation shield 4 and moreover comprises a neck tube 5 which contains the cold head 6 of a cryocooler.
- the neck tube 5 only serves as a separating wall for an evacuated region 7 of the outer jacket 3 and need not bear the weight of the helium container 1 . For this reason, it may be designed such that the heat input and the vibration transmission can be minimized, which is advantageously realized using a bellows.
- the weight of the helium container 1 and of a superconducting magnet arrangement 26 disposed in the helium container is borne by the suspension tubes 2 which are connected to the warm end 9 of the neck tube 5 via a line 8 .
- a gas flow 10 occurs automatically and is excited and maintained by the suction effect at the cold end 11 of the cold head 6 .
- the evaporated helium thereby cools the wall 12 of the suspension tubes 2 (ideally to that extent that the heat input into the helium container 1 via the suspension tubes 2 is eliminated), is thereby heated, exits the suspension tubes 2 at approximately room temperature, and re-enters the neck tube 5 at a room temperature flange 13 of the cold head 6 .
- the gas Due to the downward gas flow 10 , the gas is cooled on the tubes 14 of the cold head 6 or on the neck tube 5 and is subsequently liquefied at the second cold stage 15 of the cold head 6 .
- the cycle is thereby closed.
- the power of the cryocooler thereby slightly decreases, but the gain due to the reduced heat input is larger than the cooling power loss.
- a less powerful cryocooler can be used than without circulating flow.
- the partial gas flows through the various suspension tubes 2 are advantageously combined in one line 8 .
- the cold head 6 may also be provided with thermal insulation 16 to reduce heat exchange between the neck tube 5 and the tubes 14 of the cold head 6 .
- FIG. 2 shows thermal insulation 16 between the room temperature flange 13 and the first cold stage 17 of the two-stage cold head 6 .
- the tubes of further cold stages may also be thermally insulated by insulation 16 . It is only important to provide a sufficiently large gap 19 between the thermal insulation 16 and the neck tube wall 18 to permit sufficiently good thermal contact between the gas and the neck tube wall 18 .
- the neck tube wall 18 of the present invention is not cooled by a gas flowing towards the warm end. As already mentioned above, the contribution of the heat input via the neck tube wall 18 is rather small in the present case compared to the overall heat input.
- Indirect cooling of the radiation shield 4 similar to a non-actively cooled system (i.e. without cryocooler)—using evaporating nitrogen is also possible ( FIG. 3 ).
- the first cold stage 17 of the cold head 6 of the cryocooler must be connected to a nitrogen container 20 in a heat-conducting manner such that nitrogen which evaporates can be re-liquefied on the cold contact surface 21 .
- a flow impedance (e.g. a valve 22 ) may be integrated in the connecting line 8 ( FIG. 4 ) to control the gas flow.
- the cooling flow can be actively controlled using a pump 23 ( FIG. 5 ).
- the valve 22 or pump 23 may also be installed together in the connecting line 8 .
- the partial gas-flows of the different suspension tubes 2 are preferably initially combined in a connecting line 8 before integrating a valve 22 or a pump 23 .
- the pressure in the helium container 1 (and possibly also in the nitrogen container 20 ) is advantageously kept at a constant level above the surrounding pressure.
- This can be realized using a heater 24 in the liquid helium ( FIG. 1 , FIG. 2 and FIG. 3 ) or using a heater in the liquid nitrogen 25 ( FIG. 3 ).
- the inventive cryostat configuration is particularly suited for cooling a magnet arrangement 26 which is part of an apparatus for magnetic resonance, in particular, magnetic resonance imaging (MRI) or nuclear magnetic resonance spectroscopy (NMR).
- MRI magnetic resonance imaging
- NMR nuclear magnetic resonance spectroscopy
- the inventive cryostat configuration considerably reduces, in particular, the heat input via the suspension tubes of an actively cryocooler-cooled high-resolution NMR magnet system thereby permitting use of a less powerful cryocooler.
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- Engineering & Computer Science (AREA)
- Physics & Mathematics (AREA)
- Mechanical Engineering (AREA)
- Thermal Sciences (AREA)
- General Engineering & Computer Science (AREA)
- Chemical & Material Sciences (AREA)
- Combustion & Propulsion (AREA)
- Containers, Films, And Cooling For Superconductive Devices (AREA)
- Magnetic Resonance Imaging Apparatus (AREA)
- Filling Or Discharging Of Gas Storage Vessels (AREA)
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
DE102004037172.5 | 2004-07-30 | ||
DE102004037172A DE102004037172B4 (de) | 2004-07-30 | 2004-07-30 | Kryostatanordnung |
Publications (1)
Publication Number | Publication Date |
---|---|
US20060021355A1 true US20060021355A1 (en) | 2006-02-02 |
Family
ID=35457012
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
US11/183,941 Abandoned US20060021355A1 (en) | 2004-07-30 | 2005-07-19 | Cryostat configuration |
Country Status (4)
Country | Link |
---|---|
US (1) | US20060021355A1 (fr) |
EP (1) | EP1628109B1 (fr) |
JP (1) | JP3996935B2 (fr) |
DE (1) | DE102004037172B4 (fr) |
Cited By (29)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US20090007573A1 (en) * | 2004-11-09 | 2009-01-08 | Oxford Instruments Superconductivity Limited | Cryostat assembly |
US20090049863A1 (en) * | 2007-08-21 | 2009-02-26 | Cryomech, Inc. | Reliquifier and recondenser |
US20090145910A1 (en) * | 2007-12-11 | 2009-06-11 | Searete Llc, A Limited Liability Corporation Of The State Of Delaware | Temperature-stabilized storage containers with directed access |
US20090145912A1 (en) * | 2007-12-11 | 2009-06-11 | Searete Llc, A Limited Liability Corporation Of The State Of Delaware | Temperature-stabilized storage containers |
US20090145164A1 (en) * | 2007-12-11 | 2009-06-11 | Searete Llc, A Limited Liability Corporation Of The State Of Delaware | Temperature-stabilized storage systems |
US20090283534A1 (en) * | 2008-05-13 | 2009-11-19 | Searete Llc | Storage container including multi-layer insulation composite material having bandgap material and related methods |
US20090286022A1 (en) * | 2008-05-13 | 2009-11-19 | Searete Llc | Multi-layer insulation composite material including bandgap material, storage container using same, and related methods |
US20100213200A1 (en) * | 2007-12-11 | 2010-08-26 | Searete Llc, A Limited Liability Corporation Of The State Of Delaware | Temperature-stabilized storage systems |
US20110155745A1 (en) * | 2007-12-11 | 2011-06-30 | Searete LLC, a limited liability company of the State of Delaware | Temperature-stabilized storage systems with flexible connectors |
US20110219785A1 (en) * | 2010-03-11 | 2011-09-15 | Quantum Design, Inc. | Method and apparatus for controlling temperature in a cryocooled cryostat using static and moving gas |
WO2012074549A1 (fr) * | 2010-11-29 | 2012-06-07 | Tokitae Llc | Systèmes de stockage stabilisés en température |
US20120167598A1 (en) * | 2010-09-14 | 2012-07-05 | Quantum Design, Inc. | Vacuum isolated multi-well zero loss helium dewar |
US8215835B2 (en) | 2007-12-11 | 2012-07-10 | Tokitae Llc | Temperature-stabilized medicinal storage systems |
US8322147B2 (en) | 2007-12-11 | 2012-12-04 | Tokitae Llc | Methods of manufacturing temperature-stabilized storage containers |
DE102011078608A1 (de) | 2011-07-04 | 2013-01-10 | Bruker Biospin Ag | Kryostatanordnung |
US8377030B2 (en) | 2007-12-11 | 2013-02-19 | Tokitae Llc | Temperature-stabilized storage containers for medicinals |
US8603598B2 (en) | 2008-07-23 | 2013-12-10 | Tokitae Llc | Multi-layer insulation composite material having at least one thermally-reflective layer with through openings, storage container using the same, and related methods |
US8887944B2 (en) | 2007-12-11 | 2014-11-18 | Tokitae Llc | Temperature-stabilized storage systems configured for storage and stabilization of modular units |
US9140476B2 (en) | 2007-12-11 | 2015-09-22 | Tokitae Llc | Temperature-controlled storage systems |
US20150348689A1 (en) * | 2013-01-06 | 2015-12-03 | Institute Of Electrical Engineering, Chinese Academy Of Sciences | Superconducting Magnet System for Head Imaging |
US20160055949A1 (en) * | 2013-03-27 | 2016-02-25 | Japan Superconductor Technology Inc. | Cryostat |
US9372016B2 (en) | 2013-05-31 | 2016-06-21 | Tokitae Llc | Temperature-stabilized storage systems with regulated cooling |
US9447995B2 (en) | 2010-02-08 | 2016-09-20 | Tokitac LLC | Temperature-stabilized storage systems with integral regulated cooling |
GB2540268A (en) * | 2015-07-01 | 2017-01-11 | Bruker Biospin Gmbh | Cryostat with active neck tube cooling by a second cryogen |
US20180144852A1 (en) * | 2016-11-24 | 2018-05-24 | Japan Superconductor Technology Inc. | Superconducting coil pre-cooling method and superconducting magnet apparatus |
US10839998B2 (en) * | 2017-10-09 | 2020-11-17 | Bruker Switzerland Ag | Magnet assembly with cryostat and magnet coil system, with cold reservoirs on the current leads |
US20210199377A1 (en) * | 2019-12-27 | 2021-07-01 | Korea Basic Science Institute | Helium gas liquefier and method for liquefying helium gas |
WO2021156103A1 (fr) | 2020-02-07 | 2021-08-12 | Bruker Switzerland Ag | Ensemble de mesure à résonance magnétique nucléaire (rmn) à trou froid du cryostat |
CN117128442A (zh) * | 2023-08-07 | 2023-11-28 | 北京航天试验技术研究所 | 一种恒温恒压低温杜瓦、系统及其方法 |
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JP5833284B2 (ja) * | 2006-03-17 | 2015-12-16 | シーメンス ピーエルシー | 冷却装置 |
JP5728172B2 (ja) * | 2010-06-16 | 2015-06-03 | 株式会社神戸製鋼所 | 再凝縮装置及びこれを備えたnmr分析装置 |
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US5613367A (en) * | 1995-12-28 | 1997-03-25 | General Electric Company | Cryogen recondensing superconducting magnet |
US5744959A (en) * | 1995-12-22 | 1998-04-28 | Spectrospin Ag | NMR measurement apparatus with pulse tube cooler |
US5782095A (en) * | 1997-09-18 | 1998-07-21 | General Electric Company | Cryogen recondensing superconducting magnet |
US5966944A (en) * | 1997-04-09 | 1999-10-19 | Aisin Seiki Kabushiki Kaisha | Superconducting magnet system outfitted with cooling apparatus |
US20020002830A1 (en) * | 2000-07-08 | 2002-01-10 | Bruker Analytik Gmbh | Circulating cryostat |
US20030230089A1 (en) * | 2002-06-14 | 2003-12-18 | Bruker Biospin Gmbh | Cryostat configuration with improved properties |
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DE4106135A1 (de) * | 1991-02-27 | 1992-09-03 | Spectrospin Ag | Kryomagnetsystem mit stoerungsminimiertem low-loss-heliumkryostat |
GB2329701B (en) * | 1997-09-30 | 2001-09-19 | Oxford Magnet Tech | Load bearing means in nmr cryostat systems |
GB2330194B (en) * | 1997-09-30 | 2002-05-15 | Oxford Magnet Tech | A cryogenic pulse tube refrigerator |
GB0121603D0 (en) * | 2001-09-06 | 2001-10-24 | Oxford Instr Superconductivity | Magnet assembly |
GB0125189D0 (en) * | 2001-10-19 | 2001-12-12 | Oxford Magnet Tech | A pulse tube refrigerator |
GB0125188D0 (en) * | 2001-10-19 | 2001-12-12 | Oxford Magnet Tech | A pulse tube refrigerator sleeve |
GB0401835D0 (en) * | 2004-01-28 | 2004-03-03 | Oxford Instr Superconductivity | Magnetic field generating assembly |
DE102004012416B4 (de) * | 2004-03-13 | 2006-04-20 | Bruker Biospin Gmbh | Supraleitendes Magnetsystem mit Pulsrohr-Kühler |
-
2004
- 2004-07-30 DE DE102004037172A patent/DE102004037172B4/de not_active Expired - Fee Related
-
2005
- 2005-07-19 US US11/183,941 patent/US20060021355A1/en not_active Abandoned
- 2005-07-26 EP EP05016143A patent/EP1628109B1/fr not_active Ceased
- 2005-07-29 JP JP2005220786A patent/JP3996935B2/ja not_active Expired - Fee Related
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US8603598B2 (en) | 2008-07-23 | 2013-12-10 | Tokitae Llc | Multi-layer insulation composite material having at least one thermally-reflective layer with through openings, storage container using the same, and related methods |
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CN103282717A (zh) * | 2010-11-29 | 2013-09-04 | 脱其泰有限责任公司 | 温度稳定的储存系统 |
WO2012074549A1 (fr) * | 2010-11-29 | 2012-06-07 | Tokitae Llc | Systèmes de stockage stabilisés en température |
DE102011078608A1 (de) | 2011-07-04 | 2013-01-10 | Bruker Biospin Ag | Kryostatanordnung |
DE102011078608B4 (de) | 2011-07-04 | 2023-06-22 | Bruker Switzerland Ag | Kryostatanordnung |
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US10580555B2 (en) * | 2016-11-24 | 2020-03-03 | Japan Superconductor Technology Inc. | Superconducting coil pre-cooling method and superconducting magnet apparatus |
US20180144852A1 (en) * | 2016-11-24 | 2018-05-24 | Japan Superconductor Technology Inc. | Superconducting coil pre-cooling method and superconducting magnet apparatus |
US10839998B2 (en) * | 2017-10-09 | 2020-11-17 | Bruker Switzerland Ag | Magnet assembly with cryostat and magnet coil system, with cold reservoirs on the current leads |
US20210199377A1 (en) * | 2019-12-27 | 2021-07-01 | Korea Basic Science Institute | Helium gas liquefier and method for liquefying helium gas |
US11965693B2 (en) * | 2019-12-27 | 2024-04-23 | Korea Basic Science Institute | Helium gas liquefier and method for liquefying helium gas |
WO2021156103A1 (fr) | 2020-02-07 | 2021-08-12 | Bruker Switzerland Ag | Ensemble de mesure à résonance magnétique nucléaire (rmn) à trou froid du cryostat |
DE102020201522A1 (de) | 2020-02-07 | 2021-08-12 | Bruker Switzerland Ag | NMR-Messanordnung mit kalter Bohrung des Kryostaten |
US11953570B2 (en) | 2020-02-07 | 2024-04-09 | Bruker Switzerland Ag | NMR measuring assembly with cold bore of the cryostat |
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Also Published As
Publication number | Publication date |
---|---|
DE102004037172A1 (de) | 2006-03-23 |
DE102004037172B4 (de) | 2006-08-24 |
JP2006046897A (ja) | 2006-02-16 |
EP1628109A3 (fr) | 2009-03-25 |
JP3996935B2 (ja) | 2007-10-24 |
EP1628109B1 (fr) | 2012-06-13 |
EP1628109A2 (fr) | 2006-02-22 |
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