JPH01191501A - Joint method for superconducting waveguide - Google Patents
Joint method for superconducting waveguideInfo
- Publication number
- JPH01191501A JPH01191501A JP63016603A JP1660388A JPH01191501A JP H01191501 A JPH01191501 A JP H01191501A JP 63016603 A JP63016603 A JP 63016603A JP 1660388 A JP1660388 A JP 1660388A JP H01191501 A JPH01191501 A JP H01191501A
- Authority
- JP
- Japan
- Prior art keywords
- superconducting
- joint
- metal
- faces
- waveguide
- 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
Links
- 238000000034 method Methods 0.000 title claims description 8
- 239000002184 metal Substances 0.000 claims abstract description 11
- 229910052751 metal Inorganic materials 0.000 claims abstract description 11
- 238000002844 melting Methods 0.000 claims abstract description 6
- 230000008018 melting Effects 0.000 claims abstract description 6
- 238000009792 diffusion process Methods 0.000 claims abstract description 5
- 238000005304 joining Methods 0.000 claims description 6
- 239000002887 superconductor Substances 0.000 claims description 5
- 238000004519 manufacturing process Methods 0.000 claims description 3
- 239000004020 conductor Substances 0.000 claims description 2
- 238000010438 heat treatment Methods 0.000 claims description 2
- 239000011261 inert gas Substances 0.000 claims description 2
- 239000010409 thin film Substances 0.000 claims description 2
- 230000007547 defect Effects 0.000 abstract description 9
- 239000000463 material Substances 0.000 abstract description 9
- 239000005028 tinplate Substances 0.000 abstract description 5
- KRHYYFGTRYWZRS-UHFFFAOYSA-N Fluorane Chemical compound F KRHYYFGTRYWZRS-UHFFFAOYSA-N 0.000 abstract description 4
- NBIIXXVUZAFLBC-UHFFFAOYSA-N Phosphoric acid Chemical compound OP(O)(O)=O NBIIXXVUZAFLBC-UHFFFAOYSA-N 0.000 abstract description 4
- 239000007788 liquid Substances 0.000 abstract description 4
- 229910052758 niobium Inorganic materials 0.000 abstract description 3
- 239000010955 niobium Substances 0.000 abstract description 3
- GUCVJGMIXFAOAE-UHFFFAOYSA-N niobium atom Chemical compound [Nb] GUCVJGMIXFAOAE-UHFFFAOYSA-N 0.000 abstract description 3
- GRYLNZFGIOXLOG-UHFFFAOYSA-N Nitric acid Chemical compound O[N+]([O-])=O GRYLNZFGIOXLOG-UHFFFAOYSA-N 0.000 abstract description 2
- 229910000147 aluminium phosphate Inorganic materials 0.000 abstract description 2
- 239000000203 mixture Substances 0.000 abstract description 2
- 229910017604 nitric acid Inorganic materials 0.000 abstract description 2
- 238000003466 welding Methods 0.000 description 4
- 238000010894 electron beam technology Methods 0.000 description 3
- 239000001307 helium Substances 0.000 description 3
- 229910052734 helium Inorganic materials 0.000 description 3
- SWQJXJOGLNCZEY-UHFFFAOYSA-N helium atom Chemical compound [He] SWQJXJOGLNCZEY-UHFFFAOYSA-N 0.000 description 3
- 239000011324 bead Substances 0.000 description 2
- 238000005520 cutting process Methods 0.000 description 2
- 230000005684 electric field Effects 0.000 description 2
- RYGMFSIKBFXOCR-UHFFFAOYSA-N Copper Chemical compound [Cu] RYGMFSIKBFXOCR-UHFFFAOYSA-N 0.000 description 1
- 238000005275 alloying Methods 0.000 description 1
- 229910052782 aluminium Inorganic materials 0.000 description 1
- XAGFODPZIPBFFR-UHFFFAOYSA-N aluminium Chemical compound [Al] XAGFODPZIPBFFR-UHFFFAOYSA-N 0.000 description 1
- 238000000137 annealing Methods 0.000 description 1
- 230000005540 biological transmission Effects 0.000 description 1
- 229910052802 copper Inorganic materials 0.000 description 1
- 239000010949 copper Substances 0.000 description 1
- 230000006866 deterioration Effects 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 239000002245 particle Substances 0.000 description 1
Abstract
Description
【発明の詳細な説明】
(産業上の利用分野〕
本発明は、マイクロ波伝送用の導波管、特にディスクロ
ード型進行波加速管や、マイクロ波空胴共娠器等を超伝
導体で形成してマイクロ波のパワーロスを低減させた超
伝導導波管の接続方法に関するものである。[Detailed Description of the Invention] (Industrial Application Field) The present invention provides waveguides for microwave transmission, particularly disk-load type traveling wave accelerator tubes, microwave cavity co-containers, etc., using superconductors. The present invention relates to a method for connecting superconducting waveguides formed to reduce microwave power loss.
(従来の技術〕
ディスクロード型進行波管や空胴共振器はクライストロ
ンのようなマイクロ波増巾器や電子。(Prior technology) Disc-load type traveling wave tubes and cavity resonators are microwave amplifiers such as klystrons and electronics.
陽子等の粒子7Jtl速器として用いられている。これ
らの特殊な立体回路部品は単なる導波管と違い、より多
くのマイクロ波エネルギーが蓄積されるので、銅やアル
ミ等では電力損失を充分小さくすることができないため
、超伝導体を用いたものが提案されている。すなわち超
伝導体の表面抵抗は常伝導体に比較して非常に小さいた
め少ない電力で高い電界が1ワられることが期待されて
いる。It is used as a 7Jtl detector for particles such as protons. Unlike simple waveguides, these special three-dimensional circuit components store more microwave energy, and since it is not possible to reduce power loss sufficiently with copper, aluminum, etc., they are made with superconductors. is proposed. In other words, since the surface resistance of a superconductor is much smaller than that of a normal conductor, it is expected that a high electric field can be generated with a small amount of electric power.
このような導波管として超伝導共振器は例えば第2図に
示すように円筒形の超伝導材料の軸方向中央部を軸に向
って絞り、内側に断面積の小さな貫通孔(7)を設け、
両端の外周縁にボルト孔(8)を周方向に複数個穿設し
たフランジ(5)を設けた空胴単体(1)を切削等によ
り複数個作製し、これら空肩甲体(1)の接合面(9)
であるそれぞれのフランジ端面を互いに密接してボルト
(3)、ナツト(4)で締着し、内側面の当該接合部(
1G)に電子ビーム溶接やTIG溶接を施して固着させ
てこれら空胴単体(1)を複数個連結した形状である。For example, as shown in Figure 2, a superconducting resonator as such a waveguide is made by constricting the axial center of a cylindrical superconducting material and making a through hole (7) with a small cross-sectional area inside. established,
A plurality of hollow bodies (1) each having a flange (5) with a plurality of bolt holes (8) drilled in the circumferential direction on the outer periphery of both ends are prepared by cutting, etc., and these empty shoulder blades (1) are Joint surface (9)
Tighten the respective flange end faces closely together with bolts (3) and nuts (4),
1G) are fixed by electron beam welding or TIG welding, and a plurality of these single cavities (1) are connected.
そしてこのような導波管を液体ヘリウム中に浸漬するか
、液体ヘリウムの通ったパイプを導波管外周面に密着さ
せるなどして超伝導状態を実現、維持している。A superconducting state is achieved and maintained by immersing such a waveguide in liquid helium, or by closely adhering a pipe through which liquid helium passes to the outer circumferential surface of the waveguide.
(発明が解決しようとする課題〕
しかしながら、このような超伝導導波管は実際には期待
されるほどの高電界は得られない。(Problems to be Solved by the Invention) However, such a superconducting waveguide cannot actually obtain as high an electric field as expected.
この原因は主として導波管内壁面の表面欠陥によるもの
でおる。これは超伝導体であってもマイクロ波において
はある程度の抵抗が存在するため発熱があるが、通常こ
の熱は導波管仝休を超伝導状態に維持するために浸して
いる液体ヘリウムによって除去される。ところが表面欠
陥があるとその部分で表面抵抗が上昇し、局部的に多聞
の熱が発生するためそこが起点となって超伝導状態が破
壊されてしまう。このような表面欠陥は特に接合部分に
生じ易い。即ち、例えばニオブ単体で形成された超伝導
導波管の接合には通常電子ビーム)容接が用いられる。This is mainly due to surface defects on the inner wall of the waveguide. Even if the waveguide is a superconductor, it generates heat due to the presence of some resistance in the microwave, but this heat is usually removed by liquid helium, which is immersed in the waveguide to maintain it in a superconducting state. be done. However, if there is a surface defect, the surface resistance increases in that area, and a large amount of heat is generated locally, which becomes the starting point for the superconducting state to be destroyed. Such surface defects are particularly likely to occur at bonded parts. That is, for example, for joining superconducting waveguides made of simple niobium, electron beam (electron beam) welding is usually used.
ところがこの方法では接合部に溶接ビードが生じたり、
接合部付近に熱による歪を生じたりするため溶接後ビー
トを01摩したり、アニールして熱歪を取ったりしなけ
ればならず、欠陥のない均質な表面を得ることが困難で
あった。However, with this method, weld beads may occur at the joint,
Since thermal distortion occurs near the joint, it is necessary to remove the thermal distortion by grinding or annealing the bead after welding, and it is difficult to obtain a uniform surface without defects.
このように超伝導導波管の接合方法はその実用化に対す
る一つの降害であった。In this way, the method of joining superconducting waveguides has been a hindrance to its practical use.
(課題をif/I’決するための手段〕本発明はこれに
鑑み種々検討の結果、欠陥の少ない超伝導導波管の接合
方法を開発したものである。即ら超伝導体で形成された
空胴単体または内面を超伝導薄膜で形成された空胴単体
を複数個接合して超伝導導波管を製造する方法において
、当該接合面間に上記超伝導材料より融点の低い金属を
挿入して挟圧し、その後真空または不活性ガス雰囲気中
にてh0熱することにより空胴単体を互いに拡散接合す
ることを特徴とするものである。(Means for deciding if/I') In view of this, the present invention is the result of various studies and has developed a method for joining superconducting waveguides with fewer defects. In a method of manufacturing a superconducting waveguide by joining a single cavity or a plurality of single cavities whose inner surfaces are formed of a superconducting thin film, a metal having a melting point lower than that of the superconducting material is inserted between the joining surfaces. This method is characterized in that the single cavities are diffusion bonded to each other by being compressed and then heated at h0 in a vacuum or an inert gas atmosphere.
(作 用)
このように接合面間に超伝導材料より融点の低い金属を
挿入して挟圧し、加熱するのは当該金属(以下インサー
ト金属という)と超伝導材料の接触部で両者の原子を相
互に拡散させて合金化させることにより接合させる拡散
接合法を用いれば単に超伝導材料同志で拡散接合をする
場合よりも低温で短時間に接合できしかも接合部表面は
滑らかに連続したものとなり表面欠陥もなくなる利点を
有するからである。(Function) In this way, a metal with a melting point lower than that of the superconducting material is inserted between the bonding surfaces, compressed, and heated to cause the atoms of both to be heated at the contact area between the metal (hereinafter referred to as the insert metal) and the superconducting material. Using the diffusion bonding method, which involves bonding by mutually diffusing and alloying, it is possible to bond at a lower temperature and in a shorter time than simply diffusion bonding two superconducting materials, and the surface of the bonded part is smooth and continuous. This is because it has the advantage of eliminating defects.
また加熱する温度はインサート金属の融点近傍またはそ
れ以上の温度でかつ当該超伝導材料の融点未満の温度で
加熱するのがよい。The heating temperature is preferably near or above the melting point of the insert metal and below the melting point of the superconducting material.
(実施例〕 次に本発明の実施例について説明する。(Example〕 Next, examples of the present invention will be described.
第1図に示すようにニオブ製の2個の空胴単体(1)の
それぞれ一方の7ランジ端面同士を対向させた接合面間
にインサート金属として錫薄板(2)を挟みボルト(3
)、ナツト(4)で当該7ランジ(5)同士を締着して
接合面間の錫薄板(2)を挟圧し、その後この空胴単体
2個を一体化した連結体(6)を真空中にて600°C
で3時間加熱した。しかる後フッ酸、硝酸及びリン酸の
1 :1 :1の混合液で表面を化学研摩して仕上げた
。そしてこのような連結体の超伝導状態での特性を調べ
たが内面をすべて切削により仕上げた接合部のない上記
連結体形状のものと比較して同等の特性を有していた。As shown in Fig. 1, a thin tin plate (2) is inserted as an insert metal between the joint surfaces of two niobium hollow bodies (1), each with one of the seven flange end faces facing each other.
), the seven flanges (5) are tightened with nuts (4) to compress the thin tin plate (2) between the joint surfaces, and then the connecting body (6) that integrates the two single cavities is vacuumed. 600°C inside
It was heated for 3 hours. Thereafter, the surface was chemically polished using a 1:1:1 mixture of hydrofluoric acid, nitric acid, and phosphoric acid. The characteristics of such a connected body in a superconducting state were investigated, and it was found that it had the same characteristics as that of the above-mentioned connected body having no joints and whose inner surface was completely finished by cutting.
このように本発明によれば比較的低い温度で空胴単体の
接合が可能であるため母材の変質や欠陥が少なく、高品
質の超伝導導波管、特に超伝導空胴共娠器の生産性を向
上することかできる等工業上顕著な効果を秦するもので
ある。As described above, according to the present invention, it is possible to bond single cavities at relatively low temperatures, so there is little deterioration or defects in the base material, and it is possible to produce high-quality superconducting waveguides, especially superconducting cavity co-containers. It has significant industrial effects such as improving productivity.
第1図は本発明の一実施例である空111iil中体の
接合状態を示す断面図、第2図は従来例を示す一部断面
の側面図である。
1・・・・・・・・空胴単体
2・・・・・・・・錫薄板
3・・・・・・・・ボルト
4・・・・・・・・ナツト
5・・・・・・・・フランジ
6・・・・・・・・連結体
7・・・・・・・・貫通孔
8・・・・・・・・ボルト孔
9・・・・・・・・接合面
10・・・・・・・・接合部
第1図FIG. 1 is a sectional view showing a joined state of an empty 111iil core according to an embodiment of the present invention, and FIG. 2 is a partially sectional side view showing a conventional example. 1... Single cavity 2... Thin tin plate 3... Bolt 4... Nut 5... ...Flange 6...Connection body 7...Through hole 8...Bolt hole 9...Joint surface 10...・・・・・・Joint part diagram 1
Claims (1)
導薄膜で形成された空胴単体を複数個接合して超伝導導
波管を製造する方法において、当該接合面間に上記超伝
導材料より融点の低い金属を挿入して挟圧し、その後真
空または不活性ガス雰囲気中にて加熱することにより空
胴単体を互いに拡散接合することを特徴とする超伝導導
波管の製造方法。(1) In a method of manufacturing a superconducting waveguide by joining a single cavity formed of a superconductor or a plurality of single cavities whose inner surfaces are formed of a superconducting thin film, the above-mentioned A method for manufacturing a superconducting waveguide, which comprises inserting and compressing a metal having a melting point lower than that of a conductive material, and then heating the cavities in a vacuum or an inert gas atmosphere to diffusion bond the cavities to each other.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP63016603A JPH01191501A (en) | 1988-01-27 | 1988-01-27 | Joint method for superconducting waveguide |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP63016603A JPH01191501A (en) | 1988-01-27 | 1988-01-27 | Joint method for superconducting waveguide |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH01191501A true JPH01191501A (en) | 1989-08-01 |
Family
ID=11920875
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP63016603A Pending JPH01191501A (en) | 1988-01-27 | 1988-01-27 | Joint method for superconducting waveguide |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH01191501A (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
DE10028352B4 (en) * | 2000-06-08 | 2006-06-01 | Siemens Ag | Method and circuit for enabling the ignitability of at least two separately ignitable ignition stages in an occupant protection system |
CN102981054A (en) * | 2012-11-22 | 2013-03-20 | 宁夏东方钽业股份有限公司 | Processing method of high-purity niobium material residual resistivity test samples |
-
1988
- 1988-01-27 JP JP63016603A patent/JPH01191501A/en active Pending
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
DE10028352B4 (en) * | 2000-06-08 | 2006-06-01 | Siemens Ag | Method and circuit for enabling the ignitability of at least two separately ignitable ignition stages in an occupant protection system |
CN102981054A (en) * | 2012-11-22 | 2013-03-20 | 宁夏东方钽业股份有限公司 | Processing method of high-purity niobium material residual resistivity test samples |
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