JPS5943005B2 - circularly polarized antenna - Google Patents
circularly polarized antennaInfo
- Publication number
- JPS5943005B2 JPS5943005B2 JP5954078A JP5954078A JPS5943005B2 JP S5943005 B2 JPS5943005 B2 JP S5943005B2 JP 5954078 A JP5954078 A JP 5954078A JP 5954078 A JP5954078 A JP 5954078A JP S5943005 B2 JPS5943005 B2 JP S5943005B2
- Authority
- JP
- Japan
- Prior art keywords
- circularly polarized
- polarized wave
- polarization
- wave generator
- electromagnetic
- 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
Links
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01Q—ANTENNAS, i.e. RADIO AERIALS
- H01Q13/00—Waveguide horns or mouths; Slot antennas; Leaky-waveguide antennas; Equivalent structures causing radiation along the transmission path of a guided wave
- H01Q13/02—Waveguide horns
Landscapes
- Waveguide Switches, Polarizers, And Phase Shifters (AREA)
- Waveguide Aerials (AREA)
Description
【発明の詳細な説明】
この発明は円偏波発生器を有する円偏波アンテナに係り
、特に楕円偏波率の劣化を防止する回路の改良に関する
ものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a circularly polarized antenna having a circularly polarized wave generator, and particularly to an improvement in a circuit for preventing deterioration of elliptical polarization.
第1図は従来の円偏波アンテナの構成の一例を示す略断
面図で、図において1は円錐ホーン、2は円偏波発生器
、3は円形導波管、4は円形導波管3の中央に挿入され
ている電波吸収体板、5は矩形−円形導波管変換器であ
る。FIG. 1 is a schematic cross-sectional view showing an example of the configuration of a conventional circularly polarized antenna. In the figure, 1 is a conical horn, 2 is a circularly polarized wave generator, 3 is a circular waveguide, and 4 is a circular waveguide 3. The radio wave absorber plate 5 inserted in the center is a rectangular-circular waveguide converter.
いま矩形−円形導波管変換器5に入力される電磁波はそ
の電界が第1図の矢印6に示す方向にあるような偏波面
を有する直線偏波の電磁波であるとすると、この電界は
電波吸収体板4に直角な電界であるため、はとんど損失
なく円偏波発生器2に導かれ、たとえば右旋円偏波とな
り円錐ホーン1から放射される。Assuming that the electromagnetic wave input to the rectangular-circular waveguide converter 5 is a linearly polarized electromagnetic wave whose electric field has a plane of polarization in the direction shown by the arrow 6 in FIG. 1, this electric field is a radio wave. Since the electric field is perpendicular to the absorber plate 4, it is guided to the circularly polarized wave generator 2 with almost no loss, and becomes, for example, a right-handed circularly polarized wave, which is radiated from the conical horn 1.
ところで一般には円偏波発生器2と円錐ホーン1との接
続点および円錐ホーン1の開口端において電磁波は反射
されこの反射された電磁波は入射電磁波とは逆に円偏波
発生器2、円形導波管3、矩形−円形導波青変管器5の
方向に進行する。By the way, in general, electromagnetic waves are reflected at the connection point between the circularly polarized wave generator 2 and the conical horn 1 and at the open end of the conical horn 1, and the reflected electromagnetic waves are transmitted to the circularly polarized wave generator 2 and the circular guide, contrary to the incident electromagnetic wave. The wave tube 3 advances in the direction of the rectangular-circular waveguide blue tube device 5.
そしてこの反射波は円偏波発生器2によって矢印6で示
す入射波の偏波面と直角な偏波面を有する直線偏波(交
さ偏波成分という)となり円形導波管3に戻ってくるの
で電波吸収体板4に有効に吸収される。This reflected wave then returns to the circular waveguide 3 as a linearly polarized wave (referred to as a cross-polarized wave component) having a polarization plane perpendicular to the polarization plane of the incident wave as shown by the arrow 6 by the circularly polarized wave generator 2. It is effectively absorbed by the radio wave absorber plate 4.
もし電波吸収体板4がないとすればこの交さ偏波成分は
矩形−円形導波管変換器5で再び反射され円形導体管3
を通過して円偏波発生器2によって主円偏波の旋回力向
と逆方向に旋回する(上述の実施例では左旋回)円偏波
となって円錐ホーン1から放射され楕円偏波率を劣化す
る。If there is no radio wave absorber plate 4, this cross-polarized wave component will be reflected again by the rectangular-circular waveguide converter 5 and the circular conductor tube 3.
The circularly polarized wave is turned by the circularly polarized wave generator 2 in the direction opposite to the direction of rotation of the main circularly polarized wave (left rotation in the above embodiment), and is radiated from the conical horn 1 with an elliptical polarization rate. deteriorate.
円偏波発生器2の出力点の反射係数、すなわち円錐ホー
ン1の入力点から見た反射係数をFlとし、円偏波発生
器2の入力方向の反射係数をF2とすれば楕円偏波率の
劣化△ARは
で表される。If the reflection coefficient at the output point of the circularly polarized wave generator 2, that is, the reflection coefficient seen from the input point of the conical horn 1, is Fl, and the reflection coefficient in the input direction of the circularly polarized wave generator 2 is F2, then the elliptical polarization coefficient is obtained. The deterioration ΔAR of is expressed as .
第1図のような構成ではたとえば7’1=0.1(定在
波率VSWRにしてVSWR=1.22)程度であり、
かつ交さ偏波成分に対し矩形−円形導波管変換器5の回
路はカットオフになり完全反射が行われるのでF2−1
とすれば、式(1)から△AR=0.87 (d、b
)となる。In the configuration shown in Fig. 1, for example, 7'1 = 0.1 (standing wave rate VSWR = 1.22),
In addition, the circuit of the rectangular-circular waveguide converter 5 is cut off for crossed polarization components and complete reflection occurs, so F2-1
Then, from equation (1), △AR=0.87 (d, b
).
最近の高性能アンテナでは△ARが0.4db以下であ
ることを要求されるので楕円偏波率の劣化を防止する回
路である電波吸収体板4は不可欠なものとなる。Since recent high-performance antennas are required to have a ΔAR of 0.4 db or less, the radio wave absorber plate 4, which is a circuit that prevents deterioration of the elliptical polarization factor, is essential.
電波吸収体板4としては通常o、ix〜2履程度の厚さ
のマイカ等の誘電体基板に抵抗膜を被着した吸収体板を
用いているので、主偏波成分に対しても挿入損失を増加
させ、また反射波はすべて吸収するため大電力で使用す
る場合には吸収体板が焼ける等の不都合があり、また衛
星搭載用アンテナに応用する場合には打上時の衝撃、振
動に耐える吸収体板の選定及びその取付力法が困難とな
り信頼度を低下させる原因となっていた。As the radio wave absorber plate 4, an absorber plate with a resistive film coated on a dielectric substrate such as mica with a thickness of about 0, ix to 2 mm is usually used, so that it is inserted even for the main polarized wave component. In addition, since all reflected waves are absorbed, there are inconveniences such as burning of the absorber plate when used with high power, and when applied to satellite antennas, there is a risk of shock and vibration during launch. It has been difficult to select a durable absorber plate and how to attach it, resulting in a decrease in reliability.
この発明は従来のアンテナにおける上述の欠点を除去す
ることを目的とし、この目的を達するため電波吸収体を
装荷した偏分波器を用いたものであって、以下図面につ
いてこの発明の一実施例を説明する。The purpose of this invention is to eliminate the above-mentioned drawbacks of conventional antennas, and to achieve this purpose, a polarization splitter loaded with a radio wave absorber is used. Explain.
第2図はこの発明の一実施例を示す略断面図であり、第
1図と同一符号は同−又は相当部分を示し同一動作をす
る。FIG. 2 is a schematic sectional view showing an embodiment of the present invention, and the same reference numerals as in FIG. 1 indicate the same or corresponding parts and perform the same operations.
7は7at7b*7cで構成される偏分波器であり、7
aはその主導波管部、7bは主導波管部Ia内に設けら
れ矢印6に示す偏波面に対し直角な偏波面を有し円偏波
発生器2の方向から主導波管部7aに向って進行する電
磁波を反射する短絡板、7cは偏分波器7の分岐導波管
部、8は分岐導波管部7cの蓋、9は電波吸収体である
。7 is a polarization splitter composed of 7at7b*7c;
7b is provided in the main waveguide section Ia, has a polarization plane perpendicular to the polarization plane shown by arrow 6, and is directed from the direction of the circularly polarized wave generator 2 toward the main waveguide section 7a. 7c is a branching waveguide portion of the polarization splitter 7, 8 is a lid of the branching waveguide portion 7c, and 9 is a radio wave absorber.
第1図について説明したと同様に反射されて円錐ホーン
1から円錐波発生器2に入力される電磁波は、円偏波発
生器2から偏分波器7に入力される点では交さ偏波成分
となっているが、この交さ偏波成分は主導波管7aの中
央の金属製短絡板7bにより反射されて分岐導体管7c
に導かね、こ5で電波吸収体9に吸収される。The electromagnetic waves that are reflected and input from the conical horn 1 to the conical wave generator 2 in the same manner as explained with reference to FIG. However, this cross-polarized wave component is reflected by the metal shorting plate 7b at the center of the main waveguide 7a and is transmitted to the branch conductor tube 7c.
It is absorbed by the radio wave absorber 9.
以上説明したとおり、この発明によれば主偏波成分の通
過する導波管中には吸収体を設ける必要がないので、挿
入損失も減少し、また電波吸収体にも大きなブロックを
用いることができるため大電力での使用も可能となる。As explained above, according to the present invention, there is no need to provide an absorber in the waveguide through which the main polarized wave component passes, so insertion loss is reduced, and a large block can also be used for the radio wave absorber. This makes it possible to use large amounts of power.
また衛星搭載用としても、電波吸収体として磁性体粉を
樹脂で固めたフ七ツク状のものを用いればネジと接着剤
とにより取付ける等の手段が用いられるので、充分な強
度を有する信頼性の高い回路構成が可能となる。Also, when used onboard a satellite, if a glue-like material made of magnetic powder hardened with resin is used as a radio wave absorber, it can be attached with screws and adhesive, so it has sufficient strength and reliability. This enables a circuit configuration with high performance.
以上述べたようにこの発明の円偏波アンテナは特に人工
衛星搭載用アンテナとして極めて優れた性能を有してい
る。As described above, the circularly polarized antenna of the present invention has extremely excellent performance, especially as an antenna mounted on an artificial satellite.
なお第2図に示す実施例では円偏波発生器2の出力を直
接円錐ホーン1に接続する場合について説明したが、円
偏波発生器2と電磁ホーンとの間に任意の導波管装置が
介在する場合、円錐ホーン1以外の形の電磁ホーンに接
続する場合、又はその電磁ホーンを一次放射器としてこ
の電磁ホーンからの電波を集束反射する反射鏡を有する
アンテナ系から円偏波を放射する場合にもこの発明を用
い得ることは申すまでもない。In the embodiment shown in FIG. 2, a case has been described in which the output of the circularly polarized wave generator 2 is directly connected to the conical horn 1, but an arbitrary waveguide device may be connected between the circularly polarized wave generator 2 and the electromagnetic horn. radiates circularly polarized waves from an antenna system that uses the electromagnetic horn as a primary radiator and has a reflector that focuses and reflects radio waves from the electromagnetic horn. Needless to say, this invention can also be used in such cases.
さらに円偏波発生器2と円錐ホーン1との間にたとえば
高次モード発生器等を挿入したデュアルモードホーンア
ンテナの場合にも同様の効果があることは明らかである
。Furthermore, it is clear that similar effects can be obtained in the case of a dual mode horn antenna in which, for example, a higher-order mode generator or the like is inserted between the circularly polarized wave generator 2 and the conical horn 1.
また以上の説明では第2図に示す円偏波アンテナを電波
の送信に用いる場合について述べたが、電波の受信に対
しても同様に用い得ることは申すまでもない。Further, in the above description, the case where the circularly polarized antenna shown in FIG. 2 is used for transmitting radio waves has been described, but it goes without saying that it can be used similarly for receiving radio waves.
第1図は従来の円偏波アンテナの構成の一例を示す略断
面図、第2図はこの発明の一実施例を示す略断面図であ
る。
図において1は円錐ホーン、2は円偏波発生器、5は矩
形−円形導波管変換器、7は偏分波器、7aは偏分波器
7の主導波管部、7bは短絡板、7cは偏分波器7の分
岐導波管部、8は蓋、9は電波吸収体である。
なお各図中同一符号は同−又は相当部分を示すものとす
る。FIG. 1 is a schematic sectional view showing an example of the configuration of a conventional circularly polarized antenna, and FIG. 2 is a schematic sectional view showing an embodiment of the present invention. In the figure, 1 is a conical horn, 2 is a circularly polarized wave generator, 5 is a rectangular-circular waveguide converter, 7 is a polarization splitter, 7a is the main waveguide part of the polarization splitter 7, and 7b is a short circuit plate. , 7c is a branch waveguide portion of the polarization splitter 7, 8 is a lid, and 9 is a radio wave absorber. Note that the same reference numerals in each figure indicate the same or corresponding parts.
Claims (1)
所定の旋回力向を有する円偏波に変換する円偏波発生器
、この円偏波発生器の出力側に接続される電磁ホーン、
上記円偏波発生器の入力端に接続される偏分波器を有し
、上記偏分波器は上記所定の偏波面に直角な偏波面を有
する直線偏波の電磁波を反射する短絡板が設けられた主
導波管部と、上記短絡板によって反射された電磁波を吸
収する電波吸収体が設けられた分岐導波管部とを有する
ことを特徴とする円偏波アンテナ。1. A circularly polarized wave generator that inputs a linearly polarized electromagnetic wave having a predetermined plane of polarization and converts it into a circularly polarized wave having a predetermined turning force direction, and an electromagnetic horn connected to the output side of this circularly polarized wave generator. ,
The polarization splitter is connected to the input end of the circularly polarized wave generator, and the polarization splitter includes a short circuit plate that reflects linearly polarized electromagnetic waves having a polarization plane perpendicular to the predetermined polarization plane. What is claimed is: 1. A circularly polarized wave antenna comprising: a main waveguide section; and a branch waveguide section, wherein a branch waveguide section is provided with a radio wave absorber that absorbs electromagnetic waves reflected by the short circuit plate.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP5954078A JPS5943005B2 (en) | 1978-05-19 | 1978-05-19 | circularly polarized antenna |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP5954078A JPS5943005B2 (en) | 1978-05-19 | 1978-05-19 | circularly polarized antenna |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS54150950A JPS54150950A (en) | 1979-11-27 |
| JPS5943005B2 true JPS5943005B2 (en) | 1984-10-19 |
Family
ID=13116189
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP5954078A Expired JPS5943005B2 (en) | 1978-05-19 | 1978-05-19 | circularly polarized antenna |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5943005B2 (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US4797681A (en) * | 1986-06-05 | 1989-01-10 | Hughes Aircraft Company | Dual-mode circular-polarization horn |
| JPS6333206U (en) * | 1986-08-21 | 1988-03-03 |
-
1978
- 1978-05-19 JP JP5954078A patent/JPS5943005B2/en not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS54150950A (en) | 1979-11-27 |
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