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JPH0568820B2 - - Google Patents
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JPH0568820B2 - - Google Patents

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Publication number
JPH0568820B2
JPH0568820B2 JP683386A JP683386A JPH0568820B2 JP H0568820 B2 JPH0568820 B2 JP H0568820B2 JP 683386 A JP683386 A JP 683386A JP 683386 A JP683386 A JP 683386A JP H0568820 B2 JPH0568820 B2 JP H0568820B2
Authority
JP
Japan
Prior art keywords
helix
slow
wave
circuit
crossed
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
JP683386A
Other languages
Japanese (ja)
Other versions
JPS62165836A (en
Inventor
Ryuzo Oorui
Yasuhiro Itagaki
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 JP683386A priority Critical patent/JPS62165836A/en
Priority to US07/003,197 priority patent/US4855644A/en
Publication of JPS62165836A publication Critical patent/JPS62165836A/en
Publication of JPH0568820B2 publication Critical patent/JPH0568820B2/ja
Granted 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、らせん形遅波回路を有する進行波管
に関するもので、特に二つのらせんからなる交叉
らせん形遅波回路の構成に関するものである。
[Detailed Description of the Invention] [Industrial Application Field] The present invention relates to a traveling wave tube having a helical slow-wave circuit, and particularly to the configuration of a crossed helical slow-wave circuit consisting of two spirals. .

〔従来の技術〕[Conventional technology]

進行波管は近年、衛星通信地球局用中継機の終
段の電力増幅管としての要求が増えてきている
が、かかる用途に於いては、高出力化が不可欠で
ある。高出力化に伴つて、その動作電圧及び電流
は当然高くかつ大きくなるが、電極管の絶縁確
保、熱放散手段の適正化及び所要ビーム電力の確
保等の必要性から、当然その外形、寸法は増大す
る。しかし一方、ユーザのニーズは車載、航空機
搭載等の移動用を含めて、小形軽量で、取扱いが
簡便かつ低消費電力形指向にある。したがつて進
行波管の外形寸法及び消費電力を増大することな
く、高出力化をはかること、すなわち高効率化を
はかる為の何かの手段をこうじることが必須とな
つてきた。
In recent years, there has been an increasing demand for traveling wave tubes as power amplifier tubes at the final stage of repeaters for satellite communication earth stations, and high output is essential for such applications. As the output increases, the operating voltage and current will naturally become higher and larger, but due to the need to ensure insulation of the electrode tube, appropriate heat dissipation means, and ensure the required beam power, the external shape and dimensions will naturally change. increase However, on the other hand, user needs are toward small, lightweight, easy-to-handle, and low-power consumption devices, including those for mobile use such as on-vehicle and aircraft-mounted devices. Therefore, it has become essential to increase the output of the traveling wave tube without increasing its external dimensions and power consumption, that is, to find some means to increase its efficiency.

従来、進行波管の遅波回路は融点の高いモリブ
デンやダングステンの線又はテープをらせん状に
成形したらせん形遅波回路が一般に用いられてき
たが、かかるらせん形遅波回路に於いては、すで
に種々高効率の手段がとられてきている。例えば
らせんの出力端に電子の速度低下に対応した速度
テーパピツチを付加した遅波回路とか、出力端ら
せん部の高周波損失を低減する為にらせんに金メ
ツキを施した遅波回路等がその一例である。しか
し更に高出力化をはかる為にらせんの空間高調波
の電力成分を押さえ、基本波の結合インピーダン
スを高めると同時に、後進波成分を低下せしめる
ようならせん構造とすることが必要となる。
Conventionally, the slow wave circuit of a traveling wave tube has generally been a spiral slow wave circuit formed by spirally molding molybdenum or dungsten wire or tape, which have a high melting point. Various highly efficient measures have already been taken. Examples include slow-wave circuits that have a velocity taper pitch added to the output end of the helix to accommodate the slowdown of electrons, and slow-wave circuits that have gold plating on the helix to reduce high-frequency loss at the output end of the helix. be. However, in order to achieve even higher output, it is necessary to create a helical structure that suppresses the power component of the spatial harmonics of the helix, increases the coupling impedance of the fundamental wave, and at the same time reduces the backward wave component.

その一方法として、電磁波を伝ぱんする第一の
らせんとこのらせんと同一ピツチで交叉する第二
のらせんとを結合、合体した様ないわゆる交叉ら
せん形遅波回路が公知である。この交叉らせん形
遅波回路に於いては、二つのらせんの伝ぱんモー
ドが重畳されて存在することになり、らせん系全
体としては、軸方向の基本波成分電界が強くなる
為、らせんの結合インピーダンスは高くなり従つ
て高い出力が得られることが知られている。しか
しながらかかる交叉らせん系遅波回路は、その回
路の形成が難しく、ほとんど実用に供されること
がなかつた。
As one method, a so-called crossed helical slow wave circuit is known, in which a first helix that propagates electromagnetic waves and a second helix that intersects this helix at the same pitch are combined and combined. In this crossed helical slow-wave circuit, the propagation modes of the two helices exist superimposed, and the fundamental wave component electric field in the axial direction becomes stronger in the helical system as a whole, so the helical coupling It is known that impedance becomes higher and therefore higher output can be obtained. However, such a crossed helical slow wave circuit is difficult to form and has almost never been put to practical use.

交叉らせん形遅波回路について詳述すると、第
2図は、交叉らせん形遅波回路を有する進行波管
の遅波回路構体1の一部を立体図で示したもので
あるが、交叉らせん2は電磁波を伝ぱんする第1
のらせん2′とこのらせん2′と交叉する逆巻きで
かつ同一ピツチを有する第2のらせん2″を二つ
のらせんを合成した形状をなしている。交叉らせ
ん2の外周部には複数本の誘電体支柱3が配設さ
れこれ等らせん2及び複数本の誘電体支柱3は、
円筒状金属外囲器4内に収納され適当な方法を用
いて締結固定されている。先に述べたように交叉
らせん2の形状は同一ピツチで互いに交叉するよ
うに二つのらせん2′,2″を合成してなるカゴ形
で円筒形をなす複雑な形状をしている。
To explain the crossed helical slow wave circuit in detail, FIG. is the first to propagate electromagnetic waves.
It has a shape that is a composite of two helices: a second helix 2' that intersects this helix 2' and has a reverse winding and the same pitch. On the outer periphery of the intersecting helix 2, a plurality of dielectric A body support 3 is provided, and these spirals 2 and a plurality of dielectric supports 3 are
It is housed in a cylindrical metal envelope 4 and fastened and fixed using an appropriate method. As mentioned above, the shape of the crossed helix 2 is a complicated cage-shaped cylindrical shape formed by combining two helices 2' and 2'' so as to intersect with each other at the same pitch.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

かかる交叉らせん形遅波回路構体1に於いては
交叉らせん2の成形が難しくほとんど実用に供す
ることは出来ない。
In such a crossed spiral slow-wave circuit structure 1, it is difficult to form the crossed spiral 2, and it is almost impossible to put it to practical use.

例えば放電加工等の手段を用いてもかかる交叉
らせんの成形が可能としても高い加工精度と複雑
な形状加工を要求される為、低い良品率、長い工
事時間などによりコスト高となり実用に供するこ
とは不可能である。
For example, even if it is possible to form such a crossed helix using means such as electric discharge machining, it requires high processing accuracy and complex shape processing, resulting in high costs due to low quality products and long construction time, making it difficult to put it to practical use. It's impossible.

〔問題点を解決するための手段〕[Means for solving problems]

本発明は、先に述べた交叉らせん形遅波回路の
構成を実用可能な形態に改良すると共に交叉らせ
んの効果をよりくふうを施した交叉らせん形遅波
回路を成形することにより、小形軽量で高効率な
進行波管を提供することを目的としている。
The present invention improves the configuration of the above-mentioned crossed helical slow-wave circuit to a practical form, and also molds a crossed helical slow-wave circuit in which the effect of the crossed helix is improved. The aim is to provide a highly efficient traveling wave tube.

すなわち本発明による進行波管に使用される交
叉らせん形遅波回路は電磁波を伝ぱんする第1の
らせんの外周部にもう一つの第2のらせんを重ね
まきし、かつ第2のらせんの巻きピツチを第1の
らせん巻ピツチより大きくとり、互いの回路長を
等しくなるよう成形している。
That is, the crossed helical slow-wave circuit used in the traveling wave tube according to the present invention has a first helix that propagates electromagnetic waves, and a second helix overlapping the outer periphery of the first helix that propagates electromagnetic waves. The pitch is larger than the first spiral winding pitch, and the circuit lengths are made equal to each other.

次に本発明の詳細について図を参照して説明す
る。第1図は本発明による進行波管の遅波回路構
体の立体図を示しており、遅波回路構体1は交叉
らせん2の外周部に3本の誘電体支柱3が配設さ
れ、これ等が円筒状金属外囲器4内に収納されて
構成されている。交叉らせん2は、電磁波を伝ぱ
んする第1のらせん5とこれと交叉するように逆
向きの第二のらせん6を前記第一のらせん5の外
周部に重ね捲きして成形されている。更に第二の
らせん6のピツチP2は第一のらせん5のピツチ
P1より大きくなるよう配慮されており、第一の
らせん5の上に第二のらせん6を同一ピツチで巻
いた時の第一のらせん5の回路長(展開長)を
l1、第二のらせん6の回路長(展開長)をl2とす
れば第二のらせん6のピツチP2は P2=l2/l1P1 となるように捲かれている。
Next, details of the present invention will be explained with reference to the drawings. FIG. 1 shows a three-dimensional diagram of a slow-wave circuit structure of a traveling wave tube according to the present invention. is housed in a cylindrical metal envelope 4. The crossed helix 2 is formed by overlapping a first helix 5 that propagates electromagnetic waves and a second helix 6 in the opposite direction so as to intersect with the first helix 5 on the outer periphery of the first helix 5. Furthermore, the pitch P2 of the second helix 6 is the pitch of the first helix 5.
It is designed to be larger than P 1 , and the circuit length (unfolded length) of the first helix 5 when the second helix 6 is wound on the first helix 5 at the same pitch is
l 1 and the circuit length (developed length) of the second helix 6 is l 2 , the pitch P 2 of the second helix 6 is wound so that P 2 =l 2 /l 1 P 1 .

〔発明の効果〕〔Effect of the invention〕

以上説明したように本発明による進行波管に於
いては、交叉らせん形遅波回構体が極めて容易に
かつ安価で実現可能となると共に、二つのらせん
の位相のずれを修正し、交叉らせんの効果を減ず
ることのないよう成形しているので、小型軽量で
より高効率な進行波管を提供することが可能であ
る。このことは、交叉らせん2を形成する第1の
らせん5と第2のらせん6は、第1のらせん5の
上に第2のらせん6を重ね捲きしている関係で同
一ピツチである場合、二つのらせん5,6の回路
長は等しくならない。すなわち第二のらせん6は
第1のらせん5より捲径が大きいのでその分回路
長が長くなり、電磁波の有効な伝ぱんモードに位
相差が生じる。この位相のずれは、遅波回路1の
軸方向の基本波成分電界を弱め、結合インピーダ
ンスの低下につながるため、出力の低下をきたし
交叉らせんとする効果を減じることになる。
As explained above, in the traveling wave tube according to the present invention, a crossed spiral slow wave circuit structure can be realized very easily and at low cost, and the phase shift between the two spirals can be corrected, and the crossed spiral slow wave structure can be realized very easily and at low cost. Since it is molded without reducing its effectiveness, it is possible to provide a traveling wave tube that is smaller, lighter, and more efficient. This means that if the first helix 5 and the second helix 6 forming the crossed helix 2 have the same pitch because the second helix 6 is wound over the first helix 5, The circuit lengths of the two helices 5 and 6 are not equal. That is, since the second helix 6 has a larger winding diameter than the first helix 5, the circuit length becomes longer, and a phase difference occurs in the effective propagation mode of the electromagnetic waves. This phase shift weakens the fundamental wave component electric field in the axial direction of the slow wave circuit 1 and leads to a decrease in coupling impedance, resulting in a decrease in output and a reduction in the cross-helix effect.

従つて、前述したように、第1のらせん5と第
2のらせん6の回路長が等しくなるよう、第2の
らせん6のピツチを大きめにして捲いて交叉らせ
ん2を成形している。
Therefore, as described above, the crossed helix 2 is formed by winding the second helix 6 with a larger pitch so that the circuit lengths of the first helix 5 and the second helix 6 are equal.

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

第1図は、本発明の実施例による進行波管の遅
波回路構体の立体図、第2図は従来の進行波管の
遅波回路構体の立体図を示す。 1……遅波回路構体、2……交叉らせん、2′,
2″,5,6……らせん、3……誘電体支柱、4
……円筒状金属外囲器。
FIG. 1 shows a three-dimensional view of a slow-wave circuit structure of a traveling-wave tube according to an embodiment of the present invention, and FIG. 2 shows a three-dimensional view of a conventional slow-wave circuit structure of a traveling-wave tube. 1...Slow wave circuit structure, 2...Cross helix, 2',
2″, 5, 6... Helix, 3... Dielectric support, 4
...A cylindrical metal envelope.

Claims (1)

【特許請求の範囲】[Claims] 1 電磁波を伝ぱんする互に交叉した2つのらせ
んで形成される交叉らせん遅波回路を有する進行
波管に於いて前記電磁波を伝ぱんするらせん所定
のピツチで捲いた第1のらせんの上に第1のらせ
んと逆向きの方向に、第2のらせんを重ね捲きし
かつ前記第1のらせんの回路長と第2のらせんの
回路長とが等しくなるごとく前記第2のらせんの
ピツチを第1のらせんのピツチより大きく捲いて
構成された遅波回路を有する進行波管。
1. In a traveling wave tube having a crossed helical slow wave circuit formed by two intersecting helices that propagate electromagnetic waves, the helix that propagates the electromagnetic waves is wound at a predetermined pitch on top of the first helix. A second helix is wound in a direction opposite to that of the first helix, and the pitch of the second helix is adjusted so that the circuit length of the first helix is equal to the circuit length of the second helix. A traveling wave tube that has a slow wave circuit that is wound larger than the pitch of the first spiral.
JP683386A 1986-01-14 1986-01-14 Traveling-wave tube Granted JPS62165836A (en)

Priority Applications (2)

Application Number Priority Date Filing Date Title
JP683386A JPS62165836A (en) 1986-01-14 1986-01-14 Traveling-wave tube
US07/003,197 US4855644A (en) 1986-01-14 1987-01-14 Crossed double helix slow-wave circuit for use in linear-beam microwave tube

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP683386A JPS62165836A (en) 1986-01-14 1986-01-14 Traveling-wave tube

Publications (2)

Publication Number Publication Date
JPS62165836A JPS62165836A (en) 1987-07-22
JPH0568820B2 true JPH0568820B2 (en) 1993-09-29

Family

ID=11649230

Family Applications (1)

Application Number Title Priority Date Filing Date
JP683386A Granted JPS62165836A (en) 1986-01-14 1986-01-14 Traveling-wave tube

Country Status (1)

Country Link
JP (1) JPS62165836A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0858776A (en) * 1994-08-25 1996-03-05 Gurapatsuku Japan Kk Product housing box

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP4835331B2 (en) * 2006-09-04 2011-12-14 株式会社デンソー Processing device with open / close door

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0858776A (en) * 1994-08-25 1996-03-05 Gurapatsuku Japan Kk Product housing box

Also Published As

Publication number Publication date
JPS62165836A (en) 1987-07-22

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