Patent Application
20160268028
The present invention relates to a superconducting magnet.
Background art of the technical field can be found in Japanese Unexamined Patent Application Publication No. 2012-238628 (Patent Literature 1). This literature describes that “it is an object of the invention to provide a high-temperature superconducting magnet capable of detecting with a high accuracy a voltage at which a quench occurs which corresponds to a normal conduction transition phenomenon of a superconducting coil and thereby quickly detecting an occurrence of the quench and performing a protective operation, in which the occurrence of the quench is detected by winding the superconducting magnet with a parallel conductor constituted by electrically connecting constituent conductors each other by at least two points, arranging voltage terminals at a superconducting wire rod in each section of the electrically connected parallel conductor, and observing the potential difference.”
Moreover, there is also Japanese Unexamined Patent Application Publication No. Hei8(1996)-304271 (Patent Literature 2). This literature describes that “aiming at providing an apparatus and a method for detecting a quench occurrence capable of sensing a minute change thereof and observing the change of a whole system at an initial stage of the quench occurrence, the apparatus for detecting the quench of a superconducting wire rod detects by using an optical fiber wound around the superconducting wire rod, a light source emitting a deflected beam into the optical fiber, and a device that detects a polarization from the optical fiber.”
However, connection of the voltage terminal in each section by soldering, for example, would make the configuration of the superconducting coil complicated. Moreover, to detect a quench using the deflected beam, it would require a plurality of polarizing plates and mirrors to form the deflected beam, which makes the measurement system more complicated.
Thus, an object of the present invention is to provide a superconducting magnet that makes it possible to detect a temperature increase due to normal conduction transition of a superconducting coil with a simple configuration.
To solve the aforementioned problems, for example, a configuration described in one of the appended claims is employed.
This application includes a plurality of means for solving the aforementioned problem, one example of which is characterized in that “it includes: a superconducting coil that is formed by winding a first superconducting wire rod; a second superconducting wire rod, which is assembled by being thermally in contact with and electrically insulated from the superconducting coil, and which has a superconducting transition temperature lower than that of the first superconducting wire rod; voltage terminals connected at a plurality of locations on the second superconducting wire rod; a voltmeter connected to the voltage terminals; and a switch circuit connected to the voltmeter, and that the switch circuit interrupts a current to be supplied to the superconducting coil upon receiving an output from the voltmeter.”
The present invention can provide a superconducting magnet making it possible to detect a temperature increase due to normal conduction transition of a superconducting coil with a simple configuration.
[
[
[
[
[
[
Hereinbelow, embodiments of the present invention will be described with reference to drawings.
A superconducting magnet 1 of this embodiment will be described with reference to
The superconducting coil 2 is formed by winding a superconducting wire rod 16 around a winding frame 26. The superconducting wire rod 16 is connected at its end to an external power source 56 by the current leads 46a, 46b, and the superconducting coil 2 can generate a magnetic field upon receiving a current supplied from the external power source 56.
Moreover, the superconducting magnet 1 needs to cool the superconducting coil 2 to a certain temperature or lower to retain a superconducting state. In this embodiment, the superconducting coil 2 is retained under a low temperature by immersing it in a cooling medium, e.g. liquid helium, in the cryostat 36.
It should be noted that any cooling method can be used such as a method of immersing it in a liquid cooling medium or a conduction cooling method using a metal having a high thermal conductivity such as pure copper. A refrigerator (not shown) may be used for cooling the cooling medium or for conduction cooling, and a thermal shield (not shown) may be provided so as to cover the superconducting coil 2 in order to block heat penetration from the outside.
The superconducting coil 2 is connected to the external power source 56 via the current leads 46a, 46b, as described above. When operating the superconducting magnet 1, the external power source 56 should energize the superconducting coil 2, and the current must be interrupted if any failure occurs to the superconducting coil 2 or the circuit that includes the superconducting coil 2 at this time.
Especially, if there is a phenomenon (quench phenomenon) in which the temperature increases in a part of the superconducting coil 2 for some reason and an electrical resistance arises from normal conduction transition in this part, which results in a chain reaction of the normal conduction transition all over the superconducting coil 2, it is desirable to immediately stop the energization to the superconducting coil 2 and consume accumulated magnetic energy so that the superconducting coil 2 will not be broken. Causes of unexpected normal conduction transition of the superconducting coil may include deterioration and a manufacturing error of the superconducting coil 2, a failure of the refrigerator, a breakage of the thermal shield, and the like.
In order to stop the energization to the superconducting coil 2 and consume the accumulated magnetic energy when the failure of the superconducting magnet 1 occurs, the following methods can be contemplated.
For example, the electrical resistance caused by the normal conduction transition in apart of the superconducting coil 2 is detected by measuring a voltage related to the resistance using the voltage terminals 66a, 66b. The measurement of the voltage can be implemented by providing the voltage terminals 66a, 66b at unwinding portions of the superconducting wire rod 16 forming the superconducting coil 2, respectively.
The measurement result of the voltage is transmitted to a switch drive circuit 76, and the switch drive circuit 76 that received the result opens a switch 86, whereby connection between the superconducting coil 2 and the external power source 56 is interrupted to stop the energization to the superconducting coil 2. Furthermore, by opening the switch 86, a closed circuit is formed with the superconducting coil 2 and a protection circuit 96. In this closed circuit, the energy accumulated in the superconducting coil 2 is consumed as heat generated in a protection resistor included in the protection circuit 96, thereby suppressing energy release caused by the superconducting coil 2 generating the heat itself.
In this embodiment, the superconducting wire rod 16 includes a wire rod 11a that is a first superconducting wire rod and a wire rod 11b that is a second superconducting wire rod, and the wire rod 11a and the wire rod 11b are constituted by wire rods having different conducting transition temperatures. Moreover, this embodiment employs the wire rod 11a having a conducting transition temperature higher than that of the wire rod 11b.
These wire rods 11a, 11b are coated with an electrical insulating material 31 like a resin, for example, to be electrically insulated from one another while being thermally in contact with one another. The superconducting coil 2 is formed by winding a conductor 41 including the wire rod 11a, the wire rod 11b, and the electrical insulating material 31.
In the superconducting coil 2 according to this embodiment, a coil made of the wire rod 11a having a higher conducting transition temperature among the two different wire rods 11a, 11b acts as a main superconducting coil mainly intended to generate the magnetic field. On the other hand, a coil formed of the wire rod 11b having a lower conducting transition temperature acts as a sub superconducting coil mainly intended to detect the temperature increase. The external power source 56 may be connected to the main superconducting coil and the sub superconducting coil may be configured to be connected to another current source prepared separately.
Attached to both ends of the wire rod 11b are voltage terminals 21a, 21b, and a single voltage terminal 21c is attached within the winding, that is, to the intermediate portion of the wire rod. Thus, in the wire rod 11b, when the normal conduction transition occurs between the voltage terminal 21a and the voltage terminal 21c, the voltage is measured between these terminals, and if the normal conduction transition occurs between the voltage terminal 21b and the voltage terminal 21c, the voltage is measured between these terminals.
Hereinbelow, a function of detecting the temperature increase in the main superconducting coil using the sub superconducting coil formed of the wire rod 11b will be explained.
While operating the superconducting magnet 1, the current is applied from the external power source 56 to the superconducting coil 2. If there occurs transition from the superconducting state to the normal conducting state in the wire rod 11a constituting the main superconducting coil for some reason, a resistance value of the main superconducting coil changes from R1>=0 to R1>0.
Assuming the applied current as I1, a heat amount of R1I12 is generated in the portion of the main superconducting coil where the normal conduction transition occurred. Because the heat is also transferred to other portions than where the normal conduction transition occurred first, a region of which the temperature exceeds the superconducting transition temperature, namely the normal conduction transition region, expands in the wire rod 11a, and consequently the R1 of the main superconducting coil increases according to the elapsed time.
On the other hand, the heat generated in the wire rod 11a also propagates to the wire rod 11b thermally in contact with the wire rod 11a. This causes the normal conduction transition in the wire rod 11b and therefore a resistance R2a or R2b is also generated in the sub superconducting coil formed of the wire rod 11b. Assuming the current flowing through the sub superconducting coil as I2, the heat amount generated in the wire rod 11b is R2aI22 or R2bI22, for this heat generation the normal conduction transition region also expands in the sub superconducting coil, and consequently the resistance value (R2a, R2b) of the sub superconducting coil formed of the wire rod 11b also increases according to the elapsed time.
In this manner, when the normal conduction transition occurs in the superconducting coil 2, the normal conduction transition region expands in both of the main superconducting coil and the sub superconducting coil. However, compared to the wire rod 11a, the wire rod 11b has a smaller heat capacity before the normal conduction transition because it has a lower conducting transition temperature. Therefore, the propagation speed of the normal conduction transition region is higher in the wire rod 11b than in the wire rod 11a.
For example, when using a niobium titanium wire rod as the wire rod 11b and a bismuth-based copper oxide superconducting wire rod as the wire rod 11a, the propagation speed of the normal conduction transition region in the wire rod 11b can be 1000 times or more of the propagation speed in the wire rod 11a that is several mm/s.
The strength of the voltage generated in the superconducting coil increases along with the propagation of the normal conduction transition region because it depends on the size of the normal conduction transition region. Thus, the voltage generated in the sub superconducting coil formed of the wire rod 11b has a higher increase rate than the voltage generated in the main superconducting coil formed of wire rod 11a having a larger heat capacity before the normal conduction transition than that of the wire rod 11b.
Now, the superconducting magnet 1 according to this embodiment measures the voltage generated in the sub superconducting coil formed of the wire rod 11b, opens the switch 86 through the switch drive circuit 76 according to the voltage value, and interrupts the connection between the external power source 56 and the superconducting coil 2. The mechanism of interrupting sharing of the current to the superconducting coil 2 or the main superconducting coil by interrupting the connection between the external power source 56 and the superconducting coil 2 may employ a breaker instead of the switch 86. For the reasons above, the superconducting magnet 1 according to the first embodiment does not necessarily require electrical connection to detect the voltage of the main superconducting coil.
After shutting down the external power source 56, the magnetic energy 0.5 L1I12 accumulated in the main superconducting coil formed of the wire rod 11a is released by a protection resistor Rs for relaxation time of L1/Rs.
When there is a certain degree of difference between the superconducting transition temperatures of the wire rod 11a and the wire rod 11b, even in a state where the temperature increase is observed in the main superconducting coil but the normal conduction transition has not occurred yet, the normal conduction transition in the sub superconducting coil deriving from the heat propagated from the main superconducting coil can be detected, and therefore it is possible to stop the superconducting magnet 1 at a stage where the load applied to the main superconducting coil is still small.
Furthermore, an attachment position of the voltage terminal 21c maybe the position where L2a=L2b is achieved as shown in
Thus, by arranging the voltage terminals 21a, 21b, 21c as described above, it is possible to measure the difference between voltages generated at L2a and L2b, and to highly accurately detect an abnormality in the wire rod 11a assuming that there is no resistance caused by a temperature increase if the difference is zero and that there is the resistance cause by the temperature increase if any difference is detected.
Additionally, the voltage between the voltage terminal 21a and the voltage terminal 21b may be measured while the superconducting magnet 1 is properly operating, and the temperature increase in the wire rod 11a may be detected based on the difference between the measured reference voltage and a voltage measured in real time. In this case, because there is no need of arranging the voltage terminal 21c, the mechanism of detecting the temperature increase in the main superconducting coil can be simplified.
As described above, the superconducting magnet 1 according to this embodiment does not need to connect the wound superconducting wire rods in parallel with each other or to provide voltage terminal pairs by separating the superconducting wire rod into small sections in order to detect the generated voltage in the main superconducting coil, and it makes it possible to detect the generated voltage with a simple structure.
Furthermore, provided that the wire rod 11a and the wire rod 11b are thermally in contact with each other, there is no need of attaching a voltage terminal pair to the main superconducting coil formed of the wire rod 11a. That is, because no heat is applied to the wire rod 11a due to soldering, it is possible to prevent degradation of superconducting properties of the wire rod 11a.
For example, when using so-called high-temperature superconducting wire rod such as a bismuth-based copper oxide wire rod or an yttrium-based copper oxide wire rod as the wire rod 11a and 200° C. or higher heat is applied thereto by a soldering iron, its superconducting properties may be degraded. However, this embodiment can reduce the connection with soldering, which is especially effective in reducing degradation factors of the superconducting properties when fabricating the superconducting coils using the high-temperature superconducting wire rod as the main wire rod.
In this embodiment, in addition to the superconducting coil having the voltage terminal within the winding, an example of a superconducting coil capable of detecting the temperature increase using only the voltage terminal pair on both ends is described.
In the superconducting coil 2 shown in
In the second embodiment, two second superconducting wire rods 13b, 13c thermally in contact with the wire rod 11a are wound. The wire rods 13b, 13c form two sub superconducting coils having the same inductance L2′. Voltage terminals 23a, 23b, 23c, 23d are provided at both ends of the sub superconducting coils to measure voltages.
As shown in
Although the first embodiment requires an operation of identifying the position in which the inductance L2a=L2b is achieved when disposing the voltage terminal within the winding, the identifying operation can be omitted in the second embodiment, thereby reducing the load of fabricating the superconducting coil 2.
It should be noted that there may be prepared a plurality of wire rods 13b and wire rods 13c and the same number of them may be wound around the main superconducting coil. In doing so, the number of the wire rods to which the current is applied in one direction should be same as the number of the wire rods to which the current is applied in an opposite direction.
In this embodiment, in addition to the superconducting magnet formed by twisting the first superconducting wire rod and the second superconducting wire rod together, an example of a superconducting magnet capable of detecting the temperature increase by partially bringing the second superconducting wire rod into thermal contact will be described.
In the superconducting coil shown in
In the third embodiment, a second superconducting wire rod 35 is brought into contact from a surface of the superconducting coil with an outer peripheral surface of the superconducting coil formed of the wound first superconducting wire rod 11a, namely the outer peripheral surface of the superconducting coil formed into a cylindrical shape. Voltage terminals 25a, 25b are provided at both ends of the wire rod 35 to measure the voltage, and the current in the superconducting coil formed of the first wire rod 11a is interrupted according to the measure voltage, as in the first or second embodiment. Because the wire rod 35 is made shorter, unlike the first or second embodiment, the inductance due to the second wire rod is low and there is no need of forming a circuit to cancel the inductance.
Moreover, the wire rod 35 may be disposed with respect to the coil formed of the wire rod 11a as described below. First, the wire rod 35 is disposed to be parallel with the wire rod 11a as much as possible. The direction of the current applied to the wire rod 35 should be the same direction as the current applied to the wire rod 11a. By disposing the wire rod 35 and controlling the direction of the current as described above, an electromagnetic force is applied to the wire rod 35 in the direction 45 due to the direction 55 of the magnetic field generated by the superconducting coil formed of the wire rod 11a. As a result, the wire rod 35 receives a force to be pressed against the wire rod 11a, thereby reducing the contact thermal resistance between the first and second superconducting wire rods 11a, 35 and improving an accuracy of detecting the temperature increase.
It should be noted that the structures of detecting the generated voltage including the wire rod 35 and the voltage terminals 25a, 25b connected to the both ends of the wire rod 35 may be provided at a plurality of locations on the superconducting coil formed of the wire rod 11a. By disposing the structures at the plurality of locations, it is made possible to detect the temperature increase in the superconducting coil formed of the wire rod 11a with a higher accuracy.
| Filing Document | Filing Date | Country | Kind |
|---|---|---|---|
| PCT/JP2013/080847 | 11/15/2013 | WO | 00 |
