JPS63310202A - Circularly polarized wave generator - Google Patents

Circularly polarized wave generator

Info

Publication number
JPS63310202A
JPS63310202A JP14661987A JP14661987A JPS63310202A JP S63310202 A JPS63310202 A JP S63310202A JP 14661987 A JP14661987 A JP 14661987A JP 14661987 A JP14661987 A JP 14661987A JP S63310202 A JPS63310202 A JP S63310202A
Authority
JP
Japan
Prior art keywords
phase difference
circularly polarized
polarized wave
wave generator
quartz glass
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.)
Pending
Application number
JP14661987A
Other languages
Japanese (ja)
Inventor
Juji Morita
森田 重次
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 JP14661987A priority Critical patent/JPS63310202A/en
Publication of JPS63310202A publication Critical patent/JPS63310202A/en
Pending legal-status Critical Current

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

Abstract

PURPOSE:To obtain a circularly polarized wave generator which can execute a fine adjustment of a 90 deg. phase difference without necessitating a screw for fine adjustment, by combining variously and using those which consist of different materials and lengths, for a dielectric support for fixing quartz glass. CONSTITUTION:In a circularly polarized wave generator, a phase difference of a radio wave E1 being parallel to quartz glass 2 and a radio wave E2 being orthogonal to the quartz glass 2 can be brought to a fine adjustment to 90 deg.. When a dielectric support 3b has been used, a phase difference characteristic 3b is smaller than 90 deg. phase difference, and when a dielectric support 3a has been used, a phase difference characteristic 3a is a little larger than 90 deg. phase difference. As for one part among three parts of the supports of quartz 2, the dielectric support 3a is used, and as for the remaining two parts, the support 3b is used. As a result, the phase difference characteristic becomes nearer 90 deg. by combing one piece of phase difference characteristic 3a and tow pieces of 3b. In such a way, by combining variously and using the dielectric supports whose materials are different, a 90 deg. phase difference can be brought to a fine adjustment, and the electric characteristic is improved.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 この発明は、石英ガラス装荷形の円偏波発生器に関する
ものである。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a circularly polarized wave generator loaded with quartz glass.

〔従来の技術〕[Conventional technology]

第7図及び第8図は従来の円偏波発生器を示す側面断面
図及び正面図である。図中、1は円形導波管、2は円形
導波管1内に装荷された石英ガラス、3は石英ガラス2
を固定するための誘電体サポート、4は誘電体サポート
3を固定するための金具、5は位相量を調整するための
微調用ネジである。
FIGS. 7 and 8 are a side sectional view and a front view showing a conventional circularly polarized wave generator. In the figure, 1 is a circular waveguide, 2 is quartz glass loaded in the circular waveguide 1, and 3 is quartz glass 2.
4 is a metal fitting for fixing the dielectric support 3, and 5 is a fine adjustment screw for adjusting the phase amount.

この種の円偏波発生器は、第8図に示すように、石英ガ
ラス2と平行な電波E1と石英ガラス2に直交した電波
E2との位相差を90″にすることにより円偏波発生器
として機能するものである。
As shown in Figure 8, this type of circularly polarized wave generator generates circularly polarized waves by making the phase difference between the radio wave E1 parallel to the quartz glass 2 and the radio wave E2 perpendicular to the silica glass 2 to 90''. It functions as a vessel.

この位相差をもたらすには、石英ガラス2のもつ比誘電
率ε1と石英ガラス2を固定するための誘電体サポート
3の持つ比誘電体ε2とにより、石英ガラス2に平行な
電波E1を直交した電i2J E2より90″近(まで
位相を遅らせ、その後多数の微調用ネジ5で微調して9
0°の位相差となるようにする。
In order to bring about this phase difference, the radio waves E1 parallel to the quartz glass 2 are made to cross at right angles by the dielectric constant ε1 of the quartz glass 2 and the dielectric constant ε2 of the dielectric support 3 for fixing the quartz glass 2. Delay the phase to nearly 90" (nearly 90") than the electric i2J E2, then finely adjust it with the many fine adjustment screws 5 to 9
The phase difference should be 0°.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

従来の円偏波発生器は以上のように構成されているので
、90″の位相差を調整するのに多数の微調用ネジ5が
必要であり、また微調用ネジ5が多数あるので調整時間
も長時間必要であるという問題点があった。
Since the conventional circularly polarized wave generator is configured as described above, a large number of fine adjustment screws 5 are required to adjust the phase difference of 90'', and since there are many fine adjustment screws 5, the adjustment time is shortened. There was also a problem that it required a long time.

この発明は上記のような問題点を解消するためになされ
たもので、微調用ネジを必要としないで90°位相差を
微調することができる円偏波発生器を得ることを目的と
する。
This invention was made to solve the above-mentioned problems, and an object thereof is to obtain a circularly polarized wave generator that can finely adjust a 90° phase difference without requiring a fine adjustment screw.

〔問題点を解決するための手段〕[Means for solving problems]

この発明による円偏波発生器は、石英ガラスを固定する
ための誘電体サポートに材質又は長さの異なったものを
種々組み合わせて使用するようにしたものである。
The circularly polarized wave generator according to the present invention uses various combinations of dielectric supports of different materials or lengths for fixing quartz glass.

〔作用〕[Effect]

この発明においては、誘電体サポートに材質又は長さの
異なるものを種々組み合わせて使用するようにしたので
、誘電体サポートのもつ比誘電率εを変化させることが
でき、これにより90°位相差を微調することができる
In this invention, since various combinations of dielectric supports of different materials or lengths are used, the relative permittivity ε of the dielectric supports can be changed, thereby reducing the 90° phase difference. Can be fine-tuned.

〔実施例〕〔Example〕

以下、この発明の実施例を図について説明する。 Embodiments of the present invention will be described below with reference to the drawings.

第1図及び第2図はこの発明の第1の実施例による円偏
波発生器を示す側面断面図及び正面図、第3図は本実施
例に用いる石英ガラスをサポートするためのm2体サポ
ートを示す図である。これらの図において、1は円形導
波管、2は石英ガラス、3.3a、3b、3cはそれぞ
れ材πが異なる誘電体サポート、λは誘電体サポートを
固定するための金具である。本実施例では、第3図に示
すような材質の異なった微調用誘電体サポート3.3a
、3b、3cの中から誘電体サポート3a、3bを選択
し組み合わせて用いている。
1 and 2 are side sectional views and front views showing a circularly polarized wave generator according to a first embodiment of the present invention, and FIG. 3 is an m2 body support for supporting quartz glass used in this embodiment. FIG. In these figures, 1 is a circular waveguide, 2 is quartz glass, 3.3a, 3b, and 3c are dielectric supports made of different materials π, and λ is a metal fitting for fixing the dielectric support. In this embodiment, a dielectric support 3.3a for fine adjustment made of different materials as shown in FIG.
, 3b, and 3c are selected and used in combination.

このような構成になる円偏波発生器では、第2図に示す
ように石英ガラス2と平行な電波E1と石英ガラス2に
直交した電波E2の位相差を90”にすることは従来例
と同様であり、また電波E1が電波E2より90°近く
まで位相遅れをするのもまた同様であるが、誘電体サポ
ートとして材質の異なる誘電体サボー)3a、3bを組
み合わせて用いているので、従来例のような微調用ネジ
を用いることなく、90°位相差を微調すること力くで
きる。
In a circularly polarized wave generator having such a configuration, as shown in Fig. 2, the phase difference between the radio wave E1 parallel to the quartz glass 2 and the radio wave E2 perpendicular to the quartz glass 2 is set to 90'', which is different from the conventional example. It is similar, and it is also the same that the radio wave E1 is delayed in phase by nearly 90 degrees from the radio wave E2, but since a combination of dielectric supports 3a and 3b of different materials is used as the dielectric support, it is different from the conventional method. It is possible to finely adjust the 90° phase difference without using a fine adjustment screw as in the example.

これは、例えば、第3図に示す誘電体サポート3bを使
用した場合の位相差特性が第4図Gこ示す位相差特性3
bの如く90°より小さく、誘電体サポーt−3aを使
用した位相差特性が位相差特性3aの如<90”よりや
や大きい場合において、第1図に示す石英ガラス2のサ
ポート3ケ所のうち1ケ所を誘電体サポー)3aを使用
し、残り2ケ所に誘電体サポート3bを使用することに
より、位相差特性が第4図に示す位相差特性3a1個。
This means that, for example, the phase difference characteristic when using the dielectric support 3b shown in FIG. 3 is the phase difference characteristic 3 shown in FIG. 4G.
When the retardation characteristic using dielectric support t-3a is smaller than 90° as shown in b, and the retardation characteristic using dielectric support t-3a is slightly larger than <90" as shown in retardation characteristic 3a, one of the three supports of quartz glass 2 shown in FIG. By using dielectric supports 3a at one location and dielectric supports 3b at the remaining two locations, one phase difference characteristic 3a is obtained as shown in FIG.

3b2個の如くになってより90°に近くなることから
明らかである。
It is clear that the angle becomes closer to 90° when there are two pieces of 3b.

このように本実施例では、材質の異なる誘電体サポート
を種々組み合わせて用いることにより、90°位相差を
微調することができ、電気特性を良好にすることができ
る。
As described above, in this embodiment, by using various combinations of dielectric supports made of different materials, the 90° phase difference can be finely adjusted and the electrical characteristics can be improved.

第6図はこの発明の第2の実施例による円偏波発生器を
示す側面断面図であり、第5図は本実施例装置で用いる
誘電体サポートを示す。両図において、3,31,32
.33は誘電体サポートであり、これらはそれぞれ材質
は同じであるが、長さが異なるものである。本実施例装
置では、誘電体サポート3及び32を組み合わせて用い
てしする。
FIG. 6 is a side sectional view showing a circularly polarized wave generator according to a second embodiment of the present invention, and FIG. 5 shows a dielectric support used in the device of this embodiment. In both figures, 3, 31, 32
.. Dielectric supports 33 are made of the same material but have different lengths. In the device of this embodiment, the dielectric supports 3 and 32 are used in combination.

このような構成になる円偏波発生器においても、誘電体
サポートのもつ比誘電率εを変化させることができ、9
0°位相差を微調することができる。
Even in a circularly polarized wave generator having such a configuration, the relative permittivity ε of the dielectric support can be changed, and 9
The 0° phase difference can be finely adjusted.

〔発明の効果〕〔Effect of the invention〕

以上のように、この発明の円偏波発生器によれば、材質
又は長さの異なる誘電体サポートを種々組み合わせて用
いるようにしたので、微調用ネジを不要とでき、90°
位相差の微調を簡単に行うことができ、装置を安価にで
きる効果がある。
As described above, according to the circularly polarized wave generator of the present invention, dielectric supports of different materials or lengths are used in various combinations, so fine adjustment screws are not required, and the 90°
Fine adjustment of the phase difference can be easily performed, and the device can be made inexpensive.

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

第1図及び第2図はこの発明の第1の実施例による円偏
波発生器を示す側面断面図及び正面図、第3図は該実施
例に用いる材質の異なった種々の誘電体サポートを示す
図、第4図は位相差特性を示す図、第6図はこの発明の
第2の実施例による円偏波発生器を示す側面断面図、第
5図は該実施例に用いる長さの異なった種々の誘電体サ
ポートを示す図、第7図及び第8図は従来の円偏波発生
器を示す側面断面図及び正面図である。 図において、1は円形導波管、2は石英ガラス3.3a
、3b、3c、31.32.33は誘電体サポート、4
は金具である。 なお図中同一符号は同−又は相当部分を示す。
1 and 2 are side sectional views and front views showing a circularly polarized wave generator according to a first embodiment of the present invention, and FIG. 3 shows various dielectric supports made of different materials used in the embodiment. 4 is a diagram showing phase difference characteristics, FIG. 6 is a side sectional view showing a circularly polarized wave generator according to a second embodiment of the present invention, and FIG. 5 is a diagram showing the length used in this embodiment. FIGS. 7 and 8 are side sectional and front views of a conventional circularly polarized wave generator, respectively, showing different types of dielectric supports. In the figure, 1 is a circular waveguide, 2 is a quartz glass 3.3a
, 3b, 3c, 31.32.33 are dielectric supports, 4
is a metal fitting. Note that the same reference numerals in the figures indicate the same or equivalent parts.

Claims (1)

【特許請求の範囲】[Claims] (1)円形導波管内に石英ガラスを複数の誘電体サポー
トにより装荷してなる円偏波発生器において、 上記複数の誘電体サポートは、材質又は長さの種々異な
るものからなり、円偏波の発生が可能であることを特徴
とする円偏波発生器。
(1) In a circularly polarized wave generator in which quartz glass is loaded in a circular waveguide with a plurality of dielectric supports, the plurality of dielectric supports are made of various materials or lengths, and the circularly polarized wave A circularly polarized wave generator characterized by being capable of generating.
JP14661987A 1987-06-11 1987-06-11 Circularly polarized wave generator Pending JPS63310202A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP14661987A JPS63310202A (en) 1987-06-11 1987-06-11 Circularly polarized wave generator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP14661987A JPS63310202A (en) 1987-06-11 1987-06-11 Circularly polarized wave generator

Publications (1)

Publication Number Publication Date
JPS63310202A true JPS63310202A (en) 1988-12-19

Family

ID=15411831

Family Applications (1)

Application Number Title Priority Date Filing Date
JP14661987A Pending JPS63310202A (en) 1987-06-11 1987-06-11 Circularly polarized wave generator

Country Status (1)

Country Link
JP (1) JPS63310202A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN108963407A (en) * 2018-08-20 2018-12-07 中国科学院国家空间科学中心 A kind of three dovetail metallic membrane orthomode couplers

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN108963407A (en) * 2018-08-20 2018-12-07 中国科学院国家空间科学中心 A kind of three dovetail metallic membrane orthomode couplers

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