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JPH087680A - Method for manufacturing oxide superconducting wire - Google Patents

Method for manufacturing oxide superconducting wire

Info

Publication number
JPH087680A
JPH087680A JP6134175A JP13417594A JPH087680A JP H087680 A JPH087680 A JP H087680A JP 6134175 A JP6134175 A JP 6134175A JP 13417594 A JP13417594 A JP 13417594A JP H087680 A JPH087680 A JP H087680A
Authority
JP
Japan
Prior art keywords
wire
tape
temperature
tmba
current density
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
JP6134175A
Other languages
Japanese (ja)
Inventor
Masashi Yoshida
政司 吉田
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.)
Nippon Steel Corp
Original Assignee
Sumitomo Metal Industries 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 Sumitomo Metal Industries Ltd filed Critical Sumitomo Metal Industries Ltd
Priority to JP6134175A priority Critical patent/JPH087680A/en
Publication of JPH087680A publication Critical patent/JPH087680A/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

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

Abstract

(57)【要約】 【目的】優れた超伝導特性 (Jcが 15000A/cm2以上) の
TmBa2Cu3O7-xの線材を簡単に製造する方法の提供。 【構成】下記からまでの工程を特徴とするTmBa2Cu3
O7-x超伝導線材の製造方法。 Tm、BaおよびCuの酸化物、炭酸塩、硝酸塩または塩
化物の各粉末をTm:Ba:Cu=1:2:3になるように調
合し、混合粉末とする。 上記の配合粉末を銀テープに塗布するかまたは銀シ
ースに充填し、加工して線材となし、プレスまたは圧延
によってテープ状線材とする。 上記テープ状線材を、酸素分圧が 0.003〜0.03気圧
の雰囲気中で一旦 930〜945 ℃の温度まで加熱した後、
少なくとも 900℃までは毎時 0.1〜10℃の冷却速度で冷
却する。
(57) [Summary] [Purpose] Excellent superconducting properties (Jc of 15000 A / cm 2 or more)
Providing a method for easily manufacturing TmBa 2 Cu 3 O 7-x wire rods. [Structure] TmBa 2 Cu 3 characterized by the following steps
O 7-x Superconducting wire manufacturing method. Powders of oxides, carbonates, nitrates or chlorides of Tm, Ba and Cu are prepared so as to be Tm: Ba: Cu = 1: 2: 3 to obtain a mixed powder. The above-mentioned compounded powder is applied to a silver tape or filled in a silver sheath, processed into a wire, and pressed or rolled into a tape-shaped wire. After heating the above tape-shaped wire to a temperature of 930 to 945 ℃ once in an atmosphere with an oxygen partial pressure of 0.003 to 0.03 atm,
Cool down to at least 900 ℃ at a cooling rate of 0.1 to 10 ℃ per hour.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】この発明は、TmBa2Cu3O7-xの組成
式で表され、臨界電流密度が高く、電磁石、電力ケーブ
ル等に使用することのできる超伝導線材の製造方法に関
する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a method for producing a superconducting wire which is represented by the composition formula of TmBa 2 Cu 3 O 7-x and has a high critical current density and which can be used in electromagnets, power cables and the like. .

【0002】[0002]

【従来の技術】MBa2Cu3O7 (Mは、Y、Nd、Pm、Sm、E
u、Gd、Tb、Dy、Ho、Er、TmまたはYb)の組成式で表され
るY系超伝導体は、超伝導転移温度 (臨界温度、Tc)が
約90Kのいわゆる高温超伝導物質であることは既によく
知られている〔例えば、Japanese Journal of Applied
Physics Vol.26,(1987) pp.L633 〕。
2. Description of the Related Art MBa 2 Cu 3 O 7 (M is Y, Nd, Pm, Sm, E
The Y-based superconductor represented by the composition formula of u, Gd, Tb, Dy, Ho, Er, Tm or Yb) is a so-called high temperature superconducting material having a superconducting transition temperature (critical temperature, Tc) of about 90K. It is already well known [eg, Japanese Journal of Applied
Physics Vol.26, (1987) pp.L633].

【0003】この、いわゆるY系超伝導体は、セラミッ
ク特有の硬くて脆い性質のために、コイルや電力ケーブ
ルとして使用するためには金属シース管に充填して加工
したシース線材、または金属テープに塗布したテープ状
線材にするのが通常である。
This so-called Y-type superconductor has a hard and brittle characteristic peculiar to ceramics, and therefore, for use as a coil or a power cable, a sheath wire or metal tape filled and processed in a metal sheath tube is used. It is usually a coated tape-shaped wire.

【0004】上記のようなシース線材またはテープ状線
材を製造する際には、これらの超伝導体の異方性のため
に、高い臨界電流密度を得るには結晶軸のC軸を電流を
流す方向と垂直になるように結晶方位を揃える必要があ
る。
When manufacturing the above-mentioned sheath wire or tape-shaped wire, due to the anisotropy of these superconductors, an electric current is passed through the C axis of the crystal axis in order to obtain a high critical current density. It is necessary to align the crystal orientation so that it is perpendicular to the direction.

【0005】Y系超伝導体では、金属 (ハステロイ)テ
ープを基板としてレーザー蒸着法、あるいはCDV法を
用いて作製したYBa2Cu3O7線材で、C軸が配向した線材
が得られたとの報告がある (応用物理学会、1992年春季
予稿集、第1分冊、29a−W−7、および Japanese Jo
urnal of Applied Physics Vol.31,(1992) pp.L547-L54
9 を参照) 。しかし、これらの方法で線材の製造は、時
間がかかり、また製造装置のコストが高く、工業的生産
には不適切であるという欠点がある。
With respect to the Y-based superconductor, a YBa 2 Cu 3 O 7 wire rod produced by a laser deposition method or a CDV method using a metal (hastelloy) tape as a substrate, and a C-axis oriented wire rod was obtained. There is a report (The Society of Applied Physics, Spring 1992 Proceedings, Volume 1, 29a-W-7, and Japanese Jo
urnal of Applied Physics Vol.31, (1992) pp.L547-L54
See 9). However, the production of a wire by these methods is disadvantageous in that it is time-consuming, the cost of production equipment is high, and it is unsuitable for industrial production.

【0006】[0006]

【発明が解決しようとする課題】本発明は、優れた超伝
導特性、具体的にはコイルにした場合に1000ガウス以上
の磁場発生が可能な 15000A/cm2以上の臨界電流密度
(Jc) を持つY系超伝導体の中で、特に、銀の融点以下
の温度での熱処理による結晶作製が可能なTmBa2Cu3O7-x
の線材を、できるだけ簡単に製造する方法を提供するこ
とを目的とする。
DISCLOSURE OF THE INVENTION The present invention has excellent superconducting properties, specifically, a critical current density of 15000 A / cm 2 or more that can generate a magnetic field of 1000 gauss or more when formed into a coil.
Among the Y-based superconductors with (Jc), TmBa 2 Cu 3 O 7-x that can be crystallized by heat treatment at a temperature below the melting point of silver.
It is an object of the present invention to provide a method for manufacturing the above wire rod as easily as possible.

【0007】[0007]

【課題を解決するための手段】本発明の要旨は、下記
からまでの工程を特徴とするTmBa2Cu3O7-x超伝導線材
の製造方法にある。
The gist of the present invention is a method for producing a TmBa 2 Cu 3 O 7-x superconducting wire characterized by the following steps.

【0008】 Tm、BaおよびCuの酸化物、炭酸塩、硝
酸塩または塩化物の各粉末をTm:Ba:Cu=1:2:3に
なるように調合し、混合粉末とする。このとき、原料粉
末として酸化物以外の粉末、即ち、炭酸塩、硝酸塩また
は塩化物の粉末を用いた場合は、配合の前または後に仮
焼によって酸素以外の非金属元素を除去する。
Powders of oxides, carbonates, nitrates or chlorides of Tm, Ba and Cu are prepared so as to be Tm: Ba: Cu = 1: 2: 3 to obtain mixed powders. At this time, when powders other than oxides, that is, powders of carbonates, nitrates or chlorides are used as raw material powders, non-metal elements other than oxygen are removed by calcination before or after compounding.

【0009】 上記の混合粉末を銀テープに塗布する
かまたは銀シースに充填し、加工して線材となし、プレ
スまたは圧延によってテープ状線材とする。
The above-mentioned mixed powder is applied to a silver tape or filled in a silver sheath and processed into a wire, which is then pressed or rolled into a tape-shaped wire.

【0010】 上記テープ状線材を、酸素分圧が 0.0
03〜0.03気圧の雰囲気中で一旦 930〜945 ℃の温度まで
加熱した後、少なくとも 900℃までは毎時 0.1〜10℃の
冷却速度で冷却する。
The tape-shaped wire is made to have an oxygen partial pressure of 0.0
Once heated to a temperature of 930 to 945 ° C in an atmosphere of 03 to 0.03 atm, cool at a cooling rate of 0.1 to 10 ° C per hour up to at least 900 ° C.

【0011】[0011]

【作用】一般に、物質を溶融状態から結晶成長させた場
合、表面エネルギーが最小となるように結晶が配向する
場合があることが知られている。酸化物では、表面エネ
ルギーは酸素分圧に依存するため、酸素分圧を調整する
ことによって配向を制御することが可能である。
It is generally known that when a substance is grown from a molten state, the crystal may be oriented so that the surface energy is minimized. Since the surface energy of an oxide depends on the oxygen partial pressure, it is possible to control the orientation by adjusting the oxygen partial pressure.

【0012】本発明者は、各種のY系超伝導体の凝固時
の配向性を酸素分圧を変えて調査した結果、特にTmBa2C
u3O7-xについて、前記の特定の条件下で加熱および冷却
を行うことにより配向性を高めることができることを見
いだした。この知見を基礎としてなされたのが本発明で
ある。
The present inventor investigated the orientation of various Y-based superconductors at the time of solidification by changing the oxygen partial pressure, and in particular, TmBa 2 C
It was found that the orientation of u 3 O 7-x can be enhanced by heating and cooling under the above-mentioned specific conditions. The present invention is based on this knowledge.

【0013】以下、前記〜の各工程について説明す
る。
Each of the above steps 1 to 3 will be described below.

【0014】の工程:これは、一般的なY系酸化物超
伝導材の製造方法に準ずる工程である。ただし、製造目
的物がTmBa2Cu3O7-xであるから、Tmの酸化物、炭酸塩、
硝酸塩および塩化物の中の1種以上の粉末を原料粉末の
一つとする。BaおよびCuの原料としても、それらの酸化
物、炭酸塩、硝酸塩および塩化物の中の1種以上を用い
ることができる。
Step (1): This is a step according to a general method for producing a Y-based oxide superconducting material. However, since the production target is TmBa 2 Cu 3 O 7-x , Tm oxide, carbonate,
One or more powders of nitrate and chloride are used as one of the raw material powders. As the raw material of Ba and Cu, one or more kinds of oxides, carbonates, nitrates and chlorides thereof can be used.

【0015】上記の原料粉末を、Tm:Ba:Cu=1:2:
3になるように調合して混合粉末とする。なお、調合の
前の各粉末を仮焼してもよく、また、調合した後の混合
粉末を仮焼してもよい。原料粉末として酸化物以外の化
合物粉末を用いる場合は、酸素以外の非金属元素を除去
するために、仮焼は必須である。
The above raw material powder was converted into Tm: Ba: Cu = 1: 2:
It is mixed so as to be 3 to obtain a mixed powder. Each powder before compounding may be calcined, or the mixed powder after compounding may be calcined. When a compound powder other than oxide is used as the raw material powder, calcination is indispensable to remove non-metal elements other than oxygen.

【0016】の工程:上記の混合粉末を銀テープに塗
布するかまたは銀シース(鞘管)に充填し、通常の鍛
造、圧延、線引等の方法で加工して線材とし、さらに、
プレスまたは圧延によってテープ状線材とする。
Process: The above-mentioned mixed powder is applied to a silver tape or filled in a silver sheath (sheath tube) and processed into a wire by a usual method such as forging, rolling and drawing, and further,
The tape-shaped wire is made by pressing or rolling.

【0017】の工程:熱処理の工程であるが、ここで
は雰囲気の酸素分圧と加熱温度、および冷却速度の調整
が重要である。
Step: This is a heat treatment step, but here it is important to adjust the oxygen partial pressure of the atmosphere, the heating temperature, and the cooling rate.

【0018】雰囲気の酸素分圧が 0.003気圧より低い雰
囲気では、TmBa2Cu3O7構造が化学的に不安定であるため
に生成せず、また、酸素分圧が0.03気圧を超えると、C
軸のテープ面に垂直方向への配向度が低くなり、そのた
めに臨界電流密度 (Jc) が低下する。従って、酸素分圧
は 0.003〜0.03気圧の範囲に調整する必要がある。
In an atmosphere having an oxygen partial pressure of less than 0.003 atm, no TmBa 2 Cu 3 O 7 structure is chemically unstable and is not generated. If the oxygen partial pressure exceeds 0.03 atm, C
The degree of orientation of the shaft in the direction perpendicular to the tape surface becomes low, which lowers the critical current density (Jc). Therefore, it is necessary to adjust the oxygen partial pressure within the range of 0.003 to 0.03 atm.

【0019】上記の雰囲気中で、線材を 930℃以上に加
熱する。加熱時間は、線材のサイズにもよるが、およそ
10分程度でよい。930 ℃より低い温度では、TmBa2Cu3O7
が溶融しないため、結晶配向が起こらず、そのため、臨
界電流密度 (Jc) の低い線材しか得られない。一方、加
熱温度が 945℃を超えると、TmBa2Cu3O7が溶融したとき
に固相として生成する Tm2BaCuO5が急激に粒成長し、そ
のために冷却時に液相との反応がスムーズに進行せず、
その結果、TmBa2Cu3O7の形成が阻害されて臨界電流密度
(Jc) の高い線材が得られない。これらの理由から、加
熱温度は 930〜945 ℃の範囲に調整する必要がある。
The wire is heated to 930 ° C. or higher in the above atmosphere. The heating time depends on the size of the wire, but
10 minutes is enough. At temperatures below 930 ° C, TmBa 2 Cu 3 O 7
Does not melt, crystal orientation does not occur, and therefore only wires with a low critical current density (Jc) can be obtained. On the other hand, if the heating temperature exceeds 945 ° C, Tm 2 BaCuO 5 that forms as a solid phase when TmBa 2 Cu 3 O 7 melts will undergo rapid grain growth, which causes a smooth reaction with the liquid phase during cooling. Not progress,
As a result, the formation of TmBa 2 Cu 3 O 7 is hindered and the critical current density is increased.
Wires with high (Jc) cannot be obtained. For these reasons, the heating temperature needs to be adjusted within the range of 930-945 ℃.

【0020】上記のように加熱して部分溶融させた線材
を、少なくとも 900℃までは、毎時0.1〜10℃の冷却速
度で冷却する。この条件は、冷却過程で液相と Tm2BaCu
O5相との反応を行わせてTmBa2Cu3O7の生成とその結晶粒
成長を促し、しかも、前述のTm2BaCuO5 の粒成長を抑え
る条件である。
The wire rod which has been heated and partially melted as described above is cooled at a cooling rate of 0.1 to 10 ° C. per hour up to at least 900 ° C. This condition is that the liquid phase and Tm 2 BaCu
It is a condition that promotes the generation of TmBa 2 Cu 3 O 7 and its crystal grain growth by reacting with the O 5 phase, and further suppresses the grain growth of Tm 2 BaCuO 5 described above.

【0021】冷却速度が毎時 0.1℃未満では、冷却速度
が小さ過ぎて、Tm2BaCuO5 が粒成長し、そのためにTmBa
2Cu3O7の成長が阻害される。一方、毎時10℃を超える早
い冷却を行うと、液相と Tm2BaCuO5相の反応が遅いため
に、TmBa2Cu3O7の生成が少なくなり、臨界電流密度 (J
c) の高い線材が得られない。
When the cooling rate is less than 0.1 ° C./hour, the cooling rate is too small and Tm 2 BaCuO 5 grains grow, and therefore TmBa
2 Cu 3 O 7 growth is inhibited. On the other hand, when cooling is performed faster than 10 ° C per hour, the reaction between the liquid phase and the Tm 2 BaCuO 5 phase is slow, so that the formation of TmBa 2 Cu 3 O 7 is reduced and the critical current density (J
A wire with high c) cannot be obtained.

【0022】上記の諸現象は実質的に 900℃までの冷却
過程で生じるので、少なくとも 900℃までは毎時 0.1〜
10℃の冷却速度としなければならない。以下、このよう
に冷却速度を制御する冷却を「調整冷却」という。
Since the above-mentioned various phenomena substantially occur during the cooling process up to 900 ° C., at least 0.1 to 0.1
The cooling rate should be 10 ° C. Hereinafter, the cooling in which the cooling rate is controlled in this way is referred to as “adjustment cooling”.

【0023】900 ℃より低い温度域での冷却速度は、特
別に制御する必要はなく、急冷でも徐冷でもよい。しか
し、600 ℃より低温で酸素を吸収することによって高温
相 (非超伝導体の正方晶) から、低温相 (超伝導性の斜
方晶) への構造相転移が起きるので、この相転移を促進
するため 400〜500 ℃の温度に10時間程度保持するのが
良い。
The cooling rate in the temperature range lower than 900 ° C. does not need to be specially controlled and may be rapid cooling or slow cooling. However, absorption of oxygen at temperatures lower than 600 ° C causes a structural phase transition from the high-temperature phase (tetragonal crystal of non-superconductor) to the low-temperature phase (superconducting orthorhombic crystal). It is better to keep the temperature at 400-500 ℃ for about 10 hours to accelerate.

【0024】[0024]

【実施例】純度が 99.99%の Tm2O3、BaCO3 および CuO
を金属元素の原子数比 (Tm:Ba:Cu) が1:2:3にな
るように調合し、大気中で 800℃×24時間の仮焼を行
い、粉砕し、再び同じ条件で仮焼した。
EXAMPLE Tm 2 O 3 , BaCO 3 and CuO with 99.99% purity
Was mixed so that the atomic ratio of metal elements (Tm: Ba: Cu) was 1: 2: 3, calcined in the air at 800 ° C for 24 hours, pulverized, and calcined again under the same conditions. did.

【0025】得られた仮焼体を粉砕し、有機溶媒に混
ぜ、銀テープに塗布した。有機溶媒としては、エタノー
ルにPVB(ポリビニルブチラール)を混ぜたものを使
用し、銀テープは、厚さ50μm で幅5mm、長さ10cmのも
のを用いた。
The obtained calcined body was crushed, mixed with an organic solvent and applied to a silver tape. As the organic solvent, a mixture of ethanol and PVB (polyvinyl butyral) was used, and the silver tape had a thickness of 50 μm, a width of 5 mm and a length of 10 cm.

【0026】図1に、熱処理の雰囲気の酸素分圧および
保持温度を変えたときの超伝導テープの臨界電流密度(J
c)の変化を示す。試料はいずれも保持温度 (図1に示す
920℃、930 ℃、940 ℃、945 ℃および 950℃) まで50
℃/hで加熱し、10分間保持したのち、4℃/hで 850℃ま
で調整冷却し、その後室温まで炉冷した。雰囲気はアル
ゴンと酸素の混合ガスとし、その混合比を変えて酸素分
圧を変化させた。
FIG. 1 shows the critical current density (J) of the superconducting tape when the oxygen partial pressure of the heat treatment atmosphere and the holding temperature were changed.
The change of c) is shown. All samples were held at temperature (shown in Figure 1
920 ° C, 930 ° C, 940 ° C, 945 ° C and 950 ° C) up to 50
After heating at ℃ / h and holding for 10 minutes, the temperature was adjusted to 850 ℃ at 4 ℃ / h, and then cooled to room temperature. The atmosphere was a mixed gas of argon and oxygen, and the oxygen partial pressure was changed by changing the mixing ratio.

【0027】なお、Y系超伝導体材料は、TmBa2Cu3O7
限らず、いずれも高温で結晶成長させた場合には半導体
となり、室温まで冷却する過程で酸素を吸収して超伝導
体になることが知られている。この半導体相から超伝導
体相への相転移を完全に行わせるために、すべての試料
を室温まで炉冷した後、酸素中、400 ℃で2日間保持し
た。臨界電流密度の測定は、77Kで4端子法を用いて行
った。
The Y-based superconductor material is not limited to TmBa 2 Cu 3 O 7 , but any of them becomes a semiconductor when crystal is grown at a high temperature and absorbs oxygen in the process of cooling to room temperature to superconduct. It is known to become a body. In order to complete the phase transition from the semiconductor phase to the superconductor phase, all samples were furnace-cooled to room temperature and then kept in oxygen at 400 ° C. for 2 days. The measurement of the critical current density was carried out at 77K using the four-terminal method.

【0028】図1は、上記の測定結果をグラフにしたも
のである。図示のとおり、保持温度が 940℃で、酸素分
圧が0.01気圧のときに、最も高い臨界電流密度が得られ
た。
FIG. 1 is a graph showing the above measurement results. As shown in the figure, the highest critical current density was obtained when the holding temperature was 940 ° C and the oxygen partial pressure was 0.01 atm.

【0029】945℃では、電流密度の最高値は、 940℃
の場合の値より小さくなり、また、そのときの酸素分圧
は0.03気圧であり、 940℃の場合より高くなっている。
At 945 ° C, the maximum current density is 940 ° C
The oxygen partial pressure at that time is 0.03 atm, which is higher than that at 940 ° C.

【0030】保持温度が 950℃の場合は、電流密度のピ
ークは0.03気圧にあるが、その値は15000 A/cm2よりも
小さい。また、保持温度が 940℃より低くなると、ピー
クとなる酸素分圧は 940℃の場合よりも低くなり、電流
密度の値は 940℃の場合より小さくなる。保持温度が 9
20℃では、臨界電流密度が 15000A/cm2以下の線材しか
得られない。
When the holding temperature is 950 ° C., the peak of the current density is 0.03 atm, but the value is smaller than 15000 A / cm 2 . When the holding temperature is lower than 940 ° C, the peak oxygen partial pressure becomes lower than that at 940 ° C, and the current density value becomes smaller than that at 940 ° C. Hold temperature is 9
At 20 ° C, only wires with a critical current density of 15000 A / cm 2 or less can be obtained.

【0031】以上、図1から、酸素分圧が 0.003気圧以
上で0.03気圧以下、保持温度が 930℃以上で 945℃以下
の場合に、臨界電流密度が 15000A/cm2以上の線材が得
られることがわかる。
As described above, from FIG. 1, a wire having a critical current density of 15000 A / cm 2 or more can be obtained when the oxygen partial pressure is 0.003 atm or more and 0.03 atm or less and the holding temperature is 930 ° C or more and 945 ° C or less. I understand.

【0032】図2は、調整冷却を終了する温度の影響を
みた試験結果である。即ち、酸素分圧が0.01気圧の雰囲
気中で 940℃に10分間保持した後、4℃/hの冷却速度で
850℃から920 ℃までの種々の温度まで冷却し、その
後、炉冷した場合の臨界電流密度の変化を示している。
FIG. 2 shows the test results of the influence of the temperature at which the adjustment cooling is completed. That is, after maintaining at 940 ℃ for 10 minutes in an atmosphere with an oxygen partial pressure of 0.01 atmosphere, at a cooling rate of 4 ℃ / h
The change in critical current density is shown when the furnace is cooled after cooling to various temperatures from 850 ℃ to 920 ℃.

【0033】調整冷却を終了する温度が 900℃以下であ
れば、15000 A/cm2以上の高い電流密度が得られてい
る。880 ℃以下であれば電流密度は顕著に増加し、しか
もその値はあまり変化しないことがわかる。
When the temperature at which the controlled cooling is completed is 900 ° C. or lower, a high current density of 15000 A / cm 2 or higher is obtained. It can be seen that if the temperature is 880 ° C or lower, the current density remarkably increases and the value does not change much.

【0034】図3は、調整冷却における冷却速度の影響
を調べた結果を示すものである。即ち、酸素分圧が0.01
気圧の雰囲気中で 940℃に10分間保持した後、 850℃ま
で冷却したときの冷却速度と臨界電流密度の関係を示
す。図示のとおり、その冷却速度が 0.1℃/h〜10℃/hの
範囲にあるとき 15000A/cm2以上の臨界電流密度が得ら
れている。
FIG. 3 shows the results of examining the influence of the cooling rate in the controlled cooling. That is, the oxygen partial pressure is 0.01
The graph below shows the relationship between the cooling current and the critical current density when cooled to 850 ° C after holding it at 940 ° C for 10 minutes in an atmospheric pressure atmosphere. As shown in the drawing, when the cooling rate is in the range of 0.1 ° C / h to 10 ° C / h, the critical current density of 15000 A / cm 2 or more is obtained.

【0035】[0035]

【発明の効果】本発明の製造方法によれば、臨界電流密
度が 15000A/cm2以上で、例えば、ECRプラズマ発生
用のコイル等に実用化が可能なTmBa2Cu3O7-xの組成の超
伝導線材が比較的容易に製造できる。
According to the manufacturing method of the present invention, the composition of TmBa 2 Cu 3 O 7-x having a critical current density of 15000 A / cm 2 or more and being practically applicable to, for example, a coil for ECR plasma generation. The superconducting wire can be manufactured relatively easily.

【図面の簡単な説明】[Brief description of drawings]

【図1】TmBa2Cu3O7-x超伝導線材の部分溶融加熱温度お
よびその雰囲気 (酸素分圧) と臨界電流密度(Jc)との関
係を示す図である。
FIG. 1 is a diagram showing a relationship between a partial melting heating temperature of a TmBa 2 Cu 3 O 7-x superconducting wire and its atmosphere (oxygen partial pressure) and a critical current density (Jc).

【図2】同じく、調整冷却終了温度と臨界電流密度(Jc)
との関係を示す図である。
[Fig. 2] Similarly, adjusted cooling end temperature and critical current density (Jc)
It is a figure which shows the relationship with.

【図3】同じく、調整冷却時の冷却速度と臨界電流密度
(Jc)との関係を示す図である。
[Fig. 3] Similarly, cooling rate and critical current density during controlled cooling
It is a figure which shows the relationship with (Jc).

フロントページの続き (51)Int.Cl.6 識別記号 庁内整理番号 FI 技術表示箇所 H01B 12/04 ZAA Continuation of the front page (51) Int.Cl. 6 Identification code Office reference number FI technical display location H01B 12/04 ZAA

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】Tm、BaおよびCuの酸化物、炭酸塩、硝酸塩
または塩化物の各粉末をTm:Ba:Cu=1:2:3になる
ように調合した混合粉末を銀テープに塗布するかまたは
銀シースに充填し、加工して線材となし、プレスまたは
圧延によってテープ状線材とした後、酸素分圧が 0.003
〜0.03気圧の雰囲気中で一旦 930〜945 ℃の温度まで加
熱した後、少なくとも 900℃までは毎時 0.1〜10℃の冷
却速度で冷却することを特徴とするTmBa2Cu3O7-x超伝導
線材の製造方法。
1. A silver tape is coated with a mixed powder prepared by mixing powders of oxides, carbonates, nitrates or chlorides of Tm, Ba and Cu in a ratio of Tm: Ba: Cu = 1: 2: 3. Or, fill it into a silver sheath, process it into a wire rod, and press or roll it into a tape-shaped wire rod.
TmBa 2 Cu 3 O 7-x superconductivity characterized by heating to a temperature of 930 to 945 ℃ in an atmosphere of ~ 0.03 atm and then cooling at a cooling rate of 0.1 to 10 ℃ per hour up to at least 900 ℃. Manufacturing method of wire.
JP6134175A 1994-06-16 1994-06-16 Method for manufacturing oxide superconducting wire Pending JPH087680A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP6134175A JPH087680A (en) 1994-06-16 1994-06-16 Method for manufacturing oxide superconducting wire

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP6134175A JPH087680A (en) 1994-06-16 1994-06-16 Method for manufacturing oxide superconducting wire

Publications (1)

Publication Number Publication Date
JPH087680A true JPH087680A (en) 1996-01-12

Family

ID=15122202

Family Applications (1)

Application Number Title Priority Date Filing Date
JP6134175A Pending JPH087680A (en) 1994-06-16 1994-06-16 Method for manufacturing oxide superconducting wire

Country Status (1)

Country Link
JP (1) JPH087680A (en)

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