JPS6047761B2 - airtight high frequency window - Google Patents

airtight high frequency window

Info

Publication number
JPS6047761B2
JPS6047761B2 JP5521178A JP5521178A JPS6047761B2 JP S6047761 B2 JPS6047761 B2 JP S6047761B2 JP 5521178 A JP5521178 A JP 5521178A JP 5521178 A JP5521178 A JP 5521178A JP S6047761 B2 JPS6047761 B2 JP S6047761B2
Authority
JP
Japan
Prior art keywords
frequency window
high frequency
dielectric disk
airtight
airtight high
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
Application number
JP5521178A
Other languages
Japanese (ja)
Other versions
JPS54146561A (en
Inventor
久明 佐藤
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
NEC Corp
Original Assignee
Nippon Electric Co Ltd
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Nippon Electric Co Ltd filed Critical Nippon Electric Co Ltd
Priority to JP5521178A priority Critical patent/JPS6047761B2/en
Publication of JPS54146561A publication Critical patent/JPS54146561A/en
Publication of JPS6047761B2 publication Critical patent/JPS6047761B2/en
Expired legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01PWAVEGUIDES; RESONATORS, LINES, OR OTHER DEVICES OF THE WAVEGUIDE TYPE
    • H01P1/00Auxiliary devices
    • H01P1/08Dielectric windows

Landscapes

  • Waveguide Connection Structure (AREA)
  • Microwave Tubes (AREA)

Description

【発明の詳細な説明】 本発明は、例えば、進行波管やクライストロンのような
マイクロ波管において真空部と外部導波管との間に設け
られる気密性の高周波窓に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an airtight high frequency window provided between a vacuum section and an external waveguide in a microwave tube such as a traveling wave tube or a klystron.

進行波管やクライストロンのようなマイクロ波管は、電
子ビームを射出する電子銃、電子ビームを捕捉するコレ
クタ、電子ビームとの相互作用によりマイクロ波を増幅
するマイクロ波増幅部、マイクロ波増幅部と外部導波管
との接続部となる入出力結合部などから構成され、入出
力結合部においては、マイクロ波管内部の気密性を保持
し、さらにマイクロ波をできるだけ損失なしに透過させ
るための気密高周波窓が用いられている。
A microwave tube such as a traveling wave tube or klystron consists of an electron gun that emits an electron beam, a collector that captures the electron beam, a microwave amplification section that amplifies the microwave through interaction with the electron beam, and a microwave amplification section. It consists of an input/output coupling section that connects with an external waveguide, and the input/output coupling section maintains airtightness inside the microwave tube and also has airtightness to allow microwaves to pass through with as little loss as possible. A high frequency window is used.

しカルて、この気密窓の気密性が不十分な場合は、当然
マイクロ波管の真空度の劣化となり、マイクロ波管の性
能の低下および寿命短縮という結果をもたらす。第1図
は従来の一般的な気密高周波窓を示すものてあり、第1
図において、出力導波管1と外部導波管3との間に円形
導波管2を形成し、円形導波管3内の中間に、誘電体円
板4を気密ろう付けしている。
However, if the airtightness of the airtight window is insufficient, the degree of vacuum of the microwave tube will naturally deteriorate, resulting in a decrease in performance and a shortened lifespan of the microwave tube. Figure 1 shows a conventional general airtight high frequency window.
In the figure, a circular waveguide 2 is formed between an output waveguide 1 and an external waveguide 3, and a dielectric disk 4 is hermetically brazed in the middle of the circular waveguide 3.

すなわち、気密保持は誘電体円板4の円周面ろう付け部
5だけて保持されている。このような従来の気密窓の構
造では、動作周波数が高く、したがつて、誘電体円板4
の厚みを薄くする必要がある場合は、円板周辺の真空封
止面に面積が小さくなり、そのため接合面の機械的強度
が弱まり、十分な気密保持の信頼性は得られないという
欠点があつた。このような円周面接合の欠点をなくすた
めに、第2図の如き気密窓が提案されている。
That is, airtightness is maintained only by the circumferential surface brazing portion 5 of the dielectric disk 4. In such a conventional hermetic window structure, the operating frequency is high, and therefore the dielectric disk 4
If it is necessary to reduce the thickness of the disc, the vacuum sealing surface around the disk will have a smaller area, which weakens the mechanical strength of the joint surface and has the disadvantage that sufficient airtightness cannot be maintained reliably. Ta. In order to eliminate such drawbacks of the circumferential surface joint, an airtight window as shown in FIG. 2 has been proposed.

第2図において、誘電体円板4の周縁部の両面および円
周部に金属化層6および7を形成し、周縁部の金属化層
6にフランジBa) 9a付きの円形導波管8、9をそ
れぞれろう付けして、出力導波管1と外部導波管3との
間の気密保持をしている。この構造によれは、誘電体円
板4を導くしても封止部の長さを長くすることができ、
第1図の従来例の場合に比ベマイクロ波管内部の気密性
を高度に保j持てきる。ところで、第2図の構造の気密
窓について種々調査した処、一見同じような構造をして
いても、ある場合には非常に良好な高周波特性を有し、
またある場合には、異常発熱または気密破れを起す7こ
とが認められた。そこでさらに調査を続けたところ、上
記の特性のバラツキの原因は、ろう付け部の半径方向の
長さにあることを見出した。本発明は、上記のような誘
電体円板の周縁部両面ろう付けによる気密窓の特性のバ
ラツキに対する新しい認識に基きなされたもので、マイ
クロ波透過特性の奥好な、かつ気密保持におても十分信
頼できるヌニ密高周波窓を提供することを目的とし゛ζ
いる。本発明の気密高周波窓は、誘電体円板の半径R2
と、円形導波管の半径R1との差R2−R1を、伝ぱん
半波長のほぼ整数倍(NXI2)電気長さにされている
In FIG. 2, metallized layers 6 and 7 are formed on both sides of the peripheral edge of the dielectric disk 4 and on the circumference, and a circular waveguide 8 with a flange Ba) 9a is formed on the metallized layer 6 on the peripheral edge. 9 are brazed to each other to maintain airtightness between the output waveguide 1 and the external waveguide 3. With this structure, even if the dielectric disk 4 is guided, the length of the sealing part can be increased,
Compared to the conventional example shown in FIG. 1, the airtightness inside the microwave tube can be maintained to a high degree. By the way, after conducting various investigations on airtight windows with the structure shown in Figure 2, we found that although they may have a seemingly similar structure, in some cases they have very good high-frequency characteristics.
In some cases, it was observed that abnormal heat generation or airtight failure occurred7. After further investigation, it was discovered that the cause of the above-mentioned variation in properties was the length of the brazed portion in the radial direction. The present invention was made based on the new recognition of the variation in the characteristics of airtight windows due to double-sided brazing of the peripheral edge of the dielectric disk as described above, and it is possible to improve the microwave transmission characteristics and maintain airtightness. The aim is to provide a sufficiently reliable high-frequency window.
There is. The airtight high frequency window of the present invention has a radius R2 of the dielectric disk.
The difference R2-R1 between the radius R1 of the circular waveguide and the radius R1 of the circular waveguide is set to be approximately an integral multiple (NXI2) of the propagation half wavelength.

以下第3図を参照して本発明の詳細な説明する。The present invention will be described in detail below with reference to FIG.

第3図において、誘電体円板4は、第2図の場合と同様
に、その円周部及びフランジとの接合部に金属化層7と
6がそれぞれ形成されているから、この部分は、外端を
短絡されたラデイアルラインを形成している。従つて、
フランジ8aと9aの内側より外側をみたインピーダン
スZは、誘電体円板4の外半径R2と円形導波管8の内
半径R1との差、R2−R1に大きく影響される。最も
理想的条件は、λ:動作波長、n:正の整数 すなわち、これは、フランジ8aと9aの内側より外側
を見たインピーダンスの大きさが零ときであるのは明ら
かである。
In FIG. 3, as in the case of FIG. 2, the dielectric disk 4 has metallized layers 7 and 6 formed at its circumferential portion and the joint portion with the flange, respectively, so that these portions are It forms a radial line whose outer ends are short-circuited. Therefore,
The impedance Z when looking from the inside to the outside of the flanges 8a and 9a is greatly influenced by the difference between the outer radius R2 of the dielectric disk 4 and the inner radius R1 of the circular waveguide 8, R2-R1. It is clear that the most ideal condition is when λ is the operating wavelength and n is a positive integer, that is, the impedance when looking outward from the inside of the flanges 8a and 9a is zero.

この場合、金属化層で囲まれた部分はいわゆるチョーク
効果により、高;周波的には短絡されているのと同様で
、異常発熱、気密破れといつた問題は起らなくなる。こ
の際、注意すべきは、該ラデイアルライン内は高誘電体
で構成されているから、いわゆる波長縮小効果があり、
上記条件を満足する実寸法(電気長)は意外に小さいこ
とである。一例として、14GHz帯で用いられる高周
波窓の寸法としては、比誘電率9.2の誘電体を用いた
場合、である。
In this case, the portion surrounded by the metallized layer is equivalent to being short-circuited in terms of high frequency due to the so-called choke effect, and problems such as abnormal heat generation and leakage of airtight do not occur. At this time, it should be noted that since the inside of the radial line is composed of a high dielectric material, there is a so-called wavelength reduction effect.
The actual size (electrical length) that satisfies the above conditions is surprisingly small. As an example, the dimensions of a high frequency window used in the 14 GHz band are as follows when a dielectric material with a relative dielectric constant of 9.2 is used.

もちろん、高周波窓としての最終寸法を決定する際には
、R1、R2の他に、誘電体円板の厚さ、あるいは第3
図の円形導波管8の寸法1等を、■SWRl共振周波数
に注意して選定しなければならない。本発明を採用する
ことにより、今まで時たま経験されたこの種高周波窓の
異常発熱あるいは気密破れが起らなくされた。図面の簡
単な説明第1図は、誘電体円板周面ろう付けの従来の気
密高周波窓の断面図、第2図は、誘電体円板周縁両面ろ
う付けの場合の従来の気密高周波窓の断面図、第3図は
、本発明の一実施例の断面図てある。
Of course, when determining the final dimensions of the high frequency window, in addition to R1 and R2, the thickness of the dielectric disk or the third
Dimensions 1, etc. of the circular waveguide 8 shown in the figure must be selected paying attention to the resonance frequency of ①SWRl. By employing the present invention, abnormal heat generation or airtight failure of this type of high frequency window, which has occasionally been experienced in the past, has been prevented from occurring. Brief Description of the Drawings Figure 1 is a cross-sectional view of a conventional airtight high-frequency window with dielectric disk circumferential surfaces brazed, and Figure 2 is a cross-sectional view of a conventional airtight high-frequency window with dielectric disk circumferential sides brazed on both sides. The cross-sectional view, FIG. 3, is a cross-sectional view of one embodiment of the present invention.

1・・・・・・出力導波管、3・・・・・・外部導波管
、4・・・・誘電体円板、6・・・・・・周縁部金属化
層、7・・・・・・円周部金属化層、8と9・・・・・
・円形導波管、8aと9a・・・・フランジ。
DESCRIPTION OF SYMBOLS 1...Output waveguide, 3...External waveguide, 4...Dielectric disk, 6...Peripheral metallized layer, 7... ...Circumferential metallization layer, 8 and 9...
・Circular waveguide, 8a and 9a...flange.

Claims (1)

【特許請求の範囲】[Claims] 1 周縁部の両面および円周面に金属化層が形成された
誘電体円板と、この誘電体円板の前記周縁部両面の金属
化層にろう付けされたフランジ付き円形導波管とからな
る気密高周波窓において、前記誘電体円板の半径と前記
円形導波管の半径との差を、動作波長λに対してほぼλ
/2の整数倍の電気長に選んだことを特徴とする気密高
周波窓。
1. A dielectric disk having metallized layers formed on both sides of the peripheral edge and the circumferential surface, and a flanged circular waveguide brazed to the metallized layers on both sides of the peripheral edge of the dielectric disk. In the airtight high frequency window, the difference between the radius of the dielectric disk and the radius of the circular waveguide is approximately λ with respect to the operating wavelength λ.
An airtight high-frequency window characterized by having an electrical length that is an integral multiple of /2.
JP5521178A 1978-05-09 1978-05-09 airtight high frequency window Expired JPS6047761B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP5521178A JPS6047761B2 (en) 1978-05-09 1978-05-09 airtight high frequency window

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP5521178A JPS6047761B2 (en) 1978-05-09 1978-05-09 airtight high frequency window

Publications (2)

Publication Number Publication Date
JPS54146561A JPS54146561A (en) 1979-11-15
JPS6047761B2 true JPS6047761B2 (en) 1985-10-23

Family

ID=12992293

Family Applications (1)

Application Number Title Priority Date Filing Date
JP5521178A Expired JPS6047761B2 (en) 1978-05-09 1978-05-09 airtight high frequency window

Country Status (1)

Country Link
JP (1) JPS6047761B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0480155A (en) * 1990-07-19 1992-03-13 Sumitomo Rubber Ind Ltd Manufacture of sheet feed roller

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH044352Y2 (en) * 1985-12-26 1992-02-07
JPS6314357U (en) * 1986-07-14 1988-01-30
JP2006313075A (en) * 2005-05-06 2006-11-16 Kyocera Corp Waveguide and temperature characteristic measuring instrument

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0480155A (en) * 1990-07-19 1992-03-13 Sumitomo Rubber Ind Ltd Manufacture of sheet feed roller

Also Published As

Publication number Publication date
JPS54146561A (en) 1979-11-15

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