JPH02257528A - Manufacture of oxide superconductor - Google Patents
Manufacture of oxide superconductorInfo
- Publication number
- JPH02257528A JPH02257528A JP1080051A JP8005189A JPH02257528A JP H02257528 A JPH02257528 A JP H02257528A JP 1080051 A JP1080051 A JP 1080051A JP 8005189 A JP8005189 A JP 8005189A JP H02257528 A JPH02257528 A JP H02257528A
- Authority
- JP
- Japan
- Prior art keywords
- oxide
- wire
- laser beam
- silver
- metal core
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Pending
Links
- 239000002887 superconductor Substances 0.000 title claims abstract description 19
- 238000004519 manufacturing process Methods 0.000 title claims description 11
- 239000000463 material Substances 0.000 claims abstract description 19
- 229910052751 metal Inorganic materials 0.000 claims abstract description 11
- 239000002184 metal Substances 0.000 claims abstract description 11
- 229910052709 silver Inorganic materials 0.000 claims abstract description 9
- 239000004332 silver Substances 0.000 claims abstract description 9
- 230000001678 irradiating effect Effects 0.000 claims abstract 2
- 238000000034 method Methods 0.000 claims description 8
- 239000002994 raw material Substances 0.000 claims description 4
- 239000013078 crystal Substances 0.000 abstract description 13
- RYGMFSIKBFXOCR-UHFFFAOYSA-N Copper Chemical compound [Cu] RYGMFSIKBFXOCR-UHFFFAOYSA-N 0.000 abstract description 9
- BQCADISMDOOEFD-UHFFFAOYSA-N Silver Chemical compound [Ag] BQCADISMDOOEFD-UHFFFAOYSA-N 0.000 abstract description 8
- 238000002844 melting Methods 0.000 abstract description 8
- 230000008018 melting Effects 0.000 abstract description 8
- 238000006243 chemical reaction Methods 0.000 abstract description 3
- 238000007747 plating Methods 0.000 abstract description 3
- 101100298225 Caenorhabditis elegans pot-2 gene Proteins 0.000 abstract 1
- 229910009203 Y-Ba-Cu-O Inorganic materials 0.000 abstract 1
- 230000002542 deteriorative effect Effects 0.000 abstract 1
- 239000010410 layer Substances 0.000 description 10
- 239000010949 copper Substances 0.000 description 3
- 239000000155 melt Substances 0.000 description 3
- 239000012071 phase Substances 0.000 description 3
- 230000000087 stabilizing effect Effects 0.000 description 3
- 239000011247 coating layer Substances 0.000 description 2
- 238000002425 crystallisation Methods 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- 239000012779 reinforcing material Substances 0.000 description 2
- RTAQQCXQSZGOHL-UHFFFAOYSA-N Titanium Chemical compound [Ti] RTAQQCXQSZGOHL-UHFFFAOYSA-N 0.000 description 1
- AYJRCSIUFZENHW-UHFFFAOYSA-L barium carbonate Inorganic materials [Ba+2].[O-]C([O-])=O AYJRCSIUFZENHW-UHFFFAOYSA-L 0.000 description 1
- 230000015572 biosynthetic process Effects 0.000 description 1
- 150000004649 carbonic acid derivatives Chemical class 0.000 description 1
- 239000011248 coating agent Substances 0.000 description 1
- 238000000576 coating method Methods 0.000 description 1
- 230000000052 comparative effect Effects 0.000 description 1
- 238000001816 cooling Methods 0.000 description 1
- 229910052802 copper Inorganic materials 0.000 description 1
- 230000008025 crystallization Effects 0.000 description 1
- 230000006866 deterioration Effects 0.000 description 1
- 238000009792 diffusion process Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000010438 heat treatment Methods 0.000 description 1
- 239000011810 insulating material Substances 0.000 description 1
- 239000007788 liquid Substances 0.000 description 1
- 239000007791 liquid phase Substances 0.000 description 1
- 238000000465 moulding Methods 0.000 description 1
- 150000002823 nitrates Chemical class 0.000 description 1
- 231100000989 no adverse effect Toxicity 0.000 description 1
- 239000000843 powder Substances 0.000 description 1
- 238000001953 recrystallisation Methods 0.000 description 1
- 230000003014 reinforcing effect Effects 0.000 description 1
- 238000005245 sintering Methods 0.000 description 1
- 239000000344 soap Substances 0.000 description 1
- 239000007787 solid Substances 0.000 description 1
- 229910001220 stainless steel Inorganic materials 0.000 description 1
- 239000010935 stainless steel Substances 0.000 description 1
- 238000010025 steaming Methods 0.000 description 1
- 238000001308 synthesis method Methods 0.000 description 1
- 239000010936 titanium Substances 0.000 description 1
- 229910052719 titanium Inorganic materials 0.000 description 1
Classifications
-
- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
- Y02E—REDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
- Y02E40/00—Technologies for an efficient electrical power generation, transmission or distribution
- Y02E40/60—Superconducting electric elements or equipment; Power systems integrating superconducting elements or equipment
Landscapes
- Crystals, And After-Treatments Of Crystals (AREA)
- Superconductors And Manufacturing Methods Therefor (AREA)
- Laser Beam Processing (AREA)
Abstract
Description
【発明の詳細な説明】
[産業上の利用分野]
本発明は、酸化物超電導体の製造方法に係り、特に結晶
の配向性、すなわち超電導特性および電気的、機械的安
定性に優れた線状の酸化物超電導体の製造方法に関する
。Detailed Description of the Invention [Industrial Application Field] The present invention relates to a method for producing an oxide superconductor, and in particular to a method for producing an oxide superconductor, in particular a linear oxide superconductor that has excellent crystal orientation, that is, superconducting properties, and electrical and mechanical stability. The present invention relates to a method for producing an oxide superconductor.
[従来の技術]
近年、酸化物超電導物質の開発が著しい速度で進められ
ており、La系、Y系、旧糸、TI系等の超電導物質の
利用が有力視されている。[Prior Art] In recent years, the development of oxide superconducting materials has progressed at a remarkable speed, and the use of superconducting materials such as La-based, Y-based, old yarn, and TI-based materials is considered to be promising.
しかしながら、これらの物質はその超電導特性に異方性
、すなわち結晶方位による特性の差が著しく、通常の合
成法によって得られた原料粉末を成型後焼結しただけで
はランダムな結晶方位のものしか得られないため、実用
的レベルに達する電気的、磁気的特性が得られないとい
う問題がある。However, these materials have anisotropy in their superconducting properties, that is, there are significant differences in properties depending on the crystal orientation, and simply molding and sintering the raw material powder obtained by normal synthesis methods only yields materials with random crystal orientation. Therefore, there is a problem in that electrical and magnetic properties that reach a practical level cannot be obtained.
上記の問題を解決する方法として、酸化物超電導物質を
溶融し、この融体を温度勾配を有する電気炉内で相対的
に移動させて結晶成長させることにより結晶の配向性を
高めることが試みられている。As a method to solve the above problem, an attempt has been made to increase crystal orientation by melting an oxide superconducting material and moving this melt relatively in an electric furnace with a temperature gradient to grow crystals. ing.
また、超電導体、たとえば線状の超電導体中にフローテ
ィングゾーンを形成して溶融、凝固させることにより結
晶の配向性を高めることも試みられている。Furthermore, attempts have been made to improve crystal orientation by forming a floating zone in a superconductor, such as a linear superconductor, and melting and solidifying the superconductor.
[発明が解決しようとする課題]
しかしながら、前者の溶融温度勾配結晶化法では温度勾
配の設定に限界があり、熱伝導により大きな勾配を炉内
に形成することが不可能なため、結晶配向の制御が困難
であるという難点をaする。[Problem to be solved by the invention] However, in the former melting temperature gradient crystallization method, there is a limit to the setting of the temperature gradient, and it is impossible to form a large gradient in the furnace by heat conduction, so it is difficult to change the crystal orientation. A disadvantage is that it is difficult to control.
一方、後者のフローティングゾーンによる方法において
は、液相から安定に結晶化する相しか得られない上、そ
の成長速度は数印〜数mm/hrと極めて遅いという難
点を有する。特にこの方法においては、Y−Da−Cu
−0系酸化物の場合、溶融→再結晶によって絶縁物質で
あるY 2 BaCu0x相が生成され、超電導物質で
あるYBa2 Cu30X相が生成されないという致命
的な欠点を有する。On the other hand, the latter method using a floating zone has the disadvantage that only a phase that stably crystallizes from the liquid phase can be obtained, and that the growth rate thereof is extremely slow, ranging from several marks to several mm/hr. In particular, in this method, Y-Da-Cu
In the case of -0-based oxide, a fatal drawback is that the insulating material Y2BaCu0x phase is produced by melting and recrystallization, but the superconducting material YBa2 Cu30X phase is not produced.
また上記いずれの方法においても、線材化する場合に安
定化材や機械的な補強部材との11i合化を図る必要が
あるという問題もある。この場合、金属線を補強材およ
び安定化材として使用することも考えられるが、酸化物
の結晶化の際の熱処理時に金属線との拡散反応を生じ、
超電導特性が低下するという難点を有する。Further, in any of the above methods, there is also a problem that it is necessary to integrate 11i with a stabilizing material or a mechanical reinforcing member when forming the wire into a wire. In this case, it is possible to use metal wire as a reinforcing material and a stabilizing material, but a diffusion reaction with the metal wire occurs during heat treatment during crystallization of the oxide.
It has the disadvantage that superconducting properties deteriorate.
本発明は上記の難点を解決するためになされたもので、
レーザビ・−ムを用いて結晶の配向性、すなわち超電導
特性および電気的安定性や機械的強度に優れた線状の酸
化物超電導体を製造する方法を提供することをその目的
とする。The present invention has been made to solve the above-mentioned difficulties.
The object of the present invention is to provide a method for producing a linear oxide superconductor having excellent crystal orientation, that is, superconducting properties, electrical stability, and mechanical strength using a laser beam.
[課題を解決するための手段]
上記目的を達成するために、本発明の酸化物超電導体の
製造方法は、外周に銀を被覆した金属心線の外側に、溶
融した酸化物超電導物質あるいは酸化物超電導物質を構
成する元素を含む原料物質を付着凝固させて凝固層を形
成した後、前記凝固層にレーザビームを照射し、この照
射により形成される溶融帯域を急速に移動させるように
したものである。[Means for Solving the Problems] In order to achieve the above object, the method for producing an oxide superconductor of the present invention provides a method for producing an oxide superconductor in which a molten oxide superconducting material or an oxide After a raw material containing elements constituting a superconducting material is adhered and solidified to form a solidified layer, the solidified layer is irradiated with a laser beam, and the molten zone formed by this irradiation is rapidly moved. It is.
本発明における酸化物超電導物質としては特に限定され
ず、たとえばLa−Ba−Cu−0系、La−8r−C
a−Cu−0系、Y−Ba−Cu−0系、旧−3r−C
a−Cu−0系、Tl−Ba−Ca−Cu−0系等の酸
化物を挙げることができる。The oxide superconducting material in the present invention is not particularly limited, and includes, for example, La-Ba-Cu-0, La-8r-C
a-Cu-0 series, Y-Ba-Cu-0 series, old-3r-C
Examples include a-Cu-0 type oxides, Tl-Ba-Ca-Cu-0 type oxides, and the like.
また、酸化物超電導物質を構成する元素を含む原料物質
としては、これ等の元素を含む酸化物、炭酸塩、硝酸塩
、金属石けん等が用いられ、−例を挙げればY−Ba−
Cu−0系の場合、Y2O6、BaC03、CuOが使
用される。In addition, as the raw material containing the elements constituting the oxide superconducting material, oxides, carbonates, nitrates, metal soaps, etc. containing these elements are used; for example, Y-Ba-
In the case of Cu-0, Y2O6, BaC03, and CuO are used.
本発明における金属心線としては、銅、ステンレス、チ
タン等凝固層形成時に溶解しないものであればよく、銀
被覆はメツキや蒸青等により施される。The metal core wire in the present invention may be made of copper, stainless steel, titanium, etc., as long as it does not dissolve during the formation of the solidified layer, and the silver coating may be applied by plating, steaming blue, or the like.
また本発明におけるレーザビームは、Ar1YAG 5
CO2等のCW(連続)レーザによって形成され、特に
銀被覆層の外側に凝固層が形成された線材の軸方向に垂
直な断面において対称的な温度分布が形成されるように
複数本照射し、かつビーム径が相互に重なり合うように
照射することが好ましい。Further, the laser beam in the present invention is Ar1YAG5
A CW (continuous) laser such as CO2 is used to irradiate multiple lasers so that a symmetrical temperature distribution is formed in a cross section perpendicular to the axial direction of the wire, especially in which a solidified layer is formed on the outside of the silver coating layer. It is also preferable to irradiate the beams so that the beam diameters overlap each other.
このため断面円形の線材に対しては同心固状の温度分布
を形成するように、等角度で多数本のレーザビームを線
材中心へ向かって照射することが行われる。レーザビー
ムとしては、たとえばビーム径20μmφ程度のものを
使用して、50μ−程度の長さの溶融帯域を形成し、線
材(あるいはビーム)をl= l0cIII / se
e程度の速度で移動させる。For this reason, a wire having a circular cross section is irradiated with multiple laser beams at equal angles toward the center of the wire so as to form a concentric solid temperature distribution. For example, a laser beam with a beam diameter of about 20 μmφ is used to form a melting zone with a length of about 50 μm, and the wire (or beam) is
Move at a speed of about e.
レーザビームの出力は、凝固層が完全に溶融する大きさ
に調整される。The power of the laser beam is adjusted to a level that completely melts the solidified layer.
[作用]
本発明においては、凝固層がレーザビームにより非常に
狭い帯域で急速に溶融、凝固せしめられるため、非常に
大きな温度勾配を達成することができ、これにより非常
に高い配向性を有する結晶が得られ、超電導特性に優れ
た線材を得ることができる。さらに銀被覆層がレーザビ
ームを反射するため、金属心線と酸化物との反応を防ぐ
バッファ層の役目を果すとともに、レーザビームのエネ
ルギーを金属心線が吸収し断面方向に結晶が成長して軸
方向の配向性を低下させることが防止される。さらに金
属心線が安定化材および補強材の役目を果すため、電気
的、機械的安定性に優れた長尺線材の製造が可能になる
。[Operation] In the present invention, since the solidified layer is rapidly melted and solidified in a very narrow band by a laser beam, it is possible to achieve a very large temperature gradient, which allows crystals with very high orientation to be formed. can be obtained, and a wire with excellent superconducting properties can be obtained. Furthermore, since the silver coating layer reflects the laser beam, it acts as a buffer layer to prevent the reaction between the metal core wire and the oxide, and the metal core wire absorbs the energy of the laser beam, causing crystals to grow in the cross-sectional direction. This prevents deterioration of axial orientation. Furthermore, since the metal core wire serves as a stabilizing material and a reinforcing material, it is possible to manufacture a long wire material with excellent electrical and mechanical stability.
なお、銀は酸化物超電導物質の超電導特性に対して悪影
響を及ぼさないことが知られている。Note that silver is known to have no adverse effect on the superconducting properties of oxide superconducting materials.
[実施例]
第1図は本発明の方法に用いられる装置の一実施例を示
す概略図である。同図において1は外径20μmφの銀
メツキ銅線、2は溶融ルツボ、3は溶融酸化物、4は上
部冷却器、5は下部冷却器、6はレーザビームを示す。[Example] FIG. 1 is a schematic diagram showing an example of an apparatus used in the method of the present invention. In the figure, 1 is a silver-plated copper wire with an outer diameter of 20 μmφ, 2 is a melting crucible, 3 is a molten oxide, 4 is an upper cooler, 5 is a lower cooler, and 6 is a laser beam.
上記の溶融ルツボ2内にY−Ba−Cu−0系酸化物(
Y:Ba:Cu −1:2:3 )を収容し、ヒータ7
によりルツボ内を1200℃以上に加熱して酸化物3を
溶融させた。この融体の液面3′をガス8により加圧し
、ルツボ下部のダイス9より上部冷却器4で冷却された
銀メ・ツキ銅線1を通過させ、その外周に融体を約10
cfll/seeで噴出させ、直ちに下部冷却器5内で
ガス冷却を施した後、レーザビーム6を外周より照射し
た。レーザビームは出力50hW 、ビーム径20μl
φの30本を用い、外径100μ■φの線材10の外周
より等角度で照射した。Y-Ba-Cu-0 based oxide (
Y:Ba:Cu -1:2:3), and the heater 7
The inside of the crucible was heated to 1200° C. or higher to melt the oxide 3. The liquid surface 3' of this melt is pressurized by gas 8, and a silver-plated copper wire 1 cooled by an upper cooler 4 is passed through a die 9 at the bottom of the crucible, and about 10
After ejecting at a rate of cfll/see and immediately cooling with gas in the lower cooler 5, a laser beam 6 was irradiated from the outer periphery. The laser beam has an output of 50 hW and a beam diameter of 20 μl.
Using 30 wires with diameters of φ, irradiation was performed at equal angles from the outer periphery of a wire 10 with an outer diameter of 100 μιφ.
第2図は、このようにして得られた超電導線11を示し
たもので、銅線12の外周に銀メツキ層13が施された
銀メツキ銅線1の外側に結晶化した酸化物層14が形成
された構造を有する。FIG. 2 shows the superconducting wire 11 obtained in this way, in which a silver plating layer 13 is applied to the outer periphery of the copper wire 12. An oxide layer 14 crystallized on the outside of the silver-plated copper wire 1 It has a structure in which
このようにして得られた超電導線の軸方向の結晶の配向
性および臨界電流密度(外部磁界OT、 77K)等を
下表に示した。The axial crystal orientation, critical current density (external magnetic field OT, 77K), etc. of the superconducting wire thus obtained are shown in the table below.
なお比較例として実施例と同径の銅線を使用し、他は実
施例と同様の方法により製造した超電導線*:銅線表面
の隣接層に配向性なし
[発明の効果]
以上述べたように、本発明の酸化物超電導体の製造方法
によれば、高い結晶の配向性を有し、これにより臨界電
流密度の高い超電導体が容易に得られる上、その制御も
容易であり、かつ電気的、機械的安定性に優れた超電導
体を高速で製造することができ、実用的な方法としてそ
の価値は極めて大である。As a comparative example, a copper wire with the same diameter as in the example was used, and the other parts were manufactured in the same manner as in the example.Superconducting wire*: No orientation in the layer adjacent to the surface of the copper wire [Effects of the invention] As stated above. In addition, according to the method for producing an oxide superconductor of the present invention, a superconductor having a high crystal orientation and a high critical current density can be easily obtained, and it is also easy to control the superconductor. It is possible to produce superconductors with excellent physical and mechanical stability at high speed, and its value as a practical method is extremely high.
第1図は本発明の方法に用いられる装置の一実施例を示
す概略図、第2図は第1図の装置により製造された超電
導線の断面図である。
1・・・・・・・・・・・・銀メツキ銅線2・・・・・
・・・・溶融ルツボ
3・・・・・・・・・溶融酸化物
4.5・・・冷却器
6・・・・・・・・・レーザビームFIG. 1 is a schematic diagram showing an embodiment of the apparatus used in the method of the present invention, and FIG. 2 is a sectional view of a superconducting wire manufactured by the apparatus of FIG. 1. 1・・・・・・・・・Silver plated copper wire 2・・・・・・
...Melting crucible 3...Melted oxide 4.5...Cooler 6...Laser beam
Claims (2)
酸化物超電導物質あるいは酸化物超電導物質を構成する
元素を含む原料物質を付着凝固させて凝固層を形成した
後、前記凝固層にレーザビームを照射し、この照射によ
り形成される溶融帯域を急速に移動させることを特徴と
する酸化物超電導体の製造方法。(1) After forming a solidified layer by adhering and solidifying a melted oxide superconducting material or a raw material containing an element constituting the oxide superconducting material on the outside of a metal core wire whose outer periphery is coated with silver, the solidified layer is A method for producing an oxide superconductor, which comprises irradiating a laser beam onto the oxide superconductor and rapidly moving a molten zone formed by the irradiation.
の酸化物超電導体の製造方法。(2) The method for manufacturing an oxide superconductor according to claim 1, wherein a plurality of laser beams are irradiated.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1080051A JPH02257528A (en) | 1989-03-30 | 1989-03-30 | Manufacture of oxide superconductor |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1080051A JPH02257528A (en) | 1989-03-30 | 1989-03-30 | Manufacture of oxide superconductor |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH02257528A true JPH02257528A (en) | 1990-10-18 |
Family
ID=13707443
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP1080051A Pending JPH02257528A (en) | 1989-03-30 | 1989-03-30 | Manufacture of oxide superconductor |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH02257528A (en) |
-
1989
- 1989-03-30 JP JP1080051A patent/JPH02257528A/en active Pending
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| US5149681A (en) | Melt texturing of long superconductor fibers | |
| JP2866265B2 (en) | Method for producing high critical temperature superconducting flexible conductor | |
| EP0498306B1 (en) | Method of preparing oxide superconducting material | |
| US5047386A (en) | Apparatus for continuous manufacture of high temperature superconducting wires from molten superconducting oxides | |
| JPH02257528A (en) | Manufacture of oxide superconductor | |
| JPH02257527A (en) | Manufacture of oxide superconductor | |
| US5270296A (en) | High critical temperature superconducting wire with radially grown crystallites | |
| JPH02257526A (en) | Manufacture of oxide superconductor | |
| JPH02257529A (en) | Manufacture of oxide superconductor | |
| CH682358A5 (en) | Ceramic high temp. superconductor prodn. - by pouring starting material into mould, heating, cooling, thermally treating in oxygen@ and cooling, for shield magnetic fields in switching elements | |
| JPH02239102A (en) | Production of oxide superconductor | |
| JPH02257525A (en) | Manufacture of oxide superconductor | |
| JPH027309A (en) | Manufacture of oxide type superconductive wire | |
| JPH0316726B2 (en) | ||
| JPH02258692A (en) | Production of oxide superconductor | |
| JP3181642B2 (en) | Manufacturing method of oxide superconducting wire | |
| JPH02258699A (en) | Production of oxide superconductor | |
| JPH0362978A (en) | Method of producing oxide superconductor circuit | |
| JPH06234509A (en) | Method for producing oxide superconductor and device therefor | |
| US5346883A (en) | Method of manufacturing superconductive products | |
| JPH02258693A (en) | Production of oxide superconductor | |
| JPH02258669A (en) | Production of oxide superconductor | |
| JP3121864B2 (en) | Method for producing Bi-based oxide superconducting conductor by melting method | |
| JPH02258697A (en) | Production of oxide superconductor | |
| JPH03150208A (en) | Preparation of oxide superconductive fiber |