JPS5951761B2 - Linear polarization circular polarization switcher - Google Patents
Linear polarization circular polarization switcherInfo
- Publication number
- JPS5951761B2 JPS5951761B2 JP1032578A JP1032578A JPS5951761B2 JP S5951761 B2 JPS5951761 B2 JP S5951761B2 JP 1032578 A JP1032578 A JP 1032578A JP 1032578 A JP1032578 A JP 1032578A JP S5951761 B2 JPS5951761 B2 JP S5951761B2
- Authority
- JP
- Japan
- Prior art keywords
- ferrimagnetic
- polarization
- circularly polarized
- switcher
- polarized wave
- 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
- H01P—WAVEGUIDES; RESONATORS, LINES, OR OTHER DEVICES OF THE WAVEGUIDE TYPE
- H01P1/00—Auxiliary devices
- H01P1/165—Auxiliary devices for rotating the plane of polarisation
- H01P1/17—Auxiliary devices for rotating the plane of polarisation for producing a continuously rotating polarisation, e.g. circular polarisation
- H01P1/174—Auxiliary devices for rotating the plane of polarisation for producing a continuously rotating polarisation, e.g. circular polarisation using a magnetic element
Description
【発明の詳細な説明】
この発明は、直線偏波と円偏波を電気的に切□換えるマ
イクロ波回路に関筆名ものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a microwave circuit that electrically switches between linearly polarized waves and circularly polarized waves.
最初に、従来から知られているフェリ磁性体を用いた非
可逆円偏波発生器について説明を行ない、次にこの発明
の説明を行なう。First, a conventionally known irreversible circularly polarized wave generator using a ferrimagnetic material will be explained, and then the present invention will be explained.
第1図a、 bは、非可逆円偏波発生器の構造を示す
図で、第1図aは斜視図、第1図すはA−A′断面図で
ある。FIGS. 1a and 1b are diagrams showing the structure of an irreversible circularly polarized wave generator, with FIG. 1a being a perspective view and FIG. 1 being a sectional view taken along line A-A'.
正方形または丸形の所定寸法フェリ磁性体1の両端面を
除く全面をメタライズし、メッキ導波管2を形成する。A plated waveguide 2 is formed by metallizing the entire surface of a square or round ferrimagnetic material 1 of a predetermined size except for both end surfaces.
その後、メッキ導波管2上の四面に、対称的に、互に隣
の磁極の極性が反対になるように、所定寸法の永久磁石
3を配置することにより構成される。Thereafter, permanent magnets 3 of predetermined dimensions are arranged symmetrically on all four sides of the plated waveguide 2 so that the polarities of adjacent magnetic poles are opposite to each other.
次に、非可逆円偏波発生器の動作原理を説明すると、以
下のようになる。Next, the operating principle of the irreversible circularly polarized wave generator will be explained as follows.
第2図は、動作説明をするための図であるが、x −x
’線に平行な電界成分を持つ、疑似TE01波が図示の
ような方向に伝播する場合を考えると、フェリ磁性体1
はマイクロ波に対して正の透磁率μヤを示し、Y−Y′
線に平行な電界成分を持つ電波の場合には、負の透磁率
μ−を示す。FIG. 2 is a diagram for explaining the operation, and x −x
Considering the case where a pseudo TE01 wave with an electric field component parallel to the line propagates in the direction shown, the ferrimagnetic material 1
shows a positive magnetic permeability μya for microwaves, and Y−Y′
Radio waves with electric field components parallel to the line exhibit negative magnetic permeability μ-.
入射する直線偏波は、z−z’線方向に電界成分を持つ
疑似TE01波であるから、電界をx−x’線とY−Y
’線方向成分に分離して考えると、上記のように、フェ
リ磁性体のそれぞれに対して示す透磁率が異なり、伝播
定数が異なることになる。Since the incident linearly polarized wave is a pseudo TE01 wave with an electric field component in the z-z' line direction, the electric field can be divided into the xx' line and the Y-Y line.
'When considered separately into linear components, as mentioned above, the magnetic permeability shown for each ferrimagnetic material is different, and the propagation constant is different.
従って、永久磁石3::の磁界の強さと長さを適当に選
定すると、円偏疲発生器とすることが出来る。Therefore, by appropriately selecting the strength and length of the magnetic field of the permanent magnet 3, a circular fatigue generator can be obtained.
ただし、通常のビス形、誘電体形とは違い、動作は非可
逆である。However, unlike the normal screw type and dielectric type, the operation is irreversible.
以上が、フェリ磁性体を用いた非可逆円偏波発生器の動
作原理であり、これを利用して円偏波直線偏波切換器を
作ろうとするものである。The above is the operating principle of an irreversible circularly polarized wave generator using a ferrimagnetic material, and it is intended to use this to create a circularly polarized wave/linear polarized wave switcher.
この発明は、電気的に円直偏波切換を行なうとするもの
で、以下に詳細な説明を行なう。This invention performs circular polarization switching electrically, and will be described in detail below.
第3図に、この発萌による直線偏波円偏波切換器の一実
施例の構造を示すもので、メッキ導波管2の外側に、図
示のような、フェリ磁性体ヨーク5を装着し、コイノし
6を巻いた構造となっている。FIG. 3 shows the structure of an embodiment of a linearly polarized/circularly polarized wave switching device based on this sprouting, in which a ferrimagnetic yoke 5 as shown is attached to the outside of the plated waveguide 2. , it has a structure in which Koinoshi 6 is wound.
第4図は、動作説明のための図であるが、コイルに流す
パルス電流の方向を切換えると第4図aあるいは第4図
すに示す状態となる。FIG. 4 is a diagram for explaining the operation, and when the direction of the pulse current flowing through the coil is changed, the state shown in FIG. 4a or FIG. 4S is obtained.
今、図示のような電波伝播方向に、直線偏波が入射した
場合、フェリ磁性体ヨーク5の長さを適当に選定すると
、第4図aの場合右回り、第4図すの場合左回りの円偏
波が発生する。Now, when a linearly polarized wave is incident in the radio wave propagation direction as shown in the figure, if the length of the ferrimagnetic yoke 5 is appropriately selected, it will rotate clockwise in the case of Figure 4 a, and counterclockwise in the case of Figure 4 S. circularly polarized waves are generated.
またフエリ磁性体1内の磁化4を消去するようなパルス
電流を流すと、フェリ磁性体は消磁されて、誘電体的動
作をすることになり、入射直線偏波は、偏波面は回転せ
ず、そのま・直線偏波の出力となる。Furthermore, when a pulse current that erases the magnetization 4 in the ferrimagnetic material 1 is applied, the ferrimagnetic material is demagnetized and behaves like a dielectric material, and the plane of polarization of the incident linearly polarized wave does not rotate. , the output is straight and linearly polarized.
以上のように、コイルに流すパルス電流に応じて、右旋
、左旋の円偏波および直線偏波の切換を行なうことが出
来る。As described above, it is possible to switch between right-handed circularly polarized waves, left-handed circularly polarized waves, and linearly polarized waves depending on the pulsed current flowing through the coil.
第5図は、この発明による直線偏波円偏波切換器の他の
実施例の構造を示すもので、フェリ磁性体ヨーク5をよ
り対称的に配置したものである。FIG. 5 shows the structure of another embodiment of the linear polarization/circular polarization switching device according to the present invention, in which the ferrimagnetic yoke 5 is arranged more symmetrically.
以上のように、この発明による直線偏波円偏波切換器で
は、コイルに流すパルス電流で、円偏波(右旋、左旋)
直線偏波の切換を行なうことが出来る効果を有する。As described above, in the linear polarization/circular polarization switching device according to the present invention, circular polarization (right-handed rotation, left-handed rotation) is generated by pulsed current flowing through the coil.
This has the effect of being able to switch linearly polarized waves.
第1図は従来のフェリ磁性体を用いた非可逆円偏波発生
器の構造を示す図、第2図は非可逆円偏波発生器の動作
説明のための図、第3図はこの発明による直線偏波円偏
波切換器の一実施例の構造を示す図、第4図は直線偏波
円偏波切換器の動作説明のための図、第5図はこの発明
による直線偏波円偏波切換器の他の実施例の構造を示す
図である。
図中、1はフェリ磁性体、2はメッキ導波管、3は永久
磁石、4は磁化、5はフェリ磁性体ヨーク、6はコイル
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
て示しである。Fig. 1 is a diagram showing the structure of a conventional irreversible circularly polarized wave generator using a ferrimagnetic material, Fig. 2 is a diagram for explaining the operation of the irreversible circularly polarized wave generator, and Fig. 3 is a diagram of the present invention. Fig. 4 is a diagram for explaining the operation of the linear polarization circular polarization switch according to the present invention, and Fig. 5 is a diagram showing the structure of an embodiment of the linear polarization circular polarization switch according to the present invention. It is a figure which shows the structure of another Example of a polarization switcher. In the figure, 1 is a ferrimagnetic material, 2 is a plated waveguide, 3 is a permanent magnet, 4 is magnetization, 5 is a ferrimagnetic yoke, and 6 is a coil. In the drawings, the same or corresponding parts are designated by the same reference numerals.
Claims (1)
全面をメタライズしてメッキ導波管を形成し、コイルを
巻いた適当な寸法のフェリ磁性体ヨークをメッキ導波管
の外側に配置し、フェリ磁性体内の電波伝播垂直方向面
内に四極磁石磁化分布が残留するような構成にしたこと
を特徴とする直線偏波円偏波切換器。 □ □[Claims] 1. A plated waveguide is formed by metallizing the entire surface of a square or round ferrimagnetic rod except for both end surfaces, and a ferrimagnetic yoke of an appropriate size around which a coil is wound is attached to the plated waveguide. 1. A linearly polarized/circularly polarized wave switching device, characterized in that it is arranged outside of the ferrimagnetic body and configured so that the magnetization distribution of the quadrupole magnet remains in the plane in the direction perpendicular to the propagation of radio waves in the ferrimagnetic body. □ □
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP1032578A JPS5951761B2 (en) | 1978-02-01 | 1978-02-01 | Linear polarization circular polarization switcher |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP1032578A JPS5951761B2 (en) | 1978-02-01 | 1978-02-01 | Linear polarization circular polarization switcher |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS54103653A JPS54103653A (en) | 1979-08-15 |
JPS5951761B2 true JPS5951761B2 (en) | 1984-12-15 |
Family
ID=11747057
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP1032578A Expired JPS5951761B2 (en) | 1978-02-01 | 1978-02-01 | Linear polarization circular polarization switcher |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS5951761B2 (en) |
Families Citing this family (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP0185895A3 (en) | 1980-11-29 | 1986-08-13 | Nissha Printing Co., Ltd. | Apparatus for coloring an article by transfer printing |
-
1978
- 1978-02-01 JP JP1032578A patent/JPS5951761B2/en not_active Expired
Also Published As
Publication number | Publication date |
---|---|
JPS54103653A (en) | 1979-08-15 |
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