JP5060275B2 - Superconducting coil device - Google Patents

Description

  The present invention relates to a superconducting coil device used for a liquid refrigerant cooling type superconducting magnet typified by a superconducting magnetic energy storage device and a refrigerator cooling type superconducting magnet.

  Superconducting magnetic energy storage (hereinafter abbreviated as SMES) has features such as higher storage efficiency and faster energy input / output compared to other energy storage devices. It is being advanced. In this case, in order to take out predetermined electric power, in order to avoid making the voltage higher than necessary, it is often designed to increase the current capacity of the superconducting coil.

  Therefore, a current of 500 A to 1 kA or more is supplied to the superconducting coil. In order to allow a superconducting current to flow through the superconducting coil in a magnetically stable manner, the filament diameter of the superconducting coil needs to be reduced to a certain extent. Therefore, it is difficult to increase the current capacity of the superconducting coil by increasing the diameter of the superconducting wire.

  To increase the current capacity of the superconducting coil while reducing the filament diameter, it is sufficient to increase the number of filaments in the superconducting element wire, but it is difficult to increase the number of filaments in the superconducting element wire due to problems in manufacturing equipment. Accompanying sex.

  Therefore, in order to increase the current capacity of the superconducting coil, a method is known in which a plurality of superconducting wires are bundled to form a collective conductor. Examples of conductors obtained by this method include cable-in-conduit conductors and Rutherford conductors. However, in these conductors, current concentrates on specific wires, and if the electrical resistance between the wires is reduced to prevent it, a coupling current flows between the wires, causing a large AC loss. Therefore, there is a problem that handling is difficult.

  On the other hand, as a method for increasing the current capacity, a configuration has been proposed in which a plurality of superconducting coils made of conductors having a small current capacity are connected in parallel instead of increasing the capacity of the conductor as described above. In this case, since the electric resistance of each superconducting coil is zero, the current flowing through each superconducting coil has a current distribution corresponding to a slight ratio of connection resistance. In extreme cases, the distribution ratio is several times between the parallel coils. There may be a problem of current flow.

  As a method for solving this problem, for example, with respect to a plurality of superconducting coils housed in a cooling container, each superconducting coil leads its terminals individually out of the container with individual current leads. It has been proposed to improve the distribution of current flowing in each superconducting coil by connecting a power source between the current leads (see, for example, Patent Document 1).

According to this, the distribution of the current flowing through each superconducting coil is determined by the resistance value of the current lead. The influence of the connection resistance can be reduced by setting the resistance value of the current lead to a certain large resistance value. As a result, the distribution ratio of the current flowing through the superconducting coils connected in parallel does not increase several times due to slight variations in connection resistance, and the current drift problem that a large current flows in a specific coil is avoided. I can do it.
JP 2006-332513 A

  However, in an actual circuit, a case where the critical current differs among the superconducting coils often occurs. Further, since the connection resistance between the coil terminals and the current cable connected thereto is different between each superconducting coil, even if the current lead connected to each superconducting coil is set to a constant value, each superconducting coil In other words, it is impossible to simultaneously flow up to different critical currents (intentional flow of different currents to each superconducting coil).

  If it is possible to energize in the magnetic flux flow region, such as an oxide superconducting coil, it can be expected to energize in a state where a minute voltage is generated. It becomes impossible to energize while keeping the coil balance by equalizing the voltage generated at both ends. Further, when the superconducting coil is quenched for some reason, the coil balance is in a good state (the critical current Ic of each superconducting coil and the energizing current Iop of each superconducting coil are in a state where Iop / Ic is substantially equal in each superconducting coil). If not, a large quench current is induced in a particular coil with a low Iop / Ic value, causing the coil to be mechanically damaged. The same can be said in common regardless of the type of oxide or metal.

  Due to the existence of such problems, a plurality of superconductivity has been achieved so far while reducing the drift, coupling loss, etc. in the collective conductor and reducing the difference in Iop / Ioc between the coils by balancing the coils. There was an inconvenience that it was difficult to energize the coil simultaneously.

  The present invention has been made in view of such circumstances, and in a superconducting coil device in which a plurality of superconducting coils are connected in parallel, the coil balance between the superconducting coils is taken to reduce the difference in Iop / Ioc. An object of the present invention is to provide a superconducting coil device that can be used.

A superconducting coil device according to the present invention includes a plurality of superconducting coils, a cooling container that houses and cools the plurality of superconducting coils, and pulls out one end of each superconducting coil to the outside of the cooling container. A first current lead connected to one pole of a power supply device for supplying current to the superconducting coil, and a second current lead connected to the other pole of the power supply device while pulling out the other end of each superconducting coil to the outside of the cooling vessel. 2 current leads, and a plurality of resistance portions provided in series with each superconducting coil in a current path from one end of each superconducting coil to one pole of the power supply device via the first current lead. the plurality of resistor portions, Ri configurable der is individually resistance, the electric current flowing through each of said superconducting coils, Iop of each of the superconducting coil, wherein each superconducting coil A field current, when the Ic of each of the superconducting coils, the resistance value of each resistor section, the so Iop / Ic are substantially equal to each other in each superconducting coil, is set.

  According to this configuration, the plurality of superconducting coils are cooled in the cooling container. In addition, one end of each superconducting coil is pulled out of the cooling container by a plurality of first current leads. Then, the other end of each superconducting coil is pulled out of the cooling container and connected to one pole of the power supply device by the second current lead. Furthermore, a plurality of resistance portions, which are provided in series with each superconducting coil and individually set with a resistance value in a current path from one end of each superconducting coil to one pole of the power supply device via the first current lead, are provided. Is provided.

  Then, since multiple superconducting coils are connected in parallel, it becomes possible to use a wire with a small current capacity as a superconducting wire. As a result, when using a large current capacity conductor such as a cable-in-conduit conductor or a rutherford conductor As described above, it becomes easy to reduce current concentration on a specific strand and increase in coupling loss. In addition, since the current value Iop of each superconducting coil can be adjusted by individually setting the resistance value of each resistance unit connected in series with each superconducting coil, the critical current between each superconducting coil can be adjusted. The difference in the ratio (Iop / Ic) between Ic and energization current Iop is reduced, and it becomes easy to balance the coils between the superconducting coils.

  Moreover, it is preferable that the said resistance part is arrange | positioned outside the said cooling container.

  According to this configuration, since the resistance portion is provided outside the cooling container, the possibility that the superconducting coil is heated by heat generated by the resistance portion is reduced. Further, if it is provided outside the cooling container, the Iop flowing through each coil by energization can be easily adjusted.

Further, in the plurality of resistance portions, the difference between the maximum value and the minimum value of the resistance values at the environmental temperature of each of the resistance portions is within a range of 5.0 × 10 ⁻⁷ Ω to 2.0 × 10 ⁻⁴ Ω. It is preferable that the resistance value of each resistance portion is set so that

According to this configuration, if the difference between the resistance values of the resistance portions is 2.0 × 10 ⁻⁴ Ω or less, the resistance values of the resistance portions can be reduced to approximately 2.0 × 10 ⁻⁴ Ω or less. Therefore, it becomes easy to exclude the heat generated by the resistance portion by forced cooling. Moreover, since the difference in resistance value of the resistance portion is 5.0 × 10 ⁻⁷ Ω or more, the difference in resistance value of the resistance portion approximates the resistance value of the connection resistance in the superconducting coil or current lead, and the energization current The risk of difficulty in adjusting Iop is reduced.

  Further, it is preferable that the plurality of resistance portions are cables, and the resistance value is set according to the length of the cable.

  According to this structure, the said resistance value is set according to the length of the cable connected in series with each superconducting coil. Then, since the cable has low resistance, if the resistance value is set by setting the length of the cable, it becomes easy to set a delicate resistance value for each resistance portion (each cable). As a result, it becomes easy to set the resistance value of each resistance portion (each cable) so as to reduce the difference in the ratio (Iop / Ic) between the critical current Ic and the conduction current Iop between the respective superconducting coils. .

  The plurality of resistance portions may be cables, and the resistance values may be set according to the thickness of the cables.

  Then, since the cable has a low resistance, if the resistance value is set by setting the thickness of the cable, it becomes easy to set a delicate resistance value for each resistance portion (each cable). As a result, it becomes easy to set the resistance value of each resistance portion (each cable) so as to reduce the difference in the ratio (Iop / Ic) between the critical current Ic and the conduction current Iop between the respective superconducting coils. .

  The plurality of resistance portions may be cables, and the resistance values may be set according to the material of the cables.

  Then, since the cable has low resistance, if the resistance value is set by setting the material of the cable, it is easy to set a delicate resistance value for each resistance portion (each cable). It becomes easy to set the resistance value of each resistance portion (each cable) so as to reduce the difference in the ratio (Iop / Ic) between the critical current Ic and the conduction current Iop between the superconducting coils.

  The plurality of resistance portions may be cables, and the resistance value may be set according to at least one of a length, a thickness, and a material of the cable.

  In the cable, the conductor is exposed in at least a part of the length direction, and the exposed conductor is exposed to one of the one end of each superconducting coil, the first current lead, and the power supply device. And the resistance value is preferably set according to the position of the connection location.

  According to this configuration, the other part of the power supply device can be changed by simply changing the connection portion between the exposed conductor portion of the cable and one end of each superconducting coil, the first current lead, and the power supply device. The length of the cable between the first electrode and the first current lead, that is, the resistance value can be changed, so that the difference in the ratio (Iop / Ic) between the critical current Ic and the conduction current Iop is reduced. It becomes easy to set the resistance value of the resistance portion (each cable).

  In the superconducting coil device having such a configuration, a plurality of superconducting coils are cooled in a cooling container. In addition, one end of each superconducting coil is pulled out of the cooling container by a plurality of first current leads. Then, the other end of each superconducting coil is pulled out of the cooling container and connected to one pole of the power supply device by the second current lead. Furthermore, the other poles of the power supply device and the plurality of first current leads drawn to the outside of the cooling container are connected to each other by a plurality of resistance portions each having a predetermined resistance value.

  Then, since multiple superconducting coils are connected in parallel, it becomes possible to use a wire with a small current capacity as a superconducting wire. As a result, when using a large current capacity conductor such as a cable-in-conduit conductor or a rutherford conductor As described above, it becomes easy to reduce current concentration on a specific strand and increase in coupling loss. Further, by individually setting the resistance value of each first current lead connected to one end of each superconducting coil, the conduction current Iop of each superconducting coil can be adjusted, so that between each superconducting coil, The difference in the ratio (Iop / Ic) between the critical current Ic and the energization current Iop is reduced, and it becomes easy to balance the coils between the superconducting coils.

  Embodiments according to the present invention will be described below with reference to the drawings. In addition, the structure which attached | subjected the same code | symbol in each figure shows that it is the same structure, The description is abbreviate | omitted. FIG. 1 is a circuit diagram showing an example of the configuration of a superconducting coil device according to an embodiment of the present invention. A superconducting coil device 1 shown in FIG. 1 includes, for example, superconducting coils A and B, external electrodes 3 and 4, internal electrodes 6, current leads 7 and 8 (first current leads), current leads 10 (second current leads), Electrical resistance adjusting cables 11 and 12 (resisting portion) and a cryostat 15 (cooling container) that accommodates the superconducting coils A and B are provided.

  The superconducting coils A and B are wound around, for example, the same frame to constitute a single pancake coil 2 that is a single pancake type coil body. Single pancake coil 2 includes superconducting coils A and B, external electrodes 3 and 4, and internal electrode 6.

  FIG. 2 is a schematic view showing the entire single pancake coil 2 shown in FIG. FIG. 3 is a cross-sectional view of the single pancake coil 2 shown in FIG. The single pancake coil 2 is configured by superconducting coils A and B being concentrically wound around a substantially cylindrical winding frame 20.

  The winding frame 20 is orthogonal to the cylindrical winding drum 21 around which the superconducting coils A and B are wound, and the direction in which the winding drum 21 extends from both axial ends of the winding drum 21 to the circumferential direction of the winding drum 21. And a flange 22 extending in the direction.

  And, for example, the tape-shaped superconducting wire A1 constituting the superconducting coil A and the tape-like superconducting wire B1 constituting the superconducting coil B are stacked in the thickness direction and in the stacked order. The single pancake coil 2 is configured by being concentrically wound around the upper portion of the winding frame 20 a predetermined number of times. In the winding state of the superconducting wires A1 and B1, the superconducting wire A1 is located on the radially inner side of the single pancake coil 2, and the superconducting wire B1 is located on the radially outer side of the single pancake coil 2.

  Further, inside the single pancake coil 2, the superconducting wire A1 and the superconducting wire B1 are not electrically connected except for the internal electrode 6, and the two superconducting coils independent of the superconducting coil A and the superconducting coil B are provided. Is configured.

  In addition, the internal electrode 6 is incorporated in a part of the winding drum 21. The internal electrode 6 is, for example, a bar-shaped copper member having a substantially semicircular cross section and extending in one direction. Then, one end on the winding start side of the superconducting wires A1 and B1 is connected to the internal electrode 6 by, for example, solder 64. One end of a current lead 10 is connected to the internal electrode 6.

  An external electrode 3 made of, for example, a flat copper member is attached to the other end of the superconducting wire A1. Furthermore, one end of a current lead 7 is connected to the external electrode 3. Moreover, the external electrode 4 made of, for example, a flat copper member is attached to the other end of the superconducting wire B1. Further, one end of a current lead 8 is connected to the external electrode 4.

  The cryostat 15 is, for example, a vacuum heat insulating container that houses the single pancake coil 2 together with liquid nitrogen or liquid helium. The cryostat 15 is configured to hold the single pancake coil 2 at an extremely low temperature while being thermally shielded from the external environment. The cryostat 15 may be of a type that cools the single pancake coil 2 with a refrigerator.

  The current leads 7, 8, and 10 are, for example, a superconducting current lead made of a superconductor that is exposed to cryogenic temperature in the cryostat 15, and copper or a copper alloy that is taken out of the cryostat 15 and exposed to room temperature. A low resistance metal conductor is connected in series. The superconducting current lead side of the current leads 7, 8, 10 is connected to the external electrodes 3, 4 and the internal electrode 6.

  A positive electrode of a DC power supply 100 (power supply device) is connected to a portion of the current lead 10 drawn out of the cryostat 15. Further, the negative electrode of the DC power supply 100 is connected to the portion of the current lead 7 drawn out of the cryostat 15 via the electric resistance adjusting cable 11. The negative electrode of the DC power supply 100 is connected to the portion of the current lead 8 drawn out of the cryostat 15 via the electric resistance adjusting cable 12.

  Thereby, a direct current is supplied from the direct current power source 100 to the superconducting coils A and B accommodated in the cryostat 15.

The electric resistance adjusting cables 11 and 12 are arranged outside the cryostat 15 and are, for example, cables having a cross-sectional area of 30 mm ² and a length of 500 mm. A part of the covering of the electric resistance adjusting cables 11 and 12 is removed over the entire length in the longitudinal direction, and the conductor is exposed. In addition, at least one of a connection portion between the electric resistance adjustment cables 11 and 12 and the current leads 7 and 8 and a connection portion between the electric resistance adjustment cables 11 and 12 and the DC power source 100 can be freely changed. ing.

  In this case, the current is changed by changing at least one of the connection location between the electrical resistance adjustment cables 11 and 12 and the current leads 7 and 8 and the connection location between the electrical resistance adjustment cables 11 and 12 and the DC power source 100. The resistance value Ra between the lead 7 and the DC power source 100 and the resistance value Rb between the current lead 8 and the DC power source 100 can be individually changed and set. Therefore, it becomes easy to set arbitrary resistance values Ra and Rb by changing the resistance values generated in the electric resistance adjusting cables 11 and 12.

  When the energizing current flowing through the superconducting coil is Iop, and the critical current of the superconducting coil is Ic, the electric resistance is adjusted so that Iop / Ic in the superconducting coil A and Iop / Ic in the superconducting coil B are substantially equal. A resistance value Ra and a resistance value Rb are set by the cables 11 and 12.

  The resistance value is set by setting at least one of the connection location between the electrical resistance adjustment cables 11 and 12 and the current leads 7 and 8 and the connection location between the electrical resistance adjustment cables 11 and 12 and the DC power source 100. It is not restricted to the example which sets Ra and resistance value Rb, For example, you may make it set resistance value Ra and resistance value Rb by setting the length of the electric resistance adjustment cables 11 and 12, respectively.

  The internal electrode 6 may be configured by connecting individual electrodes to the superconducting coils A and B, respectively. Further, instead of the current lead 10, a plurality of current leads may be connected in parallel so as to connect the individual electrodes and the DC power supply 100. Further, an electric resistance adjusting cable may be connected between the current lead 10 and the DC power supply 100.

  According to the superconducting coil device 1 configured as described above, by connecting a plurality of superconducting coils A and B in parallel, it becomes possible to use a wire having a small current capacity as the superconducting wires A1 and B1. This makes it easy to avoid technical problems such as current concentration and coupling loss on specific wires, which are problematic for large-capacity conductors such as cable-in-conduit conductors and Razaford conductors. Further, by individually adjusting the DC resistance (resistance values Ra and Rb) between the current leads 7 and 8 connected to the superconducting coils A and B and the DC power source 100, Iop of each superconducting coil A and B is adjusted. / Ic can be made substantially equal, and energization is possible with the coil balanced.

Also, the environmental temperature in the operating state of the superconducting coil device 1, for example, the difference in DC resistance between the current leads 7 and 8 and the DC power supply 100 at room temperature where the superconducting coil device 1 is installed is 5.0 ×. When the resistance values Ra and Rb are individually adjusted so as to be within the range of 10 ⁻⁷ Ω to 2.0 × 10 ⁻⁴ Ω, if one of the electric resistance adjustment cables 11 and 12 is set to approximately 0Ω, The heat generated by the resistance corresponding to the adjustment is 200 W at the maximum even when the current is 1000 A. If the heat generation is 200 W at maximum, stable energization is possible by forcibly cooling the heat generation part. Since the resistance heat generated by the adjustment is generated outside the cryostat 15 that cools the superconducting coil, the cooling efficiency of the superconducting coils A and B is hardly affected.

When the difference in DC resistance is smaller than 5.0 × 10 ⁻⁷ Ω, it approaches the value of the connection resistance of the circuit system, and it becomes difficult to adjust the Iop / Ic of the superconducting coils A and B to be equal. If the difference in DC resistance from the current leads 7 and 8 to the DC power supply 100 is larger than 2.0 × 10 ⁻⁴ Ω, the heat generated by the adjusted resistance becomes too large, and the Iop of the superconducting coils A and B is increased. Even if / Ic can be made equal, stable energization cannot be performed. A more desirable difference in DC resistance from each current lead to the power source is 2.0 × 10 ⁻⁶ Ω to 8.0 × 10 ⁻⁵ Ω.

  For example, as shown in FIG. 4, superconducting coils A and B in the single pancake coil 2 shown in FIG. 1 are further connected in parallel with a superconducting coil C to provide external electrodes 5, whereby three superconducting coils are arranged in parallel. You may comprise the connected single pancake coil 2a. Then, by connecting the external electrode 5 to the DC power source 100 via the current lead 9 (first current lead) and the electric resistance adjusting cable 13 (resistor portion), the superconducting coil device 1a may be configured. Good.

  For example, as shown in FIG. 5, the electrical resistance adjusting cables 11, 12, 13 are accommodated in the cryostat 15, and one end of the electrical resistance adjusting cables 11, 12, 13 is connected to the outside of the cryostat 15 by the current lead 7. It may be pulled out and connected to the DC power supply 100.

In the superconducting coil device 1a having such a configuration, the resistance values Ra, Rb, and Rc of the electric resistance adjusting cables 11, 12, and 13 are set so that, for example, all Iop / Ic in the superconducting coils A, B, and C are substantially equal. Is set. Further, the resistance values Ra, Rb are set so that the difference between the maximum value and the minimum value of the resistance values Ra, Rb, Rc is in the range of 5.0 × 10 ⁻⁷ Ω to 2.0 × 10 ⁻⁴ Ω. , Rc are set.

  A plurality of superconducting coils may be connected in parallel, and four or more superconducting coils may be connected in parallel. Moreover, the several superconducting coil should just be accommodated in the cryostat 15, and is not restricted to the example comprised as a single pancake coil.

  Hereinafter, the superconducting coil device 1 shown in FIG. 1 and the superconducting coil device 1a shown in FIG. Comparative Example 1 and Comparative Example 2 with the cable removed will be described.

(Comparative Example 1)
FIG. 6 is a circuit diagram illustrating a configuration of the superconducting coil device 101 according to the first comparative example. The superconducting coil device 101 shown in FIG. 6 does not include the electric resistance adjusting cables 11 and 12, and the current leads 7 and 8 are directly connected to the negative electrode of the DC power supply 100.

  Specifically, a superconducting wire A1 made of a Y-based tape wire having a width of 10 mm, a thickness of 0.12 mm, and a length of 5650 mm, and a superconducting wire made of a Y-based tape wire having a width of 10 mm, a thickness of 0.12 mm, and a length of 5670 mm. Two Y-based tape wires with B1 were prepared. Then, a glass cloth tape having a width of 10 mm and a thickness of 0.1 mm and these two superconducting wires A1 and B1 are overlapped, and each of the nine layers is wound around the winding frame 20 shown in FIG. Was made.

  Further, one end on the winding start side of the superconducting wires A1 and B1 was connected to the internal electrode 6 with solder. Then, external electrodes 3 and 4 were attached to the other ends of the superconducting wires A1 and B1, respectively. Inside the coil, except for the internal electrode 6, the superconducting wires A1 and B1 are not electrically connected, and constitute two independent superconducting coils of the superconducting coil A and the superconducting coil B.

  This single pancake coil 2 was mounted in a cryostat 15. The current lead 10 connected to the internal electrode 6 is shared by the superconducting coil A and the superconducting coil B. The external electrodes 3 and 4 are connected to individual current leads 7 and 8, respectively.

  Then, liquid nitrogen was introduced into the cryostat 15 to cool the single pancake coil 2. Furthermore, the current supplied to the superconducting coil device 101 was gradually increased by the DC power source 100, and the voltage Va at both ends of the superconducting coil A and the voltage Vb at both ends of the superconducting coil B were measured.

  FIG. 7 is a graph showing experimental results in Comparative Example 1. The horizontal axis indicates the current value supplied from the DC power source 100 to the superconducting coil device 101, that is, the total current It of the current Ia flowing through the superconducting coil A and the current Ib flowing through the superconducting coil B.

  The total current It when the electric field reference of 1.0 μV / cm is used is 102A when the reference is applied to the voltage Va of the inner superconducting wire A1 (superconducting coil A), and the voltage of the outer superconducting wire B1 (superconducting coil B). When the standard was applied to Vb, it was 116 A, and the difference between the two was 14 A.

  In addition, when the total current It is 102 A, a voltage corresponding to an electric field of 1.0 μV / cm is generated in the superconducting coil A and reaches a critical current, whereas almost no voltage is generated in the superconducting coil B. Absent. When a current of 50 A flows through each tape wire, the maximum empirical magnetic field generated by the superconducting coil is 5.6 mT. The critical currents of the superconducting coils A and B measured in advance at a liquid nitrogen temperature of 77.3 K and a magnetic field of 5.6 mT were 53 A and 63 A, respectively. When Iop / Ic of superconducting coil A was 53A / 53A = 1.00, Iop / Ic of superconducting coil B was (102−53) A / 63A = 0.78, and a difference of 22% occurred between the two. .

  Further, the above-described single pancake coil 2 in Comparative Example 1 was mounted on a refrigerator-cooled cryostat 15 to constitute a superconducting coil device 101 shown in FIG. The single pancake coil 2 was cooled to 20K, energized, and the voltages at both ends of the superconducting coil A and the superconducting coil B were measured.

  The total current It of current Ia and current Ib when using the electric field reference of 1.0 μV / cm is 510A when the reference is applied to the voltage Va of the inner superconducting wire A1 (superconducting coil A), and the outer superconducting wire B1. When the standard was applied to the voltage Vb of (superconducting coil B), it was 578 A, and the difference between them was 68 A.

  Further, when a current of 250 A is flowing through each of the superconducting wires A1 and B1, the maximum empirical magnetic field generated by the superconducting coil is 16.8 mT. The critical currents measured in advance for the superconducting coils A and B at a temperature of 20K and a magnetic field of 28.0 mT were 263A and 312A, respectively. When Iop / Ic of the superconducting coil A is 263A / 263A = 1.00, Iop / Ic of the superconducting coil B is (510-263) A / 312A = 0.79, and a difference of 21% occurs between the two. .

(Comparative Example 2)
FIG. 8 is a circuit diagram showing a configuration of a superconducting coil device 101a according to Comparative Example 2. The superconducting coil device 101 a shown in FIG. 8 does not include the electric resistance adjusting cables 11, 12, 13, and the current leads 7, 8, 9 are directly connected to the negative electrode of the DC power supply 100.

  Specifically, a superconducting wire A1 made of a Y-based tape wire having a width of 10 mm, a thickness of 0.2 mm, and a length of 4500 mm, and a superconducting wire made of a Y-based tape wire having a width of 10 mm, a thickness of 0.2 mm, and a length of 4507 mm. Three Y-based tape wires of B1 and a superconducting wire C1 made of a Y-based tape wire having a width of 10 mm, a thickness of 0.2 mm, and a length of 4515 mm were prepared. Then, a glass cloth tape having a width of 10 mm and a thickness of 0.1 mm and these three superconducting wires A1, B1, and C1 are overlapped, and each of the seven layers is wound around the reel 20 shown in FIG. Coil 2 was produced.

  Further, one end on the winding start side of the superconducting wires A1, B1, C1 was connected to the internal electrode 6 by soldering. Then, external electrodes 3, 4, and 5 were attached to the other ends of the superconducting wires A1, B1, and C1, respectively. Inside the coil, the superconducting wires A 1, B 1, C 1 are not electrically connected except for the internal electrode 6, and constitutes three independent superconducting coils of the superconducting coil A, the superconducting coil B, and the superconducting coil C. is doing.

  This single pancake coil 2 was mounted in a cryostat 15. The current lead 10 connected to the internal electrode 6 is shared by the superconducting coil A, the superconducting coil B, and the superconducting coil C. The external electrodes 3, 4, 5 are connected to individual current leads 7, 8, 9, respectively.

  Then, liquid nitrogen was introduced into the cryostat 15 to cool the single pancake coil 2. Further, the current supplied to the superconducting coil device 101 is gradually increased by the DC power source 100, and the voltage Va at both ends of the superconducting coil A, the voltage Vb at both ends of the superconducting coil B, and the voltage Vc at both ends of the superconducting coil C are obtained. Each was measured.

  The total current It of the current Ia flowing through the superconducting coil A, the current Ib flowing through the superconducting coil B, and the current Ic flowing through the superconducting coil C when the electric field reference of 1.0 μV / cm is used is the superconducting wire A1 (superconducting). 165A is applied to the voltage Va of the coil A), 191A is applied to the voltage Vb of the central superconducting wire B1 (superconducting coil B), and 191A is applied to the voltage Vc of the outer superconducting wire C1 (superconducting coil C). Then, it became 168 A, and the difference between the maximum value and the minimum value of the current values in the currents Ia, Ib, and Ic was 26 A.

  Further, when 50 A of current flows through each of the superconducting wires A1, B1, and C1, the maximum empirical magnetic field generated by the superconducting coil is 2.1 mT. The critical currents of the superconducting coils A, B, and C measured in advance at a liquid nitrogen temperature of 77.3 K and a magnetic field of 2.1 mT were 56 A, 59 A, and 64 A, respectively.

  In the current-voltage characteristics of the outer superconducting wire C1, the total current It when using an electric field reference of 1.0 μV / cm is 168 A. Therefore, Iop / Ic of the superconducting coil A in this state is {56+ ( 168-165)} A / 56A = 1.05, Iop / Ic of superconducting coil C is 64A / 64A = 1.00, Iop / Ic of superconducting coil B is (168-59-64) A / 59A = 0. That would be 76. That is, the difference between the maximum value and the minimum value at each Iop / Ic of the three coils was 1.05-0.76 = 29%.

  Further, the above-described single pancake coil 2 in Comparative Example 2 was mounted on a refrigerator-cooled cryostat 15 to constitute a superconducting coil device 101a shown in FIG. The single pancake coil 2 was cooled to 20K, energized, and the voltages at both ends of the superconducting coil A, superconducting coil B, and superconducting coil C were measured.

  The total current It of the superconducting coil A, the superconducting coil B, and the superconducting coil C when the electric field reference of 1.0 μV / cm is used is 825 A when the reference is applied to the voltage of the superconducting coil A, and the reference is applied to the voltage of the superconducting coil B. It was 957 A when applied, and 838 A when the standard was applied to the voltage of the superconducting coil C, and the difference between the maximum value and the minimum value of each total current It in the three superconducting coils was 132 A.

  Further, when a current of 270 A flows through each of the superconducting wires A1, B1, and C1, the maximum empirical magnetic field generated by the superconducting coil is 11.3 mT.

  The critical currents of the superconducting coils A, B, and C measured in advance at a temperature of 20K and a magnetic field of 11.3 mT were 280A, 294A, and 318A, respectively.

  In the current-voltage characteristics of the outer superconducting wire C1, the total current It when using an electric field reference of 1.0 μV / cm is 838A, so that the Iop / Ic of the superconducting coil A is {280+ (838-825). } When A / 280A = 1.05, Iop / Ic of superconducting coil C is 318A / 318A = 1.00, and Iop / Ic of superconducting coil B is (838-293-318) A / 294A = 0.77. Yes, the difference between the maximum value and the minimum value of each Iop / Ic in the three superconducting coils was 1.05-0.77 = 28%.

Example 1
In the superconducting coil device 1 shown in FIG. 1, the single pancake coil 2 produced in Comparative Example 1 was mounted in a cryostat 15 introduced with liquid nitrogen and cooled. Further, the external electrodes 3 and 4 of the superconducting coils A and B are connected to the individual current leads 7 and 8, respectively, and in the middle of the cable connecting the current leads 7 and 8 to the DC power source 100, a conductor cross-sectional area of 30 mm ² , The electric resistance adjusting cables 11 and 12 having a total length of 500 mm (the covering is partially removed in the longitudinal direction and the electric resistance can be adjusted by selecting an appropriate length) 7 and 8 were connected in series.

Further, the length of the portion used by the electric resistance adjusting cable 11 connected to the current lead 7 for the inner superconducting wire A1 (superconducting coil A) is set to 200 mm, and the outer superconducting wire B1 (superconducting coil B) is used. The length of the portion of the electric resistance adjusting cable 12 connected to the current lead 8 is 115 mm. At this time, the difference between the lengths of the portions used by the two cables for adjusting electrical resistance is 85 mm, and the difference in electrical resistance is 5.0 × 10 ⁻⁵ Ω.

  Then, the current supplied to the superconducting coil device 1 was gradually increased by the DC power source 100, and the voltage Va at both ends of the superconducting coil A and the voltage Vb at both ends of the superconducting coil B were measured.

  FIG. 9 is a graph showing experimental results of Example 1 in which the superconducting coil device 1 shown in FIG. The horizontal axis represents the current value supplied from the DC power source 100 to the superconducting coil device 1, that is, the total current It of the current Ia flowing through the superconducting coil A and the current Ib flowing through the superconducting coil B.

  The total current It when the electric field reference of 1.0 μV / cm is used is 116A when the reference is applied to the voltage Va of the inner superconducting wire A1 (superconducting coil A), and the voltage of the outer superconducting wire B1 (superconducting coil B). When the standard is applied to Vb, it becomes 117 A, and the difference between them is only 1 A.

  When Iop / Ic of superconducting coil A is 53A / 53A = 1.00, Iop / Ic of superconducting coil B is (116−53) A / 63A = 1.00, and the difference between the two is Comparative Example 1. Thus, the coil balance could be ideally reduced.

  Further, the above-described single pancake coil 2 in Example 1 was mounted on a refrigerator-cooled cryostat 15 to constitute the superconducting coil device 1 shown in FIG. The single pancake coil 2 was cooled to 20K, energized, and the voltages at both ends of the superconducting coil A and the superconducting coil B were measured.

  When the electric field reference of 1.0 μV / cm is used, the total current It of current Ia and current Ib is 574A when the reference is applied to the voltage Va of the inner superconducting wire A1 (superconducting coil A), and the outer superconducting wire B1. When the standard is applied to the voltage Vb of (superconducting coil B), it is 585A, and the difference between them is only 11A.

  In addition, the maximum empirical magnetic field generated by the superconducting coil is 28.0 mT when 250 A of current flows through the superconducting wires A1 and B1. The critical currents measured in advance for the superconducting coils A and B at a temperature of 20K and a magnetic field of 28.0 mT were 263A and 312A, respectively. When Iop / Ic of superconducting coil A is 263A / 263A = 1.00, Iop / Ic of superconducting coil B is (574-263) A / 312A = 1.00, and the difference between the two is 21 in Comparative Example 1. % To 0%, and the coil balance was ideally achieved.

(Example 2)
In the superconducting coil device 1a shown in FIG. 4, the single pancake coil 2 produced in Comparative Example 2 was mounted in a cryostat 15 introduced with liquid nitrogen and cooled. Further, the external electrodes 3, 4, 5 of the superconducting coils A, B, C are connected to the individual current leads 7, 8, 9, respectively, and the middle of the cable connecting from the current leads 7, 8, 9 to the DC power supply 100. In addition, the conductor cross-sectional area is 30 mm ² , and the overall length is 500 mm (the coating is partially removed in the longitudinal direction and the electrical resistance can be adjusted by selecting an appropriate length). Cables 11, 12, and 13 were connected in series with current leads 7, 8, and 9.

  Further, the length of the portion used by the electric resistance adjusting cable 11 connected to the current lead 7 for the inner superconducting wire A1 (superconducting coil A) is set to 230 mm, and the central superconducting wire B1 (superconducting coil B) is used. The length of the portion of the electric resistance adjusting cable 12 connected to the current lead 8 used is 200 mm, and the electric resistance adjusting cable is connected to the current lead 9 for the superconducting wire C1 (superconducting coil C). The length of the portion used by the cable 13 was set to 230 mm, and the characteristics of both-end voltage and current of each superconducting coil were examined.

At this time, the difference in length between the shortest cable and the longest cable in each electric resistance adjustment cable is 30 mm, and the difference in electric resistance is 1.8 × 10 ⁻⁵ Ω. The total current It when using the electric field reference of 1.0 μV / cm is 179 A when the reference is applied to the voltage Va of the superconducting coil A and 176 A when the reference is applied to the voltage Vb of the superconducting coil B. When the standard was applied to the voltage Vc of the superconducting coil C, it was 181A.

  In the current-voltage characteristics of the superconducting coil A, the total current It when using an electric field reference of 1.0 μV / cm is 179 A. Therefore, the Iop / Ic of the superconducting coil A in this state is 56 A / 56 A = 1. .00, Iop / Ic of superconducting coil B is {59+ (179-176)} A / 59A = 1.05, and Iop / Ic of superconducting coil C is (179-56-62) /64=0.95. become.

  That is, the difference between the maximum value and the minimum value of each Iop / Ic in the three coils was 1.05-0.95 = 10%. Thus, according to Example 2, each Iop / Ic difference of the three coils could be reduced from 29% in Comparative Example 2 to 10%, and the coil balance could be improved.

  Further, the above-described single pancake coil 2 in Example 2 was mounted on a refrigerator-cooled cryostat 15 to constitute a superconducting coil device 1a shown in FIG. The single pancake coil 2 was cooled to 20K, energized, and the voltages at both ends of the superconducting coil A, superconducting coil B, and superconducting coil C were measured.

  The total current It of the superconducting coil A, the superconducting coil B, and the superconducting coil C when the electric field reference of 1.0 μV / cm is used is 895 A when the reference is applied to the voltage of the superconducting coil A, and the reference is applied to the voltage of the superconducting coil B. When applied to the voltage of the superconducting coil C, it was 905 A when applied, and the difference between the maximum value and the minimum value of each total current It in the three superconducting coils was 25 A.

  Further, the maximum empirical magnetic field generated by the superconducting coil was 12.4 mT when 300 A current was flowing through each of the superconducting wires A1, B1, and C1.

  In addition, the critical currents measured in advance for superconducting coils A, B, and C at a temperature of 20K and a magnetic field of 12.4 mT were 278A, 292A, and 315A, respectively. In the current-voltage characteristics of the outer superconducting wire A1, the total current It is 895 A when using the electric field reference of 1.0 μV / cm. Therefore, Iop / Ic of the superconducting coil A in this state is 278 A / 278 A. = 1.00, Iop / Ic of superconducting coil B is {292+ (895-880)} A / 292A = 1.05, Iop / Ic of superconducting coil C is (895-292-307) /315=0.94 It turns out that.

  That is, a value of 1.05-0.94 = 11% was obtained as the difference between the maximum value and the minimum value of each Iop / Ic in the superconducting coils A, B, and C. Thus, according to Example 2, the difference between the maximum value and the minimum value of each Iop / Ic of the three coils can be reduced from 28% of Comparative Example 2 to 11%, and the coil balance can be improved. It was.

  In the first and second embodiments, the internal electrode 6 is commonly used by a plurality of superconducting coils. However, as with the external electrode, an internal electrode may be used for each superconducting coil.

  Moreover, in Example 1 and Example 2, as a method of adjusting each DC electric resistance between the current lead connected to each superconducting coil and the power source, the length of the electric resistance adjusting cables 11, 12 (13) is adjusted. However, the same effect can be expected by adjusting the thickness and material of the electric resistance adjusting cables 11 and 12 (13).

For example, in the first embodiment, when a copper cable having a conductor cross-sectional area of 60 mm ² is used as the electric resistance adjusting cables 11 and 12, the length of the portion used by the electric resistance adjusting cable 11 is set to 400 mm. Even when the length of the portion used by the cable 12 is 230 mm, the same effect as in the first embodiment can be obtained.

Further, in Example 1, when the cable material is changed from copper to aluminum and a cable having a conductor cross-sectional area of 30 mm ² is used, the length of the portion used by the electric resistance adjusting cable 11 is 131 mm, and the electric resistance adjusting cable is used. Even when the length of the portion 12 used is 76 mm, the same effect as in the first embodiment can be obtained.

  As described above, according to the superconducting coil device according to the present invention, the coil balance between the plurality of superconducting coils is taken, and each strand is energized while reducing the difference in Iop / Ioc, and simultaneously with the plurality of superconducting coils. It is possible to generate a magnetic field. This makes it possible to supply a large current of a class of 500 A or more in total to the superconducting coil, and to avoid technical problems such as drift and coupling loss of the collective conductor of superconducting power equipment such as SMES. The coil device can be configured with a simple configuration.

It is a circuit diagram which shows an example of a structure of the superconducting coil apparatus which concerns on one Embodiment of this invention. It is the schematic which shows the whole single pancake coil shown in FIG. It is sectional drawing of the single pancake coil shown in FIG. It is a circuit diagram which shows the modification of the superconducting coil apparatus shown in FIG. It is a circuit diagram which shows the modification of the superconducting coil apparatus shown in FIG. 6 is a circuit diagram showing a configuration of a superconducting coil device according to Comparative Example 1. FIG. 10 is a graph showing experimental results in Comparative Example 1. 6 is a circuit diagram showing a configuration of a superconducting coil device according to Comparative Example 1. FIG. It is a graph which shows the experimental result of Example 1 which concerns on one Embodiment of this invention.

Explanation of symbols

1, 1a Superconducting coil device 2, 2a Single pancake coil 3, 4, 5 External electrode 6 Internal electrode 7, 8, 9, 10 Current lead 11, 12, 13 Electric resistance adjusting cable 15 Cryostat 100 DC power supply A, B , C Superconducting coil A1, B1, C1 Superconducting wire Ic Critical current Iop Energizing current It Total current

Claims (8)

A plurality of superconducting coils;
A cooling vessel that houses and cools the plurality of superconducting coils;
A first current lead connected to one of the poles of a power supply device for pulling out one end of each superconducting coil to the outside of the cooling container and supplying current to the plurality of superconducting coils;
A second current lead that connects the other end of each superconducting coil to the outside of the cooling vessel and connects to the other pole of the power supply device;
In a current path from one end of each superconducting coil to one pole of the power supply device via the first current lead, a plurality of resistance units provided in series with each superconducting coil,
Wherein the plurality of resistor section includes Ri configurable der is individually resistance,
When the energizing current flowing through each superconducting coil is Iop of each superconducting coil, and the critical current of each superconducting coil is Ic of each superconducting coil, the resistance value of each resistance unit is the value in each superconducting coil. A superconducting coil device, wherein Iop / Ic is set to be substantially equal to each other . The superconducting coil device according to claim 1, wherein the resistance portion is disposed outside the cooling container. The plurality of resistance portions are:
The resistance of each resistor is set so that the difference between the maximum value and the minimum value of the resistance value at the environmental temperature of each resistor is within the range of 5.0 × 10 ⁻⁷ Ω to 2.0 × 10 ⁻⁴ Ω. The superconducting coil device according to claim 1, wherein a resistance value is set. The plurality of resistance portions are:
It is a cable and the said resistance value is set according to the length of the said cable. The superconducting coil apparatus of any one of Claims 1-3 characterized by the above-mentioned. The plurality of resistance portions are:
The superconducting coil device according to any one of claims 1 to 3, wherein the resistance value is set according to a thickness of the cable. The plurality of resistance portions are:
It is a cable and the said resistance value is set according to the material of the said cable. The superconducting coil apparatus of any one of Claims 1-3 characterized by the above-mentioned. The plurality of resistance portions are cables;
The superconducting coil device according to any one of claims 1 to 3, wherein the resistance value is set according to at least one of a length, a thickness, and a material of the cable. The cable is
The conductor is exposed in at least part of the length direction,
In the exposed portion, one end of each superconducting coil, the first current lead, and any one of the power supply device and the exposed conductor are connected,
The superconducting coil device according to any one of claims 4 to 7, wherein the resistance value is set according to a position of the connection location.

Images