JPH04333B2 - - Google Patents
Info
- Publication number
- JPH04333B2 JPH04333B2 JP11804681A JP11804681A JPH04333B2 JP H04333 B2 JPH04333 B2 JP H04333B2 JP 11804681 A JP11804681 A JP 11804681A JP 11804681 A JP11804681 A JP 11804681A JP H04333 B2 JPH04333 B2 JP H04333B2
- Authority
- JP
- Japan
- Prior art keywords
- tube
- barrel
- comb
- frequency circuit
- traveling wave
- 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
- 230000000737 periodic effect Effects 0.000 claims description 4
- 238000010894 electron beam technology Methods 0.000 description 4
- BGPVFRJUHWVFKM-UHFFFAOYSA-N N1=C2C=CC=CC2=[N+]([O-])C1(CC1)CCC21N=C1C=CC=CC1=[N+]2[O-] Chemical compound N1=C2C=CC=CC2=[N+]([O-])C1(CC1)CCC21N=C1C=CC=CC1=[N+]2[O-] BGPVFRJUHWVFKM-UHFFFAOYSA-N 0.000 description 2
- 230000005389 magnetism Effects 0.000 description 2
- 238000000034 method Methods 0.000 description 2
- RYGMFSIKBFXOCR-UHFFFAOYSA-N Copper Chemical compound [Cu] RYGMFSIKBFXOCR-UHFFFAOYSA-N 0.000 description 1
- 230000002730 additional effect Effects 0.000 description 1
- 230000002411 adverse Effects 0.000 description 1
- XAGFODPZIPBFFR-UHFFFAOYSA-N aluminium Chemical compound [Al] XAGFODPZIPBFFR-UHFFFAOYSA-N 0.000 description 1
- 229910052782 aluminium Inorganic materials 0.000 description 1
- 230000005540 biological transmission Effects 0.000 description 1
- 238000007796 conventional method Methods 0.000 description 1
- 229910052802 copper Inorganic materials 0.000 description 1
- 239000010949 copper Substances 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 239000000463 material Substances 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J23/00—Details of transit-time tubes of the types covered by group H01J25/00
- H01J23/12—Vessels; Containers
Landscapes
- Microwave Tubes (AREA)
Description
【発明の詳細な説明】
本発明は、ビーム集束装置として周期永久磁石
(以下PPMという)を使用した進行波管の支持構
造に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a support structure for a traveling wave tube using a periodic permanent magnet (hereinafter referred to as PPM) as a beam focusing device.
周知のように、進行波管は、電子ビームを発生
させる電子銃部と、電子ビームと相互作用を行な
う高周波回路部と、電子ビームを捕促するコレク
タ部と、高周波の入出力回路部と、電子ビームを
集束させるビーム集束装置と、管球支持部(ケー
スの一部)等から構成されている。 As is well known, a traveling wave tube includes an electron gun section that generates an electron beam, a high frequency circuit section that interacts with the electron beam, a collector section that captures the electron beam, and a high frequency input/output circuit section. It consists of a beam focusing device that focuses the electron beam, a tube support part (part of the case), etc.
従来のPPM集束進行波管の代表的な高周波回
路の構造を第1図に示す。第1図aは、高周波回
路のひとつの断面を示したものであり、同図にお
いて1はヘリツクス、2は絶縁支柱、3はバレル
を示す。バレル3は真空外囲器を兼ねている。4
はPPMを構成するマグネツトを示し、第1図a
と直角方向の断面をPPM部だけについて示せば
第1図bのようになつている。b図において、4
がマグネツト、8がポールピースである。再びa
図にもどり、5は管球支持台、6はクランプ、7
は止めねじを示す。5の立体図は第1図cに示さ
れる。このように、従来の管球の高周波回路部の
支持方法は、PPMを構成するポールピースまた
はマグネツトを介して行なうものが一般的であつ
た。 Figure 1 shows the structure of a typical high-frequency circuit of a conventional PPM focused traveling wave tube. FIG. 1a shows a cross section of one of the high-frequency circuits, in which 1 is a helix, 2 is an insulating column, and 3 is a barrel. Barrel 3 also serves as a vacuum envelope. 4
Figure 1a shows the magnets that make up the PPM.
If the cross section in the direction perpendicular to is shown for only the PPM part, it will look like Figure 1b. In figure b, 4
is the magnet and 8 is the pole piece. a again
Returning to the diagram, 5 is the tube support, 6 is the clamp, 7
indicates a set screw. A three-dimensional view of 5 is shown in Figure 1c. As described above, the conventional method of supporting the high-frequency circuit section of the bulb has generally been through the pole piece or magnet that constitutes the PPM.
ところが、最近は進行波管を高出力化したいと
いう要請が強くなつており、このような場合、第
1図に示すような従来の支持構造では以下のよう
な問題が生ずることがわかつてきた。問題の第1
は、管球が高出力になると、管内損失(高周波損
失及び直流損失)も一般にそれに応じて増加する
から、ヘリツクス及び絶縁支柱で発生した熱がバ
レルに伝わり、バレルを非常な高温にする。この
熱はマグネツト4を通して支持台5に伝えられる
が、その過程においてマグネツトの温度を上昇せ
しめ、その結果、マグネツトの磁界を弱めてビー
ム透過に悪影響を与える。問題の第2は、バレル
とポールピースの間のすき間の存在である。通常
の進行波管においては、ポールピース8はバレル
3に対して固着されておらず、両者の間には径方
向に2/100〜5/100ミリメートルのすき間がある
が、これはバレルからマグネツトへの熱の移動を
妨げる方向に働き、ヘリツクスの温度上昇を招い
て好ましくない。問題の第3は、マグネツトの外
径精度及び内外径の偏芯を厳しく抑えておかない
と、マグネツト4の面と支持台5の面が管軸方向
の全区間にわたつて面接触せず従つて熱の伝達を
悪くする点にある。 However, recently there has been a strong demand to increase the output of traveling wave tubes, and in such cases it has been found that the following problems occur with the conventional support structure shown in FIG. Problem number one
As the power of the tube increases, the loss within the tube (high frequency loss and DC loss) generally increases accordingly, so the heat generated in the helix and insulating struts is transferred to the barrel, making the barrel extremely hot. This heat is transferred to the support base 5 through the magnet 4, but in the process raises the temperature of the magnet, which weakens the magnetic field of the magnet and adversely affects beam transmission. The second problem is the existence of a gap between the barrel and the pole piece. In a normal traveling wave tube, the pole piece 8 is not fixed to the barrel 3, and there is a gap of 2/100 to 5/100 mm in the radial direction between them, but this is due to the fact that the pole piece 8 is not fixed to the barrel 3. This is undesirable because it acts in the direction of hindering the transfer of heat to the helix, causing an increase in the temperature of the helix. The third problem is that unless the outside diameter accuracy of the magnet and the eccentricity of the inside and outside diameters are strictly controlled, the surface of the magnet 4 and the surface of the support base 5 will not come into surface contact over the entire section in the tube axis direction. The problem is that it impairs heat transfer.
本発明の目的は、以上のような従来構造の欠点
を除き、高出力の進行波管において効果のある新
しい管球支持構造を提供することである。 SUMMARY OF THE INVENTION An object of the present invention is to provide a new tube support structure that is effective in high-power traveling wave tubes and eliminates the drawbacks of the conventional structures as described above.
本発明は、ビーム集束装置として周期永久磁石
を用いた進行波管において、ケースの一部をなす
高周波回路部支持部品は断面がくしの歯状をして
おり、くしの歯の上面は円弧状に加工され、円弧
の径は進行波管の高周波回路部の真空外囲器であ
るバレルの外径と一致しており、管球と前記支持
部品が高周波回路部の管軸方向にわたつて全体的
に密着固定されたことを特徴とする。 The present invention provides a traveling wave tube that uses a periodic permanent magnet as a beam focusing device, in which a high-frequency circuit support component that forms a part of the case has a comb-shaped cross section, and the upper surface of the comb teeth is arc-shaped. The diameter of the circular arc matches the outer diameter of the barrel, which is the vacuum envelope of the high-frequency circuit section of the traveling wave tube, and the tube and the supporting parts are It is characterized by being closely fixed to.
本発明に係る進行波管の高周波回路の構造を第
2図に示す。第2図aにおいて、バレル3の内部
までは従来と同一であるが、管球の支持構造が従
来と異なつているのが示されている。すなわち、
支持台5′の立体図を第2図cに示すように、支
持台はバレルを直接的に受けている。支持台5′
の上面に設けられたくしの歯状の突起は、その上
面がバレルに丁度面接触するように円弧面状に加
工されている。そして、くしの歯の間の間隙部に
はポールピース8が入り込み、くしの歯の部分に
は断面がc形の第2図bに示すマグネツトを上方
よりはめ込む。このような新しい支持構造におい
ては、第1に、バレル内で発生した熱の大部分が
マグネツトを介することなく支持台側に伝えられ
るため、マグネツト自身の温度上昇を防ぐことが
できる。また第2に、支持台5′とバレル3とは
間に空隙のない、完全に密着した構造であるから
両者間の熱抵抗を極めて小さくできバレルの温度
上昇を比較的低く抑えることができる。第3に、
マグネツトの外径精度や内外径の偏芯について従
来ほど気を使わずにすむ。第4に、附加的な効果
として、c形マグネツトは、従来のようにふたつ
割りにしてバレルにはめ込む手続が不要であり、
マグネツト組込みに要する時間が短かくてすむ。
ここで注意を要するのは、マグネツトをc形にし
たことによる円周方向の偏磁の発生の恐れである
が、ポールピース自身は完全な軸対称性を保つて
いるため、軸上磁界でみれば偏磁は緩和されて、
実用上問題とならないことである。 FIG. 2 shows the structure of the high frequency circuit of the traveling wave tube according to the present invention. In FIG. 2a, the inside of the barrel 3 is the same as the conventional one, but it is shown that the tube support structure is different from the conventional one. That is,
As shown in FIG. 2c, a three-dimensional view of the support base 5', the support base directly receives the barrel. Support stand 5'
The comb tooth-shaped protrusions provided on the upper surface of the barrel are machined into an arcuate shape so that the upper surface is just in surface contact with the barrel. The pole piece 8 is inserted into the gap between the teeth of the comb, and a magnet having a c-shaped cross section as shown in FIG. 2b is fitted into the teeth of the comb from above. In such a new support structure, firstly, most of the heat generated within the barrel is transmitted to the support stand side without passing through the magnet, so that the temperature of the magnet itself can be prevented from increasing. Secondly, since the support base 5' and the barrel 3 are in complete contact with each other with no space between them, the thermal resistance between them can be extremely small, and the temperature rise in the barrel can be kept relatively low. Thirdly,
There is no need to worry as much about the magnet's outer diameter accuracy and eccentricity of the inner and outer diameters as before. Fourth, as an additional effect, the C-shaped magnet does not require the conventional procedure of breaking it into two pieces and fitting them into the barrel.
The time required to incorporate the magnet is short.
What you need to be careful about here is the risk of biased magnetism occurring in the circumferential direction due to the C-shaped magnet, but since the pole piece itself maintains perfect axial symmetry, it will not be seen in the axial magnetic field. If the biased magnetism is relaxed,
This is not a problem in practice.
以上の説明は、進行波管のひとつとしてヘリツ
クス形進行波管を例にとつたが、PPMの集束の
結合空胴形進行波管にも本発明が適用できるのは
明らかである。また発明の主旨からして支持台
5′の材質としては熱伝導性の良い銅またはアル
ミニウムが最適であるのは明らかである。 Although the above explanation has taken a helical traveling wave tube as an example of a traveling wave tube, it is clear that the present invention can also be applied to a coupled cavity traveling wave tube for PPM focusing. Further, in view of the gist of the invention, it is clear that copper or aluminum, which has good thermal conductivity, is optimal as the material for the support base 5'.
第1図は従来の進行波管の管球支持構造を示
す。a図は横断面を示し、b図はPPMの縦断面
図を、c図は管球支持台の立体図を示す。第2図
は本発明による進行波管の管球支持構造を示す。
a図は横断面を示し、b図はマグネツトの側面図
を示し、c図は管球支持台の立体図を示す。
1…ヘリツクス、2…絶縁支柱、3…バレル、
4…マグネツト、5,5′…管球支持台、6…ク
ランプ、7…止めねじ、8…ポールピース。
FIG. 1 shows a conventional traveling wave tube support structure. Figure a shows a cross section, figure b shows a longitudinal cross section of the PPM, and figure c shows a three-dimensional view of the tube support. FIG. 2 shows a tube support structure for a traveling wave tube according to the present invention.
Figure a shows a cross section, figure b shows a side view of the magnet, and figure c shows a three-dimensional view of the tube support. 1...Helix, 2...Insulating strut, 3...Barrel,
4... Magnet, 5, 5'... Tube support stand, 6... Clamp, 7... Set screw, 8... Pole piece.
Claims (1)
として周期永久磁石を備え、支持部品によつて支
持された進行波管において、ケースの一部をなす
高周波回路部支持部品は断面がくしの歯状をして
おり、くしの歯の上面は円弧状に加工され、前記
円弧の径は高周波回路部の真空外囲器であるバレ
ルの外径と一致しており、支持部品の円弧部とバ
レルは密着され、くしの歯の間の各間隙部には周
期永久磁石を構成するポールピースが入り込み、
くしの歯の部分にはC形の磁石をはめ込むことに
より管球と前記支持部品が高周波回路部の管軸方
向にわたつて全体的に密着固定されたことを特徴
とする進行波管。1. In a traveling wave tube that is equipped with a periodic permanent magnet as a beam focusing device around the high-frequency circuit section of the tube and is supported by a support component, the high-frequency circuit section support component that forms part of the case has a comb-shaped cross section. The upper surface of the teeth of the comb is machined into an arc shape, and the diameter of the arc matches the outer diameter of the barrel, which is the vacuum envelope of the high frequency circuit section, and the arc part of the support part and the barrel are The pole pieces constituting the periodic permanent magnet are inserted into each gap between the teeth of the comb.
1. A traveling wave tube characterized in that the tube and the support component are closely fixed as a whole in the tube axis direction of the high frequency circuit section by fitting C-shaped magnets into the teeth of the comb.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP11804681A JPS5818838A (en) | 1981-07-28 | 1981-07-28 | Support structure of traveling-wave tube |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP11804681A JPS5818838A (en) | 1981-07-28 | 1981-07-28 | Support structure of traveling-wave tube |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5818838A JPS5818838A (en) | 1983-02-03 |
| JPH04333B2 true JPH04333B2 (en) | 1992-01-07 |
Family
ID=14726686
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP11804681A Granted JPS5818838A (en) | 1981-07-28 | 1981-07-28 | Support structure of traveling-wave tube |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5818838A (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2661517B2 (en) * | 1993-09-09 | 1997-10-08 | 日本電気株式会社 | Traveling wave tube |
-
1981
- 1981-07-28 JP JP11804681A patent/JPS5818838A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5818838A (en) | 1983-02-03 |
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