JPS63288954A - Production of superconductor - Google Patents

Production of superconductor

Info

Publication number
JPS63288954A
JPS63288954A JP62125110A JP12511087A JPS63288954A JP S63288954 A JPS63288954 A JP S63288954A JP 62125110 A JP62125110 A JP 62125110A JP 12511087 A JP12511087 A JP 12511087A JP S63288954 A JPS63288954 A JP S63288954A
Authority
JP
Japan
Prior art keywords
oxide
superconductor
sintered body
atomic
temperature
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
JP62125110A
Other languages
Japanese (ja)
Inventor
Nobuyuki Yoshioka
信行 吉岡
Yoshiyuki Kashiwagi
佳行 柏木
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.)
Meidensha Electric Manufacturing Co Ltd
Original Assignee
Meidensha Electric Manufacturing Co Ltd
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 Meidensha Electric Manufacturing Co Ltd filed Critical Meidensha Electric Manufacturing Co Ltd
Priority to JP62125110A priority Critical patent/JPS63288954A/en
Publication of JPS63288954A publication Critical patent/JPS63288954A/en
Pending legal-status Critical Current

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Classifications

    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10NELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10N60/00Superconducting devices
    • H10N60/01Manufacture or treatment
    • H10N60/0268Manufacture or treatment of devices comprising copper oxide

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  • Engineering & Computer Science (AREA)
  • Manufacturing & Machinery (AREA)
  • Compositions Of Oxide Ceramics (AREA)
  • Inorganic Compounds Of Heavy Metals (AREA)
  • Superconductor Devices And Manufacturing Methods Thereof (AREA)
  • Superconductors And Manufacturing Methods Therefor (AREA)

Abstract

PURPOSE:To produce a superconductor exhibiting superconductivity at above the b.p. of liquid N2 by calcining a molded body obtd. by compression molding a powder mixture consisting of Y oxide Ba oxide, and Cu oxide in oxidizing atmosphere. CONSTITUTION:A binder is mixed with a powder mixture consisting of Y oxide (e.g. Y2O3), Ba oxide (e.g. BaO), and Cu oxide (e.g. CuO), and a molded body is prepd. by compression molding the obtained mixture. Then, the molded body is calcined at 950-1,200 deg.C in oxidizing atmosphere, and a Y-Ba-Ca-O superconductor consisting of 10<=Y<=60atom.%, 20<=Ba<=50atom.%, and 30<=Cu<=65 atom.% is obtained.

Description

【発明の詳細な説明】 A、産業上の利用分野 本発明は、一定の温度で電気抵抗がゼロになる所謂超電
導体に係り、特に液体窒素温度以」二で超電導を示す超
電導体に関する。
DETAILED DESCRIPTION OF THE INVENTION A. Field of Industrial Application The present invention relates to a so-called superconductor whose electrical resistance becomes zero at a certain temperature, and particularly to a superconductor which exhibits superconductivity at temperatures above liquid nitrogen temperature.

B1発明の概要 本発明は、出発物質として、イツトリウム酸化物、バリ
ウム酸化物、及び銅酸化物の各粉末を用いて形成したイ
ツトリウム(Y)、バリウム(Ba)。
B1 Summary of the Invention The present invention provides yttrium (Y) and barium (Ba) formed using powders of yttrium oxide, barium oxide, and copper oxide as starting materials.

銅(Cu)及び酸素(O)の成分からなる焼結体で、液
体窒素温度(絶対温度77度)以上で超電導を示す超電
導体の製造方法にある。
A method for manufacturing a superconductor which is a sintered body consisting of copper (Cu) and oxygen (O) and exhibits superconductivity at a liquid nitrogen temperature (absolute temperature of 77 degrees Celsius) or higher.

C1従来の技術 西暦1911年カメリング・オンネスにより超電導現象
が発見されていらい、実用化に向けてさまざまな研究開
発が進められている。実用化には、臨界温度(’rc)
が高ければ高い程、冷却コストが安くて済むため、より
高温での超電導の可能性をめぐってその超電導材料の激
しい開発競争が展開されている。
C1 Conventional Technology Since the discovery of superconductivity by Kamerling Onnes in 1911, various research and development efforts have been underway to put it into practical use. For practical use, the critical temperature ('rc)
The higher the temperature, the lower the cooling cost, so there is intense competition to develop superconducting materials with the potential for superconductivity at higher temperatures.

これまでに明らかにされている超電導材料は、液体ヘリ
ウム温度(Tc約4に、−269℃)で冷却して使用す
るものがほとんどであり、これはヘリウムガスを液化し
た冷却剤で冷却しなければならない。ヘリウムは希少材
料で高価格であるうえ、臨界温度まで下げるための冷却
コストが非常に高くつくため、超電導材料の普及を遅ら
せる最大の原因となっている。
Most of the superconducting materials that have been revealed so far are used after being cooled to liquid helium temperature (Tc approximately 4, -269°C), which requires cooling with a coolant made from liquefied helium gas. Must be. Helium is a rare and expensive material, and the cost of cooling it down to its critical temperature is extremely high, making it the main reason for delaying the spread of superconducting materials.

ごく最近、超電導材料についての研究開発う(財界的に
ら進められ、これまでの概念を破る材料が登場しつつあ
る。
Very recently, research and development on superconducting materials has been progressing in the financial world, and materials that break with conventional concepts are appearing.

これまで知られた超電導材料の最高の’I’ cは、ニ
オブ3ゲルマニウム(N b3G e)の22.3Kに
とどまっていたが、La(ランタン)の一部をBa(バ
リウ2.)で置換したランタン・ストロンチウ12・銅
酸化物(I、aSr)tcuo4によって、これまでの
限界を超えた37にで超電導現象が始まり、33にで電
気抵抗がゼロになったことが発表され、続いて今年始め
同じくLa−8r−CuO4系で54Kを、また同物質
系で85Kを実現したと発表された。更に続いて、物質
名を「酸化物」としか明らかにされないが、ランタン・
ストロンチウム・同酸化物系と思われる新物質によって
T、c77Kを達成したと発表されるに至った。更に近
年、100Kを超えるバリウム・イブテルビウム・銅酸
化物。
The highest 'I' c of the superconducting materials known so far was 22.3K for niobium 3 germanium (Nb3Ge), but some of the La (lanthanum) was replaced with Ba (barium 2.). With lanthanum, strontium-12, and copper oxide (I, aSr) tcuo4, superconductivity began in 1937, exceeding the previous limits, and it was announced that electrical resistance became zero in 1933, and then this year Initially, it was announced that 54K was achieved using the same La-8r-CuO4 system, and that 85K was achieved using the same material. Furthermore, although the name of the substance is only disclosed as "oxide", lanthanum and
It was announced that T, c77K had been achieved using a new substance believed to be based on strontium oxides. Furthermore, in recent years, barium, ibuterbium, and copper oxides that exceed 100K.

イツトリウム系銅酸化物の超電導材料が発見されたと発
表されるに至っている。
It has been announced that a superconducting material made of yttrium-based copper oxide has been discovered.

D0発明が解決しようとする問題点 上記のように液体ヘリウムの温度は、常圧で4.2にで
あり、ヘリウムは希少材料で且つ高価格で、加えて臨界
温度まで下げるための膨張タービンなどを必要とし、冷
却コストが極めて高くつき実用化の一つの障害となって
いた。また、77に以上であれば液体窒素を使用でき、
液体ヘリウ11の使用と比較してすべての点において有
利であり、実用化が極めて容易となるため、’rcが7
7に以上の超電導材料の開発が望まれているが、その開
発は、−L述の通り未だ緒についたばかりであるのが現
状である。
D0 Problems to be solved by the invention As mentioned above, the temperature of liquid helium is 4.2 at normal pressure. The cooling cost was extremely high, which was an obstacle to practical application. Also, if it is 77 or higher, you can use liquid nitrogen,
It is advantageous in all respects compared to the use of liquid Heliu-11 and is extremely easy to put into practical use, so 'rc is 7.
Although the development of superconducting materials as described above is desired, the current situation is that, as mentioned above, the development has only just begun.

これらの点に鑑み、本発明は、77に以」二で超電導状
態となる超電導体の製造方法を提供しようとするもので
ある。
In view of these points, it is an object of the present invention to provide a method for manufacturing a superconductor that becomes superconducting in 77 or later.

E1問題点を解決ずろための手段と作用液体窒素冷却で
超電導体が使用できれば、電力。
Means and functions to solve the E1 problem If superconductors can be used with liquid nitrogen cooling, electricity can be generated.

運輸、エネルギー変換等の広い分野で利用できる点に着
目し、種々の材料の配合、焼成温度等の実験を重ねた結
果、イブトリウム(Y)、バリウノ、(I(a)、銅(
Cu)及び酸素(O)の成分からなる焼結体で、1つ焼
結体の成分のY  B a  CuにおけろYが10≦
Y≦60原子% B、が20≦Da≦50原子% Cuが30≦Cu≦65原子% の範囲であれば、液体窒素による冷却で抵抗ゼロの超電
導体が得られることを見出した。
Focusing on the fact that it can be used in a wide range of fields such as transportation and energy conversion, we conducted repeated experiments with various material formulations, firing temperatures, etc., and found that it could be used in a wide range of fields such as transportation and energy conversion.
A sintered body consisting of the components of Cu) and oxygen (O), where Y in one component of the sintered body, Y B a Cu, is 10≦
It has been found that a superconductor with zero resistance can be obtained by cooling with liquid nitrogen as long as Y≦60 atomic %, B, 20≦Da≦50 atomic %, and Cu 30≦Cu≦65 atomic %.

すなわち、イツトリウム酸化物の粉末と、バリウム酸化
物の粉末と、銅酸化物の粉末と、を混合して得た混合粉
末を加圧して形成し、 この成形体を酸化性雰囲気中で且つ950〜1200℃
の範囲で焼結することにより、イツトリウム(Y)、バ
リウム(Ba)、銅(Cu)、及び酸素(O)の成分か
らなり、且つY −Ba −CUにおける成分を前述の
範囲とした焼結体を形成すれば、液体窒素による冷却で
抵抗ゼロの超電導体が容易に得られること見出した。
That is, a mixed powder obtained by mixing yttrium oxide powder, barium oxide powder, and copper oxide powder is pressurized to form this molded body in an oxidizing atmosphere and 1200℃
By sintering in a range of We discovered that if a superconductor is formed, a superconductor with zero resistance can be easily obtained by cooling with liquid nitrogen.

なお、Y −Ba−Cuにおいて Y/J<IO原子%未満、60原子%超過Baが20原
子%未満、50原子%超過Cuが30原子未満、65原
子超過 の場合には、液体窒素で超電導が生じる焼結体を得るこ
とができなかった。
In addition, in Y-Ba-Cu, if Y/J<IO atomic %, Ba exceeding 60 atomic % is less than 20 atomic %, Cu exceeding 50 atomic % is less than 30 atomic, or exceeds 65 atomic %, superconductivity can be achieved with liquid nitrogen. It was not possible to obtain a sintered body in which .

F、実施例 以下、本発明を実施例に基づいて説明する。先ず、出発
原料として粒径10μm以下としたイツトリウム酸化物
(Y=03)の粉末、バリウム酸化物(Bao)の粉末
、銅酸化物(Cub)の粉末。
F. Examples The present invention will be explained below based on examples. First, starting materials are yttrium oxide (Y=03) powder, barium oxide (Bao) powder, and copper oxide (Cub) powder each having a particle size of 10 μm or less.

をそれぞれ20ao1%、30mo1%、50mo1%
となるよう秤量する。
respectively 20ao1%, 30mo1%, 50mo1%
Weigh it so that

次に、これらの粉末をボールミル等で上のに混合すると
供にエチルアルコールと玉石を入れ数時間十分に混合し
、得られたスラリーを約100”Cの温度で乾燥させる
Next, these powders are mixed using a ball mill or the like, and ethyl alcohol and cobblestone are added thereto and thoroughly mixed for several hours, and the resulting slurry is dried at a temperature of about 100''C.

なお、バリウム酸化物は水が存在するとBaO+HtO
→Ba(OH)tの反応により、多量の熱が発生するた
め、アルコールが用いられている。
In addition, when water is present in barium oxide, BaO + HtO
→ Alcohol is used because a large amount of heat is generated by the reaction of Ba(OH)t.

次に、バインダーとしてポリビニルアルコールを原料粉
末に対し1重量%となるようにポリビニルアルコール溶
液の形で添加する。そしてアルコールを更に加え十分混
練した後、乾燥し、ふるいにて150メツシユ以下の顆
粒状の造粒粉を得る。
Next, polyvinyl alcohol is added as a binder in the form of a polyvinyl alcohol solution so that the amount is 1% by weight based on the raw material powder. After further adding alcohol and thoroughly kneading, the mixture is dried and sieved to obtain granulated powder having a size of 150 mesh or less.

次に、この造粒粉を金型に充填した後、700kg/a
x”程度の圧力で圧縮成形して外径40xm、厚み約6
xxの成形体を作る。
Next, after filling this granulated powder into a mold, 700 kg/a
Compression molded with a pressure of about x”, outer diameter 40xm, thickness approx.
Make a molded body of xx.

次に、この成形体を焼成器に設置し、酸化性雰囲気で、
且つ約1050℃の温度で数時間加熱して焼結体(セラ
ミックス)を得る。
Next, this molded body is placed in a firing oven and heated in an oxidizing atmosphere.
A sintered body (ceramics) is obtained by heating at a temperature of about 1050° C. for several hours.

上記の製造方法により得られた焼結体を、中4If、厚
さ4 xyt、長さ一1011zの形状に切り出して第
1図に示すように電極を設けて4端子法により、焼結体
の抵抗を測定した。
The sintered body obtained by the above manufacturing method was cut into a shape of 4If in the middle, 4xyt in thickness, and 1011z in length. Electrodes were provided as shown in Figure 1, and the sintered body was cut out by the four-terminal method. Resistance was measured.

即ち第1図は、抵抗値を測定するための説明図で、焼結
体Sの長手方向の両端側に電流を流すための端子a、 
a’を設け、その内側に抵抗値を測定するための電圧端
子す、 b’を設ける、これを液体窒素の低温槽に入れ
、端子a、 a’ にIアンペアの安定化電流を流して
端子す、 b’間の電圧を電圧計(V)で測定して端子
す、 b’間の電圧降下によって抵抗値を測定する。な
お、Aは電流計を示す。
That is, FIG. 1 is an explanatory diagram for measuring the resistance value, in which terminals a for passing current through both ends of the sintered body S in the longitudinal direction,
A' is provided, and inside it is a voltage terminal for measuring the resistance value. Measure the voltage between terminals A and B' with a voltmeter (V), and measure the resistance value by the voltage drop between terminals A and B'. Note that A indicates an ammeter.

第2図は、その測定結果を示すもので、絶対温度約93
にで超電導現象が始まり、約89Kに至って電気抵抗が
ゼロになることが確認された。
Figure 2 shows the measurement results, with an absolute temperature of approximately 93
It was confirmed that the superconducting phenomenon began at about 89K, and that the electrical resistance became zero.

他の組成比についても同様な実験を行なったので、前述
の例を含めて記載する。
Similar experiments were conducted with other composition ratios, so the description will include the above-mentioned examples.

但し、表の実施例1が上述したものを示す。However, Example 1 in the table shows the above.

なお、Y、0.が501o1%未満、30mo1%超過
BaOが20mo1%未満、50mo1%超過CuOが
30111o1%未満、65Ilo1%超過では、超電
導を生じる焼結体を得ることができなかった。
Note that Y, 0. was less than 501o1%, BaO in excess of 30mo1% was less than 20mo1%, CuO in excess of 50mo1% was less than 30111o1%, and 65Ilo was more than 1%, it was not possible to obtain a sintered body that produced superconductivity.

要は、出発物質換算でイツトリウム酸化物(Y、03)
が5〜30moI%、バリウム酸化物(Bad)が20
〜50mo1%、銅酸化物(Cub)が30〜65mo
1%であれば液体窒素で抵抗ゼロとなることが判った。
In short, yttrium oxide (Y, 03) in terms of starting material
is 5 to 30 moI%, barium oxide (Bad) is 20
~50 mo1%, copper oxide (Cub) 30-65 mo
It was found that if the concentration was 1%, the resistance would be zero with liquid nitrogen.

すなわち、焼結体を構成する成分のY−Ba−Cuにお
いて、Yが10〜60原子%、Baが20〜50原子%
、 Cuが30〜65原子%であれば超電導体が得られ
ることが判った。
That is, in Y-Ba-Cu, which is a component constituting the sintered body, Y is 10 to 60 at%, and Ba is 20 to 50 at%.
It has been found that a superconductor can be obtained if the Cu content is 30 to 65 atomic %.

更に、前述の実施例Iの組成条件のy、o3=20mo
1%、 Ba0=30mo1%、CuO=50mo1%
のものについて、焼結温度を変えて調べた結果、950
℃〜1200℃の温度において焼結すれば所望の超電導
体を得ることができた。
Furthermore, y, o3=20mo of the composition conditions of Example I mentioned above.
1%, Ba0=30mo1%, CuO=50mo1%
As a result of investigating the sintering temperature by changing the sintering temperature, 950
The desired superconductor could be obtained by sintering at a temperature of 1200°C to 1200°C.

しかし、温度が950℃未満、1200℃超過では所望
の超電導現象を生ずる焼結体を得ることができなかった
However, at temperatures below 950°C and above 1200°C, it was not possible to obtain a sintered body that produced the desired superconducting phenomenon.

G1発明の効果 以上のように本発明による超電導体は、液体窒素温度(
77K)において完全に超電導状態となる。
G1 Effects of the Invention As described above, the superconductor according to the present invention has a temperature of liquid nitrogen (
It becomes completely superconducting at 77K).

しかも、Y−Ba−Cu−0の焼結体における出発物質
に、イツトリウム酸化物、バリウム酸化物、銅酸化物の
粉末を用いており、その上、加圧成形、酸化性雰囲気に
て950〜1200℃の温度で焼結していることから、
ち密で特性の安定した超電導体を容易に得ることができ
る。
Furthermore, powders of yttrium oxide, barium oxide, and copper oxide are used as starting materials for the sintered body of Y-Ba-Cu-0, and in addition, powders of yttrium oxide, barium oxide, and copper oxide are used as starting materials, and in addition, powders of 950~ Because it is sintered at a temperature of 1200℃,
A dense superconductor with stable characteristics can be easily obtained.

現在明らかにされている超電導体は、ヘリウムガスを液
化した冷却剤で冷却しなければならず、液体ヘリウムの
温度は4.2にで、しかも希少材料で高価であり、且つ
液化コストも高いため、超電導材料の実用化の壁となっ
ていた。
The currently discovered superconductor requires cooling with a coolant made from liquefied helium gas, and the temperature of liquid helium is 4.2, and it is a rare and expensive material, and the cost of liquefying it is high. This has been a barrier to the practical application of superconducting materials.

しかし、液体窒素はどこででも、しかも安く人手でき、
従来の実用化の壁は完全に取り除かれ、特に電力、運輸
等に関連した電気抵抗、及び精密計測素子、その他エネ
ルギー変換などの分野に利用可能となる等極めて優れた
効果を発揮する。
However, liquid nitrogen can be used anywhere and cheaply by hand.
The conventional barriers to practical application have been completely removed, and it has extremely excellent effects, such as being able to be used in fields such as electrical resistance, precision measurement elements, and other energy conversion related to electricity, transportation, etc.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は本発明の焼結体の抵抗値測定の方法を説明する
ための説明図、第2図は本発明の焼結体の絶対温度(K
)に対する抵抗値(10−3Ωcm)の特性曲線図を示
す。 a、 a’ ・・・電流供給用端子、b、 b’ ・・
・電圧測定端子、S・・・焼結体。 −枡■5 ξ
Figure 1 is an explanatory diagram for explaining the method of measuring the resistance value of the sintered body of the present invention, and Figure 2 is the absolute temperature (K) of the sintered body of the present invention.
) is a characteristic curve diagram of the resistance value (10-3 Ωcm). a, a'... Current supply terminal, b, b'...
・Voltage measurement terminal, S...Sintered body. −Masu■5 ξ

Claims (1)

【特許請求の範囲】 イットリウム酸化物の粉末と、バリウム酸化物の粉末と
、銅酸化物の粉末とを混合して混合粉末を得る工程と、 該混合粉末を加圧して成形体を得る工程と、該成形体を
酸化性雰囲気中で、且つ950℃〜1200℃の範囲の
温度で焼成して焼結体を形成する工程とからなり、 該焼結体がイットリウム(Y)、バリウム(Ba)、銅
(Cu)及び酸素(O)の成分からなり、且つY−Ba
−Cuにおける成分比が、 イットリウム(Y)が10≦Y≦60原子%バリウム(
Ba)が20≦Ba≦50原子%銅(Cu)が30≦C
u≦65原子% であることを特徴とする超電導体の製造方法。
[Claims] A step of mixing yttrium oxide powder, barium oxide powder, and copper oxide powder to obtain a mixed powder; and a step of pressurizing the mixed powder to obtain a compact. , a step of firing the molded body in an oxidizing atmosphere at a temperature in the range of 950°C to 1200°C to form a sintered body, and the sintered body contains yttrium (Y), barium (Ba). , consisting of copper (Cu) and oxygen (O) components, and Y-Ba
-The component ratio in Cu is yttrium (Y) to 10≦Y≦60 atomic% barium (
Ba) is 20≦Ba≦50 atomic% Copper (Cu) is 30≦C
A method for producing a superconductor, characterized in that u≦65 atomic %.
JP62125110A 1987-05-22 1987-05-22 Production of superconductor Pending JPS63288954A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP62125110A JPS63288954A (en) 1987-05-22 1987-05-22 Production of superconductor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP62125110A JPS63288954A (en) 1987-05-22 1987-05-22 Production of superconductor

Publications (1)

Publication Number Publication Date
JPS63288954A true JPS63288954A (en) 1988-11-25

Family

ID=14902095

Family Applications (1)

Application Number Title Priority Date Filing Date
JP62125110A Pending JPS63288954A (en) 1987-05-22 1987-05-22 Production of superconductor

Country Status (1)

Country Link
JP (1) JPS63288954A (en)

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