This application claims Paris convention priority from DE 10 2014 218 773.7 filed Sep. 18, 2014, the entire disclosure of which is hereby incorporated by reference.
The invention concerns a cryostat comprising a vacuum container which houses a chamber with at least one object to be cooled, wherein the vacuum container has at least one hollow neck tube which connects the chamber through the outer shell of the vacuum container to the area outside of the cryostat, wherein the neck tube houses a cooling arm of a cold head, wherein the cooling arm is thermally connected to a refrigeration device and can also be brought into thermal contact with a second thermal contact surface on the object to be cooled via a first thermal contact surface on the cooling arm.
A cryostat of this type is disclosed e.g. in U.S. Pat. No. 5,934,082 or U.S. Pat. No. 4,535,595.
In most cases, cryotechnology utilizes cooling machines for cooling objects, e.g. superconducting magnet coils. The cooling machines discharge heat from the apparatus containing the object to be cooled by means of a cold head.
These cooling machines are typically operated with helium gas as the coolant which is compressed in a compressor and expands in the cold head of the cryostat (e.g. so-called “pulse tube coolers”). The cold head and the compressor are generally connected to each other via two pressure lines. The cold head is connected to the components to be cooled either directly mechanically or via a contact medium (e.g. cryo gas or cryo liquid) or in both ways in order to ensure good heat transfer.
However, if, e.g. due to a technical defect or power failure, the compressor fails completely or partially, the previously cooled components are heated. In this situation, the cold head of the cryostat then represents a substantial thermal bridge between the components to be cooled and the external surroundings.
In its persistent operating mode, the superconducting current in a superconducting magnet can flow practically without resistance for extremely long time periods. However, heating of the magnet causes a so-called quench of the persistent operating mode after a certain time. At some point, the magnet reaches the critical transition temperature which is predetermined by the superconducting material and becomes normally conducting and thereby loses, generally abruptly, its high magnetic field.
A reduction of the thermal load after failure of the cooling machine would at least considerably extend the time period until a quench happens. This is true, in particular, for cryostat configurations that can be operated completely without or merely with minimum amounts of liquid coolant, wherein superconducting magnets are currently normally operated in a liquid helium bath.
U.S. Pat. No. 6,164,077 discloses replacement of the thermal contact between the cooling arm and the object being cooled with gas in the event of failure of the cooling device.
Since helium is becoming more and more expensive, cryostats that can be operated completely without or at least with minimum amounts of helium (low-loss or even cryo-free systems) are becoming more and more attractive both technically and economically.
However, the thermal capacity of solids significantly decreases at very low temperatures. For this reason, it would be particularly important for systems of this type using little amounts of liquid helium or no liquid helium at all to minimize the heat input into the object to be cooled in case of failure of the cooling unit.
U.S. Pat. No. 7,287,387 B2 describes a cooling unit for cooling a superconducting magnet coil and the radiation shields or chambers that surround it. Whereas cooling of the radiation shields or chambers is effected via direct thermal contact, the coil is cooled by means of re-liquefied helium. Bellows are used at the interface between the housing and the cooling unit in order to obtain vibrational decoupling. The cooling unit always remains in fixed contact with the radiation shield and the inner chamber. A pressure change in the inside of the cryostat does not change the thermal contact. It is only stated that the bellows should withstand an overpressure of 1 bar.
U.S. Pat. No. 8,069,675 B2 also describes a cold head that is flexibly connected to the cryostat. In this case, however, an actuator is operated in order to release the thermal contact. It is not an automatically functioning passive system but requires active intervention by an operator. The same also applies for the cooling configurations as disclosed e.g. in U.S. Pat. No. 5,522,226 or U.S. Pat. No. 5,430,423.
EP 0 366 818 A1 discloses a configuration with which the adjustment of the penetration depth of a cold head into a LN bath is done automatically in dependence on the pressure within the cryostat.
The above-cited U.S. Pat. No. 5,934,082 discloses a “cryo-free system”, wherein the cold head is in thermally conducting physical contact both with a heat shield and a magnet coil. The hollow space between the heat shield and the cold head is evacuated in this connection. Spring elements are provided in the cooling device for absorbing or damping oscillations.
U.S. Pat. No. 4,535,595 also describes a similar cooling system. Also in this case, the gas is not in direct contact with the cold head but the hollow space is again evacuated. This document moreover discloses a cold head that can be displaced in a vertical direction and is also in thermal contact with a heat shield and a magnet coil.
In contrast thereto, it is the underlying object of the invention, which is relatively demanding and complex when regarded in detail, to significantly and operationally safely reduce the thermal load by the cold head onto the object to be cooled in case of failure of the cooling machine in a cryostat of the above-mentioned type with simple technical means and fully automatically without requiring the intervention of an operator, wherein already existing devices can be retrofitted with as simple means as possible.
This object is achieved by the present invention in a likewise surprisingly simple and effective fashion in that the hollow volume between the inner side of the hollow neck tube, the cooling arm that is disposed at least partially in the hollow neck tube, and the object to be cooled is at least partially filled with a gas or gas mixture with positive thermal expansion coefficient, wherein the internal pressure of the gas or gas mixture pressurizes part of the cooling arm, whereas another part of the cooling arm is directly or indirectly pressurized by atmospheric pressure, that the cooling arm is mounted in such a fashion that it can be moved within the hollow neck tube by a length of at least 5 mm with its first thermal contact surface towards or away from the second thermal contact surface, and that a contact device brings or keeps the first thermal contact surface of the cooling arm in thermal contact with the second thermal contact surface on the object to be cooled when the gas or gas mixture pressure is below a predetermined low threshold pressure, whereas the contact device moves the first thermal contact surface of the cooling arm away from the second thermal contact surface of the object to be cooled when the gas or gas mixture pressure has reached or exceeded a threshold pressure, such that the thermal contact surfaces no longer contact each other in this position but are thermally separated from each other by a gap filled with gas or a gas mixture.
In case of gas mediated contact between the two contact surfaces, the mutual separation between the contact surfaces is of considerable importance for the heat transfer. In the inventive configuration, the cooling arm of the cold head is moved by the gas that expands due to heating in such a fashion that the thermal contact between the two contact surfaces is cancelled in that a gas gap is formed between the contact surfaces which increases, thereby substantially reducing the thermal input into the object to be cooled, generally a superconducting magnet. If the gap increases e.g. from 0.1 mm to 10 mm the heat input (without convection) is reduced by a factor of 100.
The reduced heat input considerably increases the time period until the magnet coil reaches its critical temperature during a quench and becomes normally conducting. This time period is an essential specification of superconducting magnets.
The contact between the cooling arm and a heat shield is also reduced by the movement and the heat input into the shield is therefore also reduced in this case. The shield is therefore heated considerably more slowly after failure of the cold head. The shield temperature is of considerable importance for any other heat input into the object to be cooled, in particular a magnet coil. Slower heating of the shield therefore automatically results in slower heating of the superconducting magnet coil, thereby extending the time period before a quench happens.
The movement that forms and increases the gap is made possible in that the cooling arm (or in variants of the invention also the entire cold head) is mounted to be movable along its axis.
There are, in principle, substantially three feasible different variants of providing thermal contact in order to ensure good thermally conducting contact between the first thermal contact surface of the cooling arm and the second thermal contact surface on the object to be cooled in an operating state below the predetermined threshold pressure of the gas or gas mixture:
1. Direct thermal contact without liquid helium: In this case a liquid helium bath is completely omitted and the two contact surfaces are in tight thermally conducting physical contact in this operating state.
2. Direct thermal contact with liquid helium: The same tight physical contact between the two contact surfaces in the operating state below the predetermined threshold pressure can also be established when the two contact surfaces are located in a liquid helium bath which further increases the thermally conducting contact at least in the edge regions.
3. Indirect thermal contact with liquid helium: In this variant, the two contact surfaces are indeed physically separated in the operating state below the predetermined threshold pressure but are located in a common liquid helium bath which ensures a good thermally conducting thermal connection between the two contact surfaces in this operating state.
In one particularly preferred embodiment of the inventive cryostat, the contact device comprises a bellows and/or a diaphragm and/or a radial seal by means of which the cooling arm is mounted in the hollow neck tube such that it can be displaced in a linear direction along its axis.
In one further advantageous embodiment of the invention, the contact device has a stop surface against which the counter surface of the cooling arm in the hollow neck tube, which is rigidly connected to the cooling arm, can abut during linear displacement along its axis towards the object to be cooled, wherein the relative positions of the surfaces are selected such that in case of mechanical contact between the stop surface and the counter surface, the first thermal contact surface of the cooling arm also comes into thermally conducting contact with the second thermal contact surface on the object to be cooled. This stop may also be adjustable in order to optimally reduce the gap between the contact surfaces. Mechanical decoupling is required to prevent transfer of detrimental vibrations from the cooling arm to the object to be cooled, in particular a superconducting magnet coil.
Without further measures, the movement would take place only when the atmospheric pressure is exceeded. For this reason, in one preferred embodiment of the inventive cryostat, the contact device has a pretensioning device that generates an additional force in addition to the pressure of the gas or gas mixture acting on the cooling arm, which additional force acts in a direction of movement of the cooling arm during linear displacement in the hollow neck tube along its axis in a direction away from the object to be cooled. The motion pressure acting on the displaceable cooling arm can thereby be reduced.
In one advantageous further development of this embodiment, the additional force on the cooling arm generated by the pretensioning device has a non-linear characteristic that depends on the path of displacement of the cooling arm due to the acting pressure of the gas or gas mixture, wherein the additional force becomes sufficiently large that the first thermal contact surface of the cooling arm is lifted off the second thermal contact surface on the object to be cooled only when a predetermined threshold pressure of the gas or gas mixture is exceeded, such that a gap separates the contact surfaces and that, even when the pressure of the gas or gas mixtures only slightly further increases, this gap quickly increases due to the additional force that acts on the cooling arm. This is advantageous in that the cooling arm is already decoupled shortly after failure of the cold head. A typical operating pressure is e.g. 200 mbar. Reaching atmospheric pressure would take a long time during which the cooling arm would transfer heat to the object to be cooled, in particular a superconducting magnet coil, due to its thermal coupling.
In particularly simple further developments of this embodiment, the pretensioning device comprises one or more pretensioning springs. These springs generate the specified pretensioning force and at the same time enable vibrational decoupling of the cooling arm from the outer shell of the object to be cooled, in particular a superconducting magnet coil.
In particularly preferred variants, the additional force exerted by the pretensioning springs on the cooling arm can be mechanically adjusted, in particular by means of one or more adjustment screws. In this fashion, the pretensioning force can be adjusted to the generated operating pressure. All cold head/cooling object combinations slightly differ from each other. For this reason, it is extremely reasonable to make the pretensioning force adjustable.
In further advantageous embodiments of the inventive cryostat, the cooling arm is mounted in such a fashion and the contact device is designed in such a fashion that the first thermal contact surface of the cooling arm inside the hollow neck tube can be moved by a length of at least 10 mm, preferably at least 20 mm, in particular at least 50 mm, towards or away from the second thermal contact surface on the object to be cooled. The thermal conduction between the contact surfaces can therefore be reduced by a factor of up to 500.
In other advantageous embodiments, the first thermal contact surface of the cooling arm is located completely or partially in liquid helium in an operating state below the predetermined threshold pressure of the gas or gas mixture and when the threshold pressure has been exceeded, it emerges from the helium bath into the surrounding gas or gas mixture due to the movement away from the second thermal contact surface of the object to be cooled. In this connection, the thermal contact between the contact surfaces in this operating state can either be provided through direct physical contact between the two contact surfaces and/or indirectly by means of the liquid helium with its excellent heat conducting properties. Liquid helium substantially represents a perfect heat bridge. Only a tiny temperature gradient will form in the helium due to convection. As soon as the cold head fails, it transfers its heat directly into the liquid helium and thus to the object to be cooled, in particular a superconducting magnet coil. When the contact surface emerges from the helium, heat is transferred only by gas, thereby considerably reducing the transfer of heat.
In one alternative embodiment, there is no liquid helium bath and the first thermal contact surface of the cooling arm is in direct physical, and therefore thermally conducting, contact with the second thermal contact surface of the object to be cooled in the operating state below the predetermined threshold pressure of the gas or gas mixture. When the threshold pressure has been exceeded, the contact surfaces are moved apart, thereby generating a thermally insulating gas gap between the two contact surfaces.
In another advantageous embodiment of the inventive cryostat, the chamber containing the object to be cooled is surrounded by a radiation shield inside the vacuum container. This considerably reduces the thermal load due to radiation and thermal conduction.
In one class of preferred embodiments, a superconducting magnet coil is arranged in the chamber as an object to be cooled. Magnet systems of this type usually consist of a magnet coil, a radiation shield, a vacuum container and one or more neck tubes that connect the magnet coil or mounting parts to the outer shell.
The present invention also concerns a magnetic resonance configuration comprising a superconducting magnet coil, in particular an NMR spectrometer configuration or an NMR tomography configuration but also an MRI or FTMS apparatus, each comprising an inventive cryostat as described above. The present invention protects the superconducting magnet coil of the magnetic resonance configuration particularly well against a quench of the persistent operating mode and is therefore particularly well suited for high-resolution measurements. A magnetic resonance configuration of this type typically comprises at least one magnet that is generally superconducting and is arranged in a cryostat, and also radio frequency components, e.g. RF coils in a room temperature bore of the cryostat and a sample position for a sample to be measured. “Normal” conventional high field NMR spectrometers operate at a proton resonance frequency of between approximately 200 MHz and 500 MHz. In contrast thereto, a high field NMR spectrometer with ultra-high resolution can be operated nowadays at proton resonance frequencies ≥800 MHz.
Further advantages of the invention can be extracted from the description and the drawing. In accordance with the invention, the features mentioned above and below may be used individually or collectively in arbitrary combination. The embodiments shown and described are not to be understood as exhaustive enumeration, rather have exemplary character for describing the invention.
The invention is illustrated in the drawing and is explained in more detail with reference to embodiments.
The chamber 12 containing the object 4 to be cooled is surrounded by a radiation shield 5 inside the vacuum container 9.
The inventive cryostat 11; 11′; 11″; 11′″ is characterized in that the hollow volume 2; 2′; 2″ between the inner side of the hollow neck tube 10, the cooling arm 1a; 1a′; 1a″; 1a′″ that is at least partially arranged therein, and the object 4 to be cooled is filled at last in part with a gas or a gas mixture with positive thermal expansion coefficient, wherein the inner pressure of the gas or gas mixture pressurizes part of the cooling arm 1a; 1a′; 1a″; 1a′″, whereas another part of the cooling arm 1a; 1a′; 1a″; 1a′″ is directly or indirectly pressurized by atmospheric pressure, that the cooling arm 1a; 1a′; 1a″; 1a′″ is mounted in such a fashion that it can be moved within the hollow neck tube 10 by a length of at least 5 mm with its first thermal contact surface 3a; 3a′; 3a″; 3a′″ towards or away from the second thermal contact surface 3b; 3b′; 3b″, and that a contact device is provided which brings or keeps the first thermal contact surface 3a; 3a′; 3a″ of the cooling arm 1a; 1a′; 1a″; 1a′″ in thermal contact with the second thermal contact surface 3b; 3b′; 3b″ on the object 4 to be cooled when the pressure of the gas or gas mixture is below a predetermined low threshold pressure, while the contact device moves the first thermal contact surface 3a; 3a′; 3a″ of the cooling arm 1a; 1a′; 1a″; 1a′″ away from the second thermal contact surface 3b; 3b′; 3b″ of the object 4 to be cooled when the pressure in the gas or gas mixture has reached or exceeded the threshold pressure such that in this position, a gap 13 filled with gas or gas mixture thermally separates the contact surfaces 3a, 3b; 3a′, 3b′; 3a″, 3b″.
The cooling arm 1a; 1a′; 1a″; 1a′″ is advantageously mounted in such a fashion and the contact device is designed in such a fashion that the first thermal contact surface 3a; 3a′; 3a″ of the cooling arm 1a; 1a′; 1a″; 1a′″ can be moved within the hollow neck tube 10 by a length of at least 10 mm, preferably at least 20 mm, in particular at least 50 mm towards or away from the second thermal contact surface 3b; 3b′; 3b″ on the object 4 to be cooled.
The contact device may comprise a bellows and/or a diaphragm and/or, as illustrated in the figures of the drawing, a radial seal 6 by means of which the cooling arm 1a; 1a′; 1a″ is mounted in the hollow neck tube 10 in such a fashion that it can be displaced in a linear direction along its axis.
The contact device has a stop surface 14a against which the cooling arm 1a; 1a′; 1a″; 1a′″ in the hollow neck tube 10 can abut with its counter surface 14b that is rigidly connected to the cooling arm 1a; 1a′; 1a″; 1a′″ during linear displacement along its axis in the direction towards the object 4 to be cooled, wherein the relative positions of the surfaces are selected such that in case of mechanical contact between the stop surface 14a and the counter surface 14b, the first thermal contact surface 3a; 3a′; 3a″ of the cooling arm 1a; 1a′; 1a″; 1a′″ also comes into thermally conducting contact with the second thermal contact surface 3b; 3b′; 3b″ on the object 4 to be cooled.
The contact device moreover comprises a pretensioning device which generates an additional force in addition to the pressure of the gas or gas mixture acting on the cooling arm 1a; 1a′; 1a″; 1a′″, which additional force acts in a direction of movement of the cooling arm 1a; 1a′; 1a″; 1a′″ during linear displacement in the hollow neck tube 10 along its axis in a direction away from the object 4 to be cooled. The pretensioning device comprises one or more pretensioning springs 7, wherein the additional force that the pretensioning springs 7 exert on the cooling arm 1a; 1a′; 1a″; 1a′″ can be mechanically adjusted by means of one or more adjustment screws 8.
In the embodiment of the inventive cryostat 11 illustrated in
Thermal decoupling between the cooling arm is and the object 4 to be cooled is achieved by generating the gas-filled gap 13 due to the gas pressure-driven movement of the cooling arm is when the predetermined threshold pressure has been reached or exceeded by heating of the gas or gas mixture. This operating state is illustrated in
In contrast thereto,
The embodiments of the inventive cryostat 11′; 11″ illustrated in
In the embodiment illustrated in
When the predetermined threshold value has been reached or exceeded through heating of the gas or gas mixture and the accompanying increase in inner pressure, the cooling arms 1a′; 1a″ of the embodiments of
In the embodiment of the inventive cryostat 11′″ illustrated in
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10 2014 218 773 | Sep 2014 | DE | national |
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