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JPS6129566B2 - - Google Patents
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JPS6129566B2 - - Google Patents

Info

Publication number
JPS6129566B2
JPS6129566B2 JP16373679A JP16373679A JPS6129566B2 JP S6129566 B2 JPS6129566 B2 JP S6129566B2 JP 16373679 A JP16373679 A JP 16373679A JP 16373679 A JP16373679 A JP 16373679A JP S6129566 B2 JPS6129566 B2 JP S6129566B2
Authority
JP
Japan
Prior art keywords
waveguide
cruciform
waves
wave
circular
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
JP16373679A
Other languages
Japanese (ja)
Other versions
JPS5686504A (en
Inventor
Fumio Takeda
Osami Ishida
Shojiro Kanitani
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric Corp
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 Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP16373679A priority Critical patent/JPS5686504A/en
Publication of JPS5686504A publication Critical patent/JPS5686504A/en
Publication of JPS6129566B2 publication Critical patent/JPS6129566B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01PWAVEGUIDES; RESONATORS, LINES, OR OTHER DEVICES OF THE WAVEGUIDE TYPE
    • H01P1/00Auxiliary devices
    • H01P1/20Frequency-selective devices, e.g. filters
    • H01P1/213Frequency-selective devices, e.g. filters combining or separating two or more different frequencies
    • H01P1/2133Frequency-selective devices, e.g. filters combining or separating two or more different frequencies using coaxial filters

Landscapes

  • Control Of Motors That Do Not Use Commutators (AREA)
  • Waveguide Switches, Polarizers, And Phase Shifters (AREA)

Description

【発明の詳細な説明】 この発明はマイクロ波アンテナ系に用いられる
帯域共用分波器の改良に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an improvement of a band-sharing duplexer used in a microwave antenna system.

なおここでは説明の便宜上、高い周波数帯H
の波と、低い周波数帯Lの波とを分岐導波線路
を用いて分波する場合について説明する。まず従
来の帯域共用分波器の働きを詳述する。
For convenience of explanation, we will use the high frequency band H.
A case will be explained in which the waves of L and the waves of the low frequency band L are separated using a branch waveguide. First, the function of a conventional band-sharing demultiplexer will be explained in detail.

第1図は従来の帯域共用分波器の構成を示すも
ので、図中1は円形導波管、2は円形テーパ導波
管、3はろ波器、4は方形導波管、5はろ波器3
と方形導波管4とで構成される分岐導波線路、6
は分岐導波線路5と円形導波管1との隔壁に設け
られた円形導波管1の管軸方向に細長い結合孔で
ある。
Figure 1 shows the configuration of a conventional band-sharing duplexer. In the figure, 1 is a circular waveguide, 2 is a circular tapered waveguide, 3 is a filter, 4 is a rectangular waveguide, and 5 is a filter. Vessel 3
and a rectangular waveguide 4;
is a coupling hole elongated in the tube axis direction of the circular waveguide 1 provided in the partition wall between the branch waveguide line 5 and the circular waveguide 1.

この帯域共用分波器においては、円形テーパ導
波管2は、Hの波は伝搬するが、Lの波はしや
断されるように、また、ろ波器3はLの波は伝
搬するが、Hの波をしや断するように設計され
ている。
In this band-sharing splitter, the circular tapered waveguide 2 allows the H wave to propagate but the L wave is slightly cut off, and the filter 3 allows the L wave to propagate. However, it is designed to cut off H waves.

また、結合孔6は、円形導波管1の周方向に
180度回転した位置に相対向するように2個設け
られている。
Further, the coupling hole 6 is formed in the circumferential direction of the circular waveguide 1.
Two pieces are provided facing each other at positions rotated 180 degrees.

いま、第1図中の端子1に円形導波管1の基本
モード波(TE11モード)である周波数LH
の波が入射した場合を考え、TE11モード波の偏
波面と結合孔6との関係を第2図に示すように選
び、TE11モード波が管軸方向に細長い結合孔6
と結合できる状態にあるものとする。
Now, the frequencies L and H , which are the fundamental mode waves (TE 11 mode) of the circular waveguide 1, are connected to the terminal 1 in Fig. 1.
Considering the case where a wave of
It shall be possible to combine with.

まず、Lの波の伝搬について述べる。一部の
Lの波は結合孔6と結合し分岐導波線路5に伝
搬するが、他のLの波は円形テーパ導波管2に
達し、円形テーパ導波管のもつしや断特性により
完全に反射される。このとき、結合孔6の大きさ
と、円形テーパ導波管2と結合孔6までの間隔を
適当に選ぶと、Lの波はすべて分岐導波線路5
に分波される。
First, we will discuss the propagation of the L wave. Part of
The L wave is coupled to the coupling hole 6 and propagated to the branch waveguide 5, but the other L waves reach the circular taper waveguide 2 and are completely reflected due to the cross-section characteristics of the circular taper waveguide. be done. At this time, if the size of the coupling hole 6 and the distance between the circular tapered waveguide 2 and the coupling hole 6 are appropriately selected, all the waves of L will be transmitted to the branch waveguide 5.
It is split into two waves.

つぎに、Hの波の伝搬について述べる。H
波は、Lの波と同様に一部の波が結合孔6を介
して分岐導波線路5に結合するが、この帯域共用
分波器においては、分岐導波線路5に設けたろ波
器3により全て反射される。このろ波器3をでき
るだけ結合孔6に接して設けると、Hの波に対
しては結合孔6を等価的に短絡することができ
る。この結果Hの波はすべて円形テーパ導波管
2を伝搬し端子に達する。
Next, we will discuss the propagation of the H wave. Similar to the L wave, a part of the H wave is coupled to the branch waveguide line 5 through the coupling hole 6, but in this band-sharing splitter, a filter provided in the branch waveguide line 5 is used. It is all reflected by vessel 3. By providing this filter 3 as close to the coupling hole 6 as possible, the coupling hole 6 can be equivalently short-circuited for H waves. As a result, all the waves of H propagate through the circular tapered waveguide 2 and reach the terminal.

したがつて、端子より入射したLHの波
は、端子にLの波が、端子にHの波が分波
される。
Therefore, the L and H waves incident from the terminal are split into an L wave at the terminal and an H wave at the terminal.

この帯域共用分波器においてはLの波の偏波
面は結合孔6に対し第2図に示す関係であること
が必要であるが、任意偏波面のLの波を分波す
る場合には、分岐導波線路5を円形導波管1の周
方向に90度おきに4本設ければよい。なお第2図
においてイは電気力線である。
In this band-sharing splitter, it is necessary that the polarization plane of the L wave has the relationship shown in Fig. 2 with respect to the coupling hole 6, but when splitting the L wave with an arbitrary polarization plane, Four branch waveguide lines 5 may be provided at intervals of 90 degrees in the circumferential direction of the circular waveguide 1. Note that in Fig. 2, A is the line of electric force.

第3図に上述の任意偏波面の波を分波すること
ができる従来の帯域共用分波器の構成例を示す。
FIG. 3 shows an example of the configuration of a conventional band-sharing demultiplexer capable of demultiplexing the above-mentioned wave of arbitrary polarization plane.

第1図,第3図に示した帯域共用分波器は、い
ずれも円形導波管1と分岐導波線路5とを結合孔
6を介して接続しているが、第4図に示すように
分岐導波線路5を同軸線路7とし、同軸線路7の
中心導体にとりつけたプローブ8により円形導波
管1と同軸線路6を結合させても分波できる。
In both of the band-sharing duplexers shown in FIGS. 1 and 3, the circular waveguide 1 and the branch waveguide 5 are connected via a coupling hole 6, but as shown in FIG. Separation can also be achieved by using a coaxial line 7 as the branch waveguide line 5 and coupling the circular waveguide 1 and the coaxial line 6 with a probe 8 attached to the center conductor of the coaxial line 7.

しかし従来の第1図,第3図のような結合孔6
を介して分波する分波器では、分岐導波線路5を
円形導波管1に直交して設ける必要があるため、
構造が複雑で、工作性に難点がある。また、第4
図に示すようなプローブ8を介して分波する分波
器ではLの波を分波するために、プローブ8を
円形導波管1中に深く、かつ電界の強い位置に挿
入することが必要なため、プローブ8のHの波
に及ぼす影響が強く、とくにHの波の電力が大
きい場合に適用できないなどの欠点があつた。
However, the conventional coupling hole 6 as shown in Figs.
In a duplexer that demultiplexes signals via a
The structure is complex and there are difficulties in workability. Also, the fourth
In the demultiplexer that demultiplexes the waves through the probe 8 as shown in the figure, in order to demultiplex the L wave, the probe 8 must be inserted deep into the circular waveguide 1 and in a position where the electric field is strong. Therefore, it has a drawback that it has a strong influence on the H wave of the probe 8, and cannot be applied especially when the power of the H wave is large.

この発明はこれらの欠点を除去するため、分岐
導波線路5を十字形導波管に設けるようにしたも
ので、以下図面を用いて詳細に説明する。
In order to eliminate these drawbacks, the present invention provides the branch waveguide line 5 in a cruciform waveguide, and will be described in detail below with reference to the drawings.

まず、十字形導波管の概略を説明する。第5図
は十字形導波管を示す。この導波管は、図中に実
線と破線で、それぞれ示す直交する二つの偏波V
ロ,偏波Hハを伝搬することができる。したがつ
て、この導波管は円形導波管1と同様に任意の偏
波を伝搬できる。また十字形導波管の特徴は、電
磁界の対称性を考慮して励振すると、基本波のし
や断周波数と、基本波の励振するために発生しや
すい高次モード波のしや断周波数との間隔が円形
導波管1の場合に比べて非常に広くなるため、基
本波のみを励振できる周波数帯域が広いという長
所がある。
First, the outline of a cruciform waveguide will be explained. FIG. 5 shows a cruciform waveguide. This waveguide has two orthogonal polarized waves V shown by solid lines and broken lines in the figure, respectively.
B, polarized waves H and C can be propagated. Therefore, like the circular waveguide 1, this waveguide can propagate arbitrary polarized waves. In addition, the characteristics of a cruciform waveguide are that when excited considering the symmetry of the electromagnetic field, the shearing frequency of the fundamental wave and the shedding frequency of higher-order mode waves that are likely to be generated due to the excitation of the fundamental wave. Since the distance between the waveguide 1 and the circular waveguide 1 is much wider than that in the case of the circular waveguide 1, there is an advantage that the frequency band in which only the fundamental wave can be excited is wide.

第6図にこの発明の一実施例を示す。図中、
1,3,5,7は第4図と同じもの、9,10は
十字形導波管、11は十字形導波管と円形導波管
1との変換器、12は十字形テーパ導波管、13
Hの波に対する整合素子である。第6図中の
A―A,B―B,C―Cにおける断面図を第7図
a,b,cにそれぞれ対応して示す。
FIG. 6 shows an embodiment of the present invention. In the figure,
1, 3, 5, and 7 are the same as in Fig. 4, 9 and 10 are cruciform waveguides, 11 is a converter between a cruciform waveguide and a circular waveguide 1, and 12 is a cruciform taper waveguide. tube, 13
is a matching element for H waves. Cross-sectional views along lines AA, BB, and CC in FIG. 6 are shown corresponding to FIGS. 7a, b, and c, respectively.

この発明においては、第7図bに示すように、
十字形導波管9に設けられる分岐導波線路5には
同軸線路7が用いられており、十字形導波管9に
接してLの波のみを伝搬する同軸形のろ波器3
が備えられている。また、同軸線路7の内導体の
十字形導波管9側の一端は延長線上の十字形導波
管9の管壁に固定されており、分岐導波線路5と
十字形導波管9とは主として磁界により結合して
いる。この構成は一般によく知られている同軸・
導波管変換器とほぼ同様である。
In this invention, as shown in FIG. 7b,
A coaxial line 7 is used as the branch waveguide line 5 provided in the cruciform waveguide 9, and a coaxial filter 3 is connected to the cruciform waveguide 9 and propagates only the L wave.
is provided. Further, one end of the inner conductor of the coaxial line 7 on the cruciform waveguide 9 side is fixed to the tube wall of the cruciform waveguide 9 on the extension line, and the branch waveguide 5 and the cruciform waveguide 9 are connected to each other. are mainly coupled by magnetic fields. This configuration is commonly known as coaxial
It is almost similar to a waveguide transducer.

また、十字形テーパ導波管12は、従来の帯域
共用分波器と同様に、Lの波はしや断するが、
Hの波は通過するように設計されている。
In addition, the cross-shaped tapered waveguide 12, like a conventional band-sharing splitter, cuts the L wave, but
H waves are designed to pass through.

このように、第6図に示すこの発明は従来の帯
域共用分波器と同様の機能を有するろ波器3,テ
ーパ導波管12、分岐導波線路5への結合手段を
備えているので、第6図中の端子から入射した
LHの波のうち、Lの波は十字形テーパ導
波管12と分岐導波線路5の取り付け位置を調整
することにより、端子にすべて分波できる。
As described above, the present invention shown in FIG. 6 is equipped with a filter 3 having the same functions as a conventional band-sharing demultiplexer, a tapered waveguide 12, and a means for coupling to the branch waveguide 5. , incident from the terminal in Figure 6
Of the L and H waves, the L wave can all be branched to the terminal by adjusting the mounting positions of the cross-shaped tapered waveguide 12 and the branch waveguide 5.

またHの波は、ろ波器3の働きにより分岐導
波線路5に洩れこむことなく、端子に伝搬でき
る。
Further, the H wave can propagate to the terminal without leaking into the branch waveguide line 5 due to the action of the filter 3.

なお、この発明においてはHの波が分岐導波
線路5と十字形導波管9との結合部により一部反
射されるため、Hの波のみが伝搬する大きさの
小さい十字形導波管10部に整合素子13を設け
ることにより、反射波を少なくしている。
In addition, in this invention, since the H wave is partially reflected by the coupling part between the branch waveguide line 5 and the cruciform waveguide 9, the cruciform waveguide is small in size and only the H wave propagates. By providing the matching element 13 in the 10th section, reflected waves are reduced.

以上は、円形導波管1を十字形導波管9に変換
した場合の分波器について説明したが、この発明
はこれに限らず円形導波管1のかわりに正方形導
波管を使用してもよい。
The above describes a duplexer in which the circular waveguide 1 is converted into a cross-shaped waveguide 9. However, the present invention is not limited to this, and a square waveguide may be used instead of the circular waveguide 1. It's okay.

以上のように、この発明に係る帯域共用分波器
では、十字形導波管9を用いるので第1図,第3
図に示すような帯域共用分波器に比べて、円形導
波管1に結合孔6を介して直交して方形導波管4
を取りつける必要がないため、電鋳加工などによ
り容易に工作できる利点がある。また、第4図に
示すような帯域共用分波器に比べて、分岐導波線
路5と十字形導波管9との結合部をHの波の電
界の弱い十字形導波管9の周辺部に取りつけるこ
とができるのでHの波の伝送電力が大きい場合
にも用いることができる利点がある。
As described above, since the band-sharing duplexer according to the present invention uses the cruciform waveguide 9, FIGS.
Compared to the band-sharing duplexer shown in the figure, a rectangular waveguide 4 is connected orthogonally to the circular waveguide 1 via the coupling hole 6.
Since there is no need to attach a wire, it has the advantage that it can be easily machined by electroforming. In addition, compared to a band-sharing splitter as shown in FIG . It has the advantage of being able to be used even when the transmission power of the H wave is large because it can be attached to the main body.

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

第1図は従来の帯域共用分波器の一部破断せる
概略構成図、第2図は電界分布と結合孔位置の関
係を示す説明図、第3図は任意偏波のLの波を
分波できる従来の帯域共用分波器の概略構成図、
第4図は分岐導波線路に同軸線路を用いた従来の
帯域共用分波器の一部破断せる構造図、第5図は
十字形導波管の電気力線を示す説明図、第6図は
この発明の一実施例を示す概略構成図、第7図は
第6図の断面形状を表わす断面図である。 図中、1は円形導波管、2は円形テーパ導波
管、3はろ波器、5は分岐導波線路、9は十字形
導波管、11はは変換器、12は十字形テーパ導
波管である。なお図中、同一あるいは相当部分に
は同一符号を付して示してある。
Figure 1 is a partially cutaway schematic diagram of a conventional band-sharing demultiplexer, Figure 2 is an explanatory diagram showing the relationship between electric field distribution and coupling hole position, and Figure 3 is an arbitrary polarized L wave splitter. A schematic configuration diagram of a conventional band-sharing demultiplexer that can
Fig. 4 is a partially cutaway structural diagram of a conventional band-sharing duplexer using a coaxial line as the branch waveguide, Fig. 5 is an explanatory diagram showing the lines of electric force in a cruciform waveguide, and Fig. 6 7 is a schematic configuration diagram showing one embodiment of the present invention, and FIG. 7 is a sectional view showing the cross-sectional shape of FIG. 6. In the figure, 1 is a circular waveguide, 2 is a circular tapered waveguide, 3 is a filter, 5 is a branch waveguide, 9 is a cruciform waveguide, 11 is a converter, and 12 is a cruciform taper guide. It is a wave tube. In the drawings, the same or corresponding parts are denoted by the same reference numerals.

Claims (1)

【特許請求の範囲】[Claims] 1 複数の周波数帯域で共用する分波器におい
て、上記複数の周波数帯域の波が伝搬できる第1
の円形導波管または正方形導波管と、上記複数の
周波数帯域の波が伝搬できる第1の十字形導波管
と、上記複数の周波数帯域の波のうち高い周波数
帯域の波だけが伝搬できる第2の十字形導波管
と、上記高い周波数帯域の波だけが伝搬できる第
2の円形導波管または正方形導波管と、上記第1
の円形導波管または正方形導波管と上記第1の十
字形導波管とを接続する変換器と、上記第1の十
字形導波管と上記第2の十字形導波管とを接続す
る十字形テーパ導波管と、上記第2の十字形導波
管と上記第2の円形導波管または正方形導波管と
を接続する変換器と、低域通過ろ波器を備えた複
数個の分岐導波線路とで構成し、上記分岐導波線
路を上記第1の十字形導波管に結合させたことを
特徴とする帯域共用分波器。
1. In a duplexer that is shared by multiple frequency bands, the first
a circular waveguide or a square waveguide; a first cross-shaped waveguide through which waves in the plurality of frequency bands can propagate; and a first cross-shaped waveguide through which waves in the plurality of frequency bands can propagate, and only waves in a high frequency band among the waves in the plurality of frequency bands can propagate. a second cruciform waveguide, a second circular waveguide or a square waveguide through which only waves in the high frequency band can propagate;
a converter that connects a circular waveguide or a square waveguide with the first cruciform waveguide; and a converter that connects the first cruciform waveguide with the second cruciform waveguide. a cruciform tapered waveguide, a transducer connecting the second cruciform waveguide and the second circular waveguide or the square waveguide, and a low-pass filter. A band-sharing duplexer comprising: a branch waveguide, and the branch waveguide is coupled to the first cruciform waveguide.
JP16373679A 1979-12-17 1979-12-17 Branching filter in common use of band Granted JPS5686504A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP16373679A JPS5686504A (en) 1979-12-17 1979-12-17 Branching filter in common use of band

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP16373679A JPS5686504A (en) 1979-12-17 1979-12-17 Branching filter in common use of band

Publications (2)

Publication Number Publication Date
JPS5686504A JPS5686504A (en) 1981-07-14
JPS6129566B2 true JPS6129566B2 (en) 1986-07-08

Family

ID=15779688

Family Applications (1)

Application Number Title Priority Date Filing Date
JP16373679A Granted JPS5686504A (en) 1979-12-17 1979-12-17 Branching filter in common use of band

Country Status (1)

Country Link
JP (1) JPS5686504A (en)

Also Published As

Publication number Publication date
JPS5686504A (en) 1981-07-14

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