JP2679378B2 - Spiral slow wave circuit structure - Google Patents

Spiral slow wave circuit structure

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Publication number
JP2679378B2
JP2679378B2 JP22292490A JP22292490A JP2679378B2 JP 2679378 B2 JP2679378 B2 JP 2679378B2 JP 22292490 A JP22292490 A JP 22292490A JP 22292490 A JP22292490 A JP 22292490A JP 2679378 B2 JP2679378 B2 JP 2679378B2
Authority
JP
Japan
Prior art keywords
wave circuit
slow wave
magnetic pole
circuit structure
input
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
Application number
JP22292490A
Other languages
Japanese (ja)
Other versions
JPH04106842A (en
Inventor
泰弘 板垣
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
NEC Corp
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 NEC Corp filed Critical NEC Corp
Priority to JP22292490A priority Critical patent/JP2679378B2/en
Publication of JPH04106842A publication Critical patent/JPH04106842A/en
Application granted granted Critical
Publication of JP2679378B2 publication Critical patent/JP2679378B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、進行波管等に使用されるらせん形遅波回路
構体に関する。
The present invention relates to a spiral slow wave circuit structure used in a traveling wave tube or the like.

〔従来の技術〕[Conventional technology]

らせん形遅波回路用の外囲器として、円板状磁極と円
筒状金属スペーサを交互に積層しろう付接合してなる外
囲器がある。この外囲器を用いると、それに収納される
らせんに磁極内径がより近接するため、磁極と組合せる
円環状半割りの永久磁石のエネルギーが同じでもより高
い中心磁束密度が得られる。従って、周波数が高く、よ
り高効率の進行波管においては、上記構成の遅波回路が
採用されてきている。
As an envelope for a spiral slow-wave circuit, there is an envelope in which disk-shaped magnetic poles and cylindrical metal spacers are alternately laminated and brazed and joined. When this envelope is used, since the inner diameter of the magnetic pole is closer to the spiral housed in it, a higher central magnetic flux density can be obtained even if the energy of the annular half permanent magnet combined with the magnetic pole is the same. Therefore, in a traveling wave tube having a high frequency and higher efficiency, the slow wave circuit configured as described above has been adopted.

第3図は従来の遅波回路構体20の断面図を示し、第4
図は第3図のB−B断面図を示すが、らせん1は、その
外周囲に3本の誘電体支柱2,3,4を配設し、外囲器5内
に収納されている。外囲器5は、円板状磁極6及び非磁
性の円筒状金属スペーサ7を交互に組合せ接合され形成
されている。外囲器5の両端にはコレクタ8及び電子銃
9を接合する円板状シールド部品10,11が具備され、さ
らにその近傍には高周波を入出力する高周波窓12,13が
配設され遅波回路用の外囲器5が構成される。外囲器5
は、円板状磁極6,円筒状金属スペーサ7,円板状シールド
部品10,11及び入出力の高周波窓12,13がろう付等によっ
て接合された後、らせん1及び3本の誘電体支柱2,3,4
を収納する穴の成形切削加工を行なうが、これは、らせ
ん1及び誘電体支柱2,3,4を焼ばめによって挿入,締結
を行なうため、締結代を適切な値にすることと穴の内周
面の凹凸を除去し鏡面状に仕上げる必要があるからであ
る。穴の削り代は、0,2〜0,3mmが一般的で、切削にはガ
ンドリルが用いられる。遅波回路5の軸方向長さは製品
によっては異なるが、回路が長くなる場合は、分割型に
するので、一回路の長さは100mm前後が一般的である。
又電子銃9側には、電子銃9を接合するシールド部品10
から円環状半割り磁石(図示せず)5個目に入力高周波
窓12を配設する場合が多い。円板状磁極6で言えば、シ
ールド部品10から第4番目と第5番目の間の円筒状金属
スペーサ7に入力高周波窓が具備されている。これは、
進行波管のパスバンド特性によって起動及び停止時にら
せん電流が一時的に増大するが、この時、電子銃より放
射された電子ビームはほとんどが回路の入力側に集中す
るので、らせん1は電子ビームの衝突によるダメージを
避けるため、らせん1の開始点を前述したようにずらし
ている。そしてその部分にはらせん1と同等の内径を有
し、融点の高い円筒状金属、例えばモリブデン等ででき
たビームカッタ18を配設してある。
FIG. 3 shows a cross-sectional view of a conventional slow wave circuit structure 20,
The drawing shows a cross-sectional view taken along the line BB in FIG. 3, but the spiral 1 is housed in an envelope 5 in which three dielectric support columns 2, 3, 4 are arranged around the outer periphery thereof. The envelope 5 is formed by alternately combining and joining discoid magnetic poles 6 and nonmagnetic cylindrical metal spacers 7. Disc-shaped shield parts 10 and 11 for joining the collector 8 and the electron gun 9 are provided at both ends of the envelope 5, and high-frequency windows 12 and 13 for inputting and outputting high-frequency waves are arranged in the vicinity of the parts to delay waves. The envelope 5 for the circuit is configured. Envelope 5
After the disk-shaped magnetic pole 6, the cylindrical metal spacer 7, the disk-shaped shield parts 10 and 11 and the input and output high-frequency windows 12 and 13 are joined by brazing, etc., the spiral 1 and 3 dielectric support columns 2,3,4
Forming and cutting of the hole for housing is performed. This is because the spiral 1 and the dielectric columns 2, 3 and 4 are inserted and fastened by shrink fitting, so the fastening allowance is set to an appropriate value and the hole This is because it is necessary to remove the irregularities on the inner peripheral surface and finish it into a mirror surface. The hole cutting allowance is generally 0,2 to 0,3 mm, and a gun drill is used for cutting. The length of the slow wave circuit 5 in the axial direction varies depending on the product, but when the circuit becomes long, it is a split type, so the length of one circuit is generally around 100 mm.
In addition, a shield component 10 for joining the electron gun 9 is provided on the electron gun 9 side.
It is often the case that the input high-frequency window 12 is disposed at the fifth annular half magnet (not shown). Speaking of the disk-shaped magnetic pole 6, an input high frequency window is provided on the cylindrical metal spacer 7 between the shield component 10 and the fourth and fifth magnetic poles. this is,
The passband characteristic of the traveling wave tube causes a temporary increase in the spiral current at start and stop, but at this time, most of the electron beam emitted from the electron gun is concentrated on the input side of the circuit, so spiral 1 is the electron beam. In order to avoid the damage caused by the collision, the starting point of spiral 1 is shifted as described above. A beam cutter 18 made of a cylindrical metal having a high melting point, such as molybdenum, having an inner diameter equal to that of the helix 1 is arranged in that portion.

従って、外囲器5は遅波回路の長さより更に長くな
る。外囲器5はガンドリルによる穴の切削加工後、その
穴にらせん及び3本の誘電体支柱2,3,4が焼ばね方式に
より挿入され締結固定されている。そしてらせん1の両
端は入出力の高周波窓12,13の中心軸導体14,15とそれぞ
れ接合されて遅波回路構体20を構成する。この遅波回路
構体20の出力端には、コレクタ8が、又入力端には電子
銃9が、回路端のシールド部品10,11と接合され、進行
波管と形成している。コレクタ8及び電子銃9は、それ
ぞれの接合端の封入皿16,17とシールド部品10,11が嵌合
し所望の同心度を得るよう設計されている。
Therefore, the envelope 5 becomes longer than the length of the slow wave circuit. In the envelope 5, after the hole is cut by a gun drill, a spiral and three dielectric support columns 2, 3, 4 are inserted and fastened and fixed in the hole by a firing spring method. Both ends of the spiral 1 are respectively joined to the central axis conductors 14 and 15 of the input and output high frequency windows 12 and 13 to form a slow wave circuit structure 20. A collector 8 is connected to the output end of the slow-wave circuit structure 20, and an electron gun 9 is connected to the input end of the slow-wave circuit structure 20 and shield components 10 and 11 at the circuit end to form a traveling wave tube. The collector 8 and the electron gun 9 are designed so that the enclosing pans 16 and 17 at their joint ends and the shield parts 10 and 11 are fitted to each other to obtain a desired concentricity.

〔発明が解決しようとする課題〕[Problems to be solved by the invention]

この従来の遅波回路構体20においては、軸方向長が10
0〜150mmの長さとなり、その中心部の穴を更に切削加工
し、内周面を鏡面仕上すると共に内径をミクロン単位で
管理する超精密加工が必要である。そのためガンドリル
による切削加工を行なっているが、その穴径によって
は、かなりの曲りが発生する。この曲りは、入出力間の
ゆるやかな曲りであるため、電子ビーム集束上特に問題
とはならず、良好なビーム透過特性が得られるが、遅波
回路構体20に電子銃9を接合する上で重大な問題とな
る。出力端のシールド部品11を基準にセンター出しを行
なって入力端方向へガンドリルで切削加工した場合、入
力端のシールド部品10との偏心はかなり大きな数字とな
る。従って、電子銃9はその接合端の封入皿16とシール
ド部品10との相互の嵌合により遅波回路構体20とのセン
ターが得られるよう設計されているため、シールド部品
10との偏心に応じて電子銃9と遅波回路構体20の穴との
中心は、当然それとほぼ同等のずれを生じる。このずれ
は電子銃9からの電子ビームの遅波回路構体20への入射
条件に重大な影響を及ぼしビーム透過特性の悪化をまね
き、正常な動作のさまたげとなる。
In this conventional slow wave circuit structure 20, the axial length is 10
The length is 0 to 150 mm, and it is necessary to further cut the hole at the center of the hole, mirror finish the inner peripheral surface, and perform ultra-precision processing to control the inner diameter in units of microns. For this reason, cutting is performed with a gun drill, but depending on the hole diameter, considerable bending occurs. Since this bend is a gentle bend between the input and the output, it does not cause any particular problem in focusing the electron beam, and good beam transmission characteristics can be obtained. However, in connecting the electron gun 9 to the slow wave circuit structure 20, It becomes a serious problem. When centering is performed with the shield component 11 at the output end as a reference and the gun end is cut in the direction of the input end, the eccentricity with the shield component 10 at the input end becomes a considerably large number. Therefore, the electron gun 9 is designed so that the center of the slow wave circuit structure 20 can be obtained by mutual fitting of the enclosing tray 16 at the joint end and the shield component 10.
Depending on the eccentricity with respect to 10, the center of the electron gun 9 and the center of the hole of the slow wave circuit structure 20 naturally deviates by about the same amount. This deviation seriously affects the conditions under which the electron beam from the electron gun 9 enters the slow-wave circuit structure 20 and causes deterioration of the beam transmission characteristics, which impedes normal operation.

〔課題を解決するための手段〕[Means for solving the problem]

本発明の遅波回路構体は、入力側高周波窓と入力端シ
ールド部品との間の任意の磁極部で分割した遅破回路本
体と入力部磁極組立とをそれぞれ独立して形成し、らせ
ん及び誘電体支柱を遅波回路に挿入した後、遅波回路と
入力部磁極組立とをろう付等により嵌合し、遅波回路構
体を構成している。
The slow-wave circuit structure of the present invention independently forms a slow-break circuit main body and an input-port magnetic pole assembly divided by an arbitrary magnetic pole portion between the input-side high-frequency window and the input-end shield component, and spiral and dielectric. After inserting the body support into the slow wave circuit, the slow wave circuit and the magnetic pole assembly of the input portion are fitted by brazing or the like to form a slow wave circuit structure.

〔実施例〕〔Example〕

本発明について図面を参照して説明する。第1図は本
発明の一実施例の遅波回路構体を用いた管球の断面図、
第2図は第1図のA−A断面図である。遅波回路構体41
は遅波回路31と入力部磁極組立32の二つのブロックに分
けられる。遅波回路の外囲器34は円板状磁極6と円筒状
金属スペーサ7、入出力の高周波窓12,13及び出力端に
はシールド部品11が入力側には接合部の磁極33とがろう
付結合され形成される。接合部磁極33は、入力側高周波
窓12から2つめの磁極となるよう構成されている。そし
て、外囲器34の中心穴を切削加工後、らせん1及び3本
の誘電体支柱2,3,4は焼ばめ法により外囲器34の中心穴
に挿入され締結固定される。その後らせん1の端は入出
力の高周波窓12,13の中心軸導体14,15にそれぞれ接合さ
れて遅波回路31が構成されている。
The present invention will be described with reference to the drawings. FIG. 1 is a sectional view of a tube using a slow wave circuit structure according to an embodiment of the present invention,
FIG. 2 is a sectional view taken along line AA of FIG. Slow wave circuit structure 41
Is divided into two blocks, a slow wave circuit 31 and an input magnetic pole assembly 32. The envelope 34 of the slow wave circuit has the disk-shaped magnetic pole 6, the cylindrical metal spacer 7, the high-frequency windows 12 and 13 for input and output, the shield component 11 at the output end, and the magnetic pole 33 at the junction on the input side. It is formed by being attached. The junction magnetic pole 33 is configured to be the second magnetic pole from the input side high frequency window 12. Then, after cutting the center hole of the envelope 34, the spiral 1 and the three dielectric columns 2, 3, 4 are inserted into the center hole of the envelope 34 by shrink fitting and fastened and fixed. After that, the ends of the spiral 1 are joined to the central axis conductors 14 and 15 of the input and output high frequency windows 12 and 13, respectively, to form a slow wave circuit 31.

一方入力部磁極組立32は、1個の接合部磁極33と2個
の円板状磁極6,3個の円筒状金属スペーサ7及び1個の
シールド部品10が組合せられ、ろう付結合されている。
そして内径は遅波回路の外囲器34の中心穴と同等に切削
加工された後、ビームカッタ18が配設されて形成され
る。接合部磁極33はそれぞれ円板状磁極6の厚さの約1/
2としている。
On the other hand, the input magnetic pole assembly 32 includes one joint magnetic pole 33, two disc-shaped magnetic poles 6, three cylindrical metal spacers 7 and one shield component 10, which are brazed together. .
Then, the inner diameter is machined in the same manner as the center hole of the envelope 34 of the slow wave circuit, and then the beam cutter 18 is disposed and formed. Each of the junction magnetic poles 33 is approximately 1 / thick of the thickness of the disk-shaped magnetic pole 6.
2

こうして形成された遅波回路31と入力部磁極組立32を
双方の接合部磁極33を突き合せ、高周波ろう付等により
接合する。この時、両方のセンターを合わせるため適当
なマンドリルを通してろう付接合する。このようにして
遅波回路構体41は形成される。
The slow wave circuit 31 and the input magnetic pole assembly 32 formed in this manner are joined to each other at their joint magnetic poles 33 and joined by high-frequency brazing or the like. At this time, brazing is performed through an appropriate mandrill to match both centers. In this way, the slow wave circuit structure 41 is formed.

外囲器34の出力端のシールド部品11の中心を基準にし
て切削加工した場合、入力端のシールド部品10とは、か
なりの偏心を生じる。一方、入力部磁極組立32の軸方向
長約10mm、内径、下穴及び削り代を外囲器34と同等とし
た場合、入力部シールド10及び接合部磁極33と切削後中
心穴との偏心は、許容できる範囲内に加工可能である。
これ等を適当なマンドリルを通して接合部磁極33どうし
を突合せ接合することにより、電子銃9と遅波回路構体
41との同心度をより良好な状態にすることができる。
When cutting is performed with the center of the shield component 11 at the output end of the envelope 34 as a reference, a considerable eccentricity occurs with the shield component 10 at the input end. On the other hand, when the axial length of the input magnetic pole assembly 32 is about 10 mm, the inner diameter, the prepared hole and the machining allowance are the same as those of the envelope 34, the eccentricity between the input shield 10 and the joint magnetic pole 33 and the center hole after cutting is It can be processed within an acceptable range.
These are butt-joined to each other through the appropriate magnetic mandrel to join the magnetic poles 33 of the joint portion, so that the electron gun 9 and the slow wave circuit structure
The concentricity with 41 can be improved.

〔発明の効果〕〔The invention's effect〕

以上説明したように、本発明は、入力側の磁極組立を
一部独立して形成した後、遅波回路と、らせん内径とビ
ームカッタ内径を基準に相互のセンターを合致させ接合
して構成される遅波回路構体である。従って電子銃と良
好な同心度が確保できるため、ビーム透過特性がより向
上するという効果を有する。
As described above, the present invention is configured by forming the magnetic pole assembly on the input side partially independently, and then joining the slow wave circuit and the centers of the helix and the beam cutter so that their centers match each other. It is a slow wave circuit structure. Therefore, since good concentricity with the electron gun can be secured, there is an effect that the beam transmission characteristics are further improved.

【図面の簡単な説明】 第1図は本発明の一実施例の管球断面図、第2図は第1
のA−A断面図、第3図は従来の遅波回路構体を用いた
管球断面図、第4図は第3図のB−B断面図である。 1……らせん、2,3,4……誘電体支柱、5,3,4……外囲
器、6……円板状磁極、7……円筒状金属スペーサ、8
……コレクタ、9……電子銃、10,11……円板状シール
ド部品、12,13……高周波窓、14,15……中心軸導体、1
6,17……封入皿、18……ビームカッタ、20,41……遅波
回路構体、31……遅波回路、32……入力部磁極組立、33
……接合部磁極。
BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 is a sectional view of a tube of an embodiment of the present invention, and FIG.
3 is a sectional view taken along line AA of FIG. 3, FIG. 3 is a sectional view of a tube using a conventional slow wave circuit structure, and FIG. 4 is a sectional view taken along line BB of FIG. 1 ... helix, 2,3,4 ... dielectric support, 5,3,4 ... enclosure, 6 ... disc-shaped magnetic pole, 7 ... cylindrical metal spacer, 8
…… Collector, 9 …… Electron gun, 10,11 …… Disc-shaped shield parts, 12,13 …… High frequency window, 14,15 …… Center axis conductor, 1
6,17 …… Enclosure tray, 18 …… Beam cutter, 20,41 …… Slow wave circuit structure, 31 …… Slow wave circuit, 32 …… Input part magnetic pole assembly, 33
...... Joint magnetic pole.

Claims (1)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】円板状磁極と円筒状金属スペーサを交互に
積層して固着し一端部に出力側高周波窓とコレクタを接
続する円板状シールド部品を有し他端部に入力側高周波
窓と接合部磁極を有する外囲器内にらせんおよび複数の
誘電支柱を内蔵してなる遅波回路と、円板状磁極と円筒
状金属スペーサを交互に積層して固着し一端部に電子銃
を接合する円板状シールド部品を有し他端部に接合部磁
極を有する入力側磁極組立とを、前記遅波回路と入力側
磁極組立の接合部磁極同士を付き合せて接合したことを
特徴とするらせん形遅波回路構体。
1. A disk-shaped shield component for alternately connecting an output-side high-frequency window and a collector, wherein disk-shaped magnetic poles and cylindrical metal spacers are alternately laminated and fixed, and an input-side high-frequency window is provided at the other end. And a slow wave circuit having a spiral and a plurality of dielectric struts in an envelope having a junction magnetic pole, a disk-shaped magnetic pole and a cylindrical metal spacer are alternately laminated and fixed, and an electron gun is attached to one end. An input side magnetic pole assembly having a disc-shaped shield component to be joined and a junction magnetic pole at the other end, and the joining magnetic poles of the slow wave circuit and the input side magnetic pole assembly are joined together. Swirl type slow wave circuit structure.
JP22292490A 1990-08-24 1990-08-24 Spiral slow wave circuit structure Expired - Lifetime JP2679378B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP22292490A JP2679378B2 (en) 1990-08-24 1990-08-24 Spiral slow wave circuit structure

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP22292490A JP2679378B2 (en) 1990-08-24 1990-08-24 Spiral slow wave circuit structure

Publications (2)

Publication Number Publication Date
JPH04106842A JPH04106842A (en) 1992-04-08
JP2679378B2 true JP2679378B2 (en) 1997-11-19

Family

ID=16789999

Family Applications (1)

Application Number Title Priority Date Filing Date
JP22292490A Expired - Lifetime JP2679378B2 (en) 1990-08-24 1990-08-24 Spiral slow wave circuit structure

Country Status (1)

Country Link
JP (1) JP2679378B2 (en)

Also Published As

Publication number Publication date
JPH04106842A (en) 1992-04-08

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