This invention relates to improving the configuration of a heat station that transfers heat from a circulating cryogen cooling an external load to the reciprocating flow of gas internal to the cold end of a high capacity expander operating on the GM or Stirling cycle, producing refrigeration at cryogenic temperatures.
GM and Stirling cycle refrigerators produce refrigeration at cryogenic temperatures in an expander by flowing gas at a high pressure through a regenerator type heat exchanger to the cold end of a piston reciprocating in a cylinder as the displaced volume is increasing, then lowering the pressure and flowing the gas back through the regenerator as the piston reduces the displaced volume. Refrigeration is made available to cool a load by conduction of heat through the walls of the cold end cap of the cylinder, that encloses the cold displaced volume. The cold end cap and means for transferring heat to the gas in the expander is referred to as the cold heat station.
Most cryogenic refrigerators that are used to cool cryopumps, superconducting MRI magnets, and laboratory research instruments use GM type refrigerators. Most of these applications require relatively small amounts of cooling, 1 to 50 W, at temperatures between 4 and 70 K that is transferred to the refrigerator heat station by conduction. There is now a growing need for refrigerators that can cool loads of 300 to 1,000 W at temperatures near 75 K, which can be cooled most practically by a circulating cryogen. The cryogen can be circulated as a gas by a cold fan or room temperature compressor, as a liquid by a pump, or as a gas or liquid by natural convection. The simplest form of natural convection is to condense a cryogen and have the liquid drain to a load where it evaporates, then returns to the condensing surface as a gas.
It is the object of this invention to provide a high capacity GM expander with a cold heat station that can cool or condense a cryogen, is compact, efficient, and easy to mount and connect to the circulating piping. This requires minimizing the temperature difference between the circulating cryogen and the gas in the expander while minimizing the pressure drop of the circulating cryogen that is flowing through the heat station. Minimizing the pressure drop is important because the power input to a cold fan or pump becomes part of the heat load on the refrigerator. Minimizing the temperature difference involves the design of the internal and external heat exchangers that transfers heat from the circulating gas, through the cold end cap to the internal heat exchanger, which transfers heat to the gas in the expander.
U.S. Pat. No. 4,277,949 to Longsworth shows a system that transfers heat from a remote load using helium that is circulated by a compressor at room temperature cooled by tubes wrapped around the expander heat stations. Loads at different temperatures are connected to the circulating helium by convective couplings which enable the load to be thermally disconnected from the refrigerator. An example of a system that cools a remote load by natural convection of a condensing cryogen is described in U.S. Pat. No. 8,375,742 to Wang.
The heat station of this invention involves the novel combination of several components that enable an advantageous way to mount the expander. The advantageous way to mount the expander requires a compact heat station at the cold end of the expander so that the size of the hole in the mounting plate is minimized and the attachment of the circulating tubes is simplified. Heat exchangers that have been known to be used between the regenerator and expansion space in regenerative expanders include an annular gap, perforated plates, wire screens, corrugated sheet metal, and slots that are cut by wire electric discharge machining (EDM), milling or sawing. Narrow slots that create fins between the slots can be sized to have the best heat transfer relative to pressure drop and void volume.
It is advantageous to form closely spaced fins by using a folded copper ribbon. The ribbon can be formed to have a good balance between the three functional properties, heat transfer, pressure drop, and void volume, at a much lower cost than any of the machining methods. It can even be formed into narrower gaps than can be machined and can be stretched or compressed to change the relationships between the three functional properties.
Folded ribbons can be used to optimize heat transfer in the expander cold end, and more advantageously can be optimized for transferring heat from the circulating flow of cryogen that is bringing heat from a remote load to the outside of the expander cold end. An optimum geometry has been found to be to have an external folded ribbon, that is removing heat from the load, thermally bonded to the outside of a cylindrical cold heat station, and have fins, formed by machined slots or an internal folded ribbon, thermally bonded to the inside of the cold heat station. Heat is thus transferred radially directly from the external folded ribbon on the (copper) heat station shell to the internal fins with a minimal temperature difference. The reason why fins formed by a folded ribbon are more advantageous on the outside of the cold heat station than the inside is because there is no concern for void volume in the external fins thus the surface area and the flow area can be large and the cost advantage is much greater. The folded ribbon requires less material than machined fins and thus is more compact. This arrangement of internal and external heat exchangers enables the diameter of the cold end to be minimized and thus the mounting hole in the vacuum housing can be minimized. A small mounting hole is only possible however if there are no radial fittings on the cold heat station. A novel way of circulating cryogen within the outer housing enables having the tubes that connect to the circulating cryogen mounted on the bottom.
Heat is transferred most efficiently from a load if the circulating cryogen condenses in the external fins and evaporates at the load. Nitrogen can be used to condense and evaporate for loads in the temperature range of about 65 K to 85 K and neon can be used for loads in the temperature range of about 22 K to 35 K. Helium can be used at any temperature within the range of the refrigerators that use helium as a refrigerant.
The present invention comprises a heat station on a GM expander, for cooling a circulating cryogen, that is compact, efficient, and easy to mount and connect to the circulating piping. The heat station comprises a shell that has external and internal fins thermally connected to it that are aligned parallel to the axis of the shell, in a cylindrical housing that has inlet and outlet ports that connect to the circulating gas piping. The diameter of the housing is minimized by using folded ribbon on the external heat exchanger and locating the inlet and outlet ports on the bottom of the housing so that the diameter of the hole for mounting the expander on the warm flange of the cryostat is minimized. The fins in the external heat exchanger can be configured to allow different circulation patterns in the housing for different cryogens and orientations.
The drawings use the same number to show the same part, and the words up and top refer towards the warm end while down and bottom refer towards the cold end.
The pressure boundary at the cold end of cylinder 2 of expander 100, shown in
Expander 200, shown in
Another means of directing a circulating gaseous cryogen through external heat exchanger 14 is shown in
Expander 300 has an extension 12b below regenerator 3 that has a close fit inside sleeve 17 which in turn has a close fit inside internal heat exchanger 6. Extension 12b has a smaller diameter than displacer 1 and thus divides the cold displaced volume into an inner displaced volume, 5a, and an outer displaced volume, 5b. Seal 49 prevents gas from leaking between displaced volumes 5a and 5b and forces gas to flow through radial passages 15 into cold displaced volume 5b, where some of it remains, and the balance flows through internal heat exchanger 6 into cold displaced volume 5a. Volume 5b is approximately 15% of the total cold displaced volume, which means that only about 85% of the gas that would flow through internal heat exchanger 6 in expanders 100 and 200, flows internal heat exchanger 6 in expander 300. This might be thermodynamically advantageous because the last 15% of the gas that flows out of regenerator 3 is significantly warmer than the first 85% so even though less gas flows through internal heat exchanger 6 it is colder on average.
Table 1 has an example that compares an external heat exchanger made by machining fins on the outside of shell 4 with a folded ribbon. The design is based on transferring 400 W of cooling at 80 K by circulating 5 g/s of helium at 200 kPa in which both designs have the same temperature differences, in the gas and the fins, and the same pressure drop. The thickness of the machined fin is at its root and the weight of copper for the machined fin includes the material removed from the groove.
The folded ribbon is seen to provide a significant reduction in the diameter of housing 16 and the amount of material needed to make the fins.
In the claims top and bottom, and up and down, refer to the expander when the axis is vertical with the cold end down.
Number | Name | Date | Kind |
---|---|---|---|
3334491 | Cowans | Aug 1967 | A |
3600903 | Chellis | Aug 1971 | A |
3620029 | Longsworth | Nov 1971 | A |
3673809 | Bamberg | Jul 1972 | A |
3802211 | Bamberg | Apr 1974 | A |
3851173 | Taylor | Nov 1974 | A |
4277949 | Longsworth | Jul 1981 | A |
4389850 | Sarcia | Jun 1983 | A |
4478046 | Saito | Oct 1984 | A |
4792346 | Sarcia | Dec 1988 | A |
4796430 | Malaker | Jan 1989 | A |
4912932 | Malaker | Apr 1990 | A |
5088289 | Mita | Feb 1992 | A |
5092119 | Sarcia | Mar 1992 | A |
5447034 | Kuriyama | Sep 1995 | A |
5542254 | Pruitt | Aug 1996 | A |
5609034 | Mita | Mar 1997 | A |
5647217 | Penswick | Jul 1997 | A |
5735127 | Pfotenhauer | Apr 1998 | A |
5743091 | Penswick | Apr 1998 | A |
6070414 | Ross | Jun 2000 | A |
6141971 | Hanes | Nov 2000 | A |
6256997 | Longsworth | Jul 2001 | B1 |
6311491 | Conrad | Nov 2001 | B1 |
6327862 | Hanes | Dec 2001 | B1 |
6546738 | Sekiya | Apr 2003 | B2 |
7225859 | Mochizuki et al. | Jun 2007 | B2 |
8375742 | Wang | Feb 2013 | B2 |
8448461 | Longsworth | May 2013 | B2 |
8959929 | Nun | Feb 2015 | B2 |
10274230 | Bao et al. | Apr 2019 | B2 |
10520226 | Morie | Dec 2019 | B2 |
10753653 | Longsworth | Aug 2020 | B2 |
20020088237 | Rudick | Jul 2002 | A1 |
20020134088 | Rudick | Sep 2002 | A1 |
20030019217 | Sekiya | Jan 2003 | A1 |
20030192324 | Smith | Oct 2003 | A1 |
20040026067 | Mochizuki et al. | Feb 2004 | A1 |
20040189105 | Maezawa | Sep 2004 | A1 |
20050120721 | O'Baid | Jun 2005 | A1 |
20050166604 | Park | Aug 2005 | A1 |
20060137339 | Sakamoto | Jun 2006 | A1 |
20070227159 | Murayama | Oct 2007 | A1 |
20080101965 | Zhang | May 2008 | A1 |
20080276626 | Xu | Nov 2008 | A1 |
20090049863 | Wang | Feb 2009 | A1 |
20090079276 | Ueda | Mar 2009 | A1 |
20090193805 | Berchowitz | Aug 2009 | A1 |
20100229572 | Raiju | Sep 2010 | A1 |
20110011079 | Kamen | Jan 2011 | A1 |
20110126553 | Ball-Difazio | Jun 2011 | A1 |
20110126554 | Morris | Jun 2011 | A1 |
20110219810 | Longsworth | Sep 2011 | A1 |
20120085121 | Longsworth | Apr 2012 | A1 |
20120285181 | Dunn | Nov 2012 | A1 |
20120304668 | Xu | Dec 2012 | A1 |
20130074522 | Xu | Mar 2013 | A1 |
20130327065 | Xu | Dec 2013 | A1 |
20140013775 | Koizumi | Jan 2014 | A1 |
20140020407 | Xu | Jan 2014 | A1 |
20140208774 | Morie | Jul 2014 | A1 |
20140374054 | Xu | Dec 2014 | A1 |
20150176867 | Longsworth | Jun 2015 | A1 |
20150253042 | Matsui | Sep 2015 | A1 |
20150276273 | Nakano | Oct 2015 | A1 |
20160097567 | Hiratsuka | Apr 2016 | A1 |
20160123631 | Xu | May 2016 | A1 |
20160216010 | Longsworth | Jul 2016 | A1 |
20160223227 | Nakano | Aug 2016 | A1 |
20160223228 | Nakano | Aug 2016 | A1 |
20160252280 | Suzuki | Sep 2016 | A1 |
20170045043 | Yatsu | Feb 2017 | A1 |
20180023849 | Longsworth | Jan 2018 | A1 |
20180058730 | Le Bordays | Mar 2018 | A1 |
20180066878 | Longsworth | Mar 2018 | A1 |
20180094837 | Morie | Apr 2018 | A1 |
20190011170 | Morie | Jan 2019 | A1 |
Number | Date | Country |
---|---|---|
1231407 | Oct 1999 | CN |
1760604 | Apr 2006 | CN |
1959298 | May 2007 | CN |
103261816 | Aug 2013 | CN |
104534715 | Apr 2015 | CN |
104729137 | Jun 2015 | CN |
206238523 | Jun 2017 | CN |
112011100912 | Jan 2013 | DE |
2741940 | Jun 1997 | FR |
2002-081774 | Mar 2002 | JP |
2002-243291 | Aug 2002 | JP |
2003-028527 | Jan 2003 | JP |
2003-166768 | Jun 2003 | JP |
2016075429 | May 2016 | JP |
1020030028830 | Apr 2003 | KR |
10-2013-0041395 | Apr 2013 | KR |
WO-2010144158 | Dec 2010 | WO |
WO-2011115790 | Sep 2011 | WO |
2016068039 | Aug 2017 | WO |
Entry |
---|
International Preliminary Report on Patentability dated Oct. 15, 2010, from the corresponding International Application No. PCT/US2018/026482. |
Korean Notice of Allowance dated Mar. 25, 2022, for the Corresponding Korean Patent Application No. 10-2020-7031905. |
Chinese Office Action dated Jul. 28, 2021, for the Corresponding Chinese Patent Application No. 201880092077.2. |
Korean Office Action dated Aug. 30, 2021, for the Corresponding Korean Patent Application No. 10-2020-7031905. |
Notice of Reasons for Refusal dated Nov. 2, 2021, for the Corresponding Japanese Patent Application No. 2020-552189. |
Extended European Search Report dated Jan. 5, 2022, for the Corresponding European Patent Application No. 18913476.0. |
Japanese Decision to Grant dated Feb. 1, 2022, for the Corresponding Japanese Patent Application No. 2020-552189. |
Chinese Office Action dated Mar. 7, 2022, for the Corresponding Chinese Patent Application No. 201880092077.2. |
International Search Report and Written Opinion of the International Searching Authority dated Nov. 5, 2019, from the corresponding International Application No. PCT/US2018/026482. |
U.S. Office Action dated Jan. 13, 2020, from related U.S. Appl. No. 15/947,003. |
Notice of Allowance dated Apr. 17, 2020, from related U.S. Appl. No. 15/947,003. |
Number | Date | Country | |
---|---|---|---|
20200318864 A1 | Oct 2020 | US |
Number | Date | Country | |
---|---|---|---|
Parent | 15947003 | Apr 2018 | US |
Child | 16909773 | US |