Patent Application
20170309384
The present invention relates to a superconducting coil.
Priority is claimed on Japanese Patent Application No. 2014-236194, filed on Nov. 21, 2014, the content of which is incorporated herein by reference.
In recent years, as superconducting wires, oxide superconducting wires (hereinafter, simply referred to as superconducting wires) have been developed, which are referred to as bismuth-based superconducting wires such as Bi2212 (Bi2Sr2CaCu2O8+δ) or Bi2223 (Bi2Sr2Ca2Cu3O10+δ) or yttrium-based superconducting wires such as RE123 (REBa2Cu3O7-δ), RE: rare earth element, for example, yttrium). Since the superconducting wires can be used in a relatively high temperature region, application development to superconducting coils is advanced. As a superconducting wire, a wire which is formed in a tape shape is known, and a superconducting coil which uses the superconducting wire, a pancake coil, a double pancake coil, or a superconducting coil in which a plurality of these coils are laminated had been developed.
In the superconducting coil, an electrode for supplying current to the wound superconducting wire is provided. Since the electrode is formed of a normal conductive member, a structure for decreasing heat generation from the electrode is required. For example, in a superconducting coil disclosed in Patent Document 1, an end portion of a wound superconducting wire is drawn out and is soldered so as to follow an electrode formed in an L shape. Accordingly, heat generation in the electrode is decreased.
[Patent Document 1] Japanese Unexamined Patent Application, First Publication No. 2012-164859
In general, in a superconducting coil, after a superconducting wire is wound, the superconducting wire is impregnated with a resin. Accordingly, in order to drawn out the superconducting wire from the superconducting coil, it is necessary to peel off the superconducting wire from the impregnating resin near the end portion of the superconducting coil. As a result of this work, a load is applied to an oxide superconductor of the superconducting wire, and there is a concern that superconducting characteristics may deteriorate.
In addition, a conductive member may be disposed around the superconducting coil such as a case where the superconducting coil is interposed between metal flanges for cooling a coil or the like from an upper surface and a lower surface of the conducting coil. If an electrode approaches the conductive member, there is a concern that discharging from the electrode to the flanges may be generated, withstand voltage of the superconducting coil decreases. Accordingly, in a case where the electrode is provided along an outer periphery of the superconducting coil, it is necessary to solder the electrode such that the electrode is within a height size of the superconducting coil, which requires a great deal of labor.
The present invention is made in consideration of the above-described circumstances of the conventional art, and an object thereof is to provide a superconducting coil in which heat generation in an electrode decreases, deterioration of superconducting characteristics does not easily occur, and withstand voltage can be increased by an easy work process.
In order to achieve the object, a superconducting coil according to an aspect of the present invention, includes: a coil body around which a superconducting wire is wound; an electrode member which includes a first surface, a second surface, a base portion, and an extension portion, the first surface facing an outer peripheral surface of the coil body, the second surface being positioned to be opposite to the first surface, the base portion being solder-joined to the superconducting wire of the coil body on the first surface, the extension portion extending from the second surface to the outside of the coil body; an electrode superconducting wire which extends from the second surface of the electrode member toward the extension portion and is solder-joined to the base portion and the extension portion, in which a relationship among a width W1 of the superconducting wire of the coil body, a width W2 of the base portion of the electrode member, and a width W3 of the electrode superconducting wire satisfies W1>W2≧W3.
According to the configuration of the aspect, since the electrode superconducting wire is solder-joined to the electrode member, current which flows to the electrode member is bypassed by the electrode superconducting wire, and it is possible to decrease heat generation of the electrode member.
In addition, according to the configuration of the aspect, the electrode member is solder-joined to the superconducting wire positioned on the outer peripheral surface of the coil body. Accordingly, since the electrode member can be joined to the superconducting wire by exposing only one surface of the superconducting wire positioned on the outer peripheral surface of the coil body, even in a case where a resin is impregnated into the coil body, a load is not easily added to the superconducting wire. Accordingly, in a connection process of the electrode member, deterioration of the superconducting characteristics does not easily occur.
Moreover, according to the configuration of the aspect, width sizes of the electrode member and the electrode superconducting wire are smaller than a width size of the superconducting wire of the coil body. Therefore, the electrode member does not protrude from an upper end and a lower end of the coil body in a width direction (with respect to the width size) of the coil body. Accordingly, even in a case where the coil body is interposed between conductive flanges, or the like, a distance between the flanges, and the electrode member and the electrode superconducting wire is secured, and it is possible to increase the withstand voltage of the superconducting coil.
The electrode member may include a third surface which extends in a direction intersecting a direction in which the second surface extends and a boundary portion which is positioned between the second surface and the third surface, and the electrode superconducting wire may be solder-joined to the base portion and the extension portion to cover the second surface, the third surface, and the boundary portion.
The relationship between a critical current density value Ic1 of the coil body and a critical current density value Ic2 of the electrode superconducting wire may satisfy Ic2≧Ic1.
In a case where the critical current density value of the electrode superconducting wire is lower than the critical current density value of the coil body, if current equal to or more than the critical current density value of the electrode superconducting wire flows to the coil body, the current flows to the electrode member, there is a concern that heat may be generated in the electrode member. According to the configuration of the aspect, since the critical current density value of the electrode superconducting wire is higher than the critical current density value of the coil body, current can flow to the superconducting coil up to the critical current density value of the coil body. Accordingly, it is possible to sufficiently exert capability of the superconducting coil.
Moreover, as described above, in the superconducting coil according to the aspect, the width of the electrode superconducting wire is narrower than the width of the superconducting wire of the coil body. It is possible to select the electrode superconducting wire by defining the width of the electrode superconducting wire based on the critical current density value of the superconducting wire.
A groove which extends from the second surface of the electrode member toward the extension portion and is larger than a width of the electrode superconducting wire over the base portion and the extension portion may be provided, and the electrode superconducting wire may be solder-joined to the base portion and the extension portion inside the groove.
According to the configuration of the aspect, since the solder-joining can be performed in a state where the electrode superconducting wire is disposed along the groove of the electrode member, workability of the solder-joining increases. In addition, the electrode superconducting wire is not disposed to be inclined with respect to the electrode member, and it is possible to prevent the electrode superconducting wire from protruding from the upper end and the lower end of the coil body in the width direction of the coil body. Accordingly, it is possible to reliably secure the withstand voltage of the superconducting coil.
Moreover, in the electrode member, since the superconducting wire of the coil body is solder-joined to the first surface and the electrode superconducting wire is solder-joined to the second surface, current flows in the thickness direction of the electrode member. Therefore, a distance between wires is decreased by thinning the electrode member, and it is possible to decrease a connection resistance. On the other hand, the electrode member needs to have a predetermined thickness in order to obtain sufficient rigidity which is not easily deformed by its own weight or a weak external force. Since the groove is provided in the electrode member, it is possible to increase second moment of area with respect to an axis of the electrode member in the thickness direction, and it is possible to increase rigidity of the electrode member. Since the groove is provided, in the electrode member, a distance between wires decreases while sufficient rigidity is provided, and it is possible to decrease connection resistance.
The superconducting wire may include a first base material, a first oxide superconducting layer which is provided on the first base material, and a first stabilizing layer which is provided on the first oxide superconducting layer, the electrode superconducting wire may include a second base material, a second oxide superconducting layer which is provided on the second base material, and a second stabilizing layer which is provided on the second oxide superconducting layer, the first stabilizing layer may be solder-joined to face the first surface of the electrode member, and the second stabilizing layer may be solder-joined to face the second surface of the electrode member.
According to the configuration of the aspect, since the superconducting wire has a lamination structure, it is possible to easily manufacture a superconducting wire having a thin width by only cutting the superconducting wire in the width direction. Accordingly, it is possible to easily form an electrode superconducting wire having a thin width with respect to the superconducting wire of the coil body.
An outer periphery of the electrode superconducting wire may be coated with copper.
According to the configuration of the aspect, since the electrode superconducting wire is coated with copper, not only current characteristics of the electrode superconducting wire can be stabilized, and but also the inside of the electrode superconducting wire can be sealed to prevent moisture intrusion and deterioration of superconducting characteristics due to moisture can be prevented. In addition, copper has favorable compatibility with respect to solder and high bondability with respect to solder. Since the outer periphery of the electrode superconducting wire is coated with copper, solder spreads to the side portion of the electrode superconducting wire when the electrode superconducting wire and the electrode member are joined to each other, joining strength between the electrode superconducting wire and the electrode member increases, and it is possible to prevent the electrode superconducting wire from being separated from the electrode member.
The superconducting wire of the coil body may be joined to the electrode member by a first solder member, the electrode member may be joined to the electrode superconducting wire by a second solder member, and a melting point of the first solder member is different from a melting point of the second solder member.
According to the configuration of the aspect, after the electrode member and the wire are soldered by one solder member having a high melting point, the electrode member and the wire can be soldered by other solder member having a low melting point. When the joining is performed by the solder member having a low melting point, the solder member having a high melting point is not melted by melting the solder at a lower temperature than that of the solder member having a high melting point. Accordingly, the wire can be solder-joined to each of the first surface and the second surface of the electrode member.
According to the aspect, since the electrode superconducting wire is solder-joined to the electrode member, current which flows to the electrode member is bypassed by the electrode superconducting wire, and it is possible to decrease heat generation of the electrode member. In addition, since the electrode member can be joined to the superconducting wire by exposing only the stabilizing layer of the superconducting wire positioned on the outer peripheral surface of the coil body, a load is not easily added to the superconducting wire. Accordingly, in the connection process of the electrode member, deterioration of the superconducting characteristics does not easily occur. Moreover, since the width sizes of the electrode member and the electrode superconducting wire are smaller than the width size of the superconducting wire of the coil body, the distance between the conductive member and the electrode member is secured around the coil body, and it is possible to increase withstand voltage of the superconducting coil.
Hereinafter, a superconducting coil according to an embodiment of the present invention will be described with reference to the drawings. In addition, in the drawings used in descriptions below, for easy understanding of features, characteristic portions may be enlarged for the sake of convenience, and the size ratio of each component or the like is not limited to a case of being the same as an actual size ratio.
The first coil 6A is a pancake-shaped coil in which a superconducting wire 1 is concentrically and circularly wound many times in the clockwise direction. The second coil 6B is a pancake-shaped coil in which a superconducting wire 1 is concentrically and circularly wound many times in the counterclockwise direction.
A winding start end of the first coil 6A and a winding start end of the second coil 6B, which are respectively positioned inside the coils 6A and 6B, are disposed to be adjacent to each other, and the winding start ends are electrically and mechanically connected to each other by a connection plate (not shown) having good conductivity to form the coil body 6. Moreover, electrode members 2 are joined to winding terminal ends positioned on the outermost peripheries of the coils 6A and 6B to form the electrode joint portions 7. In each electrode joint portion 7, an electrode superconducting wire 3 is joined to the electrode member 2.
The coil body 6 is fixed by the impregnating resin 5 and has a strong structure against stress due to a magnetic field. As the impregnating resin 5, a thermosetting resin such as an epoxy resin, a phenol resin, a urea resin, or a melamine resin can be used. Accordingly, it is possible to improve mechanical strength (coil rigidity) of the superconducting coil 10.
In the present embodiment, as the superconducting wire 1, an yttrium based oxide superconducting wire is exemplified. The superconducting wire 1 has a structure in which an intermediate layer 15, an oxide superconducting layer 17, and a protective layer 18 are laminated on a taper-shaped base material 11 and a stabilizing layer 19 is laminated on at least the protective layer 18. In addition, the superconducting wire 1 is wound as the coils 6A and 6B in a state of being covered with an insulating coating layer 20. As shown in
As the base material 11, a nickel alloy represented by Hastelloy (trade name, manufactured by Haynes Corporation, USA), stainless steel, and textured Ni—W alloy obtained by introducing a texture to a nickel alloy are applied. The thickness of the base material 11 may be appropriately adjusted according to the purpose and may be in the range of 10 to 500 μm.
The intermediate layer 15 is formed on the upper surface of the base material 11. As an example, the intermediate layer 15 may have a structure in which a diffusion prevention layer, a bed layer, a textured layer, and a cap layer are laminated in this order from the base material 11 side. However, the intermediate layer 15 may have a configuration in which one or both of the diffusion prevention layer and the bed layer are omitted.
The oxide superconducting layer 17 may be a material known as an oxide superconductor, and specifically, REBa2Cu3Oy (RE is a rare earth element) referred to as RE-123 system can be exemplified.
The protective layer 18 is a layer formed of Ag or an Ag alloy formed on the upper surface of the oxide superconducting layer 17. The protective layer 18 function as protecting the oxide superconducting layer 17 and function as bypassing an overcurrent generated during the accident.
The stabilizing layer 19 is formed at least on the upper surface of the protective layer 18. The stabilizing layer 19 according to the present embodiment is formed by covering a laminate configured of the base material 11, the intermediate layer 15, the oxide superconducting layer 17, and the protective layer 18 in a substantially C-shaped cross section with a metal tape. The stabilizing layer 19 is joined with a solder layer 13 interposed therebetween on the outer periphery (in four direction is a cross section) of the laminate configured of the base material 11, the intermediate layer 15, the oxide superconducting layer 17, and the protective layer 18. An embedded portion 13a in which the molten solder layer 13 is embedded is formed in a portion which is not covered with the stabilizing layer 19 (that is, a portion between the side end portions of the metal tape). The thickness of the metal tape configuring the stabilizing layer 19 is not particularly limited and can be appropriately adjusted, but the thickness of the metal tape may be 10 to 300 μm.
The stabilizing layer 19 is made of a material having good conductivity. For example, it is preferable to use a material configured of a relatively inexpensive material such as copper, brass, copper alloy such as Cu—Ni alloy, stainless steel or the like. The stabilizing layer 19 functions as a bypass in which the current of the oxide superconducting layer 17 is commutated, along with the protective layer 18.
Moreover, the stabilizing layer 19 may be formed by soldering a metal tape only to the upper surface of the protective layer 18. In addition, the stabilizing layer 19 may be formed by a known method such as a plating method or a sputtering method.
The superconducting wire 1 configured as described above is wound as the coils 6A and 6B in a state in which the coating layer 20 surrounding the entire periphery is formed. For example, the coating layer 20 can be formed by spirally winding an insulating tape such as a polyimide tape so as to surround the entire periphery of the superconducting wire 1.
As the method of winding the insulating tape, in addition to the method of winding the insulating tape in a spiral manner, there is a method of surrounding by a co-winding or the like.
The superconducting wire 1 according to the present embodiment is wound in a coil shape in a state where the base material 11 is positioned inward and the stabilizing layer 19 is positioned outward. Accordingly, the stabilizing layer 19 of the superconducting wire 1 is disposed outward on a winding terminal end portion of the superconducting wire 1. In addition, if the stabilizing layer 19 is positioned outward in the winding terminal end portion, the superconducting wire 1 in which the front surface and the rear surface are inversely disposed inside the coils 6A and 6B may be used so as to be connected. That is, the coils 6A and 6B may be manufactured by winding a wire which is connected to a superconducting wire which is wound in a coil shape in a state where the base material 11 is positioned outward in the winding start end portion and in which the base material 11 is positioned inward midway.
In the winding terminal end portion of the superconducting wire 1 configured as described above, the electrode member 2 is joined onto the stabilizing layer 19 of the superconducting wire 1 to form the electrode joint portion 7.
As shown in
The electrode member 2 is formed in an L shape, and the electrode member 2 includes a base portion 2a which is disposed along the winding terminal end portion of the superconducting wire 1 of the first coil 6A and an extension portion 2b which extends from one end of the base portion 2a to the outside of the coil body 6. Moreover, the electrode member 2 has a first surface 2c as a front surface, and a second surface 2d (a surface on the base portion 2a) and a third surface 2f (a surface on the extension portion 2b) as a rear surface, with respect to the entire length extending over the base portion 2a and the extension portion 2b. In addition, the electrode member 2 has a boundary portion 2e between the base portion 2a and the extension portion 2b. In the electrode member 2, the third surface 2f extends in a direction intersecting a direction in which the second surface 2d extends, and the boundary portion 2e (a surface on the inner angle side of the boundary portion, a curved portion) is positioned between the second surface 2d and the third surface 2f. A portion of the first surface 2c faces the outer peripheral surface of the coil body 6.
The base portion 2a of the electrode member 2 is solder-joined to the exposed stabilizing layer (first stabilizing layer) 19 of the superconducting wire 1, in which the impregnating resin 5 and the coating layer 20 are removed, on the first surface 2c. The electrode member 2 is joined to the superconducting wire 1 by the first solder member 21.
In addition, the electrode member 2 is solder-joined to the electrode superconducting wire 3 over the base portion 2a and the extension portion 2b so as to cover the second surface 2d, the third surface 2f, and the boundary portion 2e (the surface on the inner angle side of the boundary portion, the curved portion) by the electrode superconducting wire 3 on the second surface 2d and the third surface 2f. The electrode member 2 is joined to the electrode superconducting wire 3 by the second solder member 22.
As the electrode member 2, a material known in the conventional art may be used, a metal having high conductivity, for example, copper, silver, gold, platinum, or an alloy containing at least one of these metals may be used, and among these, copper which is inexpensive and has excellent conductivity is preferable. In addition, the electrode member 2 may be a member in which the surface is plated with any one of solder, Sn, Ag, and Au. Preferably, the electrode member 2 has a predetermined thickness in order to obtain sufficient rigidity that is not easily deformed by its own weight or a weak external force. For example, the thickness of the electrode member 2 is approximately 1 mm to 5 mm. In addition, as described in detail later, preferably, a width W2 of the base portion 2a of the electrode member 2 is narrower than a width W1 of the superconducting wire 1. That is, preferably, W1>W2 is satisfied (refer to
Since the electrode superconducting wire 3 is provided so as to be solder-joined to the base portion 2a and the extension portion 2b of the electrode member 2, the electrode superconducting wire 3 bypasses current which flows to the electrode member 2. Accordingly, the electrode superconducting wire 3 has a function which decreases the current flowing to the electrode member 2 and decreases heat generation of the electrode member 2.
The electrode superconducting wire 3 has a layer structure similar to that of the superconducting wire 1 of the coil 6A. That is, as shown in
Preferably, the stabilizing layer (second stabilizing layer) 19 of the electrode superconducting wire 3 is provided so as to cover the outer periphery of the laminate configured of the base material (second base material) 11, the intermediate layer (second intermediate layer) 15, the oxide superconducting layer (second oxide superconducting layer) 17, and the protective layer (second protective layer) 18 (refer to
In the electrode superconducting wire 3, the stabilizing layer (second stabilizing layer) 19 positioned on the oxide superconducting layer 17 side is joined to the second surface 2d in the base portion 2a of the electrode member 2 and the third surface 2f in the extension portion 2b of the electrode member 2, by the second solder member 22. As described in detail later, preferably, a width W3 of the electrode superconducting wire 3 is the same as or is narrower than the width W2 of the electrode member 2. That is, preferably, W2≧W3 is satisfied (refer to
Since the electrode superconducting wire 3 is solder-joined to the base portion 2a and the extension portion 2b of the electrode member 2, the electrode superconducting wire 3 is curved along the boundary portion 2e between the base portion 2a and the extension portion 2b. In a bending radius R of the electrode superconducting wire 3 in the curved portion, for example, preferably, the bending radius R is 5 mm or more, and more preferably, the bending radius R is within a range of 6 to 16 mm. It is possible to prevent decreases in superconducting characteristics by setting the bending radius R of the electrode member 2 to the range. In addition, it is possible to cause the electrode joint portion 7 to be compact without increasing the sizes of the electrode joint portion 7.
Since the bending radius R of the electrode superconducting wire 3 depends on the curvature radius on the inner angle side in the boundary portion 2e, preferably, the curvature radius on the inner angle side of the boundary portion 2e is determined such that the bending radius R of the electrode superconducting wire 3 is within the above-described range.
Preferably, a critical current density value Ic2 of the electrode superconducting wire 3 is the same as a critical current density value Ic1 of the coil body 6 or is higher than the critical current density value Ic1. That is, preferably, Ic2≧Ic1 is satisfied. In a case where the critical current density value Ic2 of the electrode superconducting wire 3 is lower than the critical current density value Ic1 of the coil body 6, if current which is equal or more than the critical current density value of the electrode superconducting wire 3 flows to the superconducting coil 10, the current flows to the electrode member 2, and there is a concern that heat generation may occur in the electrode member 2. Since the critical current density value Ic2 of the electrode superconducting wire 3 is higher than the critical current density value Ic1 of the coil body 6, current can flow to the superconducting coil 10 up to the critical current density value Ic1 of the coil body 6. Accordingly, it is possible to sufficiently exert the capability of the superconducting coil 10.
In addition, the critical current density value Ic1 of the coil body 6 does not necessarily coincide with the critical current density value of the wound superconducting wire 1. Since the coil body 6 is formed by winding the superconducting wire 1, if current flows to the coil body 6, a large magnetic field is added. Due to this magnetic field, the critical current density value Ic1 of the coil body 6 may be lower than the critical current density value of the superconducting wire 1.
In the superconducting coil 10, the width W3 of the electrode superconducting wire 3 is narrower than the width W1 of the superconducting wire 1 of the coil body 6. In general, if the thickness of each layer is constant, the critical current density value of the superconducting wire decrease as the width becomes narrow. Preferably, the width W3 of the electrode superconducting wire 3 is set such that a critical current density value Ic3 of the electrode superconducting wire 3 is equal to or more than the critical current density value Ic2 of the coil body 6. In addition, preferably, the width W2 of the electrode member 2 is set such that W2≧W3 is satisfied according to the width W3 of the electrode superconducting wire 3.
The superconducting wire 1 of the coil body 6 and the electrode member 2 are joined to the each other by the first solder member 21. In addition, the electrode member 2 and the electrode superconducting wire 3 are joined to each other by the second solder member 22. Preferably, the melting points of the first solder member 21 and the second solder member 22 are different from each other.
For example, in a case where the melting point of the first solder member 21 is higher than the melting point of the second solder member 22, first, the superconducting wire 1 of the coil body 6 and the electrode member 2 are joined to each other by the first solder member 21. Next, the second solder member 22 is melted at a temperature which is equal to or more than the melting point of the second solder member 22 and is equal to or less than the melting point of the first solder member 21, and the electrode member 2 and the electrode superconducting wire 3 are joined to each other by the second solder member 22. In this procedure, the superconducting wire 1 and the electrode superconducting wire 3 can be solder-joined to the first surface 2c, the second surface 2d, and the third surface 2f of the electrode member 2 without melting the first solder member 21 by joining the electrode superconducting wire 3.
In addition, the kind of solder of each of the first solder member 21 and the second solder member 22 is not particularly limited and, for example, may be Sn, Sn—Pb based alloy solder, lead-free solder such as Sn—Ag based alloy, Sn—Bi based alloy, Sn—Cu based alloy, and Sn—In based alloy, eutectic solder, low temperature solder, or the like. In addition, these solders may be used alone or combinations of two or more may be used.
Next, a relationship among the width W1 of the superconducting wire 1 of the coil body 6, the width W2 of the base portion 2a of the electrode member 2, and the width W3 of the electrode superconducting wire 3 will be described in detail with reference to the
As shown in
In addition, in the superconducting coil 10, the relationship between the width W2 of the base portion 2a of the electrode member and the width W3 of the electrode superconducting wire 3 satisfies W2≧W3. That is, the width size (W3) of the electrode superconducting wire 3 is equal to or less than the width size (W2) of the base portion 2a of the electrode member 2. By satisfying this relationship, the electrode superconducting wire 3 is settled in the width direction of the base portion of the electrode member 2.
According to the above-described configuration, even in a case where in the superconductive coil 10, the coil body is interposed between the conductive flanges 25 on the upper surface and the lower surface of the superconducting coil 10, it is possible to secure a distance between the flanges 25, and the electrode member 2 and the electrode superconducting wire 3. If the electrode member 2 and the electrode superconducting wire 3 approach the flanges 25, there is a concern that discharging from the electrode member 2 to the flanges 25 may be generated. Since the distance between the flanges 25, and the electrode member 2 and the electrode superconducting wire 3 is secured, it is possible to increase withstand voltage of the superconducting coil 10.
In addition, here, attention is paid to the width W2 of the base portion 2a of the electrode member 2. However, preferably, the electrode member 2 is constant over the entire area and the width W2 of the base portion 2a and the width of the extension portion 2b are the same as each other.
Accordingly, the extension portion 2b of the electrode member 2 does not approach the flanges 25, and it is possible to increase the withstand voltage.
In addition, each of the superconducting wire 1 and the electrode superconducting wire 3 according to the present embodiment includes the base material 11, the oxide superconducting layer 17 provided on the base material 11, and the stabilizing layer 19 provided on the oxide superconducting layer 17. In a case where the superconducting wire having the lamination structure is adopted, it is possible to easily narrow the superconducting wire by only cutting the superconducting wire in the width direction. Accordingly, it is possible to easily manufacture the narrow electrode superconducting wire 3 with respect to the superconducting wire 1 of the coil body 6.
The electrode member 102 has a structure which is substantially similar to that of the above-described electrode member 2, but is different from the electrode member 2 in that a groove 108 is provided.
The electrode member 102 is formed in an L shape including a base portion 102a which is disposed along the winding terminal end portion of the superconducting wire 1 of the coil body 6 and an extension portion 102b which extends from one end of the base portion 102a to the outside of the coil body 6. Moreover, the electrode member 102 has a first surface 102c as a front surface, and a second surface 102d (a surface on the base portion 102a) as a rear surface and a third surface 102f (a surface on the extension portion 102b) as a rear surface, with respect to the entire length extending over the base portion 102a and the extension portion 102b. A portion of the first surface 102c faces the outer peripheral surface of the coil body 6 and is solder-joined to the superconducting wire 1 exposed from the outer peripheral surface of the coil body 6.
In addition, the electrode member 102 has a boundary portion 102e between the base portion 102a and the extension portion 102b. In the electrode member 102, the third surface 102f extends in a direction intersecting a direction in which the second surface 102d extends, and the boundary portion 102e (a surface on the inner angle side of the boundary portion, a curved portion) is positioned between the second surface 102d and the third surface 102f.
The groove 108 having a larger width than the width of the electrode superconducting wire 3 is provided on the second surface 102d in the base portion 102a, the third surface 102f in the extension portion 102b, and the boundary portion 102e (the surface on the inner angle side of the boundary portion, the curved portion). In the groove 108, the electrode superconducting wire 3 is solder-joined to the base portion 102a and the extension portion 102b so as to cover the second surface 102d, the third surface 102f, and the boundary portion 102e (the surface on the inner angle side of the boundary portion, the curved portion). The depth of the groove 108 is not particularly limited.
By providing the groove 108, since a worker can perform the solder-joining in a state where the electrode superconducting wire 3 is disposed along the groove 108 of the electrode member 102, workability of the solder-joining increases. Moreover, since the electrode superconducting wire 3 is accommodated in the groove 108, the electrode superconducting wire 3 is not disposed to be inclined to the electrode member 102. Accordingly, it is possible to prevent the electrode superconducting wire 3 from protruding from the upper end and the lower end of the coil body 6, and even in a case where flanges are disposed on the upper surface and the lower surface of the coil body 6, it is possible to reliably secure the withstand voltage of the superconducting coil 10.
In the electrode member 102, the superconducting wire 1 of the coil body 6 is solder-joined to the first surface 102c, and the electrode superconducting wire 3 is solder-joined to the second surface 102d and the third surface 102f. Current flows between the superconducting wire 1 and the electrode superconducting wire 3 in the thickness direction of the electrode member 102 inside the electrode member 102. Accordingly, the distance between the superconducting wire 1 and the electrode superconducting wire 3 with respect to the thickness direction of the electrode member 102 becomes an electric resistance. As the electrode member 102 is thinned and the distance between the superconducting wire 1 and the electrode superconducting wire 3 decreases, the electric resistance of the electrode joint portion 7 can be decreased. On the other hand, the electrode member 102 needs to have a predetermined thickness in order to obtain sufficient rigidity which is not easily deformed by its own weight or a weak external force. Since the groove 108 is provided in the electrode member 102, it is possible to increase second moment of area with respect to an axis of the electrode member 102 in the thickness direction, and it is possible to increase rigidity of the electrode member 102. By providing the groove 108, in the electrode member 102, a distance between the superconducting wire 1 and the electrode superconducting wire 3 decreases while sufficient rigidity is provided, and it is possible to decrease a connection resistance.
Hereinbefore, the embodiment of the present invention is described, and the configurations in the embodiment and combination thereof are exemplified. Accordingly, addition, omission, replacement, and other modifications of the configurations can be applied within a scope which does not depart from the present invention. In addition, the present invention is not limited to the embodiment.
For example, in the embodiment, it is described that the superconducting wire has the configuration in which the oxide superconducting layer configured of a superconductor referred to as RE-123 base (or yttrium base) is laminated on the base material. The type of the superconducting wire is not limited to the configuration, and as shown in
Moreover, although the coil body according to the above-described embodiment has a structure in which two coils are laminated, the coil body may have a structure configured of only one coil or a structure in which three or more coils are laminated.
In the above-described embodiment, the electrode member has a structure in which the extension portion is disposed on the distal end side (the position close to the distal end) of the superconducting wire of the coil body. However, the extension portion may be configured to be disposed on the side opposite to the distal end of the superconducting wire. Moreover, the structure in which the electrode member is formed in an L shape by the base portion and the extension portion is exemplified. However, the electrode member may have a T-shaped structure in which the extension portion is disposed at the center in the longitudinal direction of the base portion.
Hereinafter, the present invention will be described in more detail with reference to Examples. However, the present invention is not limited to the Examples.
(Manufacturing of Sample)
First, a superconducting wire wound as a coil was manufactured.
An intermediate layer was formed on a base material made of a tape-shaped Hastelloy (trade name, manufactured by Haynes Corporation, USA) having a width of 5 mm and a thickness of 75 μm. For the intermediate layer, Al2O3 (diffusion prevention layer), Y2O3 (bed layer), MgO (textured layer (IBAD layer)) and CeO2 (cap layer) were formed in this order (in order). Next, GdBa2Cu3O7-δ (oxide superconducting layer) was formed on the intermediate layer.
Next, a protective layer configured of Ag was formed on the oxide superconducting layer. Next, a copper tape having a thickness of 75 μm and a width of 5 mm was joined to the upper surface of the protective layer with Sn solder to form a stabilizing layer. A superconducting wire having a width of 5 mm was manufactured by the above processes. The critical current density value of this superconducting wire was measured, and as a result, the critical current density value was 250 A.
Next, a polyimide tape was wound around the outer periphery of the superconducting wire to form a coating layer, and insulation processing was performed. Next, this superconducting wire was wound 100 turns around a winding frame having a diameter of 50 mm so that the stabilizing layer was positioned outward to manufacture a coil (pancake coil). Next, two coils manufactured by the process were laminated and impregnated with an epoxy resin (impregnating resin) to form a coil body.
Next, in the winding terminal end portion of the superconducting wire wound around each coil, the impregnating resin and the coating layer were removed to expose the stabilizing layer. A pair of electrode members for forming an electrode joint portion in each coil was prepared, and the base portions of the electrode members were joined to the exposed stabilizing layers by a first solder member. Solder having a melting point of 184° C. was used as the first solder member. Moreover, for the electrode member, each of the base portion and the extension portion used a member having a width of 4 mm and a thickness of 3 mm.
Next, the electrode superconducting wire was solder-joined to each electrode member by a second solder member. The electrode superconducting wire has a layer structure similar to that of the above-described superconducting wire. However, the stabilizing layer of the electrode superconducting wire was formed so as to cover not only the upper surface of the protective layer but also the entire outer periphery of the protective layer (refer to
The electrode superconducting wire was solder-joined so that the oxide superconducting layer side of the electrode superconducting wire faced the electrode member. The electrode superconducting wire was curved at the boundary between the base portion and the extension portion of the electrode member, and the bending radius of the electrode superconducting wire in the curved portion was 15 mm. Solder having a melting point of 130° C. was used as the second solder member.
The superconducting coil of the Example shown in
Next, a current lead was connected to each electrode member (the surface opposite to the third surface 2f which was the surface to which the electrode superconducting wire 3 was joined in the extension portion 2b of the electrode member 7) of the superconducting coil, and the critical current density value of the superconducting coil and the electric resistance of the electrode joint portion were measured in liquid nitrogen (liquid nitrogen temperature). As a result, the critical current density value of the superconducting coil was 89.0 A. In addition, the electrical resistance of the two electrode joint portions was 2.1 μΩ in total (the electrical resistance of each of the two electrode joint portions was measured, and the total of the electrical resistances of the two electrode joint portions was 2.1 μΩ). When the critical current density value (89.0 A) of the superconducting coil was reached, no nonlinear resistance component appeared in the electrode joint portion. Since the critical current density value of the superconducting coil is lower than the critical current density value (150 A) of the electrode superconducting wire, it is considered that the critical current density value of the coil body appeared as the critical current density value of the superconducting coil. That is, it is considered that the critical current density value of the coil body was 89.0 A.
In addition, for comparison with the superconducting coil of the Example, a superconducting coil of Comparative Example was produced.
A superconducting coil of Comparative Example which included the same configuration as that of the above-described superconducting coil and did not include an electrode superconducting wire was manufactured. A current lead was connected to the electrode member of the superconducting coil of the Comparative Example, and the critical current density value of the superconducting coil and the electric resistance of the electrode joint portion were measured in liquid nitrogen (liquid nitrogen temperature). As a result, the critical current density value of the superconducting coil was 88.7 A, and the electrical resistance of the two electrode joint portions was 12.5 μΩ in total (the electrical resistance of each of the two electrode joint portions was measured, and the total of the electric resistances of the two electrode joint portions was 12.5 μΩ). From the above results, it was confirmed that the electric resistance at the electrode joint portion could be decreased by using the superconducting coil of the Example.
| Number | Date | Country | Kind |
|---|---|---|---|
| 2014-236194 | Nov 2014 | JP | national |
| Filing Document | Filing Date | Country | Kind |
|---|---|---|---|
| PCT/JP2015/082710 | 11/20/2015 | WO | 00 |
