JPH02221149A - Production of oxide superconductor - Google Patents

Production of oxide superconductor

Info

Publication number
JPH02221149A
JPH02221149A JP1042310A JP4231089A JPH02221149A JP H02221149 A JPH02221149 A JP H02221149A JP 1042310 A JP1042310 A JP 1042310A JP 4231089 A JP4231089 A JP 4231089A JP H02221149 A JPH02221149 A JP H02221149A
Authority
JP
Japan
Prior art keywords
superconductor
type oxide
oxide superconductor
temperature
oxide
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
Application number
JP1042310A
Other languages
Japanese (ja)
Inventor
Akira Otomo
明 大友
Akira Fukizawa
蕗澤 朗
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Resonac Holdings Corp
Original Assignee
Showa Denko KK
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Showa Denko KK filed Critical Showa Denko KK
Priority to JP1042310A priority Critical patent/JPH02221149A/en
Publication of JPH02221149A publication Critical patent/JPH02221149A/en
Pending legal-status Critical Current

Links

Classifications

    • YGENERAL 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
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02EREDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
    • Y02E40/00Technologies for an efficient electrical power generation, transmission or distribution
    • Y02E40/60Superconducting electric elements or equipment; Power systems integrating superconducting elements or equipment

Landscapes

  • Inorganic Compounds Of Heavy Metals (AREA)
  • Superconductors And Manufacturing Methods Therefor (AREA)
  • Compositions Of Oxide Ceramics (AREA)

Abstract

PURPOSE:To obtain an oxide superconductor having a high critical temp. and a high critical current density by melting oxides as starting materials for an Sr-Ca-Cu-O type oxide superconductor by heating, solidifying the molten oxides by cooling, bringing a Bi-Pb-O type oxide into contact with the resulting solid body and carrying out heat treatment. CONSTITUTION:Starting materials such as SrCO3, CaCO3 and CuO are mixed in such a ratio as to give an Sr-Ca-Cu-O type oxide superconductor. They are melted by heating in the air and solidified by cooling. Bi2O3 and PbO are brought into contact with the resulting solid body in such a ratio as to give a Bi-Pb-Sr-Ca-Cu-O type oxide superconductor and they are held at a temp. at which a superconducting phase is formed for a certain time to diffuse a Bi-Pb-O type oxide in the Sr-Ca-Cu-O type oxide. A Bi-Pb-Sr-Ca-Cu-O type oxide superconductor having a high critical temp. and a high critical current density is obtd.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明はBl −Pb −3r −Ca −Cu −0
系酸化物超伝導体の製造方法に関し、特に臨界電流密度
(J c)を高くした超伝導体の製造方法に関する。
[Detailed Description of the Invention] [Industrial Field of Application] The present invention relates to Bl-Pb-3r-Ca-Cu-0
The present invention relates to a method for manufacturing a superconductor based on oxides, and particularly to a method for manufacturing a superconductor with a high critical current density (Jc).

〔従来の技術〕[Conventional technology]

Bi−Pb −5r −Ca −Cu −0からなる酸
化物超伝導体の製造方法はB 1203.PbO。
A method for producing an oxide superconductor consisting of Bi-Pb-5r-Ca-Cu-0 is described in B 1203. PbO.

S rcOCaCO3,CuO等の化合物粉末3 ′ を混合し、まず700〜800℃で予備焼成し反応させ
る。これを粉砕後、成形し酸素濃度4〜8%の雰囲気で
830〜840℃で焼成し焼結体とする。又、焼結によ
る方法ではJcが低いので予備焼成後、溶融点以上、約
1100℃で溶融した後750〜850℃で熱処理する
方法もとられている。
Compound powder 3' such as SrcOCaCO3 and CuO is mixed and first pre-calcined at 700 to 800°C to react. This is pulverized, molded, and fired at 830 to 840°C in an atmosphere with an oxygen concentration of 4 to 8% to form a sintered body. Furthermore, since Jc is low in the sintering method, a method is also used in which after preliminary firing, the material is melted at a temperature above the melting point, approximately 1100°C, and then heat treated at 750 to 850°C.

〔発明が解決しようとする課題〕[Problem to be solved by the invention]

実用上、超伝導体の臨界温度(Tc)及びJcが共に高
いことが望ましい。高いJcを持つ超伝導体を得るため
には気孔率が小さく、かさ密度が高いことが好ましい。
In practical terms, it is desirable that the critical temperature (Tc) and Jc of the superconductor are both high. In order to obtain a superconductor with a high Jc, it is preferable that the porosity is small and the bulk density is high.

さらには、粒子がある結晶軸方向に配向していることが
好ましい。このため−般にがさ密度を高くする方法とし
て、−度溶融する方法が試みられてきた。
Furthermore, it is preferable that the particles are oriented in a certain crystal axis direction. For this reason, a method of melting has generally been attempted as a method of increasing the density of the gas.

しかしながらBl  −Pb −8r −Ca −Cu
 −0からなる酸化物超伝導体では当該超伝導体の融点
が約860℃付近であるのに対してBi2O3の融点は
820℃と低くまた860℃での蒸気圧も高い。このた
め当該超伝導体を溶融状態で保持するとBlが泡状とな
って蒸発して組成がずれると共に液相内に気孔が発生す
る。この気孔は凝固させる時に固体の中に残るため、か
ぎ密度は上がらなくなる。従ってJcは高くならない。
However, Bl -Pb -8r -Ca -Cu
-0 has a melting point of around 860°C, whereas Bi2O3 has a low melting point of 820°C and a high vapor pressure at 860°C. Therefore, when the superconductor is held in a molten state, Bl becomes bubbles and evaporates, causing a composition shift and generation of pores in the liquid phase. Since these pores remain in the solid during solidification, the key density does not increase. Therefore, Jc does not become high.

本発明はBi −Pb −8r −Ca −Cu −0
系酸化物超伝導体の製造方法において、溶融法の欠点で
ある組成ずれと気孔の発生を防ぎ高密度の超伝導体、ひ
いてはJcの高い超伝導体の製造方法を提供することを
目的とする。
The present invention provides Bi-Pb-8r-Ca-Cu-0
The purpose of this invention is to provide a method for producing a high-density superconductor, and furthermore, a high Jc superconductor, by preventing compositional deviation and porosity, which are disadvantages of the melting method, in a method for producing a oxide superconductor. .

〔課題を解決するための手段〕[Means to solve the problem]

本発明者は上記の目的を達成するために鋭意研究した結
果、比較的融点の低いBi  −Pb −0系酸化物を
除いたSr −Ca −Cu −0系酸化物のみを融解
温度以上に加熱して融解せしめた後、固化し、その後B
i−Pb−0系酸化物をこれに接触し、拡散によって超
伝導性を改善せしめることを発見し、本件発明を完成す
るに至った。
As a result of intensive research to achieve the above object, the present inventors found that only Sr-Ca-Cu-0-based oxides, excluding Bi-Pb-0-based oxides with relatively low melting points, were heated above their melting temperature. After melting and solidifying, B
It was discovered that the superconductivity could be improved by diffusion by bringing i-Pb-0 type oxide into contact with the oxide, and the present invention was completed.

すなわち本願発明の要旨はBi −Pb −Sr −C
a−Cu−0系酸化物超伝導体の製造方法に於いて、S
r −Ca −Cu −0系超伝導体用原料酸化物をそ
の融解温度以上に加熱して融解せしめた後、これを冷却
して固化しこの固形物にBlpb−o系酸化物を接触せ
しめ超伝導相の生成する温度で一定時間保持し、当該B
l  −Pb −0系酸化物の拡散により臨界温度の高
く高密度の超伝導体を製造することを特徴とする酸化物
超伝導体の製造方法にある。
That is, the gist of the present invention is Bi-Pb-Sr-C
In the method for producing an a-Cu-0 based oxide superconductor, S
The raw material oxide for the r -Ca -Cu -0 superconductor is heated above its melting temperature to melt it, then cooled and solidified, and the Blpb-o oxide is brought into contact with this solid to form a superconductor. The B
A method for producing an oxide superconductor, characterized by producing a high-density superconductor with a high critical temperature by diffusion of l-Pb-0-based oxides.

ここでSr −Ca −Cu −0系超伝導体用原料酸
化物の融解温度はBl  −Pb −3r −Ca −
Cu−0系酸化物超伝導体の融解温度と同じく1000
〜1200℃が好ましい。ただ約820℃で融点を持つ
Bi2O3やこれとpbとの複合酸化物等のような低融
点物質が含まれていないのでこれらの蒸発による気泡の
発生はみられない。よって溶融物を冷却した際、固形物
中に気孔がなく緻密な超伝導用素材が生成し得る。
Here, the melting temperature of the raw material oxide for Sr-Ca-Cu-0 superconductor is Bl-Pb-3r-Ca-
1000, which is the same as the melting temperature of Cu-0 based oxide superconductor.
~1200°C is preferred. However, since it does not contain low-melting-point substances such as Bi2O3, which has a melting point at about 820°C, and a composite oxide of Bi2O3 and PB, no bubbles are generated due to the evaporation of these substances. Therefore, when the melt is cooled, a dense superconducting material with no pores in the solid can be produced.

然る後、このSr −Ca −Cu −0からなる緻密
な超伝導用素材にBi−Pb−0系酸化物を接触させる
。Bl  −Pb −0系酸化物はB l 203゜P
bOの粉末を混合したものでもよいが、BizO3゜P
bO粉末を焼結したものでもよい。
Thereafter, a Bi-Pb-0 based oxide is brought into contact with this dense superconducting material made of Sr-Ca-Cu-0. Bl -Pb -0 series oxide has Bl 203゜P
A mixture of bO powder may be used, but BizO3゜P
It may also be made by sintering bO powder.

接触させた後、超伝導相の生成し得る温度で一定時間加
熱する。加熱温度は酸素濃度4〜8%の雰囲気で830
〜840℃が好ましい。この加熱には超伝導相の生成し
得る温度以下の温度での加熱とその後の超伝導相の生成
し得る温度での加熱の2段階以上の加熱が含まれる。
After contacting, they are heated for a certain period of time at a temperature that allows the formation of a superconducting phase. The heating temperature is 830℃ in an atmosphere with an oxygen concentration of 4 to 8%.
~840°C is preferred. This heating includes two or more stages of heating: heating at a temperature below the temperature at which a superconducting phase can be generated, and then heating at a temperature at which a superconducting phase can be generated.

この加熱の際、接触物質であるBi  −Pb −0成
分はSr −Ca −Cu −0の素材中へ拡散してゆ
き緻密なりl  −Pb −3r −Ca −Cu −
0系酸化物超伝導体が得られる。
During this heating, the Bi-Pb-0 component, which is a contact substance, diffuses into the Sr-Ca-Cu-0 material and becomes dense l-Pb-3r-Ca-Cu-
A zero-based oxide superconductor is obtained.

Bl  −Pb −8r −Ca −Cu −0系酸化
物の組成比は限定されるものではないが一般的にはBi
  :Pb :Sr :Ca :Cu−1,8:0.3
 :1.9 :2.0  :3.0の近傍の混合比が望
ましいので接触、拡散後の混合比が上記の比率になるよ
うに設定するのが好ましい。
Although the composition ratio of the Bl -Pb -8r -Ca -Cu -0 system oxide is not limited, it is generally Bi
:Pb :Sr :Ca :Cu-1,8:0.3
Since a mixing ratio in the vicinity of :1.9 :2.0 :3.0 is desirable, it is preferable to set the mixing ratio after contact and diffusion to the above ratio.

接触する方法としてはSr −Ca −Cu −0より
なる溶融物をスピンコード等により厚膜化した場合は両
面又は片面にBi−Pb−0系酸化物を塗布または蒸着
により接触することができる。また線状に加工した場合
も塗布または金属シース材中にともに充填する等をとる
ことにより可能である。
As a method of contacting, when a molten material of Sr--Ca--Cu-0 is formed into a thick film by a spin cord or the like, contact can be made by coating or vapor depositing a Bi-Pb-0 based oxide on both sides or one side. Furthermore, it is also possible to process it into a linear shape by coating it or filling it together in a metal sheath material.

〔実 施 例〕〔Example〕

次に本発明の実施例および従来の比較例を挙げて本発明
を更に詳しく説明する。
Next, the present invention will be explained in more detail by giving examples of the present invention and conventional comparative examples.

これらの方法によって得られた超伝導体の臨界温度Tc
と臨界電流密度Jcは次の方法によった。
The critical temperature Tc of superconductors obtained by these methods
and critical current density Jc were determined by the following method.

まずTcの測定は試料片を長さ10m■、幅3mmに切
り出し直流4端子法により測定した。試料片を約1′に
7分の速度で温度を下げ、約1重おきに両端子より3の
電流を導入し、内側2端子に現れる電圧の下限(1、O
X IO’V )を切ったところで抵抗を0としその温
度をTcとした。
First, Tc was measured by cutting out a sample piece to a length of 10 m and a width of 3 mm and measuring it by a DC 4-terminal method. Lower the temperature of the sample piece to about 1' at a rate of 7 minutes, introduce a current of 3 from both terminals approximately every other layer, and lower the lower limit of the voltage appearing at the inner two terminals (1, O
When X IO'V ) was cut off, the resistance was set to 0, and the temperature was set as Tc.

次にJcのn1定は以下のようにして行った。前述の試
料片の中心部を更に幅0.5■、厚さ0.3mmに加工
し、液体窒素中に浸し、温度77玉中で両端子より導入
する電流を増加しながら内側の2端子に現れる電圧を測
定し、電圧の値が測定下限(1,0X10’V)より大
きくなったところの導入した電流の値を断面積で除算し
、Jcとした。
Next, the n1 constant of Jc was determined as follows. The center part of the sample piece mentioned above was further processed to a width of 0.5 mm and a thickness of 0.3 mm, immersed in liquid nitrogen, and heated to the inner two terminals while increasing the current introduced from both terminals in a temperature of 77 mm. The voltage appearing was measured, and the value of the introduced current at the point where the voltage value became larger than the measurement lower limit (1.0 x 10'V) was divided by the cross-sectional area, and was determined as Jc.

〔実施例1〕 5rCOCaCO5,CuOを原料としS「二3゛ Ca : Cu −1,9: 2.0 : 3.0の比
となる酸化物超伝導体原料組成物を空気中で1100℃
に加熱し溶融する。溶融物を一度急冷した後Bi2O3
゜PbOの粉末を最終組成でBl  :Pb :Sr 
:Ca : Cu ”1.8 :0.3 : 1.9 
:2.0 :3.Oの比となるように添加し、よく接触
させ、酸素濃度8%の雰囲気で830℃で100時間熱
処理を行った。
[Example 1] An oxide superconductor raw material composition made of 5rCOCaCO5, CuO and having a ratio of S'23'Ca: Cu -1,9: 2.0: 3.0 was heated at 1100°C in air.
Heat to melt. After quenching the melt once, Bi2O3
゜PbO powder with final composition Bl:Pb:Sr
:Ca:Cu”1.8:0.3:1.9
:2.0 :3. They were added so as to have the same ratio as O, brought into good contact, and heat-treated at 830° C. for 100 hours in an atmosphere with an oxygen concentration of 8%.

生成した超伝導体のTcとJcの値を表1に示す。Table 1 shows the values of Tc and Jc of the produced superconductor.

〔比較例1〕 B iOP b O、S r COa 、Ca COa
 。
[Comparative Example 1] B iOP b O, S r COa , Ca COa
.

23″ CuOを原料とし、Bi  :Pb :Sr :Ca 
:Cu −1,8: 0.3 : 1.9 : 2.0
 : 3.0の比となる酸化物超伝導体原料組成物を空
気中で1100℃で加熱し溶融する。溶融物を一度急冷
した後酸素濃度8%の雰囲気で830℃で100時間熱
処理を行った。
23″ CuO is used as raw material, Bi:Pb:Sr:Ca
:Cu-1,8: 0.3: 1.9: 2.0
: An oxide superconductor raw material composition having a ratio of 3.0 is heated and melted at 1100° C. in air. After the melt was once rapidly cooled, it was heat-treated at 830° C. for 100 hours in an atmosphere with an oxygen concentration of 8%.

生成した超伝導体のTcとJcの値を表1に示す。Table 1 shows the values of Tc and Jc of the produced superconductor.

表 〔効  果〕 本発明による、気孔の少ない超伝導体は、高融点元素を
溶融した後低融点元素と接触させアニルすることで、高
いTcと高いJeを兼ね備えた超伝導体を得ることがで
きる。
Table [Effect] The superconductor with few pores according to the present invention can be obtained by melting a high melting point element and then bringing it into contact with a low melting point element and annealing to obtain a superconductor having both high Tc and high Je. can.

なお、Jc、Tcの値は各所で発表されているが、試料
の作成条件等により多少変動があるので、絶対値で比較
することは適当でない。他の条件をできるだけ一定にし
て相対的に比較することが重要である。
Note that although the values of Jc and Tc have been announced in various places, it is not appropriate to compare them in terms of absolute values, as they vary somewhat depending on the preparation conditions of the sample. It is important to make relative comparisons while keeping other conditions as constant as possible.

Claims (1)

【特許請求の範囲】[Claims] 1.Bi−Pb−Sr−Ca−Cu−O系酸化物超伝導
体の製造方法に於いて、Sr−Ca−Cu−O系超伝導
体用原料酸化物をその融解温度以上に加熱して融解せし
めた後、これを冷却して固化しこの固形物にBi−Pb
−O系酸化物を接触せしめ超伝導相の生成する温度で一
定時間保持し、当該Bi−Pb−O系酸化物の拡散によ
り臨界温度の高く高密度の超伝導体を製造することを特
徴とする酸化物超伝導体の製造方法。
1. In a method for producing a Bi-Pb-Sr-Ca-Cu-O based oxide superconductor, a raw material oxide for the Sr-Ca-Cu-O based superconductor is heated to a temperature higher than its melting temperature to melt it. After that, it is cooled and solidified, and Bi-Pb is added to this solid.
-O-based oxides are brought into contact and held at a temperature at which a superconducting phase is formed for a certain period of time, and a high-density superconductor with a high critical temperature is produced by diffusion of the Bi-Pb-O-based oxides. A method for producing an oxide superconductor.
JP1042310A 1989-02-22 1989-02-22 Production of oxide superconductor Pending JPH02221149A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1042310A JPH02221149A (en) 1989-02-22 1989-02-22 Production of oxide superconductor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1042310A JPH02221149A (en) 1989-02-22 1989-02-22 Production of oxide superconductor

Publications (1)

Publication Number Publication Date
JPH02221149A true JPH02221149A (en) 1990-09-04

Family

ID=12632452

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1042310A Pending JPH02221149A (en) 1989-02-22 1989-02-22 Production of oxide superconductor

Country Status (1)

Country Link
JP (1) JPH02221149A (en)

Similar Documents

Publication Publication Date Title
JPH01215721A (en) Compound superconductor and production thereof
JP2672926B2 (en) Method for producing yttrium-based superconductor
JPH02221149A (en) Production of oxide superconductor
JPH05194018A (en) High temperature superconductor and method for its production
JPH02279556A (en) Production of oxide superconductor
JPH04132616A (en) Production of bismuth-based oxide superconductor
JPH02255535A (en) Production of oxide superconductor
JPH027309A (en) Manufacture of oxide type superconductive wire
JPS63291317A (en) Manufacture of oxide superconductive wire rod
JP3354961B2 (en) Bi-based superconductor and method of manufacturing superconducting thick film
JPH0354103A (en) Production of oxide superconductor
JPH02192401A (en) Production of oxide superconductor and oxide superconducting wire
JPH01234327A (en) Production of oxide superconductor
JPH01141869A (en) Production of superconductor
JPH01212226A (en) Production of oxide superconducting material
JPH02120234A (en) Production of oxide superconductor
JPH01239054A (en) Production of oxide superconductor
JPH0714818B2 (en) Superconducting fibrous crystal and method for producing the same
JPH02153823A (en) Production of oxide superconductor
JPH01183450A (en) Production of formed oxide superconductor
JPH01176608A (en) Manufacture of oxide superconductive linear body
JPH01204314A (en) Manufacture of oxide superconductor
JPH02199057A (en) Production of bismuth-based oxide superconductor
JPH01141821A (en) superconductor
JPH02239522A (en) Manufacture of bi oxide superconducting wire having high critical current density