JPH0821477B2 - High frequency acceleration cavity manufacturing method - Google Patents
High frequency acceleration cavity manufacturing methodInfo
- Publication number
- JPH0821477B2 JPH0821477B2 JP2027794A JP2779490A JPH0821477B2 JP H0821477 B2 JPH0821477 B2 JP H0821477B2 JP 2027794 A JP2027794 A JP 2027794A JP 2779490 A JP2779490 A JP 2779490A JP H0821477 B2 JPH0821477 B2 JP H0821477B2
- Authority
- JP
- Japan
- Prior art keywords
- cavity
- high frequency
- joint
- frequency acceleration
- bonding
- 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 - Lifetime
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- Control Of Motors That Do Not Use Commutators (AREA)
Description
【発明の詳細な説明】 〔発明の目的〕 (産業上の利用分野) 本発明は、電子シンクロトロンや電子蓄積リング等の
加速器に使用される高周波加速空胴の製造方法に関す
る。DETAILED DESCRIPTION OF THE INVENTION [Industrial Application] The present invention relates to a method of manufacturing a high-frequency acceleration cavity used for an accelerator such as an electron synchrotron and an electron storage ring.
(従来の技術) 加速器は、電子、陽子、イオンなどの荷電粒子ビーム
を数百万電子ボルト(数MeV)から数百億電子ボルト
(数十GeV)程度の高エネルギ状態に加速するためのも
のであ、この加速器の例として、電子シンクロトロンや
電子蓄積リング等がある。(Prior Art) An accelerator is for accelerating a charged particle beam of electrons, protons, ions, etc. to a high energy state of several million electron volts (several MeV) to several tens of billions of electron volts (several tens of GeV). However, examples of this accelerator include an electron synchrotron and an electron storage ring.
高周波加速空胴は、加速器において荷電粒子にエネル
ギを与え、加速するための装置である。高周波加速空胴
内では、荷電粒子の速度に同期した数十メガヘルツから
数ギガヘルツ程度の高周波の高電界が共振により発生
し、荷電粒子はこの高周波電界により加速される。A high frequency acceleration cavity is a device for giving energy to and accelerating charged particles in an accelerator. In the high frequency acceleration cavity, a high electric field of high frequency of several tens of megahertz to several gigahertz synchronized with the velocity of charged particles is generated by resonance, and the charged particles are accelerated by this high frequency electric field.
高周波加速空胴には、種々の形式のものがあるが、第
5図は従来の多連結高周波加速空胴の一例で、設置スペ
ースを少なくするために複数の空胴(1)をつないだも
ので、3連の場合を示した。空胴(1)は外筒(2)、
端板(3)、隔壁(4)を接合部(5a)で接合して形成
される。外筒(2)、端板(3)、隔壁(4)は電気伝
導度、熱伝導度の優れた、例えば無酸素銅で製作されて
いる。端板(3)及び隔壁(4)には荷電粒子ビームが
通過するビームポート(6)及び円孔(7)が設けられ
ている。There are various types of high-frequency accelerating cavities, but Fig. 5 shows an example of a conventional multi-connection high-frequency accelerating cavity, in which multiple cavities (1) are connected to reduce the installation space. Then, the case of three stations is shown. The cavity (1) is the outer cylinder (2),
It is formed by joining the end plate (3) and the partition wall (4) at the joining portion (5a). The outer cylinder (2), the end plate (3), and the partition wall (4) are made of, for example, oxygen-free copper having excellent electric conductivity and thermal conductivity. The end plate (3) and the partition (4) are provided with a beam port (6) and a circular hole (7) through which the charged particle beam passes.
高周波電力は、アンテナ(8)から入力され、空胴
(1)の共振周波数は、チューナ(9)で微調整され
る。空胴(1)はフランジ(10)を介して加速器に接続
され、排気ポート(11)から真空に引かれ高真空に保持
される。The high frequency power is input from the antenna (8), and the resonance frequency of the cavity (1) is finely adjusted by the tuner (9). The cavity (1) is connected to the accelerator through the flange (10), and a vacuum is drawn from the exhaust port (11) to maintain a high vacuum.
空胴(1)の内面は、表皮硬化により、金属表面の数
マイクロメータと言う非常に薄い層を流れる高周波電流
をスムーズに流すため、表面粗さを数マイクロメータ以
下に仕上げるのと、表面層の加工硬化による電気抵抗値
の上昇を下げるためにも、最後の仕上げ加工は微量にす
る。Due to the skin hardening, the inner surface of the cavity (1) smoothly passes a high-frequency current flowing through a very thin layer of a metal surface, which is called a few micrometers, so that the surface roughness is finished to a few micrometers or less. In order to reduce the increase in the electric resistance value due to work hardening, the final finishing process should be done in a small amount.
接合部(5a)では、空胴(1)の強度を保ち、真空を
封じ、高周波電流をスムーズに流す必要がある。従来
は、例えば接合部の拡大図の第6図や第7図に示すごと
く電子ビーム溶接部(5b)や真空ろう付溶接部(5c)で
溶接し、目視して接合を確認していた。電子ビーム溶接
においては、空胴外側からの電子ビーム照射により、外
筒(2)の内面近くまで届く溶接層(2a)を形成し接合
する。ろう付溶接部(5c)では、800℃程度の高温で溶
融する銀ろうを接合部に置きろう溝(2b)などを設けて
はさみ込み空胴全体を800℃程度まで昇温し接合する。
これも目視により接合を確認していた。At the joint portion (5a), it is necessary to maintain the strength of the cavity (1), seal the vacuum, and allow a high-frequency current to flow smoothly. Conventionally, for example, as shown in FIGS. 6 and 7 of the enlarged view of the joint, welding is performed at the electron beam welded portion (5b) and the vacuum brazing welded portion (5c), and the joint is visually confirmed. In electron beam welding, the welding layer (2a) that reaches near the inner surface of the outer cylinder (2) is formed and joined by electron beam irradiation from the outside of the cavity. In the brazing welding part (5c), a silver brazing material that melts at a high temperature of about 800 ° C is placed in the joining part, and a brazing groove (2b) or the like is provided.
This also confirmed the joint visually.
また実願昭47−021411号(実開昭48−096400号)の願
書に添付した明細書及び図面の内容を撮影したマイクロ
フィルムによれば、高周波加速空胴を分割して製作し、
拡散接合にて接合する高周波加速空胴の製造方法が記載
されている。In addition, according to the microfilm photographed of the contents of the specification and drawings attached to the application of Japanese Utility Model Application No. 47-021411 (Japanese Utility Model Application No. 48-096400), the high-frequency accelerating cavity is divided and manufactured.
A method of manufacturing a high frequency accelerating cavity joined by diffusion joining is described.
(発明が解決しようとする課題) 高周波加速空胴では、極力、空胴内表面の電気抵抗を
小さくして、高周波電流による発熱を減少させ、電力効
率を高くすることが望まれる。(Problems to be Solved by the Invention) In a high frequency accelerating cavity, it is desired to reduce the electric resistance of the inner surface of the cavity as much as possible to reduce heat generation due to a high frequency current and improve power efficiency.
電気伝導の優れた材料を用い無い表面を滑らかに仕上
げるのは、空胴の電力効率を高くするためである。従っ
て接合部においても高周波電流に対し、十分に低い電気
抵抗を有することが望ましい。The smooth finish of the surface without using a material having excellent electrical conductivity is to increase the power efficiency of the cavity. Therefore, it is desirable that the junction also has a sufficiently low electric resistance with respect to a high frequency current.
上述の電子ビーム溶接においては、空胴外側から電子
ビーム照射により、空胴内面近くまで届くような溶融層
(2a)を形成して接合するため、電子ビームによる入射
エネルギが大きく、そのため溶融した金属が固相化し、
常温に復帰したときに変形が起きる欠点と、表面近くま
で一様に溶融層を作ることが困難であるという欠点があ
った。また一方の銀ろう付けにおいても接合部に銀ろう
材をはさみ込み真空中あるいは雰囲気中で800℃程度の
高温にあげ接合しているが、この場合には空胴使用の
際、銀ろう材が真空中に使用されるため放出ガスとして
一部放出される欠陥があった。In the above-mentioned electron beam welding, since the molten layer (2a) that reaches the inner surface of the cavity is formed by the electron beam irradiation from the outer side of the cavity to join, the incident energy due to the electron beam is large, and therefore the molten metal Solidified,
There are drawbacks that deformation occurs when the temperature returns to room temperature, and it is difficult to form a molten layer uniformly near the surface. Also, in silver brazing on one side, a silver brazing filler metal is sandwiched between the joints to raise the temperature to a high temperature of about 800 ° C in a vacuum or atmosphere, but in this case, the silver brazing filler metal is used when the cavity is used. Since it was used in a vacuum, there was a defect that it was partly released as a release gas.
また最後に述べた拡散接合では接合時に接合部が少な
くとも内部に向けて露出しているので、液相拡散接合の
際に空胴内に液層が流出して接合が不完全になる欠点が
あった。In addition, in the last-mentioned diffusion bonding, since the bonding part is exposed at least toward the inside during bonding, there is the drawback that the liquid layer flows out into the cavity during liquid phase diffusion bonding and the bonding becomes incomplete. It was
本発明は、これらの欠点を考えての対策として、残留
応力をなくし、変形を防止することと、拡散接合の中で
も接合時に接合部が溶融する液相拡散接合においても液
相が流出すること無く、接合部を導電性の高い放出ガス
の少ない合金層として形成させる高周波加速空胴の製造
方法を提供することを目的とする。The present invention, as a countermeasure against these drawbacks, eliminates residual stress and prevents deformation, and the liquid phase does not flow out even in the liquid phase diffusion bonding in which the bonding portion melts during the bonding. It is an object of the present invention to provide a method of manufacturing a high frequency acceleration cavity in which a joint portion is formed as an alloy layer having high conductivity and less emitted gas.
(課題を解決するための手段) 上記目的を達成するために、本発明においては、空胴
を分割して製作し、接合部をコ字形又はI字形に係合
し、接合部の底部に空胴材料に比べて融点が等しいか又
はそれよりも低い材料の金属箔をはさみ、拡散接合にて
接合する。(Means for Solving the Problem) In order to achieve the above object, in the present invention, a cavity is divided and manufactured, a joint is engaged in a U shape or an I shape, and a cavity is formed at the bottom of the joint. A metal foil made of a material having a melting point equal to or lower than that of the body material is sandwiched and bonded by diffusion bonding.
(作 用) 空胴材料は主としてCuを使うが、それに比べて融点が
等しいか又はそれよりも低い材料のTi,Sn等の金属箔を
コ字形又はI字形の係合部の底部の接合面間にはさんで
拡散接合するから、目視はできなくても、固相は勿論の
こと液相の拡散接合でも金属箔が液相となり、接合部周
辺が合金相となり、一体化され、真空を確保する。従っ
て目視による確認はできなくても接合による残留応力を
無くし、変形を防止することと、接合部を導電性の高
い、放出ガスの少ない合金相として形成させる高周波加
速空胴の製造方法となる。(Working) Cu is mainly used as the cavity material, but a metal foil of Ti, Sn, etc., which has a melting point equal to or lower than that of Cu, is used as the bonding surface at the bottom of the U-shaped or I-shaped engaging portion. Since the diffusion bonding is sandwiched between them, even if it is not visible, the metal foil becomes the liquid phase not only in the solid phase but also in the liquid phase diffusion bonding. Secure. Therefore, the present invention is a method of manufacturing a high-frequency acceleration cavity in which residual stress due to bonding is eliminated even if it cannot be visually confirmed, deformation is prevented, and a bonded portion is formed as an alloy phase having high conductivity and less emitted gas.
(実施例) 実施例1 以下、本発明の第1の実施例について第1図および第
2図を参照して説明する。(Example) Example 1 Hereinafter, a first example of the present invention will be described with reference to FIGS. 1 and 2.
この実施例は3連、5連、7連にも通ずるが、ここで
は3個の空胴(1)を連結して、一つの高周波加速空胴
として構成する。(2)は中空円筒形の外筒、(3)は
外筒(2)に拡散接合された円板形の端板、(3a)はノ
ーズ、(4)は複数の空胴(1)に仕切るための円板形
の隔壁である。隔壁(4)も外筒(2)に拡散接合にて
接合されている。端板(3)、隔壁(4)とも中央に円
孔(7)があり、この円孔(7)の中心をビームが通過
する。(8)は高周波加速空胴内に高周波エネルギを供
給するためのアンテナで、外筒(2)に装着されてお
り、図示しない高周波電源に接続されている。1つのア
ンテナ(8)から3個の全空胴(1)へエネルギを伝え
なければならないもので、もしエネルギの伝送が不十分
な場合は隔壁(4)にスロットを切って空胴(1)相互
間の結合を増やす場合もある。(9)は空胴(1)の共
振周波数を調整するための円筒形のチューナであり、各
空胴(1)に1個ずつ設ける。(10)はフランジであ
り、(11)は廃棄ポートである、また、第2図に示すよ
うに外筒(2)と隔壁(4)は同一方向にコ字形のいん
ろうで結合し、その結合部の底部に金属箔(12)をはさ
み、外筒を立てて、拡散溶接を行う。In this embodiment, three, five, and seven stations are connected, but here, three cavities (1) are connected to form one high-frequency acceleration cavity. (2) is a hollow cylindrical outer cylinder, (3) is a disk-shaped end plate diffusion-bonded to the outer cylinder (2), (3a) is a nose, (4) is a plurality of cavities (1) A disk-shaped partition wall for partitioning. The partition wall (4) is also joined to the outer cylinder (2) by diffusion joining. Both the end plate (3) and the partition wall (4) have a circular hole (7) at the center, and the beam passes through the center of this circular hole (7). (8) is an antenna for supplying high-frequency energy into the high-frequency acceleration cavity, which is attached to the outer cylinder (2) and is connected to a high-frequency power source (not shown). Energy must be transferred from one antenna (8) to all three cavities (1), and if the energy transfer is insufficient, the partition (4) is slotted into the cavities (1). In some cases, the number of bonds between them is increased. Reference numeral (9) is a cylindrical tuner for adjusting the resonance frequency of the cavity (1), and one tuner is provided for each cavity (1). (10) is a flange, (11) is a waste port, and as shown in FIG. 2, the outer cylinder (2) and the partition wall (4) are connected in the same direction with a U-shaped anchor, and A metal foil (12) is sandwiched between the bottoms of the joints, an outer cylinder is erected, and diffusion welding is performed.
次に上記実施例1の作用を説明する。 Next, the operation of the first embodiment will be described.
いんろうの嵌合を同一方向に合わせたのは、空胴
(2)を立てて液相の拡散接合を行えば、溶融金属箔が
流出することがなく、信頼性の高い接合ができるためで
ある。すなわち、金属箔(12)は空胴(2)の材料に比
べて融点が等しいか又はそれより低い材料であるから、
先ず金属箔(12)が液相となり、液相の拡散接合により
接合部周辺が合金層となるから、接合状態を目視できな
くても、確実に一体化され、真空を確保する。従って接
合による残留応力をなくし、変形を防止することと、接
合部を導電性の高い、放出ガスの少ない合金層として形
成させ、多連結にしたことにより、確実に電力効率の高
い平坦な電界分布が得られ、優れた高周波特性をもつ高
周波加速空胴の製造方法となる。The reason why the fittings of the anchors are aligned in the same direction is that if the cavity (2) is set up and the diffusion bonding of the liquid phase is performed, the molten metal foil will not flow out and reliable bonding can be achieved. is there. That is, the metal foil (12) has a melting point equal to or lower than that of the material of the cavity (2),
First, the metal foil (12) becomes a liquid phase, and the diffusion bonding of the liquid phase forms an alloy layer around the bonded portion. Therefore, even if the bonded state cannot be visually observed, the metal foil (12) is reliably integrated and a vacuum is secured. Therefore, by eliminating the residual stress due to bonding and preventing deformation, and by forming the bonding part as an alloy layer with high conductivity and less emitted gas and making multiple connections, it is possible to ensure a flat electric field distribution with high power efficiency. And a method of manufacturing a high frequency acceleration cavity having excellent high frequency characteristics.
実施例2 第3図に第2の実施例の要部を示す。これは金属箔
(12)をはさむ接合部のいんろうを互いに逆向けにてI
字形にしたもので、他は実施例1の通りである。Embodiment 2 FIG. 3 shows the essential parts of the second embodiment. This is done by arranging the joints sandwiching the metal foil (12) in opposite directions to each other.
It is in the shape of a letter, and the others are as in the first embodiment.
このようにしても固相拡散接合ならば、金属箔(12)
が流出することなく、実施例1と同様な作用効果が得ら
れる。If solid phase diffusion bonding is used even in this way, metal foil (12)
Does not flow out, and the same effect as that of the first embodiment can be obtained.
実施例3 第4図に第3の実施例を示す。これは実施例1の空胴
(1)が多連結であるのに対して、空胴(1)を1個だ
けにしたものであって、他は実施例1と同様である。Embodiment 3 FIG. 4 shows a third embodiment. This is the same as the first embodiment except that only one cavity (1) is provided, while the cavity (1) of the first embodiment is multi-connected.
このようにすると、発生エネルギは減少するが、実施
例1に準じた作用効果が得られる。By doing so, the generated energy is reduced, but the action and effect according to the first embodiment can be obtained.
尚、実施例3の接合部(5)は実施例2に準じてもよ
い。The joint portion (5) of the third embodiment may conform to that of the second embodiment.
以上説明したように本発明によれば、空胴を分割して
製作し、接合部をコ字形又はI字形にし、その接合部の
底部に空胴材料に比べて融点が等しいか又はそれよりも
低い材料の金属箔をはさみ、拡散接合にて接続するか
ら、固相又は液相の拡散接合により接合部周辺が、目視
はできなくても確実に合金層となり、一体化され、真空
を確保する。従って接合による残留応力をなくし、変形
を防止することと、接合部を導電性の高い、放出ガスの
少ない合金層として形成させる高周波加速空胴の製造方
法となる。As described above, according to the present invention, the cavity is divided and manufactured, and the joint is formed in a U shape or an I shape, and the bottom of the joint has a melting point equal to or higher than that of the cavity material. Since metal foil of low material is sandwiched and connected by diffusion bonding, solid-phase or liquid-phase diffusion bonding surely forms an alloy layer around the bonded part even if it is not visible, and it is integrated and secures a vacuum. . Therefore, the present invention provides a method for manufacturing a high-frequency acceleration cavity in which residual stress due to bonding is eliminated, deformation is prevented, and a bonded portion is formed as an alloy layer having high conductivity and less emitted gas.
第1図は本発明の第1の実施例の方法にて製造した高周
波加速空胴を示す縦断面図、第2図は第1図の要部拡大
図、第3図は第2の実施例の方法にて製造した第2図相
当部を示す断面図、第4図は第3の実施例の方法にて製
造した高周波加速空胴を示す上半部縦断立面図、第5図
は従来例の方法にて製造した高周波加速空胴を示す縦断
面図、第6図および第7図は第5図のそれぞれ異なる方
法で製造した接合部を示す断面図である。 1……空胴、2……外筒、 3……端板、5……接合部、 12……金属箔。FIG. 1 is a longitudinal sectional view showing a high frequency accelerating cavity manufactured by the method of the first embodiment of the present invention, FIG. 2 is an enlarged view of a main part of FIG. 1, and FIG. 3 is a second embodiment. 2 is a sectional view showing a portion corresponding to FIG. 2 manufactured by the method of FIG. 4, FIG. 4 is a vertical sectional elevation view of an upper half portion showing a high frequency acceleration cavity manufactured by the method of the third embodiment, and FIG. FIG. 6 is a vertical cross-sectional view showing a high-frequency acceleration cavity manufactured by the example method, and FIGS. 6 and 7 are cross-sectional views showing joints manufactured by the different methods of FIG. 1 ... cavity, 2 ... outer cylinder, 3 ... end plate, 5 ... joint, 12 ... metal foil.
Claims (1)
力を入力し、発生する電界により荷電粒子を加速する高
周波加速空胴の製造方法において、空胴を分割して製作
し、接合部をコ字形又は1字形のいんろうにて係合し、
接合部の底部に空胴材料に比べて融点が等しいか又はそ
れよりも低い材料の金属箔をはさみ、拡散接合にて接合
することを特徴とした高周波加速空胴の製造方法。1. A method of manufacturing a high frequency accelerating cavity in which a cavity is formed of a conductive metal, a high frequency power is input, and charged particles are accelerated by an electric field generated, the cavity is divided and manufactured, and a joint is formed. Engage with a U-shaped or 1-shaped anchor,
A method of manufacturing a high-frequency acceleration cavity, characterized in that a metal foil made of a material having a melting point equal to or lower than that of a cavity material is sandwiched at the bottom of the joint, and the layers are bonded by diffusion bonding.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2027794A JPH0821477B2 (en) | 1990-02-07 | 1990-02-07 | High frequency acceleration cavity manufacturing method |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2027794A JPH0821477B2 (en) | 1990-02-07 | 1990-02-07 | High frequency acceleration cavity manufacturing method |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH03233899A JPH03233899A (en) | 1991-10-17 |
| JPH0821477B2 true JPH0821477B2 (en) | 1996-03-04 |
Family
ID=12230883
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP2027794A Expired - Lifetime JPH0821477B2 (en) | 1990-02-07 | 1990-02-07 | High frequency acceleration cavity manufacturing method |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0821477B2 (en) |
Families Citing this family (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP5310022B2 (en) * | 2009-01-22 | 2013-10-09 | 日本電気株式会社 | Microwave band limiting filter, welding method thereof, and satellite equipped with microwave band limiting filter |
| JP5801118B2 (en) * | 2011-07-04 | 2015-10-28 | 株式会社東芝 | Vacuum container manufacturing method |
| JP5989860B2 (en) * | 2015-06-19 | 2016-09-07 | 株式会社東芝 | Vacuum container manufacturing method |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5244798Y2 (en) * | 1972-02-21 | 1977-10-12 |
-
1990
- 1990-02-07 JP JP2027794A patent/JPH0821477B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPH03233899A (en) | 1991-10-17 |
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