JPH04106840A - Collector for electron beam tube - Google Patents
Collector for electron beam tubeInfo
- Publication number
- JPH04106840A JPH04106840A JP22292390A JP22292390A JPH04106840A JP H04106840 A JPH04106840 A JP H04106840A JP 22292390 A JP22292390 A JP 22292390A JP 22292390 A JP22292390 A JP 22292390A JP H04106840 A JPH04106840 A JP H04106840A
- Authority
- JP
- Japan
- Prior art keywords
- electron beam
- collector electrode
- collector
- gas discharge
- hole
- 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.)
- Granted
Links
Landscapes
- Microwave Tubes (AREA)
Abstract
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。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a collector for an electron beam tube, and more particularly to a collector for an electron beam tube with 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。A collector for a traveling wave tube consists of an electrode that captures the electron beam that has finished interacting with high frequencies in a slow wave circuit.
When the electron beam hits the collector electrode, the kinetic energy of the electron beam is converted into thermal energy. 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
術の進歩と相俟って、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。Incidentally, in recent years, the frequency of traveling wave tubes has been increasing, and together with advances in manufacturing technology, traveling wave tubes that operate in a millimeter wave band with a frequency of 30 GHz or higher have been developed.
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 millimeter-wave band traveling wave tubes, the inner diameter of the helix constituting the slow-wave circuit is as small as about 0.5 mm, and the diameter of the electron beam passage hole at the collector entrance also changes from the inside of the collector back to the helix section, corresponding to this diameter. In order to suppress electrons, 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 structure of the collector is electrically insulated from the slow wave circuit section 2 by an insulating stone 3, and the collector electrode 21 on the slow wave circuit section 2 side has a conical shape. are doing. A single electron beam passage hole 4 through which the electron beam passes is opened at the apex of this conical partition, and the side and bottom surfaces connected to the conical partition 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くいずれも図示せず
)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 passes through the electron beam passage hole through which the electron beam passes through, for example, to a getter provided on the electron gun side. , or an ion pump provided at the output section (none of which is shown). However, in millimeter-wave band traveling wave tubes, the diameter of the electron beam passing hole at the tip of the partition wall of the collector electrode is small, so the exhaust resistance to gas increases and the degree of vacuum inside the collector deteriorates. Therefore, there is a problem in that ions are generated when the electron beam collides with gas molecules, causing problems such as fluctuations in 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。SUMMARY OF THE INVENTION An object of the present invention is to provide an electron beam tube that does not cause problems such as fluctuations in helix current and accelerated deterioration of the cathode.
〔課題を解決するための手段〕
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。[Means for Solving the Problems] The present invention provides a bottom surface and a side surface forming a vacuum envelope, and an electron beam passing hole connected to the side surface and located on the central axis of the electron beam on the slow wave circuit side. In the electron beam tube collector having a partition wall housed in a vacuum envelope, the partition wall is provided with 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。FIGS. 1(a) and 1(b) are a sectional view and a view taken along the line A-A' of a collector for a traveling wave tube 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
へソックス5の内径より若干大きくしている。In the first embodiment, as shown in FIG. 1<a) and (b),
Collector electrode 1 is electrically insulated by slow wave circuit 2 and insulating stone 3. The partition wall of the collector electrode 1 has a conical shape, and an electron beam passage hole 4 through which the electron beam passes is opened at the apex of the conical partition wall. The diameter of this hole is slightly larger than the inner diameter of the hesock 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の孔径りは、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。Furthermore, a plurality of exhaust holes 6 are opened in the conical partition wall, and have the role of exhausting gas generated within the collector electrode 1. The direction of the exhaust hole 6 is determined with consideration given to preventing the electron beam that has entered the collector electrode 1 from passing through to the outside of the collector electrode 1 again. Further, the diameter of the exhaust hole 6 is made smaller than the flow length L of the exhaust hole 6 to prevent electrons in the collector electrode 1 from easily passing through.
なお、念の為、排気用孔6を通してコレクタ電極1から
遅波口R2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をシールドする
部品を付ける構造も考えられる。As a precaution, a part that shields the exhaust hole 6 is attached to the slow wave circuit side of the conical partition wall of the collector electrode 1 to prevent electrons from going backward from the collector electrode 1 to the slow wave port R2 through the exhaust hole 6. Structure can also be considered.
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
断面図である。FIG. 2 is a sectional view of a traveling wave tube collector 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1
1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 in which the tip shape of the first partition wall 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を設けることによ
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 is cylindrical, the same effect as in the first embodiment can be obtained by providing the exhaust hole 6 on the side surface of the cylinder.
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 this embodiment, the case where the number of stages of collector electrodes is one is described, but the present invention can be applied to the collector electrode closest to the slow wave circuit even in the case of a multi-stage collector.
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 is not limited to traveling wave tubes, but can be applied to various types of electron beam tubes including 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 explained above, in the present invention, since a plurality of exhaust holes are provided in the partition wall of the collector electrode, even when the electron beam passing hole diameter of the collector electrode is small as in a millimeter wave band traveling wave tube, the collector electrode The gas generated is exhausted through the exhaust holes in this partition wall. Therefore, gas molecules in the collector electrode are less likely to be ionized by electron beam collisions, eliminating drawbacks such as fluctuations in helix current and accelerated cathode deterioration, resulting in a highly reliable traveling wave tube. 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.・
・ヘワックス、6・・・排気用孔。FIGS. 1(a) and (b) are a cross-sectional view and a view taken along the line A-A' of a collector for a traveling wave tube according to a first embodiment of the present invention, and FIG. 2 is a progress view of a collector for a traveling wave tube according to a second embodiment of the present invention. 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.・
・Hewax, 6...Exhaust hole.
Claims (1)
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。It has a bottom surface and a side surface forming a vacuum envelope, and a partition wall connected to the side surface and having an electron beam passing hole on the central axis of the electron beam on the slow wave circuit side and housed in the vacuum envelope. What is claimed is: 1. A collector for an electron beam tube, characterized in that 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 true JPH04106840A (en) | 1992-04-08 |
| JP2679377B2 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) |
Citations (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
Patent Citations (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS6030035A (en) * | 1983-07-29 | 1985-02-15 | Nec Corp | Collector for electron tube |
Also Published As
| Publication number | Publication date |
|---|---|
| JP2679377B2 (en) | 1997-11-19 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| EP0282467B1 (en) | Hollow cathode ion sources | |
| US2410054A (en) | Electron discharge apparatus | |
| JPS6398938A (en) | Magnetron | |
| US3278791A (en) | Electron discharge device having a plurality of emissive surfaces | |
| US3626230A (en) | Thermally conductive electrical insulator for electron beam collectors | |
| JPH0624099B2 (en) | Improved electron gun | |
| US3312857A (en) | Microwave amplifier utilizing multipaction to produce periodically bunched electrons | |
| US2200722A (en) | Electron discharge device | |
| JP3147227B2 (en) | Cold cathode electron gun | |
| US3466493A (en) | Circuit sever for ppm focused traveling wave tubes | |
| US2813990A (en) | Electron beam discharge device | |
| JP2679377B2 (en) | Collector for electron beam tube | |
| CA1131362A (en) | Transit-time tubes | |
| JPS594819B2 (en) | ion source | |
| US2929955A (en) | Cavity resonator for klystron tube | |
| US4839554A (en) | Apparatus for forming an electron beam sheet | |
| US3250947A (en) | Discharge device having electron grids with heights rising substantially above the grid support rims | |
| US3073987A (en) | Electron discharge device with getter | |
| US3328628A (en) | Electron tube employing a relatively long electron beam and getter material disposedat the collector | |
| US4123684A (en) | Thyratrons | |
| US3683235A (en) | Electron discharge devices | |
| JPS6229862B2 (en) | ||
| JP3079559B2 (en) | Traveling wave tube collector | |
| US2888599A (en) | Electron discharge apparatus | |
| CN119764147B (en) | An electron gun comprising segmented insulating ceramic |