JPS60146504A - Rectangular-circular waveguide converter - Google Patents

Rectangular-circular waveguide converter

Info

Publication number
JPS60146504A
JPS60146504A JP287184A JP287184A JPS60146504A JP S60146504 A JPS60146504 A JP S60146504A JP 287184 A JP287184 A JP 287184A JP 287184 A JP287184 A JP 287184A JP S60146504 A JPS60146504 A JP S60146504A
Authority
JP
Japan
Prior art keywords
waveguide
rectangular
circular
rectangular waveguide
circular waveguide
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.)
Granted
Application number
JP287184A
Other languages
Japanese (ja)
Other versions
JPH0142541B2 (en
Inventor
Toshihide Tanaka
田中 年秀
Yoshikazu Yoshimura
吉村 芳和
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial 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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP287184A priority Critical patent/JPS60146504A/en
Publication of JPS60146504A publication Critical patent/JPS60146504A/en
Publication of JPH0142541B2 publication Critical patent/JPH0142541B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01PWAVEGUIDES; RESONATORS, LINES, OR OTHER DEVICES OF THE WAVEGUIDE TYPE
    • H01P5/00Coupling devices of the waveguide type
    • H01P5/08Coupling devices of the waveguide type for linking dissimilar lines or devices
    • H01P5/082Transitions between hollow waveguides of different shape, e.g. between a rectangular and a circular waveguide

Abstract

PURPOSE:To attain excellent matching over a broad band by inserting a rectangular waveguide near square form and a long elliptic waveguide for the conversion from the rectangular waveguide into the circular waveguide. CONSTITUTION:The shape of cross section of the long elliptic waveguide 5 is as shown in Fig. (b) and close to the shape of cross section of the rectangular waveguide 1 to be converted as shown in Fig. (a). On the other hand, the rectangular waveguide 6 connected to the circular waveguide 2 to be converted as shown in Fig. (d) has the shape of cross section close to a square in matching with the shape of cross section of the circular waveguide 2 as shown in Fig. (c). Thus, the conversion between both said waveguides is conducted very smoothly. Moreover, the long elliptic waveguide 5 and the rectangular waveguide 6 close to a square are in the relation of shape as shown in Figs. (b) and (c) and the conversion of both is conducted smoothly. As a result, the rectangular-circular waveguide converter constituted above has a broad band matching characteristic.

Description

【発明の詳細な説明】 産業上の利用分野 本発明は、マイクロ波回路における各マイクロ波線路の
線路変換に関するものであシ、特に衛星放送用受信等に
おけるアンテナ、マイクロ波受信機によく利用される矩
形導波管2円形導波管の線路変換に必要とされる矩形−
円形導波管変換装置に係るのである。
DETAILED DESCRIPTION OF THE INVENTION Field of Industrial Application The present invention relates to line conversion of each microwave line in a microwave circuit, and is particularly commonly used in antennas and microwave receivers for satellite broadcast reception. Rectangular waveguide required for line conversion of two circular waveguides -
It concerns a circular waveguide conversion device.

従来例の構成とその問題点 従来の矩形−円形導波管装置の一例を第1図に示す。Conventional configuration and its problems An example of a conventional rectangular-circular waveguide device is shown in FIG.

同図では、矩形導波管1から円形導波管2への変換を円
形から矩形へテーパーを設けることによりスムーズな変
換を行なっている。しかし、この場合は全長が非常に長
くなる欠点があり、受信機等に装着する場合には不都合
である。
In the figure, a rectangular waveguide 1 is smoothly converted to a circular waveguide 2 by providing a taper from a circular shape to a rectangular shape. However, in this case, there is a drawback that the overall length is extremely long, which is inconvenient when attached to a receiver or the like.

第2図に他の従来例を示す。第2図では、矩形導波1と
円形導波管2の間に楕円形導波管4を入れて矩形−円形
導波管変換を行なっている。この方法は第1図のテーパ
一方式に比べ全長を短かくすることが出来るが、帯域幅
が狭くなる欠点がある0 なお第1図、第8図で、1は矩形導波管、2は円形導波
管、3は矩形から円形導波管へのテーパ導波管で、4は
楕円導波管である。
FIG. 2 shows another conventional example. In FIG. 2, an elliptical waveguide 4 is inserted between a rectangular waveguide 1 and a circular waveguide 2 to perform rectangular-circular waveguide conversion. This method can shorten the total length compared to the taper type shown in Figure 1, but has the disadvantage of narrowing the bandwidth.In Figures 1 and 8, 1 is a rectangular waveguide, and 2 is a rectangular waveguide A circular waveguide, 3 is a tapered waveguide from a rectangular to a circular waveguide, and 4 is an elliptical waveguide.

発明の目的 本発明はこのような欠点をなくし、広帯域で、整合イン
ピーダンスが良好で、かつ全長を短かくすることの出来
る矩形と円形の導波管変換装置を提供しようとするもの
である。
OBJECTS OF THE INVENTION The present invention aims to eliminate such drawbacks and provide a rectangular to circular waveguide conversion device that has a wide band, has good matching impedance, and can have a short overall length.

発明の構成 本発明による矩形−円形導波管変換装置は、第1の矩形
導波管に長楕円型導波管を接続し、この長楕円型導波管
に第2の矩形導波管を接続し、この第2の矩形導波管に
円形導波管を接続するようにして、上記第1の矩形導波
管と円形導波管を結合するようにしたものであり、小型
でかつ変換がスムーズに行える変換装置を得ることがで
きる。
Structure of the Invention The rectangular-circular waveguide conversion device according to the present invention connects an elongated waveguide to a first rectangular waveguide, and connects a second rectangular waveguide to the elongated waveguide. The first rectangular waveguide and the circular waveguide are connected by connecting the first rectangular waveguide and the circular waveguide to the second rectangular waveguide. It is possible to obtain a conversion device that can perform the conversion smoothly.

実施例の説明 本発明の一実施例を第3図、第4図に示す。Description of examples An embodiment of the present invention is shown in FIGS. 3 and 4.

第3図で、1は矩形導波管、2は円形導波管、5.6は
前記矩形導波管1と円形導波管2の間に接続される長楕
円型導波管及び正方形に近い矩形型導波管である。
In FIG. 3, 1 is a rectangular waveguide, 2 is a circular waveguide, and 5.6 is an oblong waveguide connected between the rectangular waveguide 1 and the circular waveguide 2, and a square waveguide. It is a nearly rectangular waveguide.

この接続の様子を第4図に示す。同図aは各導波管の接
続断面図、b、cは矩形導波管1の入力側及び円形導波
管2の入力側よりみた各入力正面図を示す。第4図で第
3図と同一符号は同一物を示す。
FIG. 4 shows how this connection is made. Figure a shows a connection sectional view of each waveguide, and figures b and c show input front views seen from the input side of the rectangular waveguide 1 and the input side of the circular waveguide 2. In FIG. 4, the same reference numerals as in FIG. 3 indicate the same parts.

すなわち、第4図では矩形導波管1から円形導波管2へ
の変換を2段階で行なって昇り、まず矩形導波管1に、
矩形断面のE面の幅すより大きい幅の平行二辺と、二つ
円弧で囲まれた第1の変換導波管である長楕円型導波管
5を接続する。この場合、接続断面において矩形導波管
1のE面で切られる長楕円型導波管5の円弧の面積と、
長楕円型導波管5の円弧で切られる矩形導波管の2つの
コーナ部の面積とがはソ等しくなるようにしているO このようにすることにより、矩形導波管1と長楕円型導
波管6は第5図の1,5の電界分布が示すようにスムー
ズに電界結合により変換される。
That is, in FIG. 4, the conversion from the rectangular waveguide 1 to the circular waveguide 2 is performed in two stages, and the rectangular waveguide 1 is first converted into the circular waveguide 2.
Two parallel sides having a width larger than the width of the E plane of the rectangular cross section are connected to an elongated elliptical waveguide 5, which is a first conversion waveguide and is surrounded by two circular arcs. In this case, the area of the arc of the long elliptical waveguide 5 cut by the E plane of the rectangular waveguide 1 in the connection cross section,
The areas of the two corners of the rectangular waveguide cut by the arc of the long elliptical waveguide 5 are made to be equal. The waveguide 6 is smoothly transformed by electric field coupling, as shown by the electric field distributions 1 and 5 in FIG.

次に、この長楕円型導波管5と円形導波管2の間に第4
図又は第5図の6に示すような断面が正方形に近い矩形
型導波管6を接続し、その次に円形導波管2を接続する
。矩形型導波管6は正規の矩形導波管10幅aに比べ横
幅a2(H面の幅に対応)が短く、縦幅b2(E面の幅
に対応)を長くして、縦幅が横幅よりわずかに長い(縦
横比約6:5)正方形に近い断面とし、その断面の各コ
ーナはわずかに曲率を持たせている。まだ、この矩形型
導波管6の横幅は円形導波管2の直径にほぼ等しクシ、
縦幅はこの直径より少し長くしている。
Next, a fourth waveguide is placed between the long elliptical waveguide 5 and the circular waveguide
A rectangular waveguide 6 having a nearly square cross section as shown in 6 in the figure or FIG. 5 is connected, and then a circular waveguide 2 is connected. The rectangular waveguide 6 has a shorter width a2 (corresponding to the width of the H plane) and a longer vertical width b2 (corresponding to the width of the E plane) than the width a of the regular rectangular waveguide 10. It has a nearly square cross section that is slightly longer than the width (an aspect ratio of about 6:5), and each corner of the cross section has a slight curvature. However, the width of this rectangular waveguide 6 is approximately equal to the diameter of the circular waveguide 2.
The vertical width is slightly longer than this diameter.

このようにすることにより、円形導波管2と矩形型導波
管6とは第6図の2,6に示すように電界結合によりス
ムーズに変換される。一方、この矩形型導波管6と長楕
円型導波管50間も第6図の5.6の電界分布からも明
らかなように、両者はスムーズに結合する。
By doing so, the circular waveguide 2 and the rectangular waveguide 6 are smoothly converted by electric field coupling as shown at 2 and 6 in FIG. On the other hand, as is clear from the electric field distribution at 5.6 in FIG. 6, the rectangular waveguide 6 and the oblong waveguide 50 are smoothly coupled.

一般に、矩形導波管に比べ円形導波管は高い特性インピ
ーダンスを呈する。すなわち、矩形導波管の特性インピ
ーダンスZwは、 但し、λg□ は管内波長で、 zo は自由空間の特性インピーダンス、a、bは矩形
導波管の長辺と短辺で、λは自由空間中の波長で、ある
Generally, a circular waveguide exhibits a higher characteristic impedance than a rectangular waveguide. In other words, the characteristic impedance Zw of a rectangular waveguide is, where λg□ is the wavelength inside the tube, zo is the characteristic impedance in free space, a, b are the long and short sides of the rectangular waveguide, and λ is the wavelength in free space. There is a wavelength of

今、矩形導波管をW’Rγ5 (a =19.05mm
 。
Now, the rectangular waveguide is defined as W'Rγ5 (a = 19.05mm
.

b=a/2)とすると、入力信号周波数が11.7GH
zおよび12.2GHzで特性インピーダンスZWRは
509 (Qおよび493(gである。
b=a/2), the input signal frequency is 11.7GH
The characteristic impedance ZWR at z and 12.2 GHz is 509 (Q and 493 (g).

一方、円形導波管の特性インピーダンスZWoおよび管
内波長λ9oは次式で表わされる。
On the other hand, the characteristic impedance ZWo and the guide wavelength λ9o of the circular waveguide are expressed by the following equation.

r:円形導波管の半径、 x(m、m):ベソセル関数Tm (x(m、+n))
=0の根、 TE11モードの時、TI(x(i 、 1 ))−〇
であり、x(1,1)=、1.841である。
r: radius of circular waveguide, x (m, m): Beso cell function Tm (x (m, +n))
= root of 0, In TE11 mode, TI(x(i, 1))-〇, and x(1,1)=, 1.841.

入力信号周波数が11.7GHzおよび12 、2GH
zの時で円形導波管がCR62(r≠8鮨)の場合、特
性インピーダンスはそれぞれ、Zwo1= 1249(
財)。
Input signal frequency is 11.7GHz and 12.2GHz
When the circular waveguide is CR62 (r≠8) at the time of z, the characteristic impedance is Zwo1 = 1249 (
wealth).

Zwo2≠930 (、Qとなり、前述の矩形導波管に
比べて約2倍の特性インピーダンスを示す。したがって
、矩形導波管と円形導波管の間の導波管変換を短い導波
管長でスムーズに結合するように構成することは簡単で
ない。
Zwo2≠930 (, Q, and the characteristic impedance is about twice that of the rectangular waveguide described above. Therefore, waveguide conversion between a rectangular waveguide and a circular waveguide can be performed with a short waveguide length. It is not easy to configure them so that they can be combined smoothly.

そこで、本装置では、前述の第4図、第5図に示すよう
に、矩形導波管1から円形導波管2への間に長楕円型導
波管5と略正方形の矩形型導波管6を設け、長楕円型導
波管5の横幅a1 を矩形導波管1の横幅a。とほぼ等
しくシ、かつ高さblは矩形導波管1の高さす。より高
くして長楕円型導波管6の特性インピーダンスを高くシ
、さらに略正方形の矩形型導波管6では横幅a2 を矩
形導波管1のa。より狭くし、高さを長楕円型導波管5
の高さbl より大きくすることにより、特性インピー
ダンスは式■、■からさらに大きくなり、円形導波管2
の特性インピーダンスに近づき、スムーズな導波管変換
を得ている。また、矩形型導波管6の長さを長楕円型導
波管5の長さよシ約1.5倍長くし、円形導波管2から
の結合をよりスムーズにしている。
Therefore, in this device, as shown in FIG. 4 and FIG. A tube 6 is provided, and the width a1 of the long elliptical waveguide 5 is the same as the width a of the rectangular waveguide 1. , and the height bl is the height of the rectangular waveguide 1. The characteristic impedance of the elongated elliptical waveguide 6 is increased by increasing the width a2 of the rectangular waveguide 1. Narrower and taller elongated waveguide 5
By increasing the height bl of the circular waveguide 2, the characteristic impedance becomes larger from the equations
The characteristic impedance is close to that of , and smooth waveguide conversion is obtained. Further, the length of the rectangular waveguide 6 is made approximately 1.5 times longer than the length of the oblong waveguide 5, thereby making the coupling from the circular waveguide 2 smoother.

第5図において、矩形導波管1でa。−19,05間。In FIG. 5, the rectangular waveguide 1 is a. -19.05 hours.

bo −9、5tnm (WR75)とし、円形導波管
20半径r # 8 mm (CR62)とすると、長
楕円型導波管5でb1磐13mm 、円弧の半径R#1
0mm 、導波管長約81mmとし、正方形型矩形導波
管6でa 丑15 rnm 、 b2共18 ran 
、導波管長約12脳とすることにより、特に12GHz
帯(約11.7〜12 、7GHz )で広帯域に整合
された矩形−円形導波管変換器を構成することが出来る
0 したがって、第4図aのように長楕円形導波管5と正方
形に近い矩形型導波管6を一体化したものの両端に矩形
導波管(WR75)及び円形4波管(CR62)のフラ
ンジを取り付けることにより、簡単な矩形−円形導波管
変換器を構成することができ、さらに第6図に示すよう
に、長楕円型導波管5及び矩形型導波管6にそれぞれフ
ランジを取り付けることにより、全長約2鋸程度の非常
に小型の矩形−円形変換アダプタとして構成することが
できる。
If bo -9, 5tnm (WR75) and circular waveguide 20 radius r # 8 mm (CR62), elongated elliptical waveguide 5 has b1 13 mm and arc radius R #1.
0 mm, the waveguide length is about 81 mm, and the square type rectangular waveguide 6 has a wave length of 15 rnm and a waveguide length of 18 ran for both a and b.
, especially at 12 GHz by setting the waveguide length to about 12 mm.
It is possible to construct a broadband matched rectangular-to-circular waveguide converter in the band (approximately 11.7 to 12 GHz, 7 GHz). Therefore, as shown in FIG. A simple rectangular-circular waveguide converter is constructed by attaching flanges of a rectangular waveguide (WR75) and a circular 4-wave tube (CR62) to both ends of an integrated rectangular waveguide 6 similar to the one shown in FIG. Furthermore, as shown in FIG. 6, by attaching flanges to the elongated waveguide 5 and the rectangular waveguide 6, a very small rectangular-circular conversion adapter with a total length of about 2 saws can be created. It can be configured as

なお、第6図で7,8はフランジ、9はフランジの留め
穴を示す。
In addition, in FIG. 6, 7 and 8 indicate flanges, and 9 indicates a fastening hole of the flange.

発明の効果 以上述べたように、本発明によれば、円形導波管と矩形
導波管の変換を広弗・域に整合良く、低損失(0,01
dB以下)でかつ非常に短い構造で構成することができ
、小型で低廉な矩形−円形導波管変換器および変換装置
を提供することができる。
Effects of the Invention As described above, according to the present invention, conversion between a circular waveguide and a rectangular waveguide can be performed with good matching over a wide range and with low loss (0,01
dB or less) and can be configured with a very short structure, making it possible to provide a small and inexpensive rectangular-circular waveguide converter and conversion device.

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

第1図は従来例におけるテーパー状の矩形−円形導波管
変換器の斜視図、第2図は楕円形導波管を介した従来の
他の矩形−円形導波管変換器の斜祖国、第3図は本発明
の一実施例における矩形−ける各導波管の開口面を示す
図、第6図は本発明の他の例で矩形−円形導波管変換ア
ダプタ例を示す要部断面図である。 1・・・・・・矩形導波管、2・・・・・・円形導波管
、5・・・・・・長楕円型導波管、6・・・・・矩形型
導波管、7,8 ・・フランジ。 代理人の氏名 弁理士 中 尾 敏 男 ほか1名第1
月 、3
FIG. 1 is a perspective view of a conventional tapered rectangular-circular waveguide converter, and FIG. 2 is a perspective view of another conventional rectangular-circular waveguide converter via an elliptical waveguide. FIG. 3 is a diagram showing the opening surface of each rectangular waveguide in one embodiment of the present invention, and FIG. 6 is a cross-sectional view of a main part showing an example of a rectangular to circular waveguide conversion adapter in another embodiment of the present invention. It is a diagram. 1... Rectangular waveguide, 2... Circular waveguide, 5... Long elliptical waveguide, 6... Rectangular waveguide, 7, 8...Flange. Name of agent: Patent attorney Toshio Nakao and 1 other person No. 1
month, 3

Claims (6)

【特許請求の範囲】[Claims] (1)第1の矩形導波管に長楕円型導波管を接続しこの
長楕円型導波管に第2の矩形導波管を接続し、この第2
の矩形導波管に円形導波管を接続することによシ、前記
第1の矩形導波管と前記円形導波管とを結合するように
したことを特徴とする矩形−円形導波管変換装置。
(1) Connect an elongated waveguide to the first rectangular waveguide, connect a second rectangular waveguide to the elongated waveguide, and connect the second rectangular waveguide to the elongated waveguide.
A rectangular-circular waveguide characterized in that the first rectangular waveguide and the circular waveguide are coupled by connecting the circular waveguide to the rectangular waveguide. conversion device.
(2)長楕円型導波管の断面の長手方向と、第2の矩形
導波管の断面の長手方向とが直交するよう忙接続したこ
とを特徴とする特許請求の範囲第1項記載の矩形−円形
導波管変換装置。
(2) The long elliptical waveguide is connected so that the longitudinal direction of the cross section of the second rectangular waveguide is orthogonal to the longitudinal direction of the cross section of the second rectangular waveguide. Rectangular-circular waveguide conversion device.
(3)第1の矩形導波管のH面とE面の幅の比を2:1
とし、第2の矩形導波管の第1の矩形導波管のH面、E
面に対応する横、縦の比を2:1以下にすることを特徴
とする特許請求の範囲第1項記載の矩形−円形導波管変
換装置。
(3) The width ratio of the H-plane and E-plane of the first rectangular waveguide is 2:1.
and the H plane of the first rectangular waveguide of the second rectangular waveguide, E
2. The rectangular-to-circular waveguide conversion device according to claim 1, wherein the horizontal to vertical ratio corresponding to the plane is 2:1 or less.
(4)第2の矩形導波管の内壁の各コーナに、一定の曲
率を持たせたととを特徴とする特許請求の範囲第1項ま
たは第3項記載の矩形−円形導波管変換装置。
(4) The rectangular-circular waveguide conversion device according to claim 1 or 3, characterized in that each corner of the inner wall of the second rectangular waveguide has a constant curvature. .
(5)長楕円型導波管の断面の2つの長辺を平行かつそ
の間隔を前記第1の矩形導波管のE面の幅より大きくし
、他の二辺を円弧で形成し、この円弧の直径を前記第1
の矩形導波管のH面の幅と同等以上の長さにしかつ、E
面とH面の対角線長より短かくすることを特徴とする特
許請求の範囲第1項記載の矩形−円形導波管変換装置。
(5) The two long sides of the cross section of the long elliptical waveguide are parallel and the distance between them is larger than the width of the E plane of the first rectangular waveguide, and the other two sides are formed by circular arcs. The diameter of the arc is the first
The length must be equal to or greater than the width of the H-plane of the rectangular waveguide, and the E
2. The rectangular-circular waveguide conversion device according to claim 1, wherein the length is shorter than the diagonal length of the H-plane.
(6)第2の矩形導波管断面の1組の平行2辺の長さを
、円形導波管の直径と同等以下にし、他の平行2辺の長
さを前記円形導波管の直径より長くすることを特徴とす
る特許請求の範囲第1項第2項。 第3項または第4項記載の矩形−円形導波管変換装置。
(6) The length of one set of two parallel sides of the second rectangular waveguide cross section is equal to or less than the diameter of the circular waveguide, and the length of the other two parallel sides is set to the diameter of the circular waveguide. Claim 1, item 2, characterized in that the length is longer. The rectangular-circular waveguide conversion device according to item 3 or 4.
JP287184A 1984-01-11 1984-01-11 Rectangular-circular waveguide converter Granted JPS60146504A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP287184A JPS60146504A (en) 1984-01-11 1984-01-11 Rectangular-circular waveguide converter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP287184A JPS60146504A (en) 1984-01-11 1984-01-11 Rectangular-circular waveguide converter

Publications (2)

Publication Number Publication Date
JPS60146504A true JPS60146504A (en) 1985-08-02
JPH0142541B2 JPH0142541B2 (en) 1989-09-13

Family

ID=11541412

Family Applications (1)

Application Number Title Priority Date Filing Date
JP287184A Granted JPS60146504A (en) 1984-01-11 1984-01-11 Rectangular-circular waveguide converter

Country Status (1)

Country Link
JP (1) JPS60146504A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2011151450A (en) * 2010-01-19 2011-08-04 Nippon Telegr & Teleph Corp <Ntt> Radio equipment
ES2394819A1 (en) * 2011-04-15 2013-02-05 Universidad De Cantabria Transducer structure of wave guidance modes based on octogonal sections (Machine-translation by Google Translate, not legally binding)
CN104078734A (en) * 2013-03-29 2014-10-01 莫列斯公司 High-frequency transmission device

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2011151450A (en) * 2010-01-19 2011-08-04 Nippon Telegr & Teleph Corp <Ntt> Radio equipment
ES2394819A1 (en) * 2011-04-15 2013-02-05 Universidad De Cantabria Transducer structure of wave guidance modes based on octogonal sections (Machine-translation by Google Translate, not legally binding)
CN104078734A (en) * 2013-03-29 2014-10-01 莫列斯公司 High-frequency transmission device
US9577309B2 (en) 2013-03-29 2017-02-21 Molex, Llc High-frequency wave transmitting device including a connecting portion for connecting a waveguide to an antenna
CN104078734B (en) * 2013-03-29 2017-03-29 莫列斯公司 High-frequency transmission devices

Also Published As

Publication number Publication date
JPH0142541B2 (en) 1989-09-13

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