The present invention relates to a cryogenic apparatus, that is to say an apparatus for low-temperature refrigeration. Such apparatus may enable a specimen to be cooled to a temperature below 10 K, so measurements may be made on the properties of the specimen at such a cold temperature.
A number of different thermo-mechanical devices are known for achieving such low temperatures, for example using pressure cycling of helium gas. For example this may be achieved using a Stirling cooler, a Gifford-McMahon cooler, a pulse tube refrigerator, or a Joule-Thomson cooler. In the case of the Gifford-McMahon cooler, high-pressure helium at a pressure typically between 10 and 30 bar is used as the working fluid, and a cylinder contains a displacer and regenerator. A mechanical valve connects the cylinder to the gas at low pressure and high pressure alternately, and the displacer is moved in synchronisation with the operation of the valve. Gas expansion takes in heat from the environment at one end of the cylinder, so one end of the cylinder may be referred to as a cold head, and is cooled to a low-temperature. However, it is not always convenient to place the specimen directly in contact with the cold head of a thermo-mechanical cooler.
According to the present invention there is provided a cryogenic apparatus, the apparatus comprising: an enclosure; a thermo-mechanical cooler which projects into the enclosure; a sample tube that also projects into the enclosure, with a closed end within the enclosure; a pump having a pump inlet and a pump outlet, and a duct to supply helium gas from the pump outlet into thermal contact with the thermo-mechanical cooler to produce cold helium; wherein the sample tube is provided with a first inlet to allow a fluid into the sample tube in the vicinity of a specimen, and a second inlet to supply fluid to a thermal element in thermal contact with the sample tube in the vicinity of the specimen, and is provided with a first outlet to withdraw fluid from within the sample tube, and is provided with a second outlet to withdraw fluid from the thermal element; wherein the apparatus also comprises a first duct including a first valve to supply the cold helium to the first inlet, and a second duct including a second valve to supply the cold helium to the second inlet; and wherein both the first outlet and the second outlet may be connected to the pump inlet.
The first valve and the second valve may be needle valves, and may be controlled by control rods that extend into the enclosure. The enclosure may be evacuated in use to suppress heat transfer by convection. The thermo-mechanical cooler may be a two-stage cooler, with a first stage that achieves an intermediate cold temperature for example between 40 K and 100 K, for example about 50 K or 60 K. The apparatus may also include a heat shield at the intermediate temperature, the heat shield being in thermal contact with the thermo-mechanical cooler at a position having the intermediate temperature, and enclosing both the sample tube and the second stage of the thermo-mechanical cooler.
The first inlet may comprise a heat exchanger, for example a block of a good thermal conductor such as copper or aluminium, and defining a flow channel for the cold helium. The heat exchanger may also be provided with an electrical heater, so that the temperature of the helium that enters the sample tube from the first inlet is at a predetermined temperature. The first inlet may be below the specimen within the sample tube.
The thermal element to which the second inlet supplies helium may be a heat exchange sleeve which surrounds and is in contact with a portion of the sample tube and so ensures that that portion of the sample tube is in good thermal contact with the heat exchange sleeve. In a modification, the heat exchange sleeve may itself form a section of the sample tube. The thermal element may be above the specimen within the sample tube.
In operation a specimen is attached to one end of a specimen support rod, which is inserted into the sample tube; the specimen support rod may have any suitable cross-section shape, and may be tubular. Any air in the sample tube would then be extracted by a pump. The apparatus can then operate in two different modes. In a first mode, which may be referred to as a dynamic mode, the first valve is actuated so that cold helium is supplied to the first inlet, and helium is extracted through the first outlet. The specimen is therefore exposed to cold helium, which may be at a temperature below 10 K, more typically below 5 K, for example 1.5 K, 3 K or 4 K, and is cooled by contact with the cold helium. In a second mode, which may be referred to as a static mode, the second valve is actuated so that cold helium is supplied to the second inlet, and helium is extracted through the second outlet, so ensuring that the thermal element and the adjacent part of the sample tube is cooled by direct contact with the cold helium. This would normally be performed after evacuating the sample tube, and then introducing a small quantity of helium gas, so the helium gas within the sample tube is at low pressure, and in this case heat transfer would be by natural convection.
It will be appreciated that the sample tube, at the end outside the enclosure, must be provided with a closure so that the sample tube can be evacuated. That end of the sample tube may be provided with a vacuum gate, so a specimen can be introduced. However, in a preferred embodiment the sample tube is provided with a gas curtain through which helium gas is introduced wherever the sample tube is opened for inserting or removing a specimen, the gas curtain ensuring outflow of helium gas from the sample tube and so preventing air from flowing into the sample tube. The gas curtain may be provided by a gas header around the sample tube that communicates with inlet slots through the wall of the sample tube, helium gas being provided to the gas header.
The thermo-mechanical cooler in most cases will produce some vibration, and it is often desirable if vibration of the specimen is inhibited. For this reason the thermo-mechanical cooler may be mechanically linked to the remainder of the apparatus by a vibration-suppressing linkage such as a bellows. This may for example be an edge-welded bellows, of a material such as stainless steel, or bellows of a flexible plastic material.
The invention will now be further and more particularly described, by way of example only, and with reference to the accompanying drawings in which:
Referring to
The top plate 18 is also provided with a port 30 so the enclosure 12 can be evacuated. Also mounted on the top plate 18 are two needle valve drives 32 (only one is shown in
Referring now to
Considering first the sample tube 20, the first port 26 (shown schematically) communicates with the space within the sample tube 20; the portion of the sample tube 20 below the first port 26 and within the upper cylindrical portion 14 is double-walled, the sample tube 20 being surrounded by a concentric tube 40 so as to define an annular space 41, and the second port 28 communicates with this annular space 41. The annular space 41 at its lower end is defined by a double walled heat exchanger 42 which has a slightly larger external diameter than the tube 40; the inner wall of the heat exchanger 42 is of copper and defines several ribs 43 that project radially outwards into the annular space 41. The inner wall of the heat exchanger 42 defines part of the sample tube 20; the annular space 41 is closed at the bottom of the heat exchanger 42 and the portion of the sample tube 20 that continues below the heat exchanger 42 is single walled.
A specimen support rod 50 extends through the sample tube 20, and there are several circular baffles 52 mounted on the support rod 50 spaced apart along its length, to inhibit heat transfer by radiation along the sample tube 20. In this example the specimen support rod 50 consists of a first thin-walled stainless steel tube that in use extends to just below the bottom of the heat exchanger 42, whose bore contains helium and is connected to a vessel 53; and a second thin-walled stainless steel tube extending from below the bottom of the heat exchanger 42 to the specimen-support block 72, with holes (not shown) through its wall near both ends. In each case the thin wall, and the use of stainless steel, suppress heat transfer by conduction. Connecting the bore of the tube to the vessel 53 provides a gas buffer to prevent gaseous oscillations within the tube.
The thermo-mechanical cooler 22 in this embodiment is a two-stage Gifford-McMahon (GM) cooler which uses high-pressure helium at a pressure typically between 10 bar and 30 bar as the working fluid, in a closed circuit. The working fluid is provided by an external compressor (not shown). Each stage of the GM cooler includes a cylinder with a movable displacer and a rotary valve to connect the cylinder alternately to high pressure and low pressure; and the GM cooler also includes a mechanism to move the displacers in synchronisation with the movement of the valve. This is a commercially-available product (e.g. from Sumitomo Heavy Industries) and its details are not the subject of the present invention. Since the thermo-mechanical cooler 22 includes moving parts, which operate typically at a frequency of about 1 Hz, the components that are subject to this oscillation are separated from the items connected to the top plate 18, firstly by connecting the thermo-mechanical cooler 22 to the support frame 21 by a vibration-suppressing rubber mount 54, and also by the provision of a vibration-suppressing stainless steel edge-welded bellows 55.
Each stage of the thermo-mechanical cooler 22 is enclosed within a stainless steel sleeve: the first stage is enclosed within a sleeve 56 which extends from above the top plate 18, and at its lower end is connected to a thermal plate 58 of copper; while the second stage, which is of smaller diameter, is enclosed within a stainless steel sleeve 60, and at its lower end terminates at a thermal plate 62 of copper. During operation of the thermo-mechanical cooler, the temperature of the thermal plate 58 is typically lowered to an intermediate low-temperature of about 50 K, while the temperature of the thermal plate 62 is lowered to about 4 K or below.
An inlet port 64 just above the top plate 18 allows helium gas, typically at a low pressure of about 200 mbar, to be fed into the sleeve 56 so it is cooled successively by the two stages of the GM cooler. There is a fluid outlet 66 through the thermal plate 62, through which liquid or gaseous helium would therefore emerge during operation. This is described in more detail below in relation to
As shown also in
As shown in
Referring now to
The heat exchange block 70 defines a flow channel through the block into the sample tube 20. The heat exchange block 70 may also be provided with an electrical heater, and a temperature sensor, so the temperature of the helium gas entering the sample tube 20 can be accurately controlled.
In a modification, the bottom end of the sample tube 20 may be closed by an impermeable end plate, and the heat exchange block 70 through which cold helium gas is fed into the sample tube 20 may instead be of annular form, forming part of the wall of the sample tube 20. The heat exchange block 70 should always be below the position of the heat exchanger 42. Arranging the heat exchange block 70 at a position above the position of the specimen-support block 72, but below the position of the heat exchanger 42, would be appropriate if the user does not wish there to be active gas flow over the specimen.
The first outlet port 26 communicates through a valve 90 to an inlet of a pump 92, while the second outlet port 28 communicates through a valve 94 to the inlet of the pump 92. The outlet of the pump 92 is connected to a gas reservoir 95, and an outlet from the gas reservoir 95 leads to the inlet port 64.
Thus in operation, the enclosure 12 is evacuated through the port 30. The thermo-mechanical cooler 22 is activated to cool the components within the enclosure 12. A specimen is mounted onto the specimen-support block 72 and the specimen-support rod 50 is inserted into the sample tube 20, the closure 24 is sealed and the orientation of the specimen set by means of the rotatable support 25. The sample tube 20 would also be evacuated, to remove any traces of air.
Cooling of the specimen is carried out by recirculating helium using the pump 92, and this may be carried out either in a dynamic mode or in a static mode. In each mode helium gas is provided to the inlet port 64, and is cooled to about 4 K in passing through the thermo-mechanical cooler 22, so typically it becomes liquefied. In the dynamic mode of operation the first needle valve 80 is opened and the second needle valve 82 is closed; the valve 90 associated with the first outlet port 26 is also open. Liquid helium flows through the first needle valve 80 and the capillary tube 81 and through the heat exchange block 70 into the sample tube 20 where it evaporates; cold gaseous helium flows over the surface of the specimen, flows up the sample tube 20 to emerge through the first outlet port 26. The pump 92 ensures helium is continuously removed from the sample tube 20, to be recirculated. This would typically involve a gas pressure within the sample tube 20 of up to 10 or 15 mbar, although this pressure can be adjusted by adjusting the flow rate through the pump 92, for example using a throttle valve. Although the liquid helium is at 4 K initially, the gas temperature in the sample tube 20 may be less than that because latent heat is required to vaporise the helium; the gas temperature and so the temperature of the specimen is therefore affected by the flow rate of gas through the sample tube 20 caused by the pump 92. For example a temperature of 1.5 K can be achieved.
In the static mode of operation the second needle valve 82 is opened and the first needle valve 80 is closed; the valve 94 associated with the second outlet port 28 is also open. Liquid helium flows through the second needle valve 82 and the capillary tube 83 into the heat exchanger 42, where it cools the wall of the sample tube 20. The resulting gaseous helium flows up the annular space 41 to emerge through the second outlet port 28, and the pump 92 ensures helium is continuously removed from the annular space 41 to be recirculated. In this mode of operation helium would also be introduced into the sample tube 20, so the pressure in the sample tube 20 is initially at for example between 200 and 800 mbar, for example between 400 and 600 mbar, when the gas is at ambient temperature; this helium gas is not recirculated. In this case the helium gas within the sample tube 20 would undergo natural convection, because the wall of the sample tube 20 in the heat exchanger 42 is being kept cold, and this natural convection lowers the temperature of the specimen. As the temperature of the gas within the sample tube 20 becomes lower, so does the gas pressure within the sample tube 20, and typically it would drop to about 10 mbar.
As another option, both the dynamic cooling mode and the static cooling mode may be performed simultaneously, by supplying the liquid helium through both the needle valves 80 and 82. An operator of the cryogenic apparatus 10 can therefore select from three different modes of operation—the static mode, the dynamic mode, and their combination—and so can achieve different rates of cooling of the specimen within the sample tube 20.
As a further option, the sample tube 20 may be provided with a gas curtain 100 below the closure 24. This feature is shown only in
The provision of the facility for both dynamic cooling and static cooling of the specimen has been found to be advantageous, as dynamic cooling can achieve more rapid cooling of the specimen, whereas static cooling is desirable where the specimen is to be exposed to low gas pressures. For example when performing static cooling, having achieved a desired low-temperature of the specimen, the gas within the sample tube 20 may then be extracted immediately before making measurements (for example using a neutron beam), so that there is no helium within the sample tube 20 while measurements are being made.
So in some applications it is advantageous to operate initially with dynamic cooling, so that the specimen is cooled down as rapidly as possible by helium gas flowing through the sample tube 20. When the desired temperature is approached, the mode of operation may be changed to static cooling, leaving some helium within the sample tube 20, and supplying the liquid helium from the outlet 66 to the heat exchanger 42, so that further cooling takes place by natural convection within the sample tube 20.
As indicated above the cryogenic apparatus 10 enables the temperature of a specimen within the sample tube 20 to be cooled to a temperature such as 1.5 K. A lower temperature can be achieved by mounting a secondary cooling insert (not shown) within the sample tube 20 in the vicinity of the specimen-support block 72, this achieving further cooling by performing helium expansion in a separate circuit from that described above. Depending on the dimensions and the mode of operation, this can achieve a temperature as low as 300 mK, or 25 mK, or even 15 mK.
Number | Date | Country | Kind |
---|---|---|---|
1517391 | Oct 2015 | GB | national |
Filing Document | Filing Date | Country | Kind |
---|---|---|---|
PCT/GB2016/053049 | 9/30/2016 | WO | 00 |
Publishing Document | Publishing Date | Country | Kind |
---|---|---|---|
WO2017/055865 | 4/6/2017 | WO | A |
Number | Name | Date | Kind |
---|---|---|---|
3182462 | Long | May 1965 | A |
3221509 | Garwin | Dec 1965 | A |
5647228 | Sager | Jul 1997 | A |
5970804 | Robbat | Oct 1999 | A |
6202439 | Mikheev | Mar 2001 | B1 |
7157999 | Kasten | Jan 2007 | B2 |
7183769 | Kasten | Feb 2007 | B2 |
7492154 | Lucas | Feb 2009 | B2 |
7639007 | Hutton | Dec 2009 | B2 |
8683816 | Krencker | Apr 2014 | B2 |
8975896 | Schett | Mar 2015 | B2 |
9234691 | Black | Jan 2016 | B2 |
9279868 | Lohman | Mar 2016 | B2 |
20060096301 | Triebe | May 2006 | A1 |
20080264071 | Saito | Oct 2008 | A1 |
20080290869 | Hutton | Nov 2008 | A1 |
20090183860 | Krencker | Jul 2009 | A1 |
20110219785 | Black et al. | Sep 2011 | A1 |
20140202174 | Wang | Jul 2014 | A1 |
20140212174 | Hayashi | Jul 2014 | A1 |
20160061493 | Morie | Mar 2016 | A1 |
20170038123 | Strickland | Feb 2017 | A1 |
20180030593 | Policandriotes | Feb 2018 | A1 |
20180320936 | Regnat | Nov 2018 | A1 |
20190011170 | Morie | Jan 2019 | A1 |
20190041103 | Kelly | Feb 2019 | A1 |
20200018524 | Graf | Jan 2020 | A1 |
Number | Date | Country |
---|---|---|
805317 | Nov 1997 | EP |
Entry |
---|
Search Report for Great Britain Application No. GB 1517391.7 dated Apr. 1, 2016. |
International Search Report for PCT Application No. PCT/GB2016/053049 dated May 4, 2017. |
Written Opinion for PCT Application No. PCT/GB2016/053049 dated May 4, 2017. |
Number | Date | Country | |
---|---|---|---|
20190041103 A1 | Feb 2019 | US |