JPS62131Y2 - - Google Patents
Info
- Publication number
- JPS62131Y2 JPS62131Y2 JP6587780U JP6587780U JPS62131Y2 JP S62131 Y2 JPS62131 Y2 JP S62131Y2 JP 6587780 U JP6587780 U JP 6587780U JP 6587780 U JP6587780 U JP 6587780U JP S62131 Y2 JPS62131 Y2 JP S62131Y2
- Authority
- JP
- Japan
- Prior art keywords
- high frequency
- helix
- traveling wave
- dielectric
- 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
- 239000003989 dielectric material Substances 0.000 claims 1
- OKTJSMMVPCPJKN-UHFFFAOYSA-N Carbon Chemical compound [C] OKTJSMMVPCPJKN-UHFFFAOYSA-N 0.000 description 3
- 229910052799 carbon Inorganic materials 0.000 description 3
- 238000010894 electron beam technology Methods 0.000 description 3
- 230000004048 modification Effects 0.000 description 3
- 238000012986 modification Methods 0.000 description 3
- 230000003321 amplification Effects 0.000 description 2
- 239000002184 metal Substances 0.000 description 2
- 238000003199 nucleic acid amplification method Methods 0.000 description 2
- 230000010355 oscillation Effects 0.000 description 2
- 229910052573 porcelain Inorganic materials 0.000 description 2
- 238000005219 brazing Methods 0.000 description 1
- 239000000919 ceramic Substances 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 238000007493 shaping process Methods 0.000 description 1
Landscapes
- Microwave Tubes (AREA)
Description
【考案の詳細な説明】 この考案は進行波管の改良に関する。[Detailed explanation of the idea] This invention relates to improvements in traveling wave tubes.
一般にビーム直進形マイクロ波管は、電子ビー
ムを使用してマイクロ波の増幅、発振を行なわせ
るもので、その代表的な管種に進行波管がある。 In general, a straight beam microwave tube uses an electron beam to amplify and oscillate microwaves, and a typical type of tube is a traveling wave tube.
進行波管は従来第1図に示すように構成され、
電子銃1、遅波回路2及びコレクタ3からなつて
いる。そして遅波回路2は第2図からも明らかな
ように、金属製の筒状外囲器4内に同軸的にヘリ
ツクス5を収容し、3個の誘電体支持体6により
支持している。尚、図中7は高周波信号入力部、
8は高周波信号出力部である。 A traveling wave tube is conventionally configured as shown in Figure 1.
It consists of an electron gun 1, a slow wave circuit 2, and a collector 3. As is clear from FIG. 2, the slow wave circuit 2 has a helix 5 coaxially accommodated within a metal cylindrical envelope 4 and supported by three dielectric supports 6. In addition, 7 in the figure is a high frequency signal input section,
8 is a high frequency signal output section.
ところで、上記構造の従来の進行波管において
は、動作時には、電子銃1の陰極より放射される
電子をビーム成形電極により所定の電子ビームを
形成し、この電子ビームを遅波回路2を通過させ
てコレクタ3に向かわせるが、ヘリツクス5周辺
には局部発振防止用減衰器を設けなければならな
い。そこで従来は、誘電体支持体6に一部減衰器
構造とした炭素抵抗層を作り減衰器として用いて
いるが、充分な効果が得られていない。 By the way, in the conventional traveling wave tube having the above structure, during operation, the electrons emitted from the cathode of the electron gun 1 are formed into a predetermined electron beam by a beam shaping electrode, and this electron beam is passed through the slow wave circuit 2. However, an attenuator must be provided around the helix 5 to prevent local oscillation. Conventionally, therefore, a carbon resistance layer having a partial attenuator structure is formed on the dielectric support 6 and used as an attenuator, but a sufficient effect has not been obtained.
この考案は上記事情に鑑みなされたもので、局
部発振を充分に防止して高周波増幅を極めて安定
に行なうことができるビーム直進形マイクロ波管
を提供することを目的とする。 This invention was developed in view of the above circumstances, and the object thereof is to provide a beam-straight microwave tube that can sufficiently prevent local oscillation and perform high frequency amplification extremely stably.
以下、図面を参照してこの考案の一実施例を詳
細に説明する。 Hereinafter, one embodiment of this invention will be described in detail with reference to the drawings.
この考案の進行波管における遅波回路は第3図
及び第4図に示すように構成されている。即ち、
金属製の筒状外囲器9内には、ヘリツクス10が
同軸的に配設され、3個の誘電体支持体11によ
り支持固定されている。この場合、誘電体支持体
11は棒状にして断面が段部11a,11bを有
する略四辺形にして前記外囲器9内面に接する側
(段部11a,11bとは反対側)は曲面に形成
されている。このような3個の誘電体支持体11
の相互間には、高周波減衰器12が合計3個、管
軸方向に配設されている。この高周波減衰器12
は例えば、セラミツクス磁器又はベアリング磁器
に炭素抵抗層を分布させたもの、焼結した炭素抵
抗体を所望特性に応じて長さ、抵抗値を変えたも
のからなり、第5図に示す如く断面円弧状にして
両端がテーパー状に形成され内面が前記ヘリツク
ス10に接し両側端は前記誘電体支持体11の段
部11a,11bに位置している。つまり段部1
1a,11bにより高周波減衰器12をヘリツク
ス10に押えつけている。尚、外囲器9と誘電体
支持体11、及び誘電体支持体11とヘリツクス
10は鑞付け又は接触保持により固定される。
又、この考案の進行波管は、上記遅波回路以外は
第1図と同様ゆえ、詳細な説明を省略する。 The slow wave circuit in the traveling wave tube of this invention is constructed as shown in FIGS. 3 and 4. That is,
A helix 10 is disposed coaxially within a metal cylindrical envelope 9 and is supported and fixed by three dielectric supports 11 . In this case, the dielectric support 11 is shaped like a rod and has a substantially quadrilateral cross section with stepped portions 11a and 11b, and the side in contact with the inner surface of the envelope 9 (the side opposite to the stepped portions 11a and 11b) is formed into a curved surface. has been done. Three such dielectric supports 11
A total of three high frequency attenuators 12 are arranged between the two in the tube axis direction. This high frequency attenuator 12
For example, it is made of ceramic porcelain or bearing porcelain with a carbon resistance layer distributed thereon, or a sintered carbon resistor whose length and resistance value are changed according to desired characteristics, and has a circular cross section as shown in Figure 5. It is formed into an arc shape with both ends tapered, and its inner surface is in contact with the helix 10, and both ends are located at the stepped portions 11a and 11b of the dielectric support 11. In other words, step part 1
The high frequency attenuator 12 is pressed against the helix 10 by 1a and 11b. Incidentally, the envelope 9 and the dielectric support 11, and the dielectric support 11 and the helix 10 are fixed by brazing or contact holding.
Moreover, since the traveling wave tube of this invention is the same as that shown in FIG. 1 except for the slow wave circuit, detailed explanation will be omitted.
この考案の進行波管は上記説明及び図示のよう
に構成され、3個の誘電体支持体11の相互間に
高周波減衰器12を配設しているので、高周波増
幅を極めて安定に行なうことができ大電力用に好
適である。又、この考案における高周波減衰器1
2は任意に反射係数が少ない位置に選定できる。
更に減衰量は形状の選択により自由に選べるた
め、製造上とりわけヘリツクス10の組立の工程
で有意義である。 The traveling wave tube of this invention is constructed as described above and illustrated, and the high frequency attenuator 12 is disposed between the three dielectric supports 11, so that high frequency amplification can be carried out extremely stably. Suitable for high power applications. Moreover, the high frequency attenuator 1 in this invention
2 can be arbitrarily selected at a position where the reflection coefficient is small.
Furthermore, since the amount of attenuation can be freely selected by selecting the shape, this is significant in terms of manufacturing, especially in the process of assembling the helix 10.
尚、上記実施例では、ヘリツクス10を3点支
持、つまり3個の誘電体支持体11を用いたが、
第6図及び第7図に示す如く4点支持、つまり4
個の誘電体支持体13を使用してもよい。この場
合は、4個の誘電体支持体13が十字方向に位置
することになり、従つて高周波減衰器14も各誘
電体支持体13相互間に位置するので合計4個必
要となる。そして、この高周波減衰器14は第8
図からも明らかなように丸棒にして両端がテーパ
ー状に形成されている。そして、やはり誘電体支
持体13の段部13a,13bによりヘリツクス
10方向へ押さえつけられている。 In the above embodiment, the helix 10 was supported at three points, that is, three dielectric supports 11 were used.
As shown in Figures 6 and 7, four-point support, that is, four
dielectric supports 13 may be used. In this case, the four dielectric supports 13 are located in the cross direction, and therefore the high frequency attenuators 14 are also located between the dielectric supports 13, so a total of four high frequency attenuators 14 are required. This high frequency attenuator 14 is the eighth
As is clear from the figure, it is a round rod with both ends tapered. Also, it is pressed in the direction of the helix 10 by the stepped portions 13a and 13b of the dielectric support 13.
又、上記実施例及び変形例における誘電体支持
体11,13はそれぞれ両端がテーパー状に形成
されていたが、第9図及び第10図に示すように
両端がテーパー状になつていない誘電体支持体1
5,16を使用してもよい。 Further, although the dielectric supports 11 and 13 in the above embodiments and modified examples were each formed with tapered ends, as shown in FIGS. Support 1
5, 16 may also be used.
以上説明したようにこの考案によれば、工業的
価値大なる進行波管を提供することができる。 As explained above, according to this invention, a traveling wave tube of great industrial value can be provided.
第1図は従来及びこの考案を説明するために用
いる進行波管を示す断面図、第2図は従来の進行
波管における要部(遅波回路)を示す断面図、第
3図はこの考案の一実施例に係る進行波管の要部
(遅波回路)を示す断面図、第4図は第2図のA
−A′線に沿つて切断し矢印方向に見た断面図、
第5図は第3図の実施例で用いる高周波減衰器を
示す斜視図、第6図はこの考案の変形例を示す断
面図、第7図は第6図のB−B′線に沿つて切断し
矢印方向に見た断面図、第8図は第6図の変形例
で用いる高周波減衰器を示す斜視図、第9図及び
第10図は高周波減衰器の変形例を示す斜視図で
ある。
9……外囲器、10……ヘリツクス、11……
誘電体支持体、11a,11b……段部、12…
…高周波減衰器。
Fig. 1 is a sectional view showing a conventional traveling wave tube and a traveling wave tube used to explain this invention, Fig. 2 is a sectional view showing the main part (slow wave circuit) in a conventional traveling wave tube, and Fig. 3 is a sectional view of this invention. A sectional view showing the main part (slow wave circuit) of a traveling wave tube according to an embodiment, FIG. 4 is A of FIG.
A cross-sectional view taken along the −A′ line and viewed in the direction of the arrow,
FIG. 5 is a perspective view showing the high frequency attenuator used in the embodiment of FIG. 3, FIG. 6 is a sectional view showing a modification of this invention, and FIG. FIG. 8 is a perspective view showing a high-frequency attenuator used in a modification of FIG. 6, and FIGS. 9 and 10 are perspective views showing modifications of the high-frequency attenuator. . 9... Envelope, 10... Helix, 11...
Dielectric support body, 11a, 11b... step part, 12...
...High frequency attenuator.
Claims (1)
複数の誘電体により支持固定してなる進行波管に
おいて、前記各誘電体支持体に段部を設け、更に
各誘電体支持体の相互間に高周波減衰器を配設
し、前記段部を利用して高周波減衰器を前記ヘリ
ツクス方向へ押しつけるようになしたことを特徴
とした進行波管。 A helix is arranged coaxially within a cylindrical envelope,
In a traveling wave tube that is supported and fixed by a plurality of dielectric materials, each of the dielectric supports is provided with a stepped portion, and a high frequency attenuator is further provided between each of the dielectric supports, and the stepped portion is utilized. A traveling wave tube characterized in that the high frequency attenuator is pressed in the direction of the helix.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP6587780U JPS62131Y2 (en) | 1980-05-14 | 1980-05-14 |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP6587780U JPS62131Y2 (en) | 1980-05-14 | 1980-05-14 |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS56166657U JPS56166657U (en) | 1981-12-10 |
| JPS62131Y2 true JPS62131Y2 (en) | 1987-01-06 |
Family
ID=29659990
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP6587780U Expired JPS62131Y2 (en) | 1980-05-14 | 1980-05-14 |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS62131Y2 (en) |
-
1980
- 1980-05-14 JP JP6587780U patent/JPS62131Y2/ja not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS56166657U (en) | 1981-12-10 |
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