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Description  |
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BACKGROUND OF THE INVENTION
The present invention relates to a low-temperature testing device which is
used for testing the temperature characteristics of specimens of, for
example, superconducting materials, and particularly to a low-temperature
testing device in which specimens can be easily changed and the
temperatures of specimens can be arbitrarily controlled.
Recently, competition in development of superconducting materials has
become progressively keener, and it is extremely important to test the
characteristics such as the critical temperature of a newly developed
material. Examples of devices that are generally used in the measurement
of the critical temperature of a new material include a device in which a
sample-receiving chamber provided adjacent to a cooling portion of a
Grifford-McMahon refrigeration unit or an improved type thereof is
received in an adiabatic vacuum vessel so that a specimen received in the
chamber can be cooled by heat transfer through a gas or a solid and a
device in which a vessel receiving liquid helium or liquid nitrogen and a
sample-receiving chamber placed adjacent to the bottom of the vessel are
provided in an adiabatic chamber typically having a vacuum layer so that a
specimen placed in the sample-receiving chamber can be cooled by heat
transfer to liquid helium or liquid nitrogen.
However, each time the specimen is changed, adiabatic vacuum in these
conventional low-temperature testing devices must be broken, and the
operation of the refrigeration machine in the former device must be
stopped. Therefore, the conventional devices each have a disadvantage in
that the low-temperature atmosphere in the sample-receiving chamber of
each of the devices which is achieved by the preceding test cannot be
retained for the next test, and the temperature of the sample-receiving
chamber thus returns to room temperature each time the specimen is
changed. Each of the conventional low-temperature testing devices also
have a disadvantage in that the temperatures of the sample-receiving
chamber and the specimen are not easily raised or lowered at a controlled
rate and a wide range.
Therefore, it is an object of the present invention to provide a
temperature testing device which is provided with a sample-receiving
chamber in which a specimen can be changed without adiabatic vacuum being
broken, and which can be always maintained at a low temperature.
It is another object of the present invention to provide a low-temperature
testing device in which the temperature of a sample-receiving chamber and
a specimen can be precisely and easily controlled over a wide range by
cooling the sample-receiving chamber with a circulating gaseous
refrigerant.
Other objects of the present invention will be made clear from the
description below.
SUMMARY OF THE INVENTION
A low-temperature testing device to which the present invention relates
comprises (a) a sample-receiving sealable chamber whose greater part is
inserted into a vacuum vessel in which a cooling portion of a
refrigeration unit is also inserted, (b) a pump for circulating a gaseous
refrigerant which is provided outside the vacuum vessel, (c) a first pipe
which causes the outlet side of a pump to connect to an inlet for the
gaseous refrigerant provided in a lower portion of the sample-receiving
chamber while passing through a heat exchanger provided on the cooling
portion of the refrigeration unit and through a temperature control means
and (d) a second pipe which causes an outlet for the gaseous refrigerant
provided approximately at an intermediate position along the length of the
sample-receiving chamber to connect to the inlet side of the pump. The
first and second pipes are provided in the vacuum vessel in which the
cooling portion of the refrigeration unit and the sample-receiving chamber
are inserted.
In this low-temperature testing device, the gaseous refrigerant such as
helium or nitrogen gas is sent through the first pipe by the pump provided
outside the vacuum vessel, cooled in the cooling portion of the
refrigeration unit while passing through the first pipe, supplied into the
sample-receiving chamber from a lower portion thereof, and brought into
contact with a specimen placed therein to cool it. The gaseous refrigerant
is then discharged from the outlet provided at the intermediate portion of
the sample-receiving chamber, is passed through the second pipe and is
returned to the pump. Therefore, the gaseous refrigerant can be circulated
through the first pipe, the sample-receiving chamber, and the second pipe.
BRIEF DESCRIPTION OF THE ATTACHED FIGURES
FIG. 1 is a sectional view of an embodiment of a temperature testing device
to which the present invention relates.
DETAILED DESCRIPTION OF THE INVENTION
In the drawing, a vacuum pump 4 is connected to a vacuum vessel 1 by means
of a pipe 3 through a valve 2. A two-stage refrigeration unit 5 employing
the Gifford-McMahon cycle is inserted into the vacuum vessel 1, a first
cooling stage 6a and a second cooling stage 6b thereof being placed in the
vacuum vessel 1. The first cooling stage 6a has cooling coils 7a.sub.1 and
7a.sub.2 and the second cooling stage 6b has a cooling coil 7b, and the
second cooling stage 6b and the cooling coil 7b are covered with a
radiation shield 49. Similarly, a sample-receiving chamber 8 which has a
cylindrical form with a bottom closed is inserted into the vacuum vessel
1. The sample-receiving chamber 8 has a gas inlet 9 and a gas outlet 10
which are provided on the bottom of the chamber 8 and at an intermediate
position along the length thereof, respectively. A cooling stage 11 made
of a band with excellent heat conductivity and a cooling coil 12 are
provided approximately in an intermediate position between the top and the
bottom of the sample-receiving chamber 8 lower than the position of the
gas outlet 10. The portion of the sample-receiving chamber 8 below the
cooling stage 11 is covered with a radiation shield 13.
Pipes 14a, 14b, 14c, 14d, 14e, 17 and 19 are pipes for supplying the
gaseous refrigerant expelled from a circulating pump 15 which is provided
on the outside of the vacuum vessel 1 to the gas inlet 9 at the bottom of
the sample-receiving chamber 8. The pipe 14a connects the outlet side of
the circulating pump 15 to the cooling coil 7a.sub.1 provided on the
refrigeration unit 5 through valves 16, 20 and a precooler 18. The pipe
14b connects the cooling coil 7a.sub.1 to the cooling coil 12 provided on
the sample-receiving chamber 8, and the pipe 14c connects the cooling coil
12 to the cooling coil 7a.sub.2. The pipe 14d connects the cooling coil
7a.sub.2 provided on the refrigeration unit 5 to the cooling coil 7b. The
pipe 14e connects the cooling coil 7b to the gas inlet 9 of the
sample-receiving chamber 8 through a temperature control means 32,
typically a heater, and a thermometer 33. The pipe 19 causes the gaseous
refrigerant supplied from the circulating pump 15 through the valves 16
and 22 to bypass without the refrigerant being passed through the
precooler 18 and the cooling coils 7a.sub.1, 12, 17a.sub.2 and 7b so as to
cause the gaseous refrigerant to combine with the pipe 14e. The pipe 17
causes the gaseous refrigerant supplied from the circulating pump 15
through the valves 16 and 21 to pass through the precooler 18 and then to
combine with the pipe 19.
A pipe 14f connects the gas outlet 10 provided approximately at the
intermediate position of the sample-receiving chamber 8 to the inlet side
of the circulating pump 15 by way of the precooler 18, a valve 23, a
radiator 24, a flow meter 25 and a flow control valve 26. A helium gas
bomb 29 is connected to the inlet side of the circulating pump 15 by means
of a pipe 28 having a valve 27.
Reference numeral 34 denotes a specimen-receiving vessel which can be
freely inserted into and extracted from the sample-receiving chamber 8 and
which is suspended by a hanger pipe 36 inserted through a cap 35 which is
provided at the top of the sample-receiving chamber 8 and can be freely
opened and closed. The specimen-receiving vessel 34 generally has a size
which can be fit into the space between the bottom of the sample-receiving
chamber 8 and the cooling stage 11. A specimen M positioned in the
receiving vessel 34 is supported by a rod 37 which is connected to the
hanger pipe 36, but the specimen M can be supported by any other support
means in place of this rod 37. The specimen-receiving vessel 34 is
generally covered with a cap 31 having an opening 30 at the top thereof.
A pipe 38 inserted into the sample-receiving chamber 8 is used when a
liquid refrigerant such as liquid helium or liquid nitrogen is inserted
into the receiving chamber 8, and a cap 39 is provided on the pipe 38.
A pipe 40 is used for discharging the gaseous refrigerant from the vacuum
vessel 1, one end thereof being connected to a cap 41 and the other end
being connected to the pipe 14e on the downstream side of the heater 32. A
pipe 42 is used for returning the gaseous refrigerant used outside the
vacuum vessel 1 in into the vacuum vessel 1, one end of the pipe 42 being
connected to a cap 42 and the other end thereof being connected to the
pipe 14f on the downstream side of a valve 44. The pipes 40 and 42 are
connected to another sample-receiving chamber 46 through adiabatic pipes
47 and 48, respectively, so that the gaseous refrigerant which is at a
temperature controlled by the device of the present invention can be
supplied to another sample-receiving chamber provided outside the vaccuum
vessel 1 by closing the valve 44 by means of a handle 45. In the
embodiment shown in the drawing, the sample-receiving chamber and the
cooling portion of the refrigeration unit are provided in the same vaccuum
vessel, but they may be provided in individual vacuum vessels.
A description will now be made of a method of operating the low-temperature
testing device.
The specimen M to be subjected to meaurement of its critical temperature
and so on is received into the receiving vessel 34 which is suspended in
the sample-receiving chamber 8 which is closed by the cap 35, as shown in
the drawing. The air in the sample-receiving chamber 8 and in each of the
pipes is then displaced by a helium gas. Then, after the valve 2 has been
opened and the vacuum pump 4 has been operated so that the pressure in the
vacuum vessel 1 is reduced to, for example, about 5.times.10.sup.-2 torr,
the refrigeration unit 5 is started. After the refrigeration unit 5 has
reached a desired cooling level, in general, the valve 2 can be closed and
the operation of the vacuum pump 4 can be stopped.
When the refrigeration unit 5 has cooled to the desired level, the valves
16, 20, 23, 44 and 26 are opened, the valves 21 and 22 are closed, and the
circulating pump 15 is activated. The gaseous refrigerant which is
discharged from the circulating pump 15 and is typically a helium gas is
cooled to some extent by being passed through the precooler 18 and then
further cooled by being passed through the cooling coil 7a.sub.1 of the
first cooling stage of the refrigeration unit. The refrigerant passed
through the coil 7a.sub.1 is passed through the pipe 14b and then through
the cooling coil 12 provided on the sample-receiving chamber 8 from which
it absorbs heat, and passed through the pipe 14c and through the cooling
coil 7a.sub.2 where the refrigerant is again cooled. The refrigerant is
then further cooled while being passed through the pipe 14d and through
the cooling coil 7b provided on the second cooling stage of the
refrigeration unit 5, passed through the pipe 14e and supplied to the
receiving chamber 8 from the gas inlet 9 at the bottom thereof.
The gaseous refrigerant supplied to the receiving chamber 8 enters the
vessel 34 from the openings in the cap 31 so as to cool the specimen M.
The refrigerant is then sucked from the gas outlet 10, sent to the
precooler 18 through the pipe 14f and returned to the inlet side of the
circulating pump 15 through the valves 23 and 26. Therefore, the helium
gas serving as the refrigerant is repeatedly circulated between a group of
the cooling coils of the refrigeration unit and the sample-receiving
chamber so that the specimen in the specimen-receiving vessel can be
cooled by the cold refrigerant supplied from the bottom of the
sample-receiving chamber 8 and by the cooling stage 11. In addition, the
temperature in the receiving chamber 8 can be lowered from room
temperature to about 10 K. due to the structure of the sample-receiving
chamber in which the heat transfer between the sample-receiving chamber
and the circumference thereof is inhibited by the radiation shield 13.
A method of measuring the critical temperature of a superconducting
material is generally a method of measuring a critical temperature in
which the temperature of a specimen is gradually raised from an extremely
low temperature or a method of measuring a critical temperature in which
the temperature of a specimen is gradually lowered from any desired
temperature. The device of the present invention can be applied to either
of these methods. When the former method is employed, the temperature in
the sample-receiving chamber 8 is lowered to a given extremely low
temperature in accordance with the aforementioned process, and the heater
32 is then operated while the temperature of the gaseous refrigerant
supplied to the receiving chamber 8 being monitored by the thermometer 33.
Although this is the simplest method, the temperature in the receiving
chamber 8 can also be gradually raised by increasing the opening of the
valve 21 or 22 while reducing the opening of the valve 20 so as to
increase the ratio of the refrigerant bypassing the cooling coil group and
flowing through the pipe 19 to the refrigerant passing through the cooling
coil group of the refrigeration unit 5 and flowing through the pipe 14e.
In this case, the temperature rise rate itself can be controlled by
controlling the output of the heater 32 and/or the increase rate of the
above-described ratio. When the latter method is employed, the temperature
in the sample-receiving chamber 8 can be lowered at any desired rate in
accordance with the process reverse to the aforementioned process.
One of the characteristics of the device of the present invention is the
fact that the specimen can be easily exchanged while the operation of the
device being continued, without the need for returning the temperature of
the sample-receiving chamber 8 which is kept at the final stage in the
preceding test to room temperature when the specimen is exchanged. In
other words, the operations of the refrigeration unit 15 and the
circulating pump 15 are continued, and the valve 27 is opened and the
valve 23 or 44 is closed in the state wherein the helium gas refrigerant
is circulated in the route flowing through the pipe 14d. The cap 35 of the
receiving chamber 8 is then opened for the purpose of extracting the
receiving vessel 34 therefrom. As a result, the system is replenished with
the helium gas in the bomb 29 by the circulating pump 15, and the helium
gas is cooled by being passed through the cooling coil group of the
refrigeration unit 5, continuously supplied to the bottom of the receiving
chamber 8, and expelled to the air from the top thereof. Therefore, the
temperature of the receiving chamber is not returned to room temperature
even if the cap 35 is removed from the sample-receiving chamber 8 when the
specimen is exchanged, and thus no air and moisture enter the receiving
chamber 8.
The above-described helium gas as well as a nitrogen gas can be used as the
gaseous refrigerant used in the device of the present invention. However,
use of the helium gas enables the specimen to be cooled to a lower
temperature than use of the nitrogen gas. The flow rate and the pressure
of the gaseous refrigerant which circulates in the device can be
arbitrarily selected, but it is typically preferable to employ a flow rate
of 10 to 50 l/min and a pressure of about 1 atm. Although the embodiment
shown in the drawing uses the two-stage refrigeration unit using the
Gifford-McMahon cycle, a Joule-Thomson circuit can be combined with the
refrigeration unit in order to achieve an even lower temperature.
The gaseous refrigerant cooled in the device of the present invention can
be employed outside the device. In this case, for example, the additional
sample-receiving chamber 46 is caused to communicate with the pipes 40 and
42 by the adiabatic pipes 47 and 48, as shown in the drawing, by sealing
the receiving chamber 8 and closing the valve 44. In addition, the device
of the present invention is typically used for maintaining the specimen at
a temperature within the range of room temperature to an extremely low
temperature, but the device can be used for maintaining the specimen at a
temperature higher than room temperature by using the heater 32 which is
included in the device. The device can also be used for maintaining the
specimen at a constant temperature of about 4 k. or about 77 K. by
stopping the circulation of the gaseous refrigerant and introducing liquid
helium or liquid nitrogen from the pipe of the sample-receiving chamber 8.
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Description  |
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