JPH0352007Y2 - - Google Patents

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Publication number
JPH0352007Y2
JPH0352007Y2 JP5583085U JP5583085U JPH0352007Y2 JP H0352007 Y2 JPH0352007 Y2 JP H0352007Y2 JP 5583085 U JP5583085 U JP 5583085U JP 5583085 U JP5583085 U JP 5583085U JP H0352007 Y2 JPH0352007 Y2 JP H0352007Y2
Authority
JP
Japan
Prior art keywords
waveguide
microwave
load impedance
phase
impedance adjustment
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
JP5583085U
Other languages
Japanese (ja)
Other versions
JPS61171304U (en
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 filed Critical
Priority to JP5583085U priority Critical patent/JPH0352007Y2/ja
Publication of JPS61171304U publication Critical patent/JPS61171304U/ja
Application granted granted Critical
Publication of JPH0352007Y2 publication Critical patent/JPH0352007Y2/ja
Expired legal-status Critical Current

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  • Waveguide Switches, Polarizers, And Phase Shifters (AREA)

Description

【考案の詳細な説明】 〔考案の利用分野〕 本考案の導波管伝送線路を用いるマイクロ波装
置において、導波管の一部に装着し負荷インピー
ダンスを調整する構造の負荷インピーダンス調整
装置に関する。
[Detailed Description of the Invention] [Field of Application of the Invention] In a microwave device using the waveguide transmission line of the present invention, the present invention relates to a load impedance adjustment device that is attached to a part of the waveguide and adjusts the load impedance.

〔考案の背景〕 マイクロ波は、既に多くの技術分野に利用され
ているが、効率よく利用するには、負荷からの反
射をできるだけ少なくする必要がある。このた
め、インピーダンス調整装置を伝送線路に入れ
て、負荷の整合をとることが行なわれている。マ
イクロ波電力が比較的大きい場合にこれまで使わ
れているインピーダンス調整装置には、導波管タ
イプの物が多い。このタイプとしては、3−スタ
ブ、スラグチユーナ、E・Hチユーナ等がある。
取り扱いと操作の容易さから、一般的に3−スタ
ブが多く使用されているので、ここでは3−スタ
ブを例に取、従来技術を説明する。
[Background of the invention] Microwaves are already used in many technical fields, but in order to use them efficiently, it is necessary to minimize reflection from loads. For this reason, an impedance adjustment device is inserted into the transmission line to match the load. Many of the impedance adjustment devices used so far when the microwave power is relatively large are of the waveguide type. Examples of this type include 3-stub, slug tuner, and E/H tuner.
Since 3-stubs are commonly used because of their ease of handling and operation, the prior art will be explained here by taking 3-stubs as an example.

第9図は、従来用いられている3−スタブを示
している。図において、1は導波管、2はフラン
ジ、3は(n/2+1/4)λgまたは(n/2+1/
8)λg 間隔に設けたスタブである。整合負荷でない場合
は、導波管内の電界最大点(矩形導波管では長辺
の中点)にそれぞれのスタブを挿入して、負荷の
整合をとる。
FIG. 9 shows a conventionally used three-stub. In the figure, 1 is a waveguide, 2 is a flange, and 3 is (n/2+1/4)λg or (n/2+1/2)
8) Stubs provided at λg intervals. If the load is not matched, each stub is inserted at the maximum electric field point within the waveguide (the midpoint of the long side in a rectangular waveguide) to match the load.

必要な挿入深さは、負荷インピーダンスにより
変化し、低インピーダンス並びに高インピーダン
スの場合には、挿入する深さは深くなる傾向があ
る。深さが深くなると、スタブの電界が高くなる
ため、何も入つていない中空導波管に比べ、マイ
クロ波耐圧が低くなり、全体として使用できるマ
イクロ波電力は、3−スタブの耐圧で限定されて
しまう欠点があつた。
The required insertion depth varies depending on the load impedance, and the insertion depth tends to be deeper for low and high impedances. As the depth increases, the electric field of the stub increases, so the microwave withstand voltage becomes lower than that of a hollow waveguide with nothing inside, and the microwave power that can be used as a whole is limited by the withstand voltage of the 3-stub. It has the disadvantage of being rejected.

〔考案の目的〕[Purpose of invention]

本考案の目的は、上記従来技術の欠点を解消す
ることであり、具体的には、中空導波管と同じ耐
圧まで使用できるマイクロ波用負荷インピーダン
ス調整装置を提供することである。
The purpose of the present invention is to eliminate the drawbacks of the prior art described above, and specifically, to provide a microwave load impedance adjustment device that can be used up to the same withstand voltage as a hollow waveguide.

〔考案の概要〕[Summary of the idea]

本考案は、誘導性窓と長さが異なる複数個の位
相導波管とを組合せて負荷インピーダンス調整装
置を構成し、耐圧を低下させる要素を排除して、
中空導波管と同じマイクロ波耐圧を確保するもの
である。
The present invention configures a load impedance adjustment device by combining an inductive window and a plurality of phase waveguides of different lengths, eliminates elements that reduce withstand voltage, and
This ensures the same microwave resistance as a hollow waveguide.

〔考案の実施例〕[Example of idea]

次に、第1図〜第8図を参照して、本考案の実
施例を詳しく説明する。
Next, embodiments of the present invention will be described in detail with reference to FIGS. 1 to 8.

本考案による負荷インピーダンス調整装置の一
例を示す第1図において、4は誘導性窓、5,
6,7は、管内波長をλgとするとき、それぞれ、
λg/16,8/λg,λg/4の長さを持つたフランジ付
き中 空導波管である。ここでは、誘導性窓4と組み合
せて負荷インピーダンスを調整する中空導波管
5,6,7を位相導波管と呼ぶことにする。
In FIG. 1 showing an example of the load impedance adjustment device according to the present invention, 4 is an inductive window;
6 and 7 are respectively, when the tube wavelength is λg,
It is a flanged hollow waveguide with lengths of λg/16, 8/λg, and λg/4. Here, the hollow waveguides 5, 6, and 7 that adjust the load impedance in combination with the inductive window 4 will be referred to as phase waveguides.

誘導性窓4は、E面寸法、すなわち、導波管開
口の短辺寸法bを変えないで、H面寸法、すなわ
ち、導波管開口の長辺寸法aを変えてサセプタン
スを調整するために、マイクロ波耐圧は中空導波
管と同じになる。
The inductive window 4 is designed to adjust the susceptance by changing the H plane dimension, that is, the long side dimension a of the waveguide opening, without changing the E plane dimension, that is, the short side dimension b of the waveguide opening. , the microwave breakdown voltage is the same as that of a hollow waveguide.

サセプタンスの位相を変える調整方法について
次に説明する。既に述べた第1図は、誘導性窓4
を位相基準面に置いた場合を示す。第2図は、位
相基準面に対してλg/16だけ位相を変えた場合、同 じく、第3図はλg/8、第4図は3λg/16、第5図は λg/4、第6図は5λg/16、第7図は3λg/8、第8
図は 7λg/16だけ位相を変化させた場合をそれぞれ示し ている。このように誘導性窓を入れる場所によつ
て位相が変わることになる。この例の利点として
は、誘導性窓と位相導波管とを組み合せた場合、
全長Lを変えないで、λg/3を8等分して段階的に 負荷インピーダンスを調整できることがあげられ
る。
An adjustment method for changing the phase of susceptance will be described next. The already mentioned FIG. 1 shows the inductive window 4.
The case where is placed on the phase reference plane is shown. Figure 2 shows that when the phase is changed by λg/16 with respect to the phase reference plane, similarly, Figure 3 is λg/8, Figure 4 is 3λg/16, Figure 5 is λg/4, and Figure 6 is is 5λg/16, Fig. 7 is 3λg/8, 8th
The figures each show the case where the phase is changed by 7λg/16. In this way, the phase changes depending on where the inductive window is inserted. The advantage of this example is that when combining an inductive window and a phase waveguide,
One advantage is that the load impedance can be adjusted in stages by dividing λg/3 into eight equal parts without changing the overall length L.

本実施例では、3分割の場合について説明した
が、分割数を更に増やせば、負荷インピーダンス
をより細く調整可能である。また、サセプタンス
の異なる同一厚さの誘導性窓を複数個準備する
と、インピーダンス調整範囲がより広くなる。
In this embodiment, the case of three divisions has been described, but if the number of divisions is further increased, the load impedance can be adjusted finer. Further, if a plurality of inductive windows of the same thickness and different susceptances are prepared, the impedance adjustment range becomes wider.

(1) 従来行なわれていた導波管内の電界最大点に
スタブ等を挿入する方法に代えて、誘導性窓を
用いてサセプタンスを変化させるために、マイ
クロ波耐圧は中空導波管と同じになる。
(1) Instead of the conventional method of inserting a stub etc. at the maximum electric field point in the waveguide, an inductive window is used to change the susceptance, so the microwave breakdown voltage is the same as that of a hollow waveguide. Become.

(2) この実施例では、λg/2を8分割して段階的に インピーダンスを調整すると説明したため、ス
タブ等のように連続的に変化される物と比較し
てインピーダンスの調整範囲が狭い印象を与え
るかもしれないが、位相導波管の分割を増せ
ば、実用上問題のない調整範囲が確保できる。
(2) In this example, since it was explained that λg/2 is divided into 8 and the impedance is adjusted stepwise, it gives the impression that the impedance adjustment range is narrow compared to something that changes continuously like a stub. However, by increasing the division of the phase waveguide, a practically acceptable adjustment range can be secured.

(3) 全長Lが一定であるから、接続される立体回
路系を固定したままで、インピーダンスを調整
可能である。
(3) Since the total length L is constant, the impedance can be adjusted while the three-dimensional circuit system to be connected remains fixed.

(4) 導波管分割数3で8種類、4で16種類、mで
2m種類のように、限られた分割数で多種類の位
相調整ができることになる。
(4) 8 types for waveguide division number 3, 16 types for 4, m
This means that many types of phase adjustments can be made with a limited number of divisions, such as 2 m types.

〔考案の効果〕[Effect of idea]

本考案によれば、マイクロ波耐圧が中空導波管
と同じで、従来の方法では極めて困難であつた大
出力マイクロ波装置、例えば、出力500KWの連
続マグネトロン発振装置の負荷インピーダンス調
整装置が得られる。
According to the present invention, the microwave breakdown voltage is the same as that of a hollow waveguide, and it is possible to obtain a load impedance adjustment device for a high-output microwave device, such as a continuous magnetron oscillator with an output of 500 KW, which was extremely difficult with conventional methods. .

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は本考案の負荷インピーダンス調整装置
の基本的構成を示す図、第2図〜第8図は誘導性
窓の位置を変えてインピーダンスを調整する状況
を説明する図、第9図は従来の3−スタブを示す
図である。 1……導波管、2……フランジ、3……スタ
ブ、4……誘導性窓、5……λg/16長さ導波管、6 ……λg/8長さ導波管、7……λg/4長さ導波管。
Figure 1 is a diagram showing the basic configuration of the load impedance adjustment device of the present invention, Figures 2 to 8 are diagrams explaining the situation in which the impedance is adjusted by changing the position of the inductive window, and Figure 9 is the conventional one. It is a figure showing 3-stub of. 1... Waveguide, 2... Flange, 3... Stub, 4... Inductive window, 5... λg/16 length waveguide, 6... λg/8 length waveguide, 7... ...λg/4 length waveguide.

Claims (1)

【実用新案登録請求の範囲】 マイクロ波伝送路に入れて負荷の整合をとる負
荷インピーダンス調整装置において、誘導性窓と
マイクロ波の位相を変えるために長さの異なるm
個の中空導波管とを組み合せてなり、中空導波管
の管軸方向の長さ12,……,nが、 1=1/2(1/2m+n1)λg 2=2/1(1/2m-1+n2)λg …………… n-1=1/2(1/4+nn-1)λg n=1/2(1/2+nn)λg m,n1,n2,……nn:任意の正の整数 λg:管内波長 であることを特徴とする負荷インピーダンス調整
装置。
[Claims for Utility Model Registration] In a load impedance adjustment device that is inserted into a microwave transmission line to match the load, an inductive window and a device having different lengths (meters) are used to change the phase of the microwave.
The lengths 1 , 2 , ..., n of the hollow waveguides in the tube axis direction are 1 = 1/2 (1/2 m + n 1 ) λg 2 = 2 /1 (1/2 m-1 +n 2 ) λg …………… n-1 = 1/2 (1/4 + n n-1 ) λg n = 1/2 (1/2 + n n ) λg m, n 1 , n 2 , ...n n : Any positive integer λg: A load impedance adjustment device characterized in that it is a tube wavelength.
JP5583085U 1985-04-15 1985-04-15 Expired JPH0352007Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP5583085U JPH0352007Y2 (en) 1985-04-15 1985-04-15

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP5583085U JPH0352007Y2 (en) 1985-04-15 1985-04-15

Publications (2)

Publication Number Publication Date
JPS61171304U JPS61171304U (en) 1986-10-24
JPH0352007Y2 true JPH0352007Y2 (en) 1991-11-11

Family

ID=30578870

Family Applications (1)

Application Number Title Priority Date Filing Date
JP5583085U Expired JPH0352007Y2 (en) 1985-04-15 1985-04-15

Country Status (1)

Country Link
JP (1) JPH0352007Y2 (en)

Also Published As

Publication number Publication date
JPS61171304U (en) 1986-10-24

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