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JPS6348381B2 - - Google Patents
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JPS6348381B2 - - Google Patents

Info

Publication number
JPS6348381B2
JPS6348381B2 JP54172855A JP17285579A JPS6348381B2 JP S6348381 B2 JPS6348381 B2 JP S6348381B2 JP 54172855 A JP54172855 A JP 54172855A JP 17285579 A JP17285579 A JP 17285579A JP S6348381 B2 JPS6348381 B2 JP S6348381B2
Authority
JP
Japan
Prior art keywords
frequency circuit
support
cover
high frequency
ppm
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
Application number
JP54172855A
Other languages
Japanese (ja)
Other versions
JPS5696444A (en
Inventor
Hisaaki Sato
Hiroyuki Hashimoto
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.)
NEC Corp
Original Assignee
Nippon Electric Co 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 Nippon Electric Co Ltd filed Critical Nippon Electric Co Ltd
Priority to JP17285579A priority Critical patent/JPS5696444A/en
Publication of JPS5696444A publication Critical patent/JPS5696444A/en
Publication of JPS6348381B2 publication Critical patent/JPS6348381B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J23/00Details of transit-time tubes of the types covered by group H01J25/00
    • H01J23/12Vessels; Containers

Landscapes

  • Microwave Tubes (AREA)

Description

【発明の詳細な説明】 本発明は、電子ビーム集束装置として周期永久
磁石(PPM)を使用したヘリツクス形進行波管
の高周波回路の支持構造に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a support structure for a high frequency circuit of a helical traveling wave tube using a periodic permanent magnet (PPM) as an electron beam focusing device.

ヘリツクス形進行波管は、電子ビームの発生さ
せる電子銃部、電子ビームと電磁波の相互作用を
行なう高周波回路部(ヘリツクス部)電子ビーム
を捕足するコレクタ部、電子ビームを集束させる
PPM、それに管球を保持、収納するケース等が
一般的な構成要素である。
A helical traveling wave tube consists of an electron gun part that generates an electron beam, a high-frequency circuit part (helix part) that interacts with the electron beam and electromagnetic waves, a collector part that captures the electron beam, and a collector part that focuses the electron beam.
Common components include the PPM and a case to hold and store the tube.

周知の如く、ヘリツクス形進行波管は、高周波
回路の構造が比較的簡単で、かつその外径が比較
的小さいため、PPMによる電子ビーム集束が簡
単に行なえるという大きな特徴をもつている。
As is well known, the helical traveling wave tube has a relatively simple high-frequency circuit structure and a relatively small outer diameter, so it has the great feature that electron beam focusing by PPM can be easily performed.

従来の代表的なヘリツクス形進行波管の構造例
を第1図に示す。第1図において、1が電子銃
部、2が高周波回路部及びPPM部、3がコレク
タ部、4がケースの一部をなすべースプレート、
5が高周波回路の支持体を、それぞれ示す。ま
た、第1図の断面A−A′を第2図に示す。第2
図において、PPMを構成するひとつのマグネツ
ト2′の外周の一部が支持体5で受けられており、
支持体5はべースプレート4にねじ等によつて固
着されている。また、マグネツト2′が支持体5
から浮かないように、通常、厚さ0.5〜1mm程度
の銅製のバンド6がマグネツト2′をはさんで支
持体5に固着される。バンド6を銅製にするの
は、高周波回路で発生した熱を支持体側に伝導で
逃がすためである。支持体5及びバンド6だけを
とり出して立体的に示すと第3図のようになる。
従来の構造では、このような支持機構が管軸方向
に沿つて数ケ所に設置され、各支持体の間は空間
のままであつた。その理由は、PPM上の任意の
位置に、マグネツトの偏磁を補正するための小磁
性体7を置いて、電子ビームの透過率の調整をす
ることができるようにしておくためである。この
場合、小磁性体7を厚いバンド6の外側においた
のでは、ビーム透過率調整の役に立たない。なぜ
ならば、バンドの厚み分だけ磁気的に隔離されて
しまうため、偏磁補正の効果が著しく弱められる
からである。
An example of the structure of a typical conventional helical traveling wave tube is shown in FIG. In FIG. 1, 1 is an electron gun section, 2 is a high frequency circuit section and a PPM section, 3 is a collector section, 4 is a base plate forming part of the case,
5 represents a support for a high frequency circuit. Further, a cross section AA' in FIG. 1 is shown in FIG. 2. Second
In the figure, a part of the outer periphery of one magnet 2' constituting the PPM is supported by a support 5.
The support body 5 is fixed to the base plate 4 with screws or the like. Also, the magnet 2' is connected to the support 5.
A copper band 6, usually about 0.5 to 1 mm thick, is fixed to the support 5 with the magnet 2' in between to prevent it from floating. The reason why the band 6 is made of copper is to conduct the heat generated in the high-frequency circuit to the support body and release it. If only the support body 5 and band 6 are taken out and shown three-dimensionally, the result will be as shown in FIG.
In the conventional structure, such support mechanisms were installed at several locations along the tube axis, leaving spaces between each support. The reason for this is that a small magnetic body 7 is placed at an arbitrary position on the PPM to correct the biased magnetism of the magnet, so that the transmittance of the electron beam can be adjusted. In this case, placing the small magnetic body 7 outside the thick band 6 is of no use in adjusting the beam transmittance. This is because they are magnetically isolated by the thickness of the band, which significantly weakens the effect of correcting biased magnetism.

ところで、このような従来構造においては、次
のような欠点があつた。すなわち、ヘリツクス形
進行波管は一般に回路の外形が小さい割に回路の
全長が長いものであり、その機械的強度はもとも
と非常に弱い。従つて、このような回路を数個の
支持体で支持した程度では、支持体で支持されな
い部分の機械的強度は非常に弱いものである。ま
た、仮に製造段階で回路の真直度が良好であつて
も、輸送中や実装中の思わぬ衝撃で回路の一部
(支持体で支持されない部分)が変形してビーム
透過特性が悪化する場合も起り得る。しかし、だ
からと言つて、支持体の数を無暗に増やすのは原
価高にもなるし、支持体相互の芯出しも困難にな
り、また前述の偏磁調整用の小磁性体を置く場所
が小なくなることにもなつて、好ましくない。
However, such a conventional structure has the following drawbacks. That is, a helical traveling wave tube generally has a long overall circuit length despite its small circuit outline, and its mechanical strength is originally very weak. Therefore, even if such a circuit is supported by several supports, the mechanical strength of the portions not supported by the supports is very weak. In addition, even if the circuit has good straightness at the manufacturing stage, unexpected impacts during transportation or mounting may deform part of the circuit (the part not supported by the support) and deteriorate the beam transmission characteristics. can also occur. However, increasing the number of supports will increase the cost, making it difficult to center each support, and where to place the small magnetic material for adjusting the biased magnetism mentioned above. This is not desirable as it also causes the value to become smaller.

以上の如き構造の欠点に鑑み、ヘリツクス回路
の機械的強度を十分保つたまま、ビーム透過率調
整も容易に行なえる別の高周波回路の支持構造が
考案されている。
In view of the above-mentioned drawbacks of the structure, another high-frequency circuit support structure has been devised that allows beam transmittance to be easily adjusted while maintaining sufficient mechanical strength of the helix circuit.

その構造の一例は、第4図に示されている。同
図に見る如く、この構造においては、まず第1
に、従来軸方向に対して数個所に分れて設置され
ていた支持体の代りに、軸方向全体にわたつて1
本の長い支持体8を用いている。また、第2に、
従来の銅製バンド(厚さ0.5〜1mm)の代りに厚
さの非常に薄いステンレス製カバー9(厚さ0.1
〜0.15mm)を用い、これを前述の長い支持体と原
理的に同一長さになるようにしている。そして、
第3に、ビーム透過調整用の小磁性体7は、厚さ
の薄いカバー9の外側にとりつけられる。
An example of its structure is shown in FIG. As shown in the figure, in this structure, the first
Now, instead of the conventional supports installed at several locations in the axial direction, one support body is installed across the entire axial direction.
A long book support 8 is used. Also, secondly,
A very thin stainless steel cover 9 (0.1mm thick) is used instead of the traditional copper band (0.5~1mm thick).
~0.15 mm), which is in principle the same length as the long support described above. and,
Thirdly, the small magnetic body 7 for beam transmission adjustment is attached to the outside of the thin cover 9.

この支持構造の第1の特徴は、高周波回路を軸
方向全体にわたつて支持しているため、従来のよ
うに宙づり状態の部分がなく、機械的に極めて強
固なものになつている点である。また、第2の特
徴は、カバー9の厚さを材料の選定により薄く
し、小磁性体とPPMの距離を近づけて、小磁性
体のPPMに及ぼす効果を大きくし、もつて機械
的強度を保つたまま、その外方から容易にビーム
調整を行なえるようにしている点である。この構
造においては、支持体8の存在する部分、すなわ
ち、PPMの下半分側には小磁性体7をとりつけ
ることはできないが、ビーム透過の調整はPPM
の上半分に小磁性体を置くだけでも、実用上十分
行なえることが確認された。
The first feature of this support structure is that because the high-frequency circuit is supported in the entire axial direction, there are no suspended parts as in conventional structures, making it mechanically extremely strong. . In addition, the second feature is that the thickness of the cover 9 can be made thinner by selecting the material, and the distance between the small magnetic material and the PPM can be reduced, thereby increasing the effect of the small magnetic material on the PPM, thereby increasing the mechanical strength. The point is that the beam can be easily adjusted from outside while maintaining the same position. In this structure, the small magnetic body 7 cannot be attached to the part where the support 8 is present, that is, the lower half of the PPM, but the beam transmission can be adjusted by the PPM.
It has been confirmed that simply placing a small magnetic material on the upper half of the device is sufficient for practical use.

ところが、上述の高周波回路支持構造には、次
のような欠点があることが見出された。すなわ
ち、カバー9を支持体8にねじ止めする場合、組
立当初は、高周波回路を強くはさみ込んだ状態で
固定するのであるが、進行波管としての動作をく
り返しているうちに、高周波回路の熱的膨張収縮
により、次第にはさみ込みの力が弱まつてくるこ
とが明らかになつた。
However, it has been found that the above-described high frequency circuit support structure has the following drawbacks. In other words, when the cover 9 is screwed to the support 8, the high-frequency circuit is tightly sandwiched in the fixation at the beginning of assembly, but as the cover 9 is repeatedly operated as a traveling wave tube, the heat of the high-frequency circuit increases. It has become clear that the pinching force gradually weakens as the material expands and contracts.

本発明の目的は、このような熱的膨張収縮のく
り返しにより、支持機構にゆるみができない支持
構造を有するヘリツク形進行波管を提供すること
である。
An object of the present invention is to provide a helical traveling wave tube having a support structure that does not allow the support mechanism to loosen due to repeated thermal expansion and contraction.

本発明によれば、電子ビーム集束装置として周
期永久磁石を使用し、ケースの一部をなす高周波
回路支持体が管軸方向にわたつて高周波回路の全
長にほゞ等しく、磁石の外径の下半分もしくはそ
の一部が支持体によつて管軸方向にわたつて受け
られ、更に管軸方向の長さが支持体と略等しく弾
性係数の大きな厚さの非常に薄いカバーを磁石を
はさんで支持体に弾性変化内でとりつけ、周期永
久磁石の磁界調整をカバーの外側から行なうこと
を特徴とする進行波管が得られる。
According to the present invention, a periodic permanent magnet is used as an electron beam focusing device, and the high-frequency circuit support member forming a part of the case extends approximately equal to the entire length of the high-frequency circuit in the tube axis direction, and extends below the outer diameter of the magnet. Half or a part of the cover is supported in the tube axis direction by a support, and a very thin cover whose length in the tube axis direction is approximately equal to the support and has a large elastic modulus is sandwiched between magnets. A traveling wave tube is obtained, which is attached to a support within an elastic range and is characterized in that the magnetic field of the periodic permanent magnet is adjusted from outside the cover.

本発明に係る高周波回路支様機構の構造例を第
5図に示す。第5図においては、カバー9は断面
が逆U字形ではなく、その両端を途中から水平方
向に折り曲げられた構造をしており、また支持体
8の両端もそれに応じてひろげられた構造となつ
ている。そしてカバー9は、ステンレス、りん青
銅等の弾性係数の大きな非磁性物質が選定され、
その材料の弾性変化内で使用するように、ねじ1
0にてとりつけられる。このような構成において
は、高周波回路に熱的膨張収縮があつてもその支
持機構にゆるみが出る確率は大いに軽減されるわ
けである。
An example of the structure of the high frequency circuit support mechanism according to the present invention is shown in FIG. In Fig. 5, the cover 9 does not have an inverted U-shaped cross section, but has a structure in which both ends are bent horizontally from the middle, and both ends of the support 8 are also spread out accordingly. ing. For the cover 9, a non-magnetic material with a large elastic modulus such as stainless steel or phosphor bronze is selected.
As used within the elastic change of that material, the screw 1
It can be installed at 0. In such a configuration, even if the high frequency circuit undergoes thermal expansion and contraction, the probability that the support mechanism will become loose is greatly reduced.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は従来のヘリツクス形進行波管の高周波
回路支持構造を示す斜視図、第2図は、第1図の
A−A′断面図、第3図は、第1図の高周波回路
支持機構を立体的に示した斜視図、第4図は改良
された従来形の高周波回路支持機構を示す斜視
図、第5図は、本発明に係る高周波回路支持機構
を示す斜視図である。図において、1が電子銃
部、2が高周波回路及びPPM部、3がコレクタ
部、4がケースの一部をなすべースプレート、5
が高周波回路支持体、6がバンド、7が小磁性
体、8が高周波回路支持体、9がカバー、10が
ねじである。
Fig. 1 is a perspective view showing a conventional high frequency circuit support structure of a helical traveling wave tube, Fig. 2 is a sectional view taken along line A-A' in Fig. 1, and Fig. 3 is a high frequency circuit support structure shown in Fig. 1. FIG. 4 is a perspective view showing an improved conventional high frequency circuit support mechanism, and FIG. 5 is a perspective view showing a high frequency circuit support mechanism according to the present invention. In the figure, 1 is the electron gun section, 2 is the high frequency circuit and PPM section, 3 is the collector section, 4 is the base plate that forms part of the case, and 5
is a high frequency circuit support body, 6 is a band, 7 is a small magnetic body, 8 is a high frequency circuit support body, 9 is a cover, and 10 is a screw.

Claims (1)

【特許請求の範囲】[Claims] 1 外周に周期永久磁石を備えた高周波回路を、
高周波回路の全長にほぼ等しい長さを有し前記周
期永久磁石のほぼ下半分を受ける溝を設けた高周
波回路支持体で支え、弾性係数の大きな非磁性材
料でできており長さが前記高周波回路支持体とほ
ぼ同じで厚さの薄いカバーを前記高周波回路の上
方からかぶせるとともに前記カバーの両端が途中
から水平方向に折り曲げられており、かつ前記高
周波回路支持体も前記カバーの両端の折り曲げに
応じて水平方向にひろげられた突出部を有してお
り、前記カバーの材料の弾性変化内で前記カバー
の両端が前記高周波回路支持体の前記突出部に固
定されていることを特徴とする進行被管。
1. A high frequency circuit with a periodic permanent magnet on the outer periphery,
The high-frequency circuit is supported by a high-frequency circuit support member having a length approximately equal to the total length of the high-frequency circuit and provided with a groove for receiving approximately the lower half of the periodic permanent magnet, and is made of a non-magnetic material with a large elastic modulus. A thin cover that is approximately the same as the support and has a thin thickness is placed over the high-frequency circuit, and both ends of the cover are bent horizontally from the middle, and the high-frequency circuit support also conforms to the bending of both ends of the cover. The traveling cover has a protrusion extending in the horizontal direction, and both ends of the cover are fixed to the protrusion of the high-frequency circuit support within an elastic change of the material of the cover. tube.
JP17285579A 1979-12-28 1979-12-28 Traveling waveguide Granted JPS5696444A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP17285579A JPS5696444A (en) 1979-12-28 1979-12-28 Traveling waveguide

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP17285579A JPS5696444A (en) 1979-12-28 1979-12-28 Traveling waveguide

Publications (2)

Publication Number Publication Date
JPS5696444A JPS5696444A (en) 1981-08-04
JPS6348381B2 true JPS6348381B2 (en) 1988-09-28

Family

ID=15949538

Family Applications (1)

Application Number Title Priority Date Filing Date
JP17285579A Granted JPS5696444A (en) 1979-12-28 1979-12-28 Traveling waveguide

Country Status (1)

Country Link
JP (1) JPS5696444A (en)

Family Cites Families (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5751458Y2 (en) * 1977-11-25 1982-11-10
JPS5474668A (en) * 1977-11-28 1979-06-14 Nec Corp Traveliing-wave tube unit

Also Published As

Publication number Publication date
JPS5696444A (en) 1981-08-04

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