JPS6240812B2 - - Google Patents
Info
- Publication number
- JPS6240812B2 JPS6240812B2 JP16585881A JP16585881A JPS6240812B2 JP S6240812 B2 JPS6240812 B2 JP S6240812B2 JP 16585881 A JP16585881 A JP 16585881A JP 16585881 A JP16585881 A JP 16585881A JP S6240812 B2 JPS6240812 B2 JP S6240812B2
- Authority
- JP
- Japan
- Prior art keywords
- pole piece
- metal cylinder
- magnetic field
- field device
- periodic magnetic
- 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
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J23/00—Details of transit-time tubes of the types covered by group H01J25/00
- H01J23/02—Electrodes; Magnetic control means; Screens
- H01J23/08—Focusing arrangements, e.g. for concentrating stream of electrons, for preventing spreading of stream
- H01J23/087—Magnetic focusing arrangements
- H01J23/0873—Magnetic focusing arrangements with at least one axial-field reversal along the interaction space, e.g. P.P.M. focusing
Landscapes
- Microwave Tubes (AREA)
Description
【発明の詳細な説明】
本発明は進行波管などに用いられる周期磁界装
置において、ポールピースとポールピースを貫通
している金属円筒との接触熱抵抗と機械的密着性
の改善をはかつた装置に関するものである。[Detailed Description of the Invention] The present invention aims to improve the contact thermal resistance and mechanical adhesion between a pole piece and a metal cylinder passing through the pole piece in a periodic magnetic field device used in a traveling wave tube or the like. It is related to the device.
従来は進行波管などの電子ビームを集束するた
めに周期磁界装置を用いる場合、ポールピースと
磁石によつてあらかじめ組立てられた周期磁界装
置の中へ進行波管を挿入するか、または、進行波
管の組立工程の途中において、らせんなどの遅波
回路部外囲器にポールピースを貫通させて置き、
進行波管が完成した後に直径に沿つて2分割した
リング状磁石を取りつけて周期磁界装置を完成さ
せているため、ポールピース内径と遅波回路部外
囲器を構成する金属円筒の外径との間に若干の差
を設け、ポールピースを金属円筒の軸方向に容易
に移動させたり、または回転させたりすることが
可能なようにしてある。その結果、らせん形遅波
回路を用いて大出力を得ようとする場合、とくに
らせん回路の出力部がらせん回路上を流れる高周
波電流によつて高温に加熱されるため、高周波出
力が制限される原因となつている。 Conventionally, when using a periodic magnetic field device such as a traveling wave tube to focus an electron beam, the traveling wave tube is inserted into a periodic magnetic field device that is preassembled with a pole piece and a magnet, or the traveling wave tube is During the tube assembly process, a pole piece is placed through the slow wave circuit envelope such as a spiral.
After the traveling wave tube is completed, a ring-shaped magnet divided into two along the diameter is attached to complete the periodic magnetic field device, so the inner diameter of the pole piece and the outer diameter of the metal cylinder that makes up the slow wave circuit envelope are different from each other. A slight difference is provided between them so that the pole piece can be easily moved or rotated in the axial direction of the metal cylinder. As a result, when trying to obtain high output using a spiral slow-wave circuit, the output section of the spiral circuit is heated to a high temperature by the high-frequency current flowing through the spiral circuit, which limits the high-frequency output. It is the cause.
従来はこれを解決するために、らせん回路支持
用誘電体にベリリヤ磁器やボロンナイトライドな
どの熱伝導率の高い材質を用い、外囲器の中に外
囲器を密着するようにらせん及び支持体を挿入し
て、らせんに発生した熱を効果的に外囲器に伝導
して外囲器の軸方向に拡散させ、極く一部はポー
ルピースとの接触部から周期磁界装置へも伝導
し、その結果としてらせん回路の冷却を行なつて
いたが、金属円筒にくらべ、容積、放熱表面積が
はるかに大きい周期磁界装置へ効果的に熱を逃が
すことができず、結局高周波出力を大幅に増加す
ることができなかつた。また、従来形のものでは
ポールピースと金属円筒との接触が不十分で機械
的補強のためにエポキシ樹脂などを用いて両者を
接着しなければならない場合もあつた。 Conventionally, in order to solve this problem, a material with high thermal conductivity such as beryllia porcelain or boron nitride was used as the dielectric material for supporting the spiral circuit, and the spiral circuit and the support were used so that the envelope was tightly attached to the inside of the envelope. By inserting the body, the heat generated in the spiral is effectively conducted to the envelope and diffused in the axial direction of the envelope, and a small portion is also conducted from the contact part with the pole piece to the periodic magnetic field device. As a result, the spiral circuit was cooled, but the heat could not be effectively dissipated to the periodic magnetic field device, which has a much larger volume and heat dissipation surface area than a metal cylinder, and in the end, the high frequency output was significantly increased. could not increase. Furthermore, in the conventional type, the contact between the pole piece and the metal cylinder was insufficient, and in some cases, it was necessary to bond the two using epoxy resin or the like for mechanical reinforcement.
本発明の目的は、このような従来形の欠点を取
り除き、金属円筒内部で発生し、かつ金属円筒ま
で導びかれてきた熱を効果的に周期磁界装置に伝
導させることにより、金属円筒内の発熱物の温度
を下げ、かつ、周期磁界装置と金属円筒とを強固
に固定し得る周期磁界装置を提供することにあ
る。 The purpose of the present invention is to eliminate such drawbacks of the conventional type, and to effectively conduct the heat generated inside the metal cylinder and led to the metal cylinder to the periodic magnetic field device, thereby reducing the heat inside the metal cylinder. It is an object of the present invention to provide a periodic magnetic field device that can lower the temperature of a heating substance and firmly fix the periodic magnetic field device and a metal cylinder.
本発明は、上記の目的を達成するために、ポー
ルピースにその中心軸に対して傾いた切開面を持
つ切開部を設け、これを金属円筒の外周に挿着し
た後、前記切開部の対向面が密着するように前記
ポールピースを圧縮し、前記金属円筒の外周と前
記ポールピースの内周とを熱的及び機械的に密着
させるようにしたものである。 In order to achieve the above object, the present invention provides a pole piece with a cutout having a cutout surface inclined with respect to its central axis, and after inserting this into the outer periphery of a metal cylinder, The pole piece is compressed so that the surfaces thereof come into close contact with each other, and the outer periphery of the metal cylinder and the inner periphery of the pole piece are thermally and mechanically brought into close contact.
以下に本発明を従来例と共に実施例によつて詳
細に説明する。 The present invention will be explained in detail below using examples as well as conventional examples.
第1図は従来の一般的な周期磁界装置とそれを
貫通する金属円筒の部分断面図で、1は磁石、2
はポールピース、3は金属円筒である。 Figure 1 is a partial cross-sectional view of a conventional general periodic magnetic field device and a metal cylinder that passes through it.
is a pole piece, and 3 is a metal cylinder.
第2図は前記従来構造の周期磁界装置のポール
ピース2と金属円筒3の関係の説明図で、図aは
ポールピース部の平面図、図bはポールピース部
の断面図である。ポールピース2と金属円筒3の
外周上を容易に移動し得るように両者間に間隙4
が設けられていることを示している。このために
従来の周期磁界装置は前述のような欠点を有して
いた。 FIG. 2 is an explanatory view of the relationship between the pole piece 2 and the metal cylinder 3 of the periodic magnetic field device having the conventional structure, where FIG. 2A is a plan view of the pole piece portion, and FIG. 2B is a sectional view of the pole piece portion. A gap 4 is provided between the pole piece 2 and the metal cylinder 3 so that the metal cylinder 3 can be easily moved on the outer periphery thereof.
This shows that it is provided. For this reason, the conventional periodic magnetic field device has the above-mentioned drawbacks.
本発明はこのような欠点を除くために、下記の
ような改良を行なつたものである。 In order to eliminate such drawbacks, the present invention has made the following improvements.
第3図は本発明にかかる周期磁界装置用ポール
ピースの圧縮加工前の形状と金属円筒との関係の
説明図で、図a,b,cはそれぞれポールピース
部の側面図、平面図、断面図である。ポールピー
ス5にはその軸に対して傾きをもつたスリツト
(切開部)6が設けられており、金属円筒3の外
径とポールピース5の内径との間には間隙4を設
け、金属円筒3の外周上をポールピース5が容易
に移動し得る構造になつている。このスリツト6
の幅とポールピース5の中心軸に対する傾きは、
スリツト6を挾んで相対する面が完全に接するよ
うにポールピース5を圧縮すると、ポールピース
5の内径がこれを貫通している金属円筒3の外径
より極く僅か小さくなり、第4図に示すように、
スリツト6の相対する面が密着すると同時にポー
ルピース5と金属円筒3との間隙もなくなつて両
者は完全に密着するように選ばれている。したが
つて、熱的接触抵抗は従来構造のものに比べて大
幅に減少すると共に機械的強度も十分に確保でき
るようになる。なお、第4図において、図a,
b,cはそれぞれポールピース部の側面図、平面
図、断面図である。なお、スリツトを挾んで相対
した面を圧縮によつて密着させたスリツト部分
6′を両側から第5図に示すようにスポツト電気
溶接用電極7で挾んでスポツト溶接してもよく、
また、ろう付け又は樹脂等の接着剤で接合すれば
より完全である。 FIG. 3 is an explanatory view of the relationship between the shape of the pole piece for a periodic magnetic field device according to the present invention before compression processing and the metal cylinder, and figures a, b, and c are a side view, a plan view, and a cross section of the pole piece portion, respectively. It is a diagram. The pole piece 5 is provided with a slit (cutout) 6 that is inclined with respect to its axis, and a gap 4 is provided between the outer diameter of the metal cylinder 3 and the inner diameter of the pole piece 5. The structure is such that the pole piece 5 can be easily moved on the outer periphery of the pole piece 3. This slit 6
The width of and the inclination of the pole piece 5 with respect to the central axis are:
When the pole piece 5 is compressed with the slit 6 in between so that the opposing surfaces are completely in contact with each other, the inner diameter of the pole piece 5 becomes very slightly smaller than the outer diameter of the metal cylinder 3 passing through it, and as shown in FIG. As shown,
The selection is made so that the opposing surfaces of the slit 6 are in close contact with each other, and at the same time, there is no gap between the pole piece 5 and the metal cylinder 3, so that they are in complete contact with each other. Therefore, thermal contact resistance is significantly reduced compared to conventional structures, and sufficient mechanical strength can also be ensured. In addition, in Figure 4, Figures a,
b and c are a side view, a plan view, and a sectional view of the pole piece portion, respectively. Incidentally, the slit portion 6', in which the opposing surfaces of the slit are held in close contact by compression, may be spot welded by being held from both sides with spot electric welding electrodes 7 as shown in FIG.
Moreover, it will be more complete if they are joined by brazing or adhesive such as resin.
なおまた、ポールピースにスリツトを入れるこ
とにより周期磁界装置の発生する軸上磁界強度の
分布に磁界強度の偏り、すなわち偏磁を生ずる場
合があるが、本発明においてはスリツトを斜めに
設けることにより、偏磁が発生してもこれを最小
に押えることができる。 Furthermore, by providing a slit in the pole piece, the distribution of the axial magnetic field intensity generated by the periodic magnetic field device may be biased in the magnetic field strength, that is, biased magnetism may occur, but in the present invention, by providing the slit diagonally, Even if biased magnetism occurs, it can be suppressed to a minimum.
以上詳述したところから明らかなように、本発
明の実施によつて金属円筒とそれに外接する周期
磁界装置との熱的及び機械的接触の強度が改善さ
れるため、例えば、らせん形進行波管に適用した
場合、高周波電力によつて加熱されたらせんの熱
を効果的に容積、表面積の大きな周期磁界装置へ
導びくことが可能になるため、進行波管の出力を
従来と同じ値に保つ場合には、らせん温度が低下
するので損失が減少し、能率が改善され、また、
出力を増加したい場合には、従来構造における出
力の場合と同じらせん温度の範囲に保ちながら、
大幅な出力の増加が可能であるなどの利点があ
る。 As is clear from the above detailed description, by implementing the present invention, the strength of the thermal and mechanical contact between the metal cylinder and the periodic magnetic field device circumscribing the metal cylinder is improved. When applied to , it becomes possible to effectively guide the heat of the helix heated by high-frequency power to a periodic magnetic field device with a large volume and surface area, keeping the output of the traveling wave tube at the same value as before. In some cases, the helix temperature is lowered, which reduces losses and improves efficiency;
If you want to increase the output, while keeping the helical temperature in the same range as for the output in the conventional structure,
It has the advantage of being able to significantly increase output.
また、周期磁界装置のポールピースにスリツト
を設けることによる偏磁の発生も、スリツトを斜
めに設けてあるので最少に押えることができ、電
子ビームの集束に与える影響は極めて僅かであ
る。 Furthermore, the generation of biased magnetism due to the provision of slits in the pole pieces of the periodic magnetic field device can be minimized because the slits are provided diagonally, and the effect on the focusing of the electron beam is extremely small.
第1図は従来の一般的な周期磁界装置の部分断
面図、第2図は第1図に示した従来の周期磁界装
置におけるポールピースとこれに内接する金属円
筒との関係の説明図、第3図は本発明にかかる周
期磁界装置のポールピースの圧縮加工前における
金属円筒との関係の説明図、第4図は本発明にか
かる周期磁界装置のポールピースの圧縮加工後の
金属円筒との関係の説明図、第5図は本発明にか
から周期磁界装置のポールピースに設けたスリツ
トの相対する面を密着させて接合する方法の一例
としてのスポツト電気溶接加工法の実施例を示す
図である。
図において、1……磁石、2……ポールピー
ス、3……金属円筒、4……ポールピースと金属
円筒との間隙、5……本発明にかかるポールピー
ス、5″……圧縮加工後のポールピース、6……
ポールピース5に設けたスリツト、6′……圧縮
加工後のスリツト、7……スポツト電気溶接用電
極。
Fig. 1 is a partial sectional view of a conventional general periodic magnetic field device, Fig. 2 is an explanatory diagram of the relationship between the pole piece and the metal cylinder inscribed therein in the conventional periodic magnetic field device shown in Fig. 1; FIG. 3 is an explanatory diagram of the relationship between the pole piece of the periodic magnetic field device according to the present invention and the metal cylinder before compression processing, and FIG. 4 is an explanatory diagram of the relationship between the pole piece of the periodic magnetic field device according to the present invention and the metal cylinder after compression processing. An explanatory diagram of the relationship, FIG. 5 is a diagram showing an embodiment of the spot electric welding process as an example of a method of closely joining the opposing surfaces of the slit provided in the pole piece of the periodic magnetic field device according to the present invention. It is. In the figure, 1... Magnet, 2... Pole piece, 3... Metal cylinder, 4... Gap between pole piece and metal cylinder, 5... Pole piece according to the present invention, 5''... After compression processing Pole piece, 6...
Slit provided in pole piece 5, 6'... slit after compression processing, 7... electrode for spot electric welding.
Claims (1)
スとリング状磁石を交互に配置した周期磁界装置
において、中心軸に対して傾いた切開面を持つた
切開部を設けた前記ポールピースを前記金属円筒
の外周に挿着後、前記切開部の対向面が密着する
ように前記ポールピースを圧縮し、前記金属円筒
の外周と前記ポールピースの内周とを熱的及び機
械的に密着させたことを特徴とする周期磁界装
置。1. In a periodic magnetic field device in which a plurality of pole pieces and ring-shaped magnets are alternately arranged in contact with the outer periphery of a metal cylinder, the pole piece is provided with a cutout having a cutout surface inclined with respect to the central axis. After the pole piece is inserted into the outer periphery of the cylinder, the pole piece is compressed so that the opposing surfaces of the incision are in close contact with each other, and the outer periphery of the metal cylinder and the inner periphery of the pole piece are thermally and mechanically brought into close contact. A periodic magnetic field device characterized by:
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP16585881A JPS5868845A (en) | 1981-10-19 | 1981-10-19 | Cyclic magnetic field device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP16585881A JPS5868845A (en) | 1981-10-19 | 1981-10-19 | Cyclic magnetic field device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5868845A JPS5868845A (en) | 1983-04-23 |
| JPS6240812B2 true JPS6240812B2 (en) | 1987-08-31 |
Family
ID=15820327
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP16585881A Granted JPS5868845A (en) | 1981-10-19 | 1981-10-19 | Cyclic magnetic field device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5868845A (en) |
-
1981
- 1981-10-19 JP JP16585881A patent/JPS5868845A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5868845A (en) | 1983-04-23 |
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