Refrigeration – Storage of solidified or liquified gas – Including cryostat
Reexamination Certificate
2003-05-19
2004-10-19
Esquivel, Denise L. (Department: 3744)
Refrigeration
Storage of solidified or liquified gas
Including cryostat
C062S006000
Reexamination Certificate
active
06804968
ABSTRACT:
This application claims Paris Convention priority of DE 102 26 498.8 filed Jun. 14, 2002 the complete disclosure of which is hereby incorporated by reference.
BACKGROUND OF THE INVENTION
The invention concerns a cryostat configuration for storing liquid helium, comprising an outer jacket accommodating a helium container, a neck pipe which is filled with gaseous helium during operation, and a refrigerator, wherein the upper end of the neck pipe is connected to the outer jacket which is at ambient temperature during operation, and the lower end of the neck pipe is connected to the helium container having liquid helium during operation, wherein the outer jacket, the helium container and the neck pipe delimit an evacuated chamber which surrounds the helium container, and wherein the refrigerator has a cooling finger which projects from the upper end of the neck pipe into the neck pipe and has a condensation body in the region of the lower end of the neck pipe which is cooled down to the temperature of liquid helium during operation.
A cryostat configuration of this type is disclosed e.g. in DE 100 33 410 C1.
Superconducting magnets are used to produce high magnetic field strengths, in particular in nuclear magnetic resonance apparatus. For operating superconducting magnets, the associated magnet coils, which are wound from a superconducting wire, must be cooled. To cool these magnet coils, they are typically disposed in liquid helium at a temperature of approximately 4.2 K. This cooling temperature is below the critical temperature (transition temperature) T
c
of the wire material and guarantees that the wire is in the superconducting state.
The cryostat configuration keeps the superconducting magnet at the predetermined operating temperature. The essential components of the cryostat configuration are a helium container which holds liquid helium and the superconducting magnet, an outer jacket, one or more neck pipes which connect the helium container to the outer jacket and which provide access to the inside of the helium container, and radiation shields which are disposed in an evacuated chamber between the helium container and the outer jacket.
The neck pipe or neck pipes are needed to charge the superconducting magnet and to fill the helium container with helium, and also permit evaporation of the helium. In particular, during a quench of a magnet coil in the helium container the magnet coil immediately heats to a temperature above the boiling temperature of liquid helium and large amounts of liquid helium are transferred into the gaseous phase. To prevent an inadmissibly high (i.e. explosive) pressure increase, the diameter of the neck pipe (or neck pipes) and of the connecting piece must be sufficiently large.
Neck pipes are usually made from stainless steel, titanium alloys or GFK. They typically have a length of approximately one meter or less and extend, perpendicular or slightly inclined, from their cold end connected to the helium container to their end connected to the outer jacket at ambient temperature.
The evacuated chamber and the radiation shields minimize heat entry into the helium container. Heat entry is effected in particular by radiation (originating in particular from the outer jacket at ambient temperature) through convection and thermal conduction from the residual gas in the evacuated chamber, through thermal conduction in the neck pipe and by convection and thermal conduction from the helium gas in the neck pipe.
Heat entry produces evaporation of the liquid helium. The lost helium must either be replenished—an expensive procedure in view of the amounts involved of approximately 0.1 I/h (liters per hour)—or refrigerators must be used for active cooling of the cryostat configuration. A cryostat configuration comprising a refrigerator for active cooling is known e.g. from EP 0 773 450 A1.
Such refrigerators consist substantially of a cold head, which is connected to a remote compressor via pressure lines and mounted via a mounting plate to the outer jacket, and of a cooling finger. The cooling finger projects into a neck pipe or into a separate opening in the evacuated chamber. During operation, the end of the cooling finger facing away from the mounting plate is cooled down to temperatures of between 2 and 3 K. Heat is either withdrawn from the helium by means of a condensation body (heat exchanger) or from the helium container via thermally conducting connections. The cooling finger typically consists of several parallel pipes, which have different functions for generating optimum cooling.
In principle, cold heads may also have several stages. A first stage, disposed closer to the mounting plate, is thereby cooled down during operation to a first low temperature while the further stages are cooled down to even lower temperatures. The different stages can be connected to the radiation shields and/or the helium container in a good thermally conducting fashion to actively cool these components.
Refrigerators for such applications can operate e.g. according to the Gifford-McMahon principle or be constructed as pulse tube coolers.
Installation of a cold finger in the neck pipe of the cryostat can cause convection in the neck pipe due to temperature gradients in the neck pipe wall or between the neck pipe wall and the cooling finger thereby producing additional, undesired heat entry into the helium container. These temperature gradients may be caused e.g. geometrically through the spatial configuration or through different thermal conductivities. These problems occur in particular if only little or no helium at all flows through the neck pipe.
In contrast thereto, it is the underlying purpose of the present invention to improve the thermal properties of a cryostat configuration with active refrigerator cooling and in particular control convection currents of gaseous helium inside a neck pipe.
SUMMARY OF THE INVENTION
This object is achieved in accordance with the invention in that the condensation body is at least partially directly surrounded by a condensation chamber which has a first lower opening which permits flow of liquid helium condensed in the condensation chamber into the helium container and which has a second opening which terminates in a lower end of a gas supply pipe, wherein the upper end of the gas supply pipe terminates inside the neck pipe in the region of the upper end thereof.
The inventive design of the cryostat configuration divides the condensation body into two regions: Helium gas is removed from the upper relatively warm region of the neck pipe via the gas supply pipe and condenses on the surface of the condensation body located within the condensation chamber. The condensed gas can drip or flow away through the first lower opening of the condensation chamber. The helium gas removed from the upper region of the neck pipe must be replaced from the underlying helium container, thereby producing a gas flow in the neck pipe. The condensation chamber does not surround a portion of the surface of the condensation body. Relatively cool helium from the direct vicinity, i.e. from the helium container, condenses on this other portion.
In this fashion, part of the energy provided for cooling the cold finger is utilized for generating a controlled helium gas flow in the neck pipe. Selection of the fraction of surface surrounded by the condensation chamber and the fraction of exposed surface of the condensation body can be used to adjust the intensity of the helium gas flow. This eliminates other undesired convection currents. In particular, the invention permits adjustment of the intensity of the convection current to the required or desired pre-cooling of the neck pipe wall (through rising, relatively cold gaseous helium).
The larger the portion of the surface of the condensation body surrounded by the condensation chamber, the larger the relative amount of condensed, originally relatively warm, helium gas from the upper region of the neck pipe and the stronger the helium gas flow in the neck pipe. The flow is also influenced by the position of
Bruker Biospin GmbH
Drake Malik N.
Esquivel Denise L.
Vincent Paul
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