JP2679377B2 - Collector for electron beam tube - Google Patents
Collector for electron beam tubeInfo
- Publication number
- JP2679377B2 JP2679377B2 JP2222923A JP22292390A JP2679377B2 JP 2679377 B2 JP2679377 B2 JP 2679377B2 JP 2222923 A JP2222923 A JP 2222923A JP 22292390 A JP22292390 A JP 22292390A JP 2679377 B2 JP2679377 B2 JP 2679377B2
- Authority
- JP
- Japan
- Prior art keywords
- electron beam
- collector
- collector electrode
- partition wall
- tube
- 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
Links
Landscapes
- Microwave Tubes (AREA)
Description
【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、電子ビーム管用コレクタに関し、特にミリ
波帯の動作周波数の電子ビーム管用コレクタに関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an electron beam tube collector, and more particularly to an electron beam tube collector having an operating frequency in the millimeter wave band.
進行波管用コレクタは、遅波回路で高周波との相互作
用が終わった電子ビームを捕捉する電極からなってお
り、電子ビームがコレクタ電極に当った時に電子ビーム
の持つ運動エネルギーが熱エネルギーに変換される。従
って、コレクタ電極は、高温に加熱されコレクタ電極を
なす金属からはガスが放出される。The traveling wave tube collector consists of an electrode that captures the electron beam that has interacted with high frequencies in the slow wave circuit.When the electron beam hits the collector electrode, the kinetic energy of the electron beam is converted into thermal energy. It Therefore, the collector electrode is heated to a high temperature and gas is released from the metal forming the collector electrode.
ところで、近年、進行波管は、高周波数化が進み製造
技術の進歩と相埃って、周波数が30GHz以上のミリ波帯
で動作させる進行波管が開発されるようになった。By the way, in recent years, traveling wave tubes have come to be developed to operate in the millimeter wave band with a frequency of 30 GHz or higher, in line with the progress of higher frequencies and dust of progress in manufacturing technology.
このようなミリ波帯進行波管では、遅波回路を構成す
るヘリックスの内径が0.5mm程度と小さくなり、この径
に応じてコレクタ入口の電子ビーム通過孔径もコレクタ
内部からヘリックス部に戻る逆行電子抑制の為、ヘリッ
クス内径程度に小さくする必要がある。In such a millimeter wave band traveling wave tube, the inner diameter of the helix that constitutes the slow wave circuit becomes as small as about 0.5 mm, and the electron beam passage hole diameter at the collector inlet also returns from the inside of the collector to the helix part according to this diameter. In order to suppress it, it is necessary to make it as small as the inner diameter of the helix.
一方、コレクタの構造は、第3図に示すように、遅波
回路部2とは絶縁石3で電気的に絶縁されており、遅波
回路部2側のコレクタ電極21の形状は円錐形をしてい
る。この円錐形の隔壁の頂点には電子ビームが通り抜け
るただ一つの電子ビーム通過孔4が開いており、円錐形
の隔壁に接続する側面及び底面は真空外囲器を形成して
いる。On the other hand, as shown in FIG. 3, the collector structure is electrically insulated from the slow wave circuit unit 2 by an insulating stone 3, and the shape of the collector electrode 21 on the slow wave circuit unit 2 side is a conical shape. doing. Only one electron beam passage hole 4 through which the electron beam passes is formed at the apex of the conical partition wall, and the side surface and the bottom surface connected to the conical partition wall form a vacuum envelope.
このようなコレクタの構造において、電子ビームがコ
レクタ電極内壁に衝突し発熱することによって発生する
ガスは、前述の電子ビームが通り抜ける電子ビーム通過
孔を通って、例えば、電子銃側に設けられたゲッタ、或
は、出力部に設けられたイオンポンプ(いずれも図示せ
ず)に吸収される。しかし、ミリ波帯進行波管では、こ
のコレクタ電極の隔壁の先端の電子ビーム通過孔径が小
さい為、ガスに対する排気抵抗が大きくなりコレクタ内
部の真空度が劣化する。その為、ガス分子に電子ビーム
が衝突することによってイオンが発生し、ヘリックス電
流の変動やカソードの劣化を早めるなどの弊害を発生さ
せる問題点がある。In such a collector structure, the gas generated when the electron beam collides with the inner wall of the collector electrode and generates heat is passed through the electron beam passage hole through which the electron beam passes, for example, a getter provided on the electron gun side. Alternatively, it is absorbed by an ion pump (not shown) provided in the output section. However, in the millimeter wave band traveling wave tube, since the electron beam passage hole diameter at the tip of the partition wall of the collector electrode is small, the exhaust resistance to gas becomes large and the degree of vacuum inside the collector deteriorates. Therefore, there is a problem that ions are generated by the collision of the electron beam with the gas molecules, which causes adverse effects such as fluctuation of the helix current and accelerated deterioration of the cathode.
本発明の目的は、ヘリックス電流の変動やカソードの
劣化を早めるなどの弊害の発生のない電子ビーム管を提
供することにある。An object of the present invention is to provide an electron beam tube that does not cause any adverse effects such as fluctuations in helix current and accelerated deterioration of the cathode.
本発明は、真空外囲器を形成する底面と側面と、該側
面に接続し遅波回路部側の電子ビームの中心軸上に電子
ビーム通過孔を備え前記真空外囲器内に収容された隔壁
とを有する電子ビーム管用コレクタにおいて、前記隔壁
に複数個の排気用孔が設けられている。The present invention includes a bottom surface and a side surface forming a vacuum envelope, and an electron beam passage hole connected to the side surface and on the central axis of the electron beam on the side of the slow wave circuit unit and housed in the vacuum envelope. In a collector for an electron beam tube having a partition, the partition has a plurality of exhaust holes.
次に、本発明の実施例について図面を参照して説明す
る。Next, embodiments of the present invention will be described with reference to the drawings.
第1図(a),(b)は本発明の第1の実施例の進行
波管用コレクタの断面図及びA−A′矢視図である。1 (a) and 1 (b) are a sectional view and a view taken along the line AA 'of a traveling wave tube collector according to a first embodiment of the present invention.
第1の実施例は、第1図(a),(b)に示すよう
に、コレクタ電極1は遅波回路2と絶縁石3により電気
的に絶縁されている。コレクタ電極1の隔壁の形状は、
円錐形をしており、円錐形の隔壁の頂点には電子ビーム
が通り抜ける電子ビーム通過孔4が開いている。この孔
径はヘリックス5の内径より若干大きくしている。In the first embodiment, as shown in FIGS. 1A and 1B, the collector electrode 1 is electrically insulated by the slow wave circuit 2 and the insulating stone 3. The shape of the partition wall of the collector electrode 1 is
It has a conical shape, and an electron beam passage hole 4 through which an electron beam passes is opened at the apex of the conical partition wall. The hole diameter is slightly larger than the inner diameter of the helix 5.
さらに、円錐形の隔壁には複数個の排気用孔6が開い
ており、コレクタ電極1内で発生したガスを排気する役
目を持っている。この排気用孔6の方向は、コレクタ電
極1内に入った電子ビームが再びコレクタ電極1外に通
り抜けないように考慮されて決められている。また、排
気用孔6の孔径Dは、排気用孔6の流さLより小さくし
て、コレクタ電極1内の電子が容易に通り抜けないよう
にしている。Further, a plurality of exhaust holes 6 are opened in the conical partition wall, and has a role of exhausting gas generated in the collector electrode 1. The direction of the exhaust hole 6 is determined in consideration of the electron beam entering the collector electrode 1 from passing through the outside of the collector electrode 1 again. Further, the hole diameter D of the exhaust hole 6 is made smaller than the flow L of the exhaust hole 6 so that the electrons in the collector electrode 1 cannot easily pass through.
なお、念の為、排気用孔6を通してコレクタ電極1か
ら遅波回路2に電子が逆行しないようにコレクタ電極1
の円錐形の隔壁の遅波回路側に排気用孔6をシードする
部品を付ける構造も考えられる。In addition, as a precaution, the collector electrode 1 should be prevented from flowing backward from the collector electrode 1 to the slow wave circuit 2 through the exhaust hole 6.
It is also conceivable to attach a component for seeding the exhaust hole 6 to the slow wave circuit side of the conical partition wall.
第2図は本発明の第2の実施例の進行波管用のコレク
タの断面図である。FIG. 2 is a sectional view of a collector for a traveling wave tube according to a second embodiment of the present invention.
第2の実施例は、第2図に示すように、コレクタ電極
11の隔壁の先端形状が円錐形状を成していない場合の例
である。In the second embodiment, as shown in FIG.
This is an example of the case where the tip shape of the partition wall of 11 does not have a conical shape.
すなわち、コレクタ電極11の隔壁の先端部分が円筒形
状の場合には、円筒側面に排気用孔6を設れることによ
っても第1の実施例と同じ効果が得られる。That is, when the tip of the partition wall of the collector electrode 11 has a cylindrical shape, the same effect as that of the first embodiment can be obtained by providing the exhaust hole 6 on the cylindrical side surface.
なお、本実施例では、コレクタ電極の段数を1段の場
合で説明したが、多段コレクタの場合においても、遅波
回路に最も近いコレクタ電極に適用できる。In the present embodiment, the case where the number of stages of the collector electrode is one has been described, but even in the case of a multi-stage collector, it can be applied to the collector electrode closest to the slow wave circuit.
また、本発明は用途が進行波管に限定されるべきもの
ではなく、クライストロンをはじめ多種の電子ビーム管
に適用可能である。Further, the application of the present invention should not be limited to traveling wave tubes, but can be applied to various electron beam tubes such as klystrons.
以上説明したように本発明は、コレクタ電極の隔壁に
複数個の排気用孔を設けているので、ミリ波帯用進行波
管のようにコレクタ電極の電子ビーム通過孔径が小さい
場合でも、コレクタ電極で発生したガスは、この隔壁の
排気用孔を通して排気される。従って、コレクタ電極内
でガス分子が電子ビームの衝突によってイオン化される
ことが少なくなるので、ヘリックス電流の変動やカソー
ドの劣化を早めるなどの欠点が除去され、信頼性の高い
進行波管が得られる効果がある。As described above, according to the present invention, since the plurality of exhaust holes are provided in the partition wall of the collector electrode, even if the electron beam passage hole diameter of the collector electrode is small like a traveling wave tube for the millimeter wave band, the collector electrode The gas generated in 1 is exhausted through the exhaust hole of this partition. Therefore, gas molecules are less likely to be ionized in the collector electrode due to collision of the electron beam, and defects such as fluctuation of the helix current and accelerated deterioration of the cathode are eliminated, and a highly reliable traveling wave tube can be obtained. effective.
第1図(a),(b)は本発明の第1の実施例の進行波
管用コレクタの断面図及びA−A′矢視図、第2図は本
発明の第2の実施例の進行波管用コレクタの断面図、第
3図は従来の電子ビーム管用コレクタの一例の断面図で
ある。 1,11,21……コレクタ電極、2……遅波回路、3……絶
縁石、4……電子ビーム通過孔、5……ヘリックス、6
……排気用孔。FIGS. 1 (a) and 1 (b) are a sectional view and a sectional view taken along the line AA 'of the traveling wave tube collector of the first embodiment of the present invention, and FIG. 2 is a progression of the second embodiment of the present invention. FIG. 3 is a sectional view of a collector for a wave tube, and FIG. 3 is a sectional view of an example of a conventional collector for an electron beam tube. 1,11,21 …… Collector electrode, 2 …… Slow wave circuit, 3 …… Insulating stone, 4 …… Electron beam passage hole, 5 …… Helix, 6
...... Exhaust hole.
Claims (1)
面に接続し遅波回路部側の電子ビームの中心軸上に電子
ビーム通過孔を備え前記真空外囲器内に収容された隔壁
とを有する電子ビーム管用コレクタにおいて、前記隔壁
に複数個の排気用孔を設けたことを特徴とする電子ビー
ム管用コレクタ。1. A vacuum envelope is provided with a bottom surface and a side surface, and an electron beam passage hole connected to the side surface and on the central axis of the electron beam on the side of the slow wave circuit section and housed in the vacuum envelope. An electron beam tube collector having a partition wall, wherein the partition wall is provided with a plurality of exhaust holes.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2222923A JP2679377B2 (en) | 1990-08-24 | 1990-08-24 | Collector for electron beam tube |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2222923A JP2679377B2 (en) | 1990-08-24 | 1990-08-24 | Collector for electron beam tube |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH04106840A JPH04106840A (en) | 1992-04-08 |
| JP2679377B2 true JP2679377B2 (en) | 1997-11-19 |
Family
ID=16789984
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP2222923A Expired - Lifetime JP2679377B2 (en) | 1990-08-24 | 1990-08-24 | Collector for electron beam tube |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP2679377B2 (en) |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS6030035A (en) * | 1983-07-29 | 1985-02-15 | Nec Corp | Collector for electron tube |
-
1990
- 1990-08-24 JP JP2222923A patent/JP2679377B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPH04106840A (en) | 1992-04-08 |
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