JPH04164865A - Method for manufacturing superconducting materials - Google Patents
Method for manufacturing superconducting materialsInfo
- Publication number
- JPH04164865A JPH04164865A JP2288013A JP28801390A JPH04164865A JP H04164865 A JPH04164865 A JP H04164865A JP 2288013 A JP2288013 A JP 2288013A JP 28801390 A JP28801390 A JP 28801390A JP H04164865 A JPH04164865 A JP H04164865A
- Authority
- JP
- Japan
- Prior art keywords
- cooling
- mold
- superconducting
- melt
- sheath
- 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.)
- Granted
Links
- 239000000463 material Substances 0.000 title claims abstract description 33
- 238000000034 method Methods 0.000 title claims abstract description 15
- 238000004519 manufacturing process Methods 0.000 title claims abstract description 11
- 239000012071 phase Substances 0.000 claims abstract description 13
- 238000001816 cooling Methods 0.000 claims abstract description 11
- 239000013078 crystal Substances 0.000 claims abstract description 11
- 238000002844 melting Methods 0.000 claims abstract description 7
- 230000008018 melting Effects 0.000 claims abstract description 7
- 239000000843 powder Substances 0.000 claims abstract description 7
- 238000005266 casting Methods 0.000 claims abstract description 5
- 239000007791 liquid phase Substances 0.000 claims abstract description 5
- 239000000155 melt Substances 0.000 claims abstract description 5
- 239000002994 raw material Substances 0.000 claims abstract description 5
- 238000010438 heat treatment Methods 0.000 claims abstract description 3
- 230000007613 environmental effect Effects 0.000 abstract description 4
- 239000004973 liquid crystal related substance Substances 0.000 abstract 1
- 230000000052 comparative effect Effects 0.000 description 6
- 239000011148 porous material Substances 0.000 description 4
- 238000005096 rolling process Methods 0.000 description 3
- 239000002887 superconductor Substances 0.000 description 3
- IJGRMHOSHXDMSA-UHFFFAOYSA-N Atomic nitrogen Chemical compound N#N IJGRMHOSHXDMSA-UHFFFAOYSA-N 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- BQCADISMDOOEFD-UHFFFAOYSA-N Silver Chemical compound [Ag] BQCADISMDOOEFD-UHFFFAOYSA-N 0.000 description 1
- 238000002441 X-ray diffraction Methods 0.000 description 1
- 229910003098 YBa2Cu3O7−x Inorganic materials 0.000 description 1
- QVGXLLKOCUKJST-UHFFFAOYSA-N atomic oxygen Chemical compound [O] QVGXLLKOCUKJST-UHFFFAOYSA-N 0.000 description 1
- 230000005540 biological transmission Effects 0.000 description 1
- 230000006866 deterioration Effects 0.000 description 1
- 238000004146 energy storage Methods 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 238000005242 forging Methods 0.000 description 1
- 239000007788 liquid Substances 0.000 description 1
- 229910052757 nitrogen Inorganic materials 0.000 description 1
- 238000000399 optical microscopy Methods 0.000 description 1
- 239000001301 oxygen Substances 0.000 description 1
- 229910052760 oxygen Inorganic materials 0.000 description 1
- 238000004663 powder metallurgy Methods 0.000 description 1
- 229910052709 silver Inorganic materials 0.000 description 1
- 239000004332 silver Substances 0.000 description 1
- 238000005245 sintering Methods 0.000 description 1
- 239000010409 thin film Substances 0.000 description 1
Landscapes
- Inorganic Compounds Of Heavy Metals (AREA)
- Superconductor Devices And Manufacturing Methods Thereof (AREA)
Abstract
Description
【発明の詳細な説明】
[産業上の利用分野]
本発明は送電線、アンテナ、超伝導マグネット、超伝導
軸受け、エネルギー貯蔵(ロードレベリング)等に用い
るバルク的な超伝導材料に関する。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to bulk superconducting materials used for power transmission lines, antennas, superconducting magnets, superconducting bearings, energy storage (load leveling), and the like.
[従来の技術]
臨界温度が液体窒素温度77Kを越え幅広い応用が期待
されるいわゆる高温超伝導体はHousuton大学の
C,W、Chuら゛が発見したLn−Ba−Cu−o系
(Lnは希土類元素を示す)、Arkansau大学の
A、M、Hermannらの発見したTl−Ba−Ca
−Cu−0系、金属材料技術研究所の前出の発見したB
1−8r−Ca−Cu−0系の3種類に大別できる。
(これらは安定性・再現性共に高い物質であるため公認
の高温超伝導体であるがこの他にもLa−3r−Nb−
0系、Tl−3r−V−0系等が鹿児島大学、日立等か
ら報告されている。)これらを用いた超伝導材料の従来
の製造方法をバルク(デバイスに用いられる薄膜に対向
した言葉)超伝導材料の代表例である線材で説明する。[Prior art] The so-called high-temperature superconductor, whose critical temperature exceeds the liquid nitrogen temperature of 77 K and is expected to find wide applications, is the Ln-Ba-Cu-o system (Ln is Tl-Ba-Ca discovered by A. M. Hermann et al. of the University of Arkansas
-Cu-0 series, B discovered by the Institute of Metal Materials Technology
It can be roughly divided into three types: 1-8r-Ca-Cu-0 system.
(These are materials with high stability and reproducibility, so they are officially recognized high-temperature superconductors, but there are also other materials such as La-3r-Nb-
0 series, Tl-3r-V-0 series, etc. have been reported by Kagoshima University, Hitachi, etc. ) The conventional manufacturing method of superconducting materials using these materials will be explained using wire rods, which are typical examples of bulk (a word opposed to thin films used in devices) superconducting materials.
その基本工程は粉末粉体冶金協会の昭和63年度春期大
会講演概要集p26〜27に述べられているように銀製
チューブ(シース)に予め作製した超伝導粉末を充填し
、線引き・ロール圧延等により成形加工した後鍋チュー
ブ内部の粉末を焼結する工程より成っていた。The basic process is as described in the Powder Metallurgy Association's 1986 Spring Conference Lecture Abstracts, pages 26-27, a silver tube (sheath) is filled with pre-prepared superconducting powder, and then wire-drawn, roll-rolled, etc. The process consisted of sintering the powder inside the ladle tube after forming.
[発明が解決しようとする課題]
しかしながら従来の製造方法では■高温超伝導体は結晶
構造に起因して異方性が強い物質であるにも関わらず結
晶方向の制御が成されていない、線引きや圧延を行なう
事により僅か配向するが粉体は互いに干渉して回転しず
らい状態にあるため配向度は低い、■粒界部等に非超伝
導体相を析出し易く超伝導体相が連続的に成長しない、
■粉体を成形した後の焼結であるため空孔が多く密度が
低い。[Problems to be solved by the invention] However, in conventional manufacturing methods, ■ Although high-temperature superconductors are materials with strong anisotropy due to their crystal structure, the crystal direction is not controlled; The degree of orientation is low because the powders interfere with each other and are difficult to rotate, although the degree of orientation is low due to rolling and rolling. does not grow continuously
■Since the powder is sintered after being molded, there are many pores and the density is low.
等の原因によりコンスタントに得られる臨界電流密度は
10’A/cm2(77K)台前半と低いものになって
いた。また空孔が多いと機械強度が弱くなるだけでなく
表面積が多くなるため劣化し易く耐久性(耐環境性)も
悪くしていた。Due to these reasons, the critical current density that can be constantly obtained is as low as 10'A/cm2 (77K). Furthermore, when there are many pores, not only does the mechanical strength become weak, but also the surface area becomes large, which makes it easy to deteriorate and deteriorates the durability (environmental resistance).
本発明はこの様な問題を解決するものであり、臨界電流
密度が高く、機械的強度、耐久性(耐環境性)に優れた
超伝導材料を容易に得んとするものである。The present invention is intended to solve these problems and to easily obtain a superconducting material having a high critical current density and excellent mechanical strength and durability (environmental resistance).
[課題を解決するための手段]
上記の問題を解決するため本発明の超伝導材料の製造方
法はバルク的な超伝導杯料の製造方法に於いて1)基本
工程が原料を溶融する工程、溶融物をシース材または型
に鋳込むと共に冷却し結晶化する工程、加熱後液相と結
晶相との混相状態で熱間加工する工程、結晶を成長させ
ると共に冷却する工程よりなること2)溶融物を訪込む
時シース材または型に一定方向の温度勾配を付け冷却す
ることを特徴とする。[Means for Solving the Problems] In order to solve the above problems, the method for producing a superconducting material of the present invention is a method for producing a bulk superconducting material, in which 1) the basic step is a step of melting raw materials; Consisting of a process of casting the melt into a sheath material or mold and cooling it to crystallize it, a process of hot working in a mixed phase state of liquid phase and crystalline phase after heating, and a process of growing crystals and cooling them 2) Melting It is characterized by cooling the sheath material or mold by applying a temperature gradient in a certain direction when visiting the object.
[実施例] 以下実施例に従い本発明の詳細な説明する。[Example] The present invention will be described in detail below with reference to Examples.
実施例−1
先ず原料Y2O3、B a C03、Cu○粉末を混合
分散した後900°C酸素雰囲気中で15時間仮焼する
0次に仮焼物を粉砕攪拌した後1350℃〜1450℃
に加熱し溶融する。溶融時間が長いとY2O3は凝集し
不均一な分散状態となるため溶融は3〜10分間と比較
的短い時間で行なう事が好ましい0次にこの溶融物を一
定方向に温度勾配を付けたシース内に鋳込み一部結晶方
向を揃え結晶化させる。結晶は大きく成長せず微細化し
た状態が好ましい0次にシースと共に1−000°C前
後即ち123相、211相、液相の混相状態に加熱した
後圧延を行なう0次に圧延をやめ一定時間ホールドした
後徐冷し超伝導材料を得る。Example-1 First, raw materials Y2O3, B a C03, and Cu○ powder are mixed and dispersed and then calcined at 900°C for 15 hours in an oxygen atmosphere.The calcined product is then crushed and stirred and then heated to 1350°C to 1450°C.
Heat to melt. If the melting time is too long, Y2O3 will aggregate and become non-uniformly dispersed, so it is preferable to melt it in a relatively short time of 3 to 10 minutes.Next, this melt is placed inside a sheath with a temperature gradient in a certain direction. It is then poured into a mold and partially aligned in the crystal direction to crystallize it. It is preferable that the crystals do not grow large and are in a fine state.The zero-th order is heated together with the sheath to around 1-000°C, that is, to a mixed phase state of 123 phase, 211 phase, and liquid phase, and then rolled.The zero-th stage rolling is stopped for a certain period of time. After being held, it is slowly cooled to obtain a superconducting material.
この様にして得られた超伝導材料の臨界電流密度をシー
ス剥離径測定した。測定温度は77にである。結果を第
1表の比較例と共に第2表に示す。The critical current density of the superconducting material thus obtained was measured by the sheath peeling diameter. The measured temperature is 77°C. The results are shown in Table 2 together with the comparative examples in Table 1.
第1表
第2表
表に示されているように本発明の製造方法より成る超伝
導材料は顕著に臨界電流密度が向上しているのが判る。As shown in Tables 1 and 2, it can be seen that the superconducting material produced by the manufacturing method of the present invention has a significantly improved critical current density.
尚実施例Aはシースの温度制御なし実施例Bはシースに
一定方向の温度勾配を付けたものである。シースに一定
方向の温度勾配を付け冷却し一部結晶方向を揃えること
によりさらに臨界電流密度は高くなりより好ましいこと
が判る。In Example A, the temperature of the sheath is not controlled, and in Example B, a temperature gradient is applied to the sheath in a fixed direction. It can be seen that by cooling the sheath with a temperature gradient in a certain direction and partially aligning the crystal directions, the critical current density becomes higher, which is more preferable.
これら実施例材料と比較例材料をX線回折・光学顕微鏡
・SEM観察等により比較したところ本発明よりなる超
伝導材料は比較例より結晶配向度が高く、123相が連
続的に成長し且つ空孔は少ないものであった。また溶融
を行なう比較例しは比較例aより空孔の数は顕著に少な
いが細長いn(ボイド)が見られた。この18の幅は比
較例aとほぼ同じであるが長さは数十倍〜数百倍長いた
め場合によっては致命的になる事が考えられる。熱間加
工は垢の発生を抑制する効果もあると言える。Comparison of these Example materials and Comparative Example materials by X-ray diffraction, optical microscopy, SEM observation, etc. showed that the superconducting material of the present invention had a higher degree of crystal orientation than the Comparative Example, with 123 phases growing continuously and voids. There were few holes. In addition, in the comparative example in which melting was performed, the number of pores was significantly smaller than in comparative example a, but elongated n (voids) were observed. The width of this 18 is almost the same as that of comparative example a, but the length is several tens to hundreds of times longer, which may be fatal in some cases. It can be said that hot processing also has the effect of suppressing the generation of scale.
尚本実施例ではYBa2Cu3O7−x材料で説明した
が結晶構造に起因した異方性を持つ材料で結晶相と液相
との混相状態を得られる材料で有れば良くまた熱間加工
も圧延の他に熱間鍛造(この場合シースではなく型に直
接鋳込んでも良い)等熱間に於ける塑性変形加工であれ
ば何等差し支えない。In this example, the YBa2Cu3O7-x material was explained, but any material that has anisotropy due to its crystal structure and that can obtain a mixed phase state of a crystalline phase and a liquid phase is sufficient. In addition, any other hot plastic deformation processing such as hot forging (in this case, casting may be performed directly into a mold instead of a sheath) may be used.
[発明の効果コ
以上述べたように本発明によれば異方性の強い物質であ
っても結晶方向を揃え且つ超伝導相を連続的に成長出来
、更に空孔の発生を抑制し高密度化を図れるため高い臨
界電流密度を持つ超伝導材料を得られる。また空孔発生
の抑制は機械的強度を高めるだけでなく表面積の減少に
つながるため劣化を少なくし耐久性(耐環境性)も向上
させることが出来る。[Effects of the Invention] As described above, according to the present invention, even in materials with strong anisotropy, the crystal orientation can be aligned and superconducting phases can be grown continuously, and the generation of vacancies can be suppressed to achieve high density. As a result, superconducting materials with high critical current densities can be obtained. In addition, suppressing the generation of pores not only increases mechanical strength but also leads to a decrease in surface area, which reduces deterioration and improves durability (environmental resistance).
以上 出願人 セイコーエプソン株式会社 代理人弁理士 鈴木喜三部 他1名that's all Applicant: Seiko Epson Corporation Representative Patent Attorney Kizobe Suzuki and 1 other person
Claims (1)
が原料(仮焼粉を含む)を溶融する工程、溶融物をシー
ス材または型に鋳込むと共に冷却し結晶化する工程、加
熱後液相と結晶相との混相状態で熱間加工する工程、結
晶成長させると共に冷却する工程よりなることを特徴と
する超伝導材料の製造方法。 2)溶融物を鋳込む時シース材または型に一定方向の温
度勾配を付け冷却することを特徴とする特許請求の範囲
第1項記載の超伝導材料の製造方法。[Claims] 1) In the method for manufacturing bulk superconducting materials, the basic process is the process of melting raw materials (including calcined powder), casting the melt into a sheath material or mold, and cooling and crystallizing. 1. A method for producing a superconducting material, comprising the following steps: a step of heating and then hot working in a mixed phase state of a liquid phase and a crystalline phase, and a step of growing crystals and cooling. 2) A method for producing a superconducting material according to claim 1, characterized in that when the melt is cast, a temperature gradient is applied to the sheath material or the mold in a certain direction for cooling.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP28801390A JP3160901B2 (en) | 1990-10-25 | 1990-10-25 | Manufacturing method of superconducting material |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP28801390A JP3160901B2 (en) | 1990-10-25 | 1990-10-25 | Manufacturing method of superconducting material |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH04164865A true JPH04164865A (en) | 1992-06-10 |
| JP3160901B2 JP3160901B2 (en) | 2001-04-25 |
Family
ID=17724682
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP28801390A Expired - Fee Related JP3160901B2 (en) | 1990-10-25 | 1990-10-25 | Manufacturing method of superconducting material |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP3160901B2 (en) |
-
1990
- 1990-10-25 JP JP28801390A patent/JP3160901B2/en not_active Expired - Fee Related
Also Published As
| Publication number | Publication date |
|---|---|
| JP3160901B2 (en) | 2001-04-25 |
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