JPH01311601A - Switch for plane of polarization - Google Patents

Switch for plane of polarization

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Publication number
JPH01311601A
JPH01311601A JP14201688A JP14201688A JPH01311601A JP H01311601 A JPH01311601 A JP H01311601A JP 14201688 A JP14201688 A JP 14201688A JP 14201688 A JP14201688 A JP 14201688A JP H01311601 A JPH01311601 A JP H01311601A
Authority
JP
Japan
Prior art keywords
waveguide
magnetic core
current
polarization
coil
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
JP14201688A
Other languages
Japanese (ja)
Inventor
Yasuo Suzuki
靖生 鈴木
Kazuaki Endo
一明 遠藤
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.)
FDK Corp
Original Assignee
FDK 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 FDK Corp filed Critical FDK Corp
Priority to JP14201688A priority Critical patent/JPH01311601A/en
Publication of JPH01311601A publication Critical patent/JPH01311601A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To reduce power consumption and the generation of heat by providing a magnetic core part outside a waveguide, forming closed loop structure in which a ferrite bar part positioning inside the waveguide is connected continuously to the magnetic core part, and winding a core across the waveguide. CONSTITUTION:The ferrite bar part 14 is arranged in the waveguide 12 with high conductivity such as aluminum, etc., and the coil 20 is wound in the periphery of the waveguide 12 on which the ferrite bar part 14 is positioned. And the magnetic core part 22 is provided outside the waveguide 12, and the closed loop structure is constituted by connecting the ferrite bar part 14 to the magnetic core part 22 continuously. Therefore, since a magnetic hysteresis curve can be formed in upright shape without generating a diamagnetic field, it is not required to supply a current only by supplying a coil current at the time of switching a plane of polarization, and even when the current is required, only a few amount of current is required. In such a way, it is possible to realize power saving, and to reduce the generation of the heat.

Description

【発明の詳細な説明】[Detailed description of the invention] 【産業上の利用分野】[Industrial application field]

本発明は、フェライトのファラデー効果を利用した偏波
面切換器に関し、更に詳しくは、導波管内部に位置する
フェライト棒部分と外側の磁心部とによって閉ループが
形成され、それにコイルを巻装した偏波面切換器に関す
るものである。 [従来の技術] 偏波面切換器は、直yI偏波で進行する電磁波の偏波面
をフェライトのファラデー効果を利用して回転させるv
i置である。この種の装置は、例えば衛星放送受信シス
テムの一部としてパラボラアンテナで集めた受信波(各
チャンネル毎に偏波面が90度傾いている)のうち、所
望のチャンネルの受信波のみを通過させるため等に用い
られている。 従来の偏波面切)^器は、導波管内にフェライト棒を挿
入し、その外側にコイルを−tI装した構造をなし、コ
イルに一定の電流を流し続けることによってフェライト
棒に所定の磁界を印加し、進行する電磁波の偏波面を回
転させている。偏波面の切り換えは、逆・向きの電流を
供給し続けることによって行う。 〔発明が解決しようとする課題] 従来の装置は、上記のようにフェライト棒の外側にコイ
ルを巻き付けた構造であるから開磁路構成であり、その
ためフェライト棒の内部に反磁界が発生する。この反磁
界によって内部の磁界が減少するから、使用中かなり大
きなコイル電流を常時供給してフェライト棒に印加され
る磁界を所定の値に保ち続ける必要がある。 これらの理由で従来の装置は省電力化し難く、発熱も大
きくなる欠点があった。 本発明の目的は、上記のような従来技術の欠点を解消し
、消費電力が少な(発熱の問題も生じないようなファラ
デー効果を利用した偏波面切換器を提供することにある
。 〔課題を解決するための手段] 上記の目的を達成できる本発明は、導波管内に配置した
フェライト棒に磁界を印加し、そのファラデー効果を利
用して進行してくる電磁波の偏波面を回転させる偏波面
切換器において、導波管の外側に磁心部を設け、導波管
内部に位置するフェライト棒部分と前記磁心部とが連続
して閉ループ構造をなし、それにコイルを巻装した偏波
面切換器である。 ここで導波管の外側に位置する磁心部は例えばコの字型
形状とし、導波管内のフェライト棒部分の両端側面と連
続するような構成とする。 コの字型形状の磁心部とフェライト棒部分とはそれぞれ
別個の部材とし接着剤等により結合した構造でもよいし
、両者を一体成形し焼結した構造でもよい、別個の部材
で組み合わせる場合には、それぞれの1sin率μが同
程度となるような材料を選択する。フェライト棒部分と
してはJlt抗が高(マイクロ波用に適しているリチウ
ム系フェライト等が好ましい。
The present invention relates to a polarization plane switching device that utilizes the Faraday effect of ferrite, and more specifically, the present invention relates to a polarization plane switching device that utilizes the Faraday effect of ferrite, and more specifically, a closed loop is formed by a ferrite rod portion located inside a waveguide and an outer magnetic core portion, and a polarization plane is formed by winding a coil around the closed loop. This relates to a wavefront switching device. [Prior art] A polarization plane switch uses the Faraday effect of ferrite to rotate the plane of polarization of electromagnetic waves traveling in direct yI polarization.
It is in i position. This type of device is used, for example, to pass only the received waves of a desired channel among the received waves collected by a parabolic antenna (the plane of polarization is tilted 90 degrees for each channel) as part of a satellite broadcast receiving system. It is used for such things. The conventional polarization plane cutter has a structure in which a ferrite rod is inserted into a waveguide and a coil is attached to the outside of the waveguide, and a predetermined magnetic field is applied to the ferrite rod by continuing to flow a constant current through the coil. The plane of polarization of the electromagnetic waves applied and traveling is rotated. The plane of polarization is switched by continuing to supply current in the opposite direction. [Problems to be Solved by the Invention] As described above, the conventional device has a structure in which a coil is wound around the outside of a ferrite rod, so it has an open magnetic path configuration, and therefore a demagnetizing field is generated inside the ferrite rod. Since this demagnetizing field reduces the internal magnetic field, it is necessary to constantly supply a fairly large coil current during use to keep the magnetic field applied to the ferrite rod at a predetermined value. For these reasons, conventional devices have the drawback of being difficult to save power and generating a lot of heat. It is an object of the present invention to provide a polarization plane switching device using the Faraday effect that eliminates the drawbacks of the prior art as described above, consumes less power (and does not cause problems with heat generation). Means for Solving] The present invention, which can achieve the above objects, applies a magnetic field to a ferrite rod placed in a waveguide, and utilizes the Faraday effect to rotate the polarization plane of advancing electromagnetic waves. In the switching device, a magnetic core is provided outside the waveguide, and the ferrite rod portion located inside the waveguide and the magnetic core continuously form a closed loop structure, and a coil is wound around the polarization plane switching device. Here, the magnetic core located outside the waveguide has, for example, a U-shape, and is configured to be continuous with the side surfaces of both ends of the ferrite rod inside the waveguide.U-shaped magnetic core The and ferrite rod portions may be separate members and bonded together using an adhesive or the like, or they may be integrally molded and sintered. If they are combined as separate members, the 1sin ratio μ of each may be the same. Select a material that has a high JLT resistance (lithium-based ferrite, etc., which is suitable for microwave use) for the ferrite rod part.

【作用] 本発明では導波管内部に位置するフェライト棒部分と導波管の外側に設けられた磁心部とが連続して閉ループ構造をなしているから、反磁界は発生しない、このためB −I!カーブ(磁気ヒステリシス曲線)は立った形になり、その角形性を利用すると偏波面を切り換える際にのみ電流を流せば後は残留磁化によって所定のファラデー回転が得られ、通常動作時における電力の供給は不要となる。また偏波面回転角の微調整骨を考慮したとしても、通常の動作時には極く僅かな電流で済む。 【実施例】[Effect] In the present invention, since the ferrite rod portion located inside the waveguide and the magnetic core portion provided outside the waveguide continuously form a closed loop structure, no demagnetizing field is generated. Therefore, B-I! The curve (magnetic hysteresis curve) has a vertical shape, and if you use its squareness to flow current only when switching the plane of polarization, the residual magnetization will then obtain the desired Faraday rotation, which can be used to supply power during normal operation. becomes unnecessary. Furthermore, even if the fine adjustment of the polarization plane rotation angle is taken into consideration, only a very small amount of current is required during normal operation. 【Example】

第1図は本発明に係る偏波面切換器の一実施例を示す断
面図である。この偏波面切換器は、衛星放送受信システ
ムにおいて受信用パラボラアンテナ等に取り付けられ、
進行する電磁波の偏波面をファラデー効果を利用して回
転させるものである。 偏波面切換器lOは、アルミニウム等の導電率の高い導
波管12内にフェライト棒部分14を配置し、その両端
にインピーダンス整合等の[1的のため誘電率が数〜十
数程度のセラミックス誘電体からなる入力変換器16と
出力変!負器!8とを取り付け、フェライト棒部分14
が位置する導波管12の周囲にコイル20を巻装した構
造である。 ここで本発明の特徴は、導波管12の外側に磁心部22
を設け、フェライト棒部分12と磁心部22とが連続し
て閉ループ構造をなすように構成した点である。 導波管12の入力側にはアンテナ方向を向(ホーン24
が取り付けられ、導波管12の出力側は低雑音増幅器に
接続される。なお出力変換器18中には不要の電磁波を
吸収させるための抵抗体26が挾み込まれる。 フェライト棒部分14は、抵抗が高くマイクロ波用に適
しているリチウム系フェライト等を用いる。磁心部22
は同じリチウム系フェライトでもよいし別の材質であっ
てもよい、別の材′質を用いる場合には、i3磁率μが
ほぼ同じ材料を選ぶ。 マイクロ波用リチウム系フェライト材tqの場合、閉ル
ープ構造だとB−Hカーブは第2図へに示すようになり
、角形で立った形状となる。 それに対して従来のような単なる棒状の開ループ構造だ
と第2図Bに示すようにB −Hカーブはかなり傾斜し
てしまう。 本発明においては、例えば所定のファラデー効果を得る
ためにBaという磁束密度が必要であるとすると、最初
に電流を流して−HHaだけの磁界をかければ後は?i
流を供給しなくてもよい、また同様にBbという磁束密
度が必要であるならば、その時に逆向きにコイル電流を
供給してHbだけの磁界をかけ、その後はコイル電流は
零でよい、つまり必要な磁束密度がBaであっても、あ
るいはBbであっても、外部から供給する磁界は零でよ
く、切り換えの際のみに必要な電流を流せば後は電流を
供給する必要はない。 それに対して第2図Bに示すような従来技術では、Ba
という磁束密度が必要であるならばHcという磁界をか
けなければならず、そのため常時コイル電流を供給し続
ける必要がある。 また逆にnbという磁束密度が必要な場合には、磁界1
(dを印加するため常時それに対応した逆向きのコイル
電流を供給し続けなければならない。 つまり本発明では原理的には偏波面を切り換える時のみ
電流を流せばよいことになり、また供給する磁界も小さ
くてよいから、省電力化できるし、コイルターン敗も少
な(て済む。 また本発明では必要な磁束密度がBa或いはnbから多
少ずれている場合でも僅かな電流を流すだけでそれらの
ml!整を行うことが可能である。 第3図は本発明の他の実施例を示す断面図であり、第4
図はその斜視図である。基本的な構成は前記第1図に示
す場合と同様であるから、対応する部分には同一符号を
付しそれらについての説明は省略する。導波管12の内
部に位置するフェライト棒部分14と外側に位置する磁
心部分22は閉ループ構成となるから、コイル20は何
処に巻き付けてもよい、この実施例ではコの字型の磁心
部22の方にコイル20を巻き付けている。 第5図は本発明におけるフェライト棒状部14とコの字
型磁心部22とを更に詳細に拡大して示したものである
。フェライト棒状部14とコの字型磁心部22とを別々
に成形して焼結し、必要があればボビンを使用して所定
の位置にコイルzoJIcS装し、その後フェライト棒
部分14の両端側面にてコの字型磁心部22の先端を組
み合わせ接着剤により密着固定する。この場合、フェラ
イト棒部分14とコの字型磁心部22とは別の材質を用
いてもよく、その場合にはi3′&11率がほぼ同じも
のを使用するのが望ましい。 また別の例としては〕□エライト棒部分14とコの字型
磁心部22とを一体成形し焼結する構成がある。その場
合には、コイル巻き付は部分を円形にして分割ボビンを
嵌め込み、ボビンを回転させながらコイルを巻き付けれ
ば組み立ては容易になる。使用可能なフェライト材料と
しては、前記リチウム系フェライトの他、ニッケルー亜
鉛系フェライト材等もある。 [発明の効果] 本発明は上記のように導波管の外側に磁心部分を設けて
導波管内に位置するフェライト棒部分とその磁心部とが
連続した閉ループ構造をなし、それにコイルを巻装した
構成であるから反磁界が発生せずI3− IIカーブは
立った形状になるため、偏波面を切り換える時のみコイ
ル電流を供給すれば、後は電流を供給せずに済むし、供
給する場合でも掻く僅かなものでよく、省電力化を図る
ことができると共に発熱を低減できる効果がある。 また偏波面を切り換える場合でも、I3− Hカー゛ブ
が立っているため従来技術よりも小さな電流で済む。 更に僅かな電流を供給し続けるようにすれば偏波面切換
え角度の微調整も可能であり、従ってJll一種類の偏
波面切l!!1器でも偏波面切換え角度が僅かに異なる
広い地域での使用が可能とな′る。
FIG. 1 is a sectional view showing an embodiment of a polarization plane switching device according to the present invention. This polarization switcher is attached to a receiving parabolic antenna, etc. in a satellite broadcast receiving system.
It rotates the plane of polarization of traveling electromagnetic waves using the Faraday effect. The polarization plane switching device IO has a ferrite rod part 14 placed inside a waveguide 12 made of aluminum or the like with high conductivity, and a ceramic material with a dielectric constant of several to ten tens for impedance matching etc. is placed at both ends of the ferrite rod part 14. Input converter 16 made of dielectric and output change! Negative device! 8 and attach the ferrite rod part 14.
It has a structure in which a coil 20 is wound around a waveguide 12 in which a waveguide 12 is located. Here, the feature of the present invention is that a magnetic core portion 22 is provided on the outside of the waveguide 12.
, and the ferrite rod portion 12 and the magnetic core portion 22 are configured to continuously form a closed loop structure. The input side of the waveguide 12 has a horn 24 facing the antenna direction.
is attached, and the output side of the waveguide 12 is connected to a low noise amplifier. Note that a resistor 26 is inserted into the output converter 18 to absorb unnecessary electromagnetic waves. The ferrite rod portion 14 is made of lithium-based ferrite or the like, which has high resistance and is suitable for microwave use. Magnetic core part 22
may be the same lithium-based ferrite or may be made of different materials. When using different materials, select materials with approximately the same i3 magnetic coefficient μ. In the case of the lithium-based ferrite material tq for microwaves, if it has a closed loop structure, the B-H curve will be as shown in FIG. 2, and will have a square, upright shape. On the other hand, if the conventional structure is a simple rod-shaped open loop structure, the B-H curve will be considerably inclined as shown in FIG. 2B. In the present invention, for example, if a magnetic flux density of Ba is required to obtain a predetermined Faraday effect, what happens if a current is first applied and a magnetic field of -HHa is applied? i
Similarly, if a magnetic flux density of Bb is required, then a coil current is supplied in the opposite direction to apply a magnetic field of only Hb, and then the coil current can be zero. In other words, even if the required magnetic flux density is Ba or Bb, the magnetic field supplied from the outside may be zero, and if the necessary current is supplied only during switching, there is no need to supply any current thereafter. On the other hand, in the prior art as shown in FIG. 2B, Ba
If such a magnetic flux density is required, a magnetic field of Hc must be applied, and therefore a coil current must be continuously supplied. Conversely, if a magnetic flux density of nb is required, the magnetic field 1
(In order to apply d, it is necessary to constantly supply a corresponding coil current in the opposite direction. In other words, in principle, in the present invention, it is only necessary to flow current only when switching the polarization plane, and the magnetic field to be supplied is Since the magnetic flux density may be small, it is possible to save power and reduce coil turn failure.Also, in the present invention, even if the required magnetic flux density is slightly different from Ba or nb, only by passing a small current, those ml can be reduced. !It is possible to perform adjustment. FIG. 3 is a sectional view showing another embodiment of the present invention, and FIG.
The figure is a perspective view thereof. Since the basic configuration is the same as that shown in FIG. 1, corresponding parts are given the same reference numerals and explanations thereof will be omitted. Since the ferrite rod portion 14 located inside the waveguide 12 and the magnetic core portion 22 located outside form a closed loop configuration, the coil 20 may be wound anywhere. A coil 20 is wound around the . FIG. 5 is a more detailed enlarged view of the ferrite rod-shaped portion 14 and the U-shaped magnetic core portion 22 in the present invention. The ferrite rod portion 14 and the U-shaped magnetic core portion 22 are separately molded and sintered, and if necessary, a coil is mounted in a predetermined position using a bobbin, and then a coil is attached to both end sides of the ferrite rod portion 14. The tips of the lever-shaped magnetic core portions 22 are assembled and tightly fixed with adhesive. In this case, different materials may be used for the ferrite rod portion 14 and the U-shaped magnetic core portion 22, and in that case, it is desirable to use materials having approximately the same i3'&11 ratio. Another example is a configuration in which the □ elite rod portion 14 and the U-shaped magnetic core portion 22 are integrally molded and sintered. In that case, assembly will be easier if the coil is wound by making the part circular and fitting the split bobbin, and then winding the coil while rotating the bobbin. In addition to the above-mentioned lithium-based ferrite, usable ferrite materials include nickel-zinc-based ferrite materials. [Effects of the Invention] As described above, the present invention provides a closed loop structure in which a magnetic core portion is provided on the outside of a waveguide, a ferrite rod portion located inside the waveguide and the magnetic core portion are continuous, and a coil is wound around it. Because of this configuration, no demagnetizing field is generated and the I3-II curve has a vertical shape, so if the coil current is supplied only when switching the polarization plane, there is no need to supply current afterwards. However, only a small amount is required, and it is possible to save power and reduce heat generation. Furthermore, even when switching the plane of polarization, a smaller current is required than in the prior art because the I3-H curve stands. Furthermore, by continuing to supply a small amount of current, it is possible to finely adjust the polarization switching angle. ! Even a single device can be used in a wide area where the polarization plane switching angle is slightly different.

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

第1図は本発明に係る偏波面切IIA器の一実施例を示
す断面図、第2図Aはそのl3−Hカーブの説明図、第
2図Bは従来技術の3−11カーブの説明図、第3図は
本発明に係る偏波面切換器の他の実施例を示す断面図、
第4図はその斜視図、第5図は本発明で用いるフェライ
ト棒部分と磁心部との一例を示す斜視図である。 10・・・偏波面切換器、12・・・導波管、14・・
・フェライト棒部分、20・・・コイル、22・・・コ
の字型磁心部。 特許出廓人  富士電気化学株式会社 代  理  人     茂  見     1第1図 第2図 A        B
FIG. 1 is a cross-sectional view showing an embodiment of the polarization plane cutter IIA device according to the present invention, FIG. 2A is an illustration of the 13-H curve thereof, and FIG. 2B is an explanation of the 3-11 curve of the prior art. 3 are sectional views showing other embodiments of the polarization plane switching device according to the present invention,
FIG. 4 is a perspective view thereof, and FIG. 5 is a perspective view showing an example of a ferrite rod portion and a magnetic core portion used in the present invention. 10...Polarization plane switcher, 12...Waveguide, 14...
- Ferrite rod part, 20... Coil, 22... U-shaped magnetic core part. Patent distributor Fuji Electrochemical Co., Ltd. Agent Shigeru Mi 1 Figure 1 Figure 2 A B

Claims (3)

【特許請求の範囲】[Claims] 1.導波管内に配置したフェライト棒に磁界を印加し、
そのファラデー効果を利用して進行してくる電磁波の偏
波面を回転させる偏波面切換器において、導波管の外側
に磁心部を設け、導波管内部に位置するフェライト棒部
分と前記磁心部とが連続して閉ループ構造をなし、それ
にコイルが巻装されている偏波面切換器。
1. A magnetic field is applied to the ferrite rod placed inside the waveguide,
In a polarization plane switching device that uses the Faraday effect to rotate the polarization plane of advancing electromagnetic waves, a magnetic core is provided outside the waveguide, and a ferrite rod portion located inside the waveguide and the magnetic core are connected to each other. A polarization switcher in which a coil is wound around a continuous closed-loop structure.
2.導波管の外側に位置する磁心部はコの字型形状をな
し、それとは別個のフェライト棒部分の両端側面に接続
されている請求項1記載の偏波面切換器。
2. 2. The polarization plane switching device according to claim 1, wherein the magnetic core located outside the waveguide has a U-shape and is connected to both end side surfaces of a separate ferrite rod portion.
3.導波管内に位置するフェライト棒部分と導波管外に
位置するコの字型形状の磁心部とが一体成形されている
請求項1記載の偏波面切換器。
3. 2. The polarization plane switching device according to claim 1, wherein the ferrite rod portion located within the waveguide and the U-shaped magnetic core portion located outside the waveguide are integrally molded.
JP14201688A 1988-06-09 1988-06-09 Switch for plane of polarization Pending JPH01311601A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP14201688A JPH01311601A (en) 1988-06-09 1988-06-09 Switch for plane of polarization

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP14201688A JPH01311601A (en) 1988-06-09 1988-06-09 Switch for plane of polarization

Publications (1)

Publication Number Publication Date
JPH01311601A true JPH01311601A (en) 1989-12-15

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Family Applications (1)

Application Number Title Priority Date Filing Date
JP14201688A Pending JPH01311601A (en) 1988-06-09 1988-06-09 Switch for plane of polarization

Country Status (1)

Country Link
JP (1) JPH01311601A (en)

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS4948264A (en) * 1972-09-14 1974-05-10
JPS5019424A (en) * 1973-05-07 1975-02-28
JPS553218A (en) * 1978-06-23 1980-01-11 Nippon Telegr & Teleph Corp <Ntt> Variable phase shifter

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS4948264A (en) * 1972-09-14 1974-05-10
JPS5019424A (en) * 1973-05-07 1975-02-28
JPS553218A (en) * 1978-06-23 1980-01-11 Nippon Telegr & Teleph Corp <Ntt> Variable phase shifter

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