JPS5828684B2 - NBYSN1-XALX - Google Patents
NBYSN1-XALXInfo
- Publication number
- JPS5828684B2 JPS5828684B2 JP49034606A JP3460674A JPS5828684B2 JP S5828684 B2 JPS5828684 B2 JP S5828684B2 JP 49034606 A JP49034606 A JP 49034606A JP 3460674 A JP3460674 A JP 3460674A JP S5828684 B2 JPS5828684 B2 JP S5828684B2
- Authority
- JP
- Japan
- Prior art keywords
- atoms
- wire
- xalx
- magnetic field
- critical
- 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.)
- Expired
Links
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
- Superconductor Devices And Manufacturing Methods Thereof (AREA)
- Superconductors And Manufacturing Methods Therefor (AREA)
Description
【発明の詳細な説明】
本発明はNby Sn 1−xkllx 金属間化合物
からなる超電導体の製造法に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method for producing a superconductor comprising a Nby Sn 1-xkllx intermetallic compound.
現在使用されている金属間化合物超電導マグネット材料
は、Nb3Sn 、 V3Gaの2種であり、これらの
材料は気相反応法または拡散による固体反応によって製
造されている。There are two types of intermetallic superconducting magnet materials currently in use: Nb3Sn and V3Ga, and these materials are manufactured by a gas phase reaction method or a solid state reaction by diffusion.
上記の如き公知の超電導体の特性は下記の表1に列記す
る通りである。The properties of the above-mentioned known superconductors are listed in Table 1 below.
上記のような特性を有する公知のNb3Sn j■3G
aは、その臨界磁場の値が220KGであるために、こ
れら公知材料を用いて製造した超電導マグネットの発生
し得る磁場は、4.2°にで最高150KGである。Known Nb3Sn j■3G having the above characteristics
Since the critical magnetic field value of a is 220 KG, the maximum magnetic field that can be generated by superconducting magnets manufactured using these known materials is 150 KG at 4.2°.
しかるに、より高い200KG程度の磁場を発生させる
ためには、上記の如き公知の超電導体線材では実現不可
能であり、より高い臨界磁場(少なくとも200KG以
上)を発生し得る超電導体材料の開発が望1れている。However, in order to generate a higher magnetic field of about 200 KG, it is impossible to achieve this with the known superconductor wires as mentioned above, and it is desirable to develop a superconductor material that can generate a higher critical magnetic field (at least 200 KG or more). 1 has been written.
一方に釦いて近年18°に以上の臨界温度を有する超電
導体材料が幾種類か開発され、これらのうち若干のもの
は前述したような所望の高い臨界磁場を有している。On the other hand, in recent years several types of superconductor materials with critical temperatures above 18 DEG have been developed, some of which have the desired high critical magnetic fields as mentioned above.
これらの例としてはNb5(Alo、75 GeO
,2s)”4]OKGおよびNb5A7: 300 K
Gを挙ザることができる。Examples of these include Nb5(Alo, 75GeO
,2s)”4]OKG and Nb5A7: 300 K
I can list G.
しかし乍ら、これらの材料は、1500°C以上の高温
処理によってのみ製造しうるため、実用超電導マグネッ
ト材料に要求される他の重要な要素である、高い臨界電
流音度を具備し得ない。However, since these materials can only be manufactured by high-temperature treatment at 1500° C. or higher, they cannot have a high critical current sonic intensity, which is another important element required for practical superconducting magnet materials.
このような理由によって上記組成の超電導材材料は実用
化し得ない現状である。For these reasons, the superconducting material having the above composition cannot be put to practical use at present.
本発明の方法は、前記の如き公知材料の諸欠点を克服し
かつ改良した超電導体の製造法に関するものであり、本
発明の要旨とするところは前述の如く、銅、錫およびア
ルミニウムからなる三元合金Cu1−y’(5n1−x
”AI!x”) y’ (y’−0,05〜30原子係
、x”−0,1〜60原子係〕と金属ニオブ塗た0、0
5〜10原子咎の範囲内でチタニウム、ハフニウムまた
はタンタルの1種もしくは2種以上を含有するニオブ基
合金とを組合せて一体とし、これを圧延、伸線等により
テープまたは線材に加工し、ついで450°〜1000
°Gの温度で10分間〜1000時間焼鈍してβ−W型
NbySn1xAlx (y = 3〜4、X−1〜3
0原子φ)の金属間化合物を形成することを特徴とする
超電導体の製造法である。The method of the present invention relates to a method for producing a superconductor which overcomes the drawbacks of the known materials as described above and is improved. Original alloy Cu1-y'(5n1-x
``AI!
It is combined with a niobium-based alloy containing one or more of titanium, hafnium or tantalum in the range of 5 to 10 atoms, processed into a tape or wire rod by rolling, wire drawing, etc., and then 450°~1000
Annealed at a temperature of °G for 10 minutes to 1000 hours to obtain β-W type NbySn1xAlx (y = 3~4, X-1~3
This is a method for producing a superconductor characterized by forming an intermetallic compound with 0 atoms φ).
本発明の方法により、製造された線材は、臨界温度にち
−いては大きな変化を示さないにも拘らず、臨界磁場に
ついては、前記化合物にお−いてX30原子咎の場合、
250KG以上、x=5原子咎の場合、300KGを得
ることができる。Although the wire manufactured by the method of the present invention does not show a large change in the critical temperature, the critical magnetic field is
250KG or more, if x=5 atomic charges, 300KG can be obtained.
しかもこの線材は、比較的低温度での拡散法で製造され
るために、Nb3Sn と同程度の高い臨界電流缶度
が、低磁場より高磁場に亙って保持されていることが確
認できた。Moreover, because this wire is manufactured using a diffusion method at a relatively low temperature, it was confirmed that the same high critical current capability as Nb3Sn was maintained in a high magnetic field rather than a low magnetic field. .
本発明方法は上記以外にパルスマグネットや交流用の多
芯線の製造にも有効である特徴を有する。In addition to the above, the method of the present invention has a feature that it is also effective in manufacturing pulsed magnets and multicore wires for alternating current.
従って、本発明の方法で製造された超電導体線材は、現
在のNb5SntたばV3Ga線材では達成し得ない2
00 KGKも達する超高磁場を発生しうる超電導マグ
ネット材料として用いることができる。Therefore, the superconductor wire produced by the method of the present invention has a
It can be used as a superconducting magnet material that can generate ultra-high magnetic fields reaching as high as 0.00 KGK.
なむ、本発明にお−いては圧延、伸線加工後に、Sn、
1−x’Alx’ (x’= 0.1〜60原子%)浴
に浸漬してもよく、その場合の数例を後記実施例に示す
。In the present invention, after rolling and wire drawing, Sn,
It may be immersed in a 1-x'Alx'(x' = 0.1 to 60 atomic %) bath, and several examples of such cases will be shown in Examples below.
本発明方法による具体的実施例を以下に詳述するが、本
発明をこれら実施例に限定するものではない。Specific examples of the method of the present invention will be described in detail below, but the present invention is not limited to these examples.
実施例 1
直径12mmのCu1−y’(5n1−x”Ad?)y
’ (y’−18原子係、グー5原子咎)合金棒に、長
手方向に貫通する3個の内径約41n7Itの孔を設け
、夫々の孔に直径4mmのニオブ棒を挿入した後、この
組合せ体を外匣が0.25mmになる1で伸線加工し、
これを真空中、750℃で300時間の熱処理を行って
、基材たるニオブ棒と組合せたCu −8n −A1合
金との境界部附近にβ−前型の金属間化合物NbySn
1−XAlX(y−3〜4、X−二5原子係)を形成さ
せた。Example 1 Cu1-y'(5n1-x"Ad?)y with a diameter of 12 mm
'(y' - 18 atoms, 5 atoms of goo) Three longitudinally penetrating holes with an inner diameter of about 41n7It are provided in the alloy rod, and after inserting a niobium rod with a diameter of 4mm into each hole, this combination is made. The body is wire-drawn using 1 with an outer box of 0.25 mm.
This was heat-treated in vacuum at 750°C for 300 hours, and a β-preform intermetallic compound NbySn was formed near the boundary between the base material niobium rod and the combined Cu-8n-A1 alloy.
1-XAlX (y-3 to 4, X-25 atoms) was formed.
このように処理した線材の超電導特性はTc=] 7°
KHc2−300KGであった。The superconducting property of the wire treated in this way is Tc= ] 7°
It was KHc2-300KG.
実施例 2
直径127rtr/lのCu1−y/(Sn、−xl/
Alx”) y’[: y’−10原子係、グー5原子
咎]合金に、長手方向に貫通する3個の内径約4mmの
孔を設け、夫々の孔に直径4mmのニオブ棒を挿入した
後、この組合せ体を外径が0.25mmKなる1で伸線
加工して得られた線材を、500℃の溶融5n1−X′
AlX′(x′−5原子%)浴に浸漬し、該浸漬処理後
不活性ガス中、750°Gの温度で150時間熱処理す
ることによって、基材たるニオブと組合せた前記三元合
金との境界附近にβ−前型のNbySnl−xAlx〔
y−3〜4、X=5原子饅〕金属間化合物を形成させた
。Example 2 Cu1-y/(Sn,-xl/
Three holes with an inner diameter of about 4 mm passing through the longitudinal direction were formed in the alloy, and a niobium rod with a diameter of 4 mm was inserted into each hole. After that, the wire rod obtained by wire drawing the assembled body with 1 having an outer diameter of 0.25 mm was heated to molten 5n1-X' at 500°C.
By immersing in an AlX'(x'-5 at. Near the boundary, β-preform NbySnl-xAlx [
y-3 to 4, X=5 atoms] An intermetallic compound was formed.
得られた線材の超電導特性はTc−175°に、Hc2
=300KGであった。The superconducting properties of the obtained wire were Tc-175°, Hc2
=300KG.
実施例 3
直径12mrnのCu1−y’(Sn、 −yeAlh
l) y’(y’=10原子係、原子−5原子φ)合金
棒に、長手方向に貫通する内径約7關の孔を設け、その
孔に直径7間のニオブ棒を挿入し、外径がO,] my
nになる1で伸線して得られる線材を7本編みにして4
20°Cの溶融5n1−X/Alx′(X′=5原子%
)浴に浸漬し、これをアルゴンガス等の不活性ガス中、
750℃の温度で150時間熱処理することによって基
材たるニオブと組合せた前記三元合金との境界部附近に
β−前型のNbySnl−XAlX(y−3〜4、x
= 5原子係)金属間化合物を形成させた。Example 3 Cu1-y'(Sn, -yeAlh
l) In a y'(y' = 10 atoms, atoms - 5 atoms φ) alloy rod, a hole with an inner diameter of approximately 7 mm is provided that penetrates in the longitudinal direction, a niobium rod with a diameter of 7 mm is inserted into the hole, and the outer diameter is The diameter is O,] my
The wire rod obtained by drawing with 1 that becomes n is woven into 7 strands and
Melting 5n1-X/Alx' at 20°C (X'=5 at.%
) in an inert gas such as argon gas,
By heat treatment at a temperature of 750° C. for 150 hours, β-preform NbySnl-XAlX (y-3 to 4, x
= 5 atoms) An intermetallic compound was formed.
このように処理した線材の超電導特性はTc−17°K
、 Hc2−300 KGであった。The superconducting property of the wire treated in this way is Tc-17°K.
, Hc2-300 KG.
実施例 4
直径12關のCu4−y’(Sn1−4hlx”) y
’(y’−10原子咎、l=原子饅)合金棒に、長手方
向に貫通する内径約7mmの孔を設け、その孔に直径7
間のニオブ棒を挿入し、外径が0.1 mmになる1で
伸線して得られる線材を3本編みにして500℃の溶融
5n1−xklx’ (x′−5原子饅)浴に浸漬し、
これを内径約0.25 mmの銅パイプに挿入してダイ
スを通して絞りを加えまたは/更に伸線加工した後真空
中、700°Cの温度で200時間熱処理することによ
って基材たるニオブと組合せた前記三元合金との境界部
附近にβ−前型のNbySnlXAlX(y−3〜4、
X=5原子%)金属間化合物を形成させた。Example 4 Cu4-y'(Sn1-4hlx") y with a diameter of 12
'(y'-10 atomic force, l=atomic force) A hole with an inner diameter of about 7 mm passing through the longitudinal direction is provided in the alloy rod, and the hole has a diameter of 7 mm.
Insert a niobium rod between the wires and draw the wire to an outer diameter of 0.1 mm.The resulting wire is braided into three strands and placed in a 500°C molten 5n1-xklx'(x'-5 atomic steam) bath. Soak,
This was inserted into a copper pipe with an inner diameter of approximately 0.25 mm, passed through a die and subjected to drawing and/or wire drawing, and then heat treated in a vacuum at a temperature of 700°C for 200 hours to combine it with the base material of niobium. β-former type NbySnlXAlX (y-3 to 4,
(X=5 atomic %) an intermetallic compound was formed.
このように処理した線材の超電導特性はTc=17°に
、Hc2−300KGであった。The superconducting properties of the wire treated in this way were Tc=17° and Hc2-300KG.
実施例 5〜20
実施例1〜4の何れかの方法で、各変数を種々峻臀に変
化させた例を表2に示す。Examples 5 to 20 Table 2 shows examples in which each variable was varied sharply using any of the methods of Examples 1 to 4.
これらの結果から得られた超電導特性を第1図むよび第
2図に示す。The superconducting properties obtained from these results are shown in Figures 1 and 2.
これらの結果から明らかな如く、方法むよび変数を変化
させた場合には、臨界温度と臨界磁場は最終的に形成さ
れるβ−W型NbySn1−x Alx(y−3〜4
、x=o〜50原子係)の組成のXのみに依存し、方法
や変数には殆んど依存しないことが判明した。As is clear from these results, when the method and variables are changed, the critical temperature and critical magnetic field are
, x=o to 50 atoms), and was found to be almost independent of methods and variables.
NbySn ] −xAlx のXの変化による臨界
温度と臨界磁場を表3に示す。Table 3 shows the critical temperature and critical magnetic field depending on the change in X of NbySn]-xAlx.
第1図はβ−W型NbySn 1−xAlx (y =
3〜4、X=O〜1)の臨界温度の組成依存性を示す
グラフ、第2図は同じくβ−W型NbySn1−xAl
x(y=3〜4、X=O〜1)の臨界磁場の組成依存比
をなすグラフである。Figure 1 shows β-W type NbySn 1-xAlx (y =
3-4, a graph showing the composition dependence of the critical temperature of
It is a graph showing the composition dependence ratio of the critical magnetic field of x (y=3 to 4, X=O to 1).
Claims (1)
−y’(5n1−yeAlbt’) y’(y’= 0
.05〜30原子饅、z= 0. ]〜60原子咎〕と
金属ニオブまたは0,05〜10原子φの範囲内でチタ
ニウム。 ジルコニウム、ハフニウム筐たはタンタルの1種もしく
ば2種以上を含有するニオブ基台金とを組合せて一体と
し、これを圧延、伸線等によりテープまたは線材に加工
し、ついで450°〜1000℃の温度で10分間〜1
000時間焼鈍してβW型NbySn1−xMx (y
= 3〜4、X−1〜30原子%)の金属間化合物を
形成することを特徴とする超電導体の製造法。[Claims] 1. Ternary alloy Cu1 consisting of copper, tin button and aluminum
-y'(5n1-yeAlbt') y'(y'= 0
.. 05-30 atoms, z=0. ] to 60 atoms φ] and metallic niobium or titanium within the range of 0.05 to 10 atoms φ. A niobium base metal containing one or more of zirconium, hafnium, or tantalum is combined into an integral body, processed into a tape or wire by rolling, wire drawing, etc., and then heated at 450° to 1000°C. 10 minutes at a temperature of ~1
After annealing for 000 hours, βW type NbySn1-xMx (y
= 3 to 4, X-1 to 30 atomic %).
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP49034606A JPS5828684B2 (en) | 1974-03-29 | 1974-03-29 | NBYSN1-XALX |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP49034606A JPS5828684B2 (en) | 1974-03-29 | 1974-03-29 | NBYSN1-XALX |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS50128993A JPS50128993A (en) | 1975-10-11 |
| JPS5828684B2 true JPS5828684B2 (en) | 1983-06-17 |
Family
ID=12419006
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP49034606A Expired JPS5828684B2 (en) | 1974-03-29 | 1974-03-29 | NBYSN1-XALX |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5828684B2 (en) |
-
1974
- 1974-03-29 JP JP49034606A patent/JPS5828684B2/en not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS50128993A (en) | 1975-10-11 |
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