JPS633202Y2 - - Google Patents
Info
- Publication number
- JPS633202Y2 JPS633202Y2 JP13238982U JP13238982U JPS633202Y2 JP S633202 Y2 JPS633202 Y2 JP S633202Y2 JP 13238982 U JP13238982 U JP 13238982U JP 13238982 U JP13238982 U JP 13238982U JP S633202 Y2 JPS633202 Y2 JP S633202Y2
- Authority
- JP
- Japan
- Prior art keywords
- waveguide
- ferrimagnetic
- ferrimagnetic material
- latching circulator
- view
- 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
- 239000002902 ferrimagnetic material Substances 0.000 description 20
- 239000004020 conductor Substances 0.000 description 13
- 230000005284 excitation Effects 0.000 description 13
- 239000003989 dielectric material Substances 0.000 description 10
- 230000005293 ferrimagnetic effect Effects 0.000 description 8
- 230000008878 coupling Effects 0.000 description 6
- 238000010168 coupling process Methods 0.000 description 6
- 238000005859 coupling reaction Methods 0.000 description 6
- 230000005484 gravity Effects 0.000 description 3
- 230000006866 deterioration Effects 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000000605 extraction Methods 0.000 description 1
- 230000005308 ferrimagnetism Effects 0.000 description 1
- 238000009434 installation Methods 0.000 description 1
- 230000005291 magnetic effect Effects 0.000 description 1
- 239000000696 magnetic material Substances 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 230000035515 penetration Effects 0.000 description 1
Landscapes
- Non-Reversible Transmitting Devices (AREA)
Description
【考案の詳細な説明】
本考案はラツチング・サーキユレータに関し、
特に回路分岐部にフエリ磁性体を配置して構成さ
れる導波管内磁路形ラツチング・サーキユレータ
において、フエリ磁性体励磁用導線の引き出し側
のフエリ磁性体側面部に誘電体材料を設置するこ
とを特徴とするラツチング・サーキユレータに関
する。[Detailed description of the invention] This invention relates to a latching circulator.
In particular, in a waveguide-internal magnetic path type latching circulator that is constructed by arranging a ferrimagnetic material at a circuit branch, it is recommended to install a dielectric material on the side surface of the ferrimagnetic material on the extraction side of the ferrimagnetic material excitation conductor. This article relates to a characteristic latching circulator.
従来、導波管回路分岐部に貫通孔を有するフエ
リ磁性体を配置し、前記フエリ磁性体材料内に該
フエリ磁性体励磁用導線を通して構成される導波
管形ラツチング・サーキユレータが、マイクロ波
周波数帯や準ミリ波周波数帯における回路切替素
子として広く使用されている。第1図に従来の導
波管形ラツチング・サーキユレータの一例を示
す。第1図aはその平面図、第1図bは断面図、
第1図cはフエリ磁性体の斜視図である。図にお
いて、1は導波管路、2はトランスフオーマ、3
はフエリ磁性体、4はフエリ磁性体励磁用導線、
5は導波管の管壁に設けられた導波管貫通孔、6
はフエリ磁性体に設けられたフエリ磁性体貫通
孔、7はフエリ磁性体の重心(すなわちトランス
フオーマの重心)、8は励磁導線の結び口を示す。
この様な従来の導波管形ラツチング・サーキユレ
ータにおいては、フエリ磁性体貫通孔6を通して
フエリ磁性体3に巻かれたフエリ磁性体励磁用導
線4は、フエリ磁性体の側面部で結び合わされ、
導波管H面方向に平行に張られ、導波管E面に垂
直な導波管貫通孔5を通つて導波管外部に引き出
されている。しかし、導線引出し部が該導線を中
心導体として同軸線路を構成する為、このような
導線の引き出し方による場合には、導波管内の電
磁波との結合により電磁波の導波管外部への漏洩
が生じ易く、また結合の仕方が一様でないのでラ
ツチング・サーキユレータとして広帯域特性が取
得しにくいという欠点がある。 Conventionally, a waveguide type latching circulator is constructed by arranging a ferrimagnetic material having a through hole in a waveguide circuit branch part and passing a conductive wire for excitation of the ferrimagnetic material into the ferrimagnetic material. It is widely used as a circuit switching element in the band and sub-millimeter wave frequency bands. FIG. 1 shows an example of a conventional waveguide type latching circulator. Figure 1a is a plan view thereof, Figure 1b is a sectional view,
FIG. 1c is a perspective view of the ferrimagnetic material. In the figure, 1 is a waveguide, 2 is a transformer, and 3 is a waveguide.
is a ferrimagnetic material, 4 is a conductive wire for exciting the ferrimagnetic material,
5 is a waveguide through hole provided in the wall of the waveguide; 6
7 shows the ferrimagnetic material through-hole provided in the ferrimagnetic material, 7 shows the center of gravity of the ferrimagnetic material (that is, the center of gravity of the transformer), and 8 shows the knot of the excitation conductor.
In such a conventional waveguide type latching circulator, the ferrimagnetic excitation wires 4 are wound around the ferrimagnetic body 3 through the ferrimagnetic body through-hole 6 and tied together at the side surface of the ferrimagnetic body.
It is stretched parallel to the waveguide H plane direction and is drawn out to the outside of the waveguide through a waveguide through hole 5 perpendicular to the waveguide E plane. However, since the conductor lead-out section forms a coaxial line with the conductor as the center conductor, when the conductor is drawn out in this way, the electromagnetic waves may leak to the outside of the waveguide due to coupling with the electromagnetic waves inside the waveguide. This problem occurs easily, and since the method of coupling is not uniform, it is difficult to obtain broadband characteristics as a latching circulator.
本考案の目的は上記の欠点を除去し、励磁導線
引き出し側のフエリ磁性体側面部に誘電体材料を
設置することにより、該励磁用導線と電磁波との
結合を弱くするとともに、広帯域周波数特性を有
するラツチング・サーキユレータを提供すること
にある。 The purpose of the present invention is to eliminate the above-mentioned drawbacks and to weaken the coupling between the excitation conductor and electromagnetic waves by installing a dielectric material on the side surface of the ferrimagnetic material on the excitation conductor lead-out side, and to improve broadband frequency characteristics. An object of the present invention is to provide a latching circulator having the following features.
以下、本考案について図面を参照して詳細に説
明する。 Hereinafter, the present invention will be described in detail with reference to the drawings.
第2図は、本考案の一実施例の導波管形ラツチ
ング・サーキユレータを示す。第2図aはその平
面図、第2図bはその断面図、第2図cはフエリ
磁性体の斜視図である。本実施例の場合、第1図
に示される従来側の場合との相異点は、第2図c
に示されるように誘電体材料9が付与されている
点にある。 FIG. 2 shows a waveguide type latching circulator according to an embodiment of the present invention. FIG. 2a is a plan view thereof, FIG. 2b is a sectional view thereof, and FIG. 2c is a perspective view of the ferrimagnetic material. In the case of this embodiment, the difference from the conventional case shown in FIG. 1 is as shown in FIG.
A dielectric material 9 is applied as shown in FIG.
フエリ磁性体励磁用導線4は、磁性体貫通孔6
の中央部に位置する結び口8において結ばれ、導
波管H面方向に平行に張られ、導波管E面に垂直
な導波管貫通孔5を通つて導波管外部に引き出さ
れている。第2図cにおいては励磁導線の結び口
8付近に誘電体材料を設置したフエリ磁性体を示
す。本実施例においては、励磁導線の結び口8の
付近に誘電体材料9を設置することにより、フエ
リ磁性体励磁用導線4と管内電磁波との結合状態
を変化させ、誘電体材料9の誘電率、大きさ、設
置位置を適当に選択することにより、該導線と管
内電磁波との結合を弱くすることが可能となる。
この結果、従来前記結合によつて生じていたラツ
チング・サーキユレータにおける電気特性の劣
下、即ち不要共振、管内電磁波漏洩等を軽減する
ことができ、従つて周波数特性を広帯域化するこ
とも可能となる。特に高周波数領域で生じやすい
ラツチング・サーキユレータの構成要素における
物理的寸法のばらつきによつて生じる電気特性の
ばらつきも、誘電体材料9がインピーダンス調整
要素として動作するため、前記物理的寸法のばら
つきによる周波数特性に対する影響をも軽減し
て、均一で良好な特性を実現することもできる。 The conductive wire 4 for excitation of the ferrimagnetic material is inserted into the magnetic material through hole 6
are tied at a knot 8 located in the center of the waveguide, stretched parallel to the waveguide H surface direction, and pulled out to the outside of the waveguide through the waveguide through hole 5 perpendicular to the waveguide E surface. There is. FIG. 2c shows a ferrimagnetic material in which a dielectric material is placed near the connection port 8 of the excitation conductor. In this embodiment, by installing a dielectric material 9 near the connection port 8 of the excitation conductor, the coupling state between the ferrimagnetic excitation conductor 4 and the electromagnetic waves in the tube is changed, and the dielectric constant of the dielectric material 9 is By appropriately selecting the size and installation position, it is possible to weaken the coupling between the conducting wire and the electromagnetic waves inside the pipe.
As a result, it is possible to reduce the deterioration of the electrical characteristics of the latching circulator that conventionally occurs due to the above-mentioned coupling, such as unnecessary resonance and leakage of electromagnetic waves in the pipe, and therefore it is also possible to widen the frequency characteristics. . Since the dielectric material 9 acts as an impedance adjustment element, variations in electrical characteristics caused by variations in physical dimensions in the components of the latching circulator, which tend to occur particularly in high frequency regions, can be avoided at high frequencies due to variations in physical dimensions. It is also possible to reduce the influence on the characteristics and achieve uniform and good characteristics.
以上詳細に説明したように、本考案はフエリ磁
性体励磁用導線の結び口付近に誘電体材料を設置
することにより、フエリ磁性体励磁用導線が電磁
波と結合するために生じる、ラツチング・サーキ
ユレータの動作周波数帯域内における不要共振お
よび高周波漏洩等を軽減することができ、また前
記誘電体材料がインピーダンス調整機能をも有す
るため、ラツチング・サーキユレータとしての均
一で良好な特性を確保できるという効果がある。 As explained in detail above, the present invention installs a dielectric material near the knot of the ferrimagnetic excitation conductor, thereby reducing the latching circulator that occurs when the ferrimagnetic excitation conductor couples with electromagnetic waves. Unnecessary resonance and high frequency leakage within the operating frequency band can be reduced, and since the dielectric material also has an impedance adjustment function, it has the effect of ensuring uniform and good characteristics as a latching circulator.
第1図aは従来のラツチング・サーキユレータ
の断面図、第1図bは第1図aのA−A′線に沿
つた縦断面図、第1図cは従来のラツチング・サ
ーキユレータで使用されているフエリ磁性体の斜
視図、第2図aは本考案によるラツチング・サー
キユレータの平面図、第2図bは第2図aのA−
A′線に沿つた縦断面図、第2図cは本考案のラ
ツチング・サーキユレータで使用されるフエリ磁
性体の斜視図である。図において、1……導波管
路、2……トランスフオーマ、3……フエリ磁性
体、4……フエリ磁性体励磁用導線、5……導波
管貫通孔、6……フエリ磁性体貫通孔、7……フ
エリ磁性性の重心、8……導線の結び口、9……
誘電体材料。
Fig. 1a is a sectional view of a conventional latching circulator, Fig. 1b is a longitudinal sectional view taken along line A-A' in Fig. 1a, and Fig. 1c is a sectional view of a conventional latching circulator. FIG. 2a is a plan view of the latching circulator according to the present invention, and FIG. 2b is a perspective view of the ferrimagnetic material shown in FIG. 2a.
FIG. 2c is a perspective view of the ferrimagnetic material used in the latching circulator of the present invention. In the figure, 1... waveguide path, 2... transformer, 3... ferrimagnetic material, 4... ferrimagnetic excitation wire, 5... waveguide through hole, 6... ferrimagnetic material penetration Hole, 7... Center of gravity of ferrimagnetism, 8... Connection for conducting wire, 9...
dielectric material.
Claims (1)
に設けたラツチング・サーキユレータにおいて、
フエリ磁性体励磁用導線の引き出し側のフエリ磁
性体側面部に誘電体材料を設置することを特徴と
するラツチング・サーキユレータ。 In a latching circulator in which a ferrimagnetic material with an excitation conductor is provided at a waveguide branch,
A latching circulator characterized in that a dielectric material is installed on the side surface of the ferrimagnetic material on the extraction side of the ferrimagnetic material excitation conductor.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP13238982U JPS5936604U (en) | 1982-09-01 | 1982-09-01 | Latching circulator |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP13238982U JPS5936604U (en) | 1982-09-01 | 1982-09-01 | Latching circulator |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5936604U JPS5936604U (en) | 1984-03-07 |
| JPS633202Y2 true JPS633202Y2 (en) | 1988-01-27 |
Family
ID=30298974
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP13238982U Granted JPS5936604U (en) | 1982-09-01 | 1982-09-01 | Latching circulator |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5936604U (en) |
-
1982
- 1982-09-01 JP JP13238982U patent/JPS5936604U/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5936604U (en) | 1984-03-07 |
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