JPH05251888A - Thin narrow band radio wave absorber - Google Patents

Thin narrow band radio wave absorber

Info

Publication number
JPH05251888A
JPH05251888A JP4988392A JP4988392A JPH05251888A JP H05251888 A JPH05251888 A JP H05251888A JP 4988392 A JP4988392 A JP 4988392A JP 4988392 A JP4988392 A JP 4988392A JP H05251888 A JPH05251888 A JP H05251888A
Authority
JP
Japan
Prior art keywords
radio wave
wave absorber
weight
narrow band
thin narrow
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
JP4988392A
Other languages
Japanese (ja)
Inventor
Hisao Kaneko
子 久 生 金
Makoto Ishikura
倉 誠 石
Manabu Teranishi
西 学 寺
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 JP4988392A priority Critical patent/JPH05251888A/en
Publication of JPH05251888A publication Critical patent/JPH05251888A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To absorb and take away only the radio wave of narrow band frequency by mixing material of high magnetic permiability and high dielectric constant with high polymer material. CONSTITUTION:Ethylene propylene diene rubber is mingled with permally and barium titanate in weight ratio of 1:1 so that the latter weight is equivalent to the 80% of the entire weight. And then, they are kneaded and pressed to obtain a sheet. Its thickness is 2mm. Or, chloprene rubber is mingled with titanate and Mn-Zn ferrite group alloy in weight ratio of 1:1 so that the latter weight is equivalent to the 80% of the entire weight. And then, they are kneaded and pressed to obtain a sheet of 2mm in thickness. So, since only the radio wave of very narrow frequency can be absorbed and taken away, and at the same time, it can be formed to a thin one, electromagnetic fault problem is effectively solved.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は新規な薄型狭帯域電波吸
収体に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a novel thin thin band electromagnetic wave absorber.

【0002】[0002]

【発明が解決しようとする課題】近年電磁波障害(EM
C)問題がクローズアップされてきており、その問題の
解決には一定周波数帯域の電波を吸収する電波吸収体が
中心的存在となっている。
In recent years, electromagnetic interference (EM
C) The problem has been highlighted, and a radio wave absorber that absorbs radio waves in a certain frequency band has become the main focus for solving the problem.

【0003】従来の技術ではGHz帯の電波吸収体は1
〜2GHz程度の帯域幅(20dB以上の吸収帯域)を
もっているのが普通である。また開発の主力も広帯域化
を目ざしているのが殆どである。
In the prior art, there are only 1 GHz band electromagnetic wave absorber.
It usually has a bandwidth of about 2 GHz (absorption band of 20 dB or more). In addition, most of the main development efforts are aimed at widening the band.

【0004】例えば特開昭51−121200号公報に
よれば、従来フェライト粉末を非磁性体中に分散させた
複合フェライト、またはカーボニル鉄粉末を非磁性体中
分散させたカーボニル鉄系磁性体等からなる電波吸収体
が知られていたが、これらはいずれも周波数帯域が狭い
ので実用範囲に限界があるとして、フェライト粉末とカ
ーボニル鉄粉末の両方を含み、広い周波数範囲にわたり
良好な電波吸収特性を有する電波吸収体が得られてい
る。
For example, according to Japanese Patent Application Laid-Open No. 51-121200, a composite ferrite in which a ferrite powder is dispersed in a non-magnetic material, or a carbonyl iron-based magnetic material in which a carbonyl iron powder is dispersed in a non-magnetic material is used. The following radio wave absorbers have been known, but since all of them have a narrow frequency band and are limited in their practical range, they contain both ferrite powder and carbonyl iron powder and have good radio wave absorption characteristics over a wide frequency range. An electromagnetic wave absorber is obtained.

【0005】しかしながら、いらない電波を除去してい
こうとするに当り、かかる広帯域の電波吸収体を用いる
とその近隣の周波数帯域の電波まで除去されてしまう。
たとえば従来の電波吸収体においては1〜2GHz程度
の帯域幅があるため、5GHzの電波のみ除去したい場
合にも4GHz〜6GHzの電波も除去されてしまうと
いう難点があった。
However, when attempting to remove unwanted radio waves, the use of such a broadband radio wave absorber also removes radio waves in the frequency band in the vicinity thereof.
For example, since the conventional radio wave absorber has a bandwidth of about 1 to 2 GHz, there is a disadvantage that even if only 5 GHz radio waves are desired to be removed, 4 GHz to 6 GHz radio waves are also removed.

【0006】[0006]

【課題を解決するための手段】かくて本発明の目的はで
きるだけ狭い吸収帯域をもつ電波吸収体を提供すること
である。
SUMMARY OF THE INVENTION An object of the present invention is thus to provide a radio wave absorber having an absorption band as narrow as possible.

【0007】本発明によれば、高透磁率材料と高誘電率
材料を高分子材料に混合せしめるときかかる目的を達成
しうることが見出されたのである。
According to the present invention, it has been found that such a purpose can be achieved when mixing a high magnetic permeability material and a high dielectric constant material into a polymeric material.

【0008】 本発明では上述のように高透磁率材料と高誘電率材料を高分子材料に混合せし めるのであり高透磁率(高μ)材料としてはμ´が10,000以上のものが用 いられ、高透磁率(高ε)材料としてはε´が5.000以上のものが用いられ る。ここにμ,εは夫々複素透磁率、複素誘電率を示し次の式によって表わされ る。[0008] The present invention in μ'is more than 10,000 high permeability material and a high dielectric constant material as described above as-Shi was mixed Mel of a and high permeability (high mu) material in the polymeric material what is use-Irare, Ipushiron' is is ... Ru with more than 5.000 as high permeability (high epsilon) materials. Where μ and ε are the complex permeability and complex permittivity, respectively, and are expressed by the following equations.

【0009】 μ=μ´−iμ″,ε=ε´−iε″ かかる高透磁率材料としては一般にパーマロイと呼ばれ
るNi−Fe系の代表的な磁性合金を用いるのが好まし
い。この合金の標準組成はNi60〜90%、Fe残部
であり、この外Mo,Cr,Mn,Cuなどが必要に応
じて少量添加される。このパーマロイは通常10,00
0の透磁率を有する。
[0009] · · μ = μ'-iμ " , ε = ε'-iε" as such high-permeability material is preferably used generally typical magnetic alloy of Ni-Fe system called permalloy. The standard composition of this alloy is 60 to 90% Ni and the balance of Fe, and in addition to this, small amounts of Mo, Cr, Mn, Cu, etc. are added as necessary. This permalloy is usually 10,000
It has a magnetic permeability of zero.

【0010】この他にNi−Co合金やMn−Znフェ
ライトを用いることもできる。
Besides, Ni-Co alloy or Mn-Zn ferrite may be used.

【0011】又高誘電率材料としてはたとえば5000
の誘電率を有るすチタン酸バリウム(BaTiO3 )を
用いるのが好適である。又チタン酸鉛(PbTiO3
を用いることもできる。上記両高特性材料とも一般に粉
体の形で用いられる。
As the high dielectric constant material, for example, 5000
It is preferable to use barium titanate (BaTiO 3 ) having a dielectric constant of. Also lead titanate (PbTiO 3 )
Can also be used. Both of the above high-performance materials are generally used in the form of powder.

【0012】これらの材料を混合する高分子材料として
はたとえばエポキシ樹脂、不飽和ポリエステル樹脂等の
合成樹脂、或はクロロプレンゴム、エチレンプロピレン
ジエンゴム(EPDM)、シリコーンゴム等の合成ゴム
が用いられる。各種樹脂乃至ゴムを1種単独で用いても
よく2種以上適宜組合わせて用いてもよい。
As the polymer material to which these materials are mixed, for example, synthetic resin such as epoxy resin and unsaturated polyester resin, or synthetic rubber such as chloroprene rubber, ethylene propylene diene rubber (EPDM) and silicone rubber is used. Various resins or rubbers may be used alone or in combination of two or more kinds.

【0013】上記高透磁率材料と高誘電率材料は重量比
で1:1の割合から1:4の範囲の量で用いられる。両
者の配合比率によって電波吸収特性(整合周波数)を変
えることができる。又両高特性材料を高分子材料と混合
するときは両高特性材料と高分子材料との合計量に対し
て70〜90重量%の範囲の量の両高特性材料を加える
のが適当である。この際高分子材料に高透磁率材料を混
合し、別に高分子材料に高誘電率材料を混合し、その両
者を更に混合するようにすることもできる。この場合の
高分子材料は同一でも別異でもよい。
The high magnetic permeability material and the high dielectric constant material are used in a weight ratio of 1: 1 to 1: 4. The radio wave absorption characteristics (matching frequency) can be changed by the mixture ratio of both. When the high-performance material and the high-polymer material are mixed, it is appropriate to add the high-performance material in an amount of 70 to 90% by weight based on the total amount of the high-performance material and the high-molecular material. .. At this time, a high magnetic permeability material may be mixed with the polymer material, a high dielectric constant material may be separately mixed with the polymer material, and both may be further mixed. In this case, the polymer materials may be the same or different.

【0014】尚、エチレンプロピレンジェンゴム(EP
DM)とパーマロイの混合物ではμ´は約1000であ
り、又同じゴムとBaTiO3 の混合物のε´は約80
0である。この外EPDMとMn−Znフェライト、ク
ロロプレンゴム(CR)とBaTiO3 、シリコーンゴ
ムとNi−Co合金の混合物がよい特性を有している。
Incidentally, ethylene propylene diene rubber (EP
For a mixture of DM) and permalloy, μ'is about 1000, and for a mixture of the same rubber and BaTiO 3 ε'is about 80.
It is 0. The outer EPDM and Mn-Zn ferrite, chloroprene rubber (CR) and BaTiO 3, a mixture of silicone rubber and Ni-Co alloy has a good characteristic.

【0015】このようにしてえられた電波吸収体は狭い
帯域の周波数の電波のみ吸収し、しかもシート厚を薄く
形成することができる。
The radio wave absorber thus obtained absorbs only radio waves of a narrow band of frequency and can be formed with a thin sheet.

【0016】以下に実施例を示す。Examples will be shown below.

【0017】[0017]

【実施例】実施例1 エチレンプロピレンジエンゴム(EPDM)にパーマロ
イとチタン酸バリウム(BaTiO3 )を重量比1:1
の割合で合計量の80重量%混入させ、混練、プレスを
行なってシートを得た。その厚みは2mmであった。
Example 1 Permalloy and barium titanate (BaTiO 3 ) were added to ethylene propylene diene rubber (EPDM) in a weight ratio of 1: 1.
80% by weight of the total amount was mixed, and kneading and pressing were performed to obtain a sheet. Its thickness was 2 mm.

【0018】この場合 μ´=1000 μ″=100 ε´=800 ε″=80 であった。In this case, μ ′ = 1000 μ ″ = 100 ε ′ = 800 ε ″ = 80.

【0019】えられた電波吸収体の電波吸収特性を測定
した結果は図1に示すグラフのとおりであった。その電
波吸収特性は4GHzに中心周波数をもち20dB以上
の帯域は3.8〜4.1GHzで狭帯域であった。
The results of measuring the radio wave absorption characteristics of the obtained radio wave absorber are shown in the graph of FIG. The radio wave absorption characteristics had a center frequency at 4 GHz and a band of 20 dB or more was 3.8 to 4.1 GHz, which was a narrow band.

【0020】実施例2 クロロプレンゴム(CR)にチタン酸鉛(PbTi
3 )とMn−Znフェライト系合金を重量比で1:1
の割合で合計量の80重量%の量混入させ混練、プレス
を行なって厚み2mmのシートを得た。
Example 2 Lead titanate (PbTi) was added to chloroprene rubber (CR).
The O 3) and Mn-Zn ferrite based alloy in a weight ratio of 1: 1
80% by weight of the total amount was mixed and kneaded and pressed to obtain a sheet having a thickness of 2 mm.

【0021】この場合 μ´=900 μ″=90 ε´=600 ε″=60 であった。In this case, μ ′ = 900 μ ″ = 90 ε ′ = 600 ε ″ = 60.

【0022】えられた電波吸収体の電波吸収特性を測定
した結果は図2に示すとおりであった。その電波吸収特
性は4GHzに中心周波数をもち、20dB以上の帯域
は3.6〜4.4GHzで狭帯域であった。
The results of measuring the radio wave absorption characteristics of the obtained radio wave absorber are shown in FIG. The radio wave absorption characteristics had a center frequency at 4 GHz, and a band of 20 dB or more was a narrow band of 3.6 to 4.4 GHz.

【0023】[0023]

【発明の効果】上述から明らかなように、本発明の電波
吸収体によればごく狭い帯域幅の周波数の電波のみ吸収
して除去することができ、しかも薄く形成することがで
きこれにより電磁波障害問題を有効に解決することがで
きる。しかも混合する両高特性材料の比率又はシート厚
みを変えることによって吸収帯域幅を適宜変化させるこ
とができる。
As is apparent from the above, according to the radio wave absorber of the present invention, it is possible to absorb and remove only radio waves having a frequency of a very narrow band width, and further, it is possible to form a thin film, which causes electromagnetic interference Can solve problems effectively. Moreover, the absorption bandwidth can be appropriately changed by changing the ratio of both high-performance materials to be mixed or the sheet thickness.

【図面の簡単な説明】[Brief description of drawings]

【図1】本発明の実施例1によりつくられた電波吸収体
の電波吸収特性を示すグラフ。
FIG. 1 is a graph showing radio wave absorption characteristics of a radio wave absorber made according to Example 1 of the present invention.

【図2】本発明の実施例2によりつくられた電波吸収体
の電波吸収特性を示すグラフ。
FIG. 2 is a graph showing the radio wave absorption characteristics of a radio wave absorber made according to Example 2 of the present invention.

Claims (3)

【特許請求の範囲】[Claims] 【請求項1】高透磁率材料と高誘電率材料を高分子材料
に混合せしめてなる薄型狭帯域電波吸収体。
1. A thin narrow-band electromagnetic wave absorber obtained by mixing a high magnetic permeability material and a high dielectric constant material with a polymer material.
【請求項2】高透磁率材料はパーマロイである請求項1
記載の薄型狭帯域電波吸収体。
2. The high magnetic permeability material is permalloy.
The thin narrow-band electromagnetic wave absorber described.
【請求項3】高誘電率材料はチタン酸バリウムである請
求項1記載の薄型狭帯域電波吸収体。
3. The thin narrow band electromagnetic wave absorber according to claim 1, wherein the high dielectric constant material is barium titanate.
JP4988392A 1992-03-06 1992-03-06 Thin narrow band radio wave absorber Pending JPH05251888A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP4988392A JPH05251888A (en) 1992-03-06 1992-03-06 Thin narrow band radio wave absorber

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP4988392A JPH05251888A (en) 1992-03-06 1992-03-06 Thin narrow band radio wave absorber

Publications (1)

Publication Number Publication Date
JPH05251888A true JPH05251888A (en) 1993-09-28

Family

ID=12843443

Family Applications (1)

Application Number Title Priority Date Filing Date
JP4988392A Pending JPH05251888A (en) 1992-03-06 1992-03-06 Thin narrow band radio wave absorber

Country Status (1)

Country Link
JP (1) JPH05251888A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US7218266B2 (en) 2000-04-10 2007-05-15 Hitachi, Ltd. Electromagnetic wave absorber, method of manufacturing the same and appliance using the same
WO2009038174A1 (en) * 2007-09-20 2009-03-26 Nitto Denko Corporation Electromagnetic wave absorber and method for electromagnetic wave absorption
CN110066469A (en) * 2019-04-17 2019-07-30 东莞市利群榕兴高分子科技有限公司 A kind of stress ethylene propylene diene monomer (EPDM) material and its preparation process applied to cable accessory

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US7218266B2 (en) 2000-04-10 2007-05-15 Hitachi, Ltd. Electromagnetic wave absorber, method of manufacturing the same and appliance using the same
WO2009038174A1 (en) * 2007-09-20 2009-03-26 Nitto Denko Corporation Electromagnetic wave absorber and method for electromagnetic wave absorption
CN110066469A (en) * 2019-04-17 2019-07-30 东莞市利群榕兴高分子科技有限公司 A kind of stress ethylene propylene diene monomer (EPDM) material and its preparation process applied to cable accessory

Similar Documents

Publication Publication Date Title
Sugimoto et al. Barium M-type ferrite as an electromagnetic microwave absorber in the GHz range
JPH0935927A (en) Composite magnetic body and electromagnetic interference suppressor using the same
Vinayasree et al. Flexible microwave absorbers based on barium hexaferrite, carbon black, and nitrile rubber for 2–12 GHz applications
KR100718145B1 (en) Resonance element, band pass filter and duplexer
JPH04150098A (en) Radio wave absorptive material
JPH05251888A (en) Thin narrow band radio wave absorber
KR20020034989A (en) Soft magnetic powder and composite magnetic material using the same
RU2414029C1 (en) Electromagnetic wave absorber
JPH0516679B2 (en)
JP2000138492A (en) Electromagnetic wave absorber
KR101004026B1 (en) Broadband two layer type electromagnetic wave absorption material sheet and method for fabricating the same
JPH01305503A (en) Radio wave absorbing material
Sugimoto et al. Compositional Dependence of the Electromagnetic Wave Absorption Properties of BaFe12− x− yTixMnyO19 in the GHz Frequency Range
JPH11186781A (en) Radiowave absorbent and radiowave absorbing box
JP2007173859A (en) Method for manufacturing electromagnetic interference suppressor
JPH05299872A (en) Wave absorber for 900mhz-band
JP2002083704A (en) Radio wave absorber
JP2000133983A (en) Radio wave absorbing body
KR102488005B1 (en) Millimeter wave shielding and absorption composite material
JPH0325888A (en) Microwave absorber
JPH0218597B2 (en)
CN114122737A (en) Particle for absorbing electromagnetic wave in GHz frequency band and electromagnetic wave absorber comprising same
JP4032709B2 (en) Filter circuit
JPH03147205A (en) Compound dielectric material
JPH0468800B2 (en)