JPH0117082Y2 - - Google Patents
Info
- Publication number
- JPH0117082Y2 JPH0117082Y2 JP18031282U JP18031282U JPH0117082Y2 JP H0117082 Y2 JPH0117082 Y2 JP H0117082Y2 JP 18031282 U JP18031282 U JP 18031282U JP 18031282 U JP18031282 U JP 18031282U JP H0117082 Y2 JPH0117082 Y2 JP H0117082Y2
- Authority
- JP
- Japan
- Prior art keywords
- electron beam
- magnetic field
- traveling wave
- permanent magnet
- wave 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
Links
- 238000010894 electron beam technology Methods 0.000 claims description 22
- 230000000737 periodic effect Effects 0.000 claims description 2
- GUTLYIVDDKVIGB-UHFFFAOYSA-N cobalt atom Chemical compound [Co] GUTLYIVDDKVIGB-UHFFFAOYSA-N 0.000 claims 1
- 229910052761 rare earth metal Inorganic materials 0.000 claims 1
- 150000002910 rare earth metals Chemical class 0.000 claims 1
- 230000005540 biological transmission Effects 0.000 description 7
- 230000008878 coupling Effects 0.000 description 3
- 238000010168 coupling process Methods 0.000 description 3
- 238000005859 coupling reaction Methods 0.000 description 3
- 230000007423 decrease Effects 0.000 description 1
- 238000000605 extraction Methods 0.000 description 1
- 230000017525 heat dissipation Effects 0.000 description 1
- 230000003993 interaction Effects 0.000 description 1
- 230000007704 transition Effects 0.000 description 1
Landscapes
- Microwave Tubes (AREA)
Description
【考案の詳細な説明】
本考案は電子ビーム集束装置として、周期永久
磁石(P.P.M)を使用した進行波管の電子ビーム
集束装置に関する。[Detailed Description of the Invention] The present invention relates to a traveling wave tube electron beam focusing device using a periodic permanent magnet (PPM) as an electron beam focusing device.
進行波管は電子ビームを射出する電子銃、電子
ビームを補捉するコレクタ、電子ビームとの相互
作用により回路波を増幅させる遅波回路部、遅波
回路部に回路波を損失なく入射させる入力結合
部、遅波回路部から回路波を損失なく負荷に伝達
するための出力結合部、及び電子ビームを集束す
る為の磁界を与える電子ビーム集束装置等から成
る。 A traveling wave tube is an electron gun that emits an electron beam, a collector that captures the electron beam, a slow wave circuit that amplifies the circuit wave through interaction with the electron beam, and an input that allows the circuit wave to enter the slow wave circuit without loss. It consists of a coupling section, an output coupling section for transmitting the circuit wave from the slow wave circuit section to the load without loss, and an electron beam focusing device that provides a magnetic field for focusing the electron beam.
PPMによる電子ビーム集束は、遅波回路部の
構造が比較的簡単であり、その外径が比較的小さ
いという特徴を有するヘリツクス形進行波管で多
く用いられているが小形軽量化が可能である事及
び取扱いが容易であるという特徴を有する為結合
空胴形進行波管にも用いられている。 Electron beam focusing using PPM is often used in helical traveling wave tubes, which have a relatively simple slow-wave circuit structure and a relatively small outer diameter, but can be made smaller and lighter. It is also used in coupled cavity traveling wave tubes because it is easy to use and handle.
ここではヘリツクス形進行波管を例にとつて述
べる。一般に用いられているヘリツクス形進行波
管は、ヘリツクス(ら線)が熱的に弱い為電子ビ
ーム集束を行なうPPMの設計にあたつては電子
ビームの透過特性を充分良好に保つよう考慮され
なければならない。通常PPMにより与えられる
磁界強度はブリリアン集束磁界強度の約2倍の強
さに設計される。又電子ビームが遅波回路部を安
定に、しかもビームリツプルが出来るだけ小さい
状態で通過するようカソードと交叉する磁界強度
が決定される。 Here, we will discuss a helical traveling wave tube as an example. Generally used helical traveling wave tubes have helices (helical lines) that are thermally weak, so when designing a PPM that focuses electron beams, consideration must be given to maintaining sufficiently good electron beam transmission characteristics. Must be. Normally, the magnetic field strength provided by PPM is designed to be approximately twice as strong as the Brilliant focusing magnetic field strength. Further, the strength of the magnetic field crossing the cathode is determined so that the electron beam passes through the slow wave circuit section stably and with as little beam ripple as possible.
このようにPPMの磁界強度はカソードと交叉
する磁界強度と一様磁界強度部とその遷移領域及
びコレクタ部と交叉する磁界強度とから構成され
る。ヘリツクス形進行波管の場合、光に述べたよ
うにヘリツクスが熱的に弱い為電子ビーム透過特
性を良好に保たないと最悪の場合ヘリツクスを損
焼し進行波管の信頼性を著しく低下するものであ
る。それ故、PPMの設計はヘリツクス形進行波
管を設計するにあたつては充分に検討を加えなけ
れば進行波管の信頼性を著しく低下させるものと
なつてしまう。 In this way, the magnetic field strength of PPM is composed of the magnetic field strength crossing the cathode, the uniform magnetic field strength part, the transition region thereof, and the magnetic field strength crossing the collector part. In the case of a helix type traveling wave tube, as mentioned in the section on light, the helix is thermally weak, so if the electron beam transmission characteristics are not maintained well, in the worst case, the helix will burn out and the reliability of the traveling wave tube will drop significantly. It is something. Therefore, when designing a helical traveling wave tube, the PPM design will significantly reduce the reliability of the traveling wave tube unless sufficient consideration is given.
本考案はPPMの一様磁界強度部の磁界を、良
好に保つようPPMを構成するポールピースの外
径を永久磁石の外径より少なくとも1つ以上小さ
くすることにより電子ビームの安定性を得ること
を特徴とした進行波管を提供するものである。 The present invention achieves stability of the electron beam by making the outer diameter of the pole piece that constitutes the PPM smaller than the outer diameter of the permanent magnet by at least one point in order to maintain a good magnetic field in the uniform magnetic field strength part of the PPM. The present invention provides a traveling wave tube characterized by:
第1図は一般に用いられている進行波管の電子
ビーム集束装置を示すものである。第1図におい
て、集束装置(P.P.M)は複数個のポールピース
1、と複数個の永久磁石2から成る。又、入出力
結合器3が遅波回路のほぼ両端に設けられてい
る。入出力結合器3は通常一つの永久磁石の一部
を通つて外部に接続される。入出力結合器3を設
けた場所の永久磁石は第2図に示すように一部に
切欠きを設けている。その為、この磁石から得ら
れる磁界強度は他の部分より低下してしまい、磁
界強度の一様性を得ることは出来ない。その補正
をする為にこの部分の永久磁界の外径を大きくす
ることで、磁界強度を一様に保つている。 FIG. 1 shows a commonly used traveling wave tube electron beam focusing device. In FIG. 1, the focusing device (PPM) consists of a plurality of pole pieces 1 and a plurality of permanent magnets 2. Further, input/output couplers 3 are provided almost at both ends of the slow wave circuit. The input/output coupler 3 is normally connected to the outside through a part of one permanent magnet. The permanent magnet at the location where the input/output coupler 3 is provided is partially cut out as shown in FIG. Therefore, the magnetic field strength obtained from this magnet is lower than that of other parts, and uniformity of the magnetic field strength cannot be obtained. To compensate for this, the outer diameter of the permanent magnetic field in this area is increased to keep the magnetic field strength uniform.
しかしながら電子ビームの透過特性を良好に保
つ為に第3図に示すような支持構造の進行波管が
考案されている。この構造は、細くて長いヘリツ
クス形進行波管の機械的強度を高めると同時に、
永久磁石2及びポールピース1の外径寸法を精度
良く抑えることにより複数個の永久磁石石2とポ
ールピース1の同心度を良好に得られ、その結果
電子ビーム透過特性を良好に保つことが出来る。
又遅波回路部で発生する熱を良好に逃すことが出
来進行波管の安定性を充分に得られるという長所
を有している。 However, in order to maintain good electron beam transmission characteristics, a traveling wave tube with a support structure as shown in FIG. 3 has been devised. This structure increases the mechanical strength of the long and thin helical traveling wave tube, and at the same time
By controlling the outer diameter dimensions of the permanent magnets 2 and the pole piece 1 with high precision, it is possible to obtain good concentricity between the plurality of permanent magnets 2 and the pole piece 1, and as a result, it is possible to maintain good electron beam transmission characteristics. .
It also has the advantage that the heat generated in the slow wave circuit section can be dissipated well and the stability of the traveling wave tube can be sufficiently obtained.
しかしながら入出力結合器3を設置したところ
の永久磁石は第2図に示したように切欠を必要と
する。その為、この部分での磁界強度が低下しそ
の為に電子ビームの透過特性を良好に保てなくな
つてしまう。 However, the permanent magnet on which the input/output coupler 3 is installed requires a notch as shown in FIG. As a result, the magnetic field strength at this portion decreases, making it impossible to maintain good electron beam transmission characteristics.
しかしながら第3図に示す支持構造を用いた場
合には、入出力結合器3の部分の永久磁石2の外
径を大きくして磁界強度の一様性を得ることが出
来ない。 However, when the support structure shown in FIG. 3 is used, it is not possible to increase the outer diameter of the permanent magnet 2 in the input/output coupler 3 to obtain uniformity in magnetic field strength.
本考案では第2図に示した切欠きのある永久磁
石2の両側に設置されたポールピース1の少なく
とも1つ以上のポールピース1の外径を永久磁石
2の外径よりも小さくすることにより磁界強度を
高めることが出来、電子ビームの透過特性を良好
に保つことが出来る。 In the present invention, the outer diameter of at least one of the pole pieces 1 installed on both sides of the notched permanent magnet 2 shown in FIG. 2 is made smaller than the outer diameter of the permanent magnet 2. It is possible to increase the magnetic field strength and maintain good electron beam transmission characteristics.
本考案を採用することにより、機械強度を高
め、複数個の永久磁石とポールピースの同心度を
良好に保ち、さらに遅波回路部の熱放散を良好に
することの出来る、第3図の様な構造において
も、入出力結合器の取り出し部の磁界強度を良好
に得ることが出来電子ビームの透過特性を良好に
保つことが出来る。 By adopting this invention, it is possible to increase mechanical strength, maintain good concentricity between multiple permanent magnets and pole pieces, and improve heat dissipation in the slow wave circuit section, as shown in Figure 3. Even in this structure, it is possible to obtain a good magnetic field strength at the extraction part of the input/output coupler, and to maintain good electron beam transmission characteristics.
第1図は従来のヘリツクス形進行波管の電子ビ
ーム集束装置を示す。第2図に入出力結合部の位
置の永久磁石を示す。第3図に本考案による電子
ビーム集束装置を示す。
1……ポールピース、2……永久磁石、3……
入出力結合器、4……回路支持体。
FIG. 1 shows a conventional helical traveling wave tube electron beam focusing device. FIG. 2 shows the permanent magnet at the input/output coupling section. FIG. 3 shows an electron beam focusing device according to the present invention. 1...Pole piece, 2...Permanent magnet, 3...
Input/output coupler, 4... circuit support.
Claims (1)
からなる周期永久磁石を使用した進行波管におい
て、ポールピースと永久磁石からなる集束装置の
うち少なくとも1個以上のポールピースの外径が
永久磁石の外径より小さい集束装置を有すること
を特徴とする進行波管。 In a traveling wave tube using a periodic permanent magnet made of a rare earth monocobalt system as an electron beam focusing device, the outer diameter of at least one pole piece of the focusing device consisting of a pole piece and a permanent magnet is smaller than the outer diameter of the permanent magnet. A traveling wave tube characterized in that it has a small focusing device.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP18031282U JPS5982948U (en) | 1982-11-29 | 1982-11-29 | traveling wave tube |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP18031282U JPS5982948U (en) | 1982-11-29 | 1982-11-29 | traveling wave tube |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5982948U JPS5982948U (en) | 1984-06-05 |
| JPH0117082Y2 true JPH0117082Y2 (en) | 1989-05-18 |
Family
ID=30390994
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP18031282U Granted JPS5982948U (en) | 1982-11-29 | 1982-11-29 | traveling wave tube |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5982948U (en) |
-
1982
- 1982-11-29 JP JP18031282U patent/JPS5982948U/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5982948U (en) | 1984-06-05 |
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