JP2004179385A - Radio wave absorbing sheet - Google Patents
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- JP2004179385A JP2004179385A JP2002343706A JP2002343706A JP2004179385A JP 2004179385 A JP2004179385 A JP 2004179385A JP 2002343706 A JP2002343706 A JP 2002343706A JP 2002343706 A JP2002343706 A JP 2002343706A JP 2004179385 A JP2004179385 A JP 2004179385A
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- radio wave
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Abstract
Description
【0001】
【発明の属する技術分野】
本発明は、合成樹脂に海綿状鉄粉を分散混合してなるシート状の電波吸収体(電波吸収シート)に関する。
【0002】
【従来の技術】
近年、移動体通信や無線LANなど、GHz帯の電波を使用する電気、電子機器が広く普及しつつある。高速道路自動料金収受システム(ETC)は、5.8GHz付近のマイクロ波帯を利用したものであるが、新たな分野としてミリ波等の高周波数帯を利用した技術開発が活発に進められている。ミリ波帯とは30〜300GHzの領域を指すが、特に60〜80GHz付近の周波数は、自動車の車間レーダーや車間通信等の高度道路交通システム(ITS)関連などへの応用が検討されており、電波ノイズ(不要電波)を効率良く吸収できる電波吸収体が必要とされている。
【0003】
電波吸収体は、入射した電波を吸収して、電波エネルギーを熱エネルギー等に変換するもので、電気・電子機器およびその周囲等において、不要電波の反射、散乱、干渉が生じる箇所に装着することにより、種々のトラブルを抑制する。従来、電波吸収体はウレタン発泡材、ゴム、樹脂、プラスチック等の絶縁体中にフェライト粉、カーボン粉、カーボニル鉄粉等が混練されたものが一般的であるが、高価格であり十分な適用が進んでいない。
【0004】
従来、3層からなる構成のもの(例えば特許文献1参照)、カップリング材を用いたもの(例えば特許文献2)、繊維強化プラスチックを用いたもの(特許文献3参照)、炭素を用いたもの(例えば特許文献4参照)、Fe−Cr合金を用いたもの(例えば特許文献5参照)、更に軟磁性金属粉末を用いたもの(例えば特許文献6参照)が開示されている。
しかし、これらはいずれも高価である。
今後は、電子機器・通信装置等の高性能・高機能化、数量の増加や利用周波数帯域の拡大により、不要電波による機器の誤作動等の電波障害問題がますます厳しくなる。このためGHz帯、特にミリ波の高周波帯において、高い電波吸収性能を有し、経済性に優れた電波吸収体が望まれている。
【0005】
この出願の発明に関する先行技術文献情報として例えば次のものがある。
【特許文献1】
特開平9−51190号公報
【特許文献2】
特開平11−45804号公報
【特許文献3】
特開2000−31685号公報
【特許文献4】
特開2000−165087号公報
【特許文献5】
特開2000−200990号公報
【特許文献6】
特開2002−118008号公報
【0006】
【発明が解決しようとする課題】
このような電波に対する社会の情勢に応じ、本発明は、GHz帯、特に電波吸収体に対する技術開発の要望が強いミリ波帯において、薄型で高い電波吸収性能を有するシート状の経済性に優れた電波吸収体(電波吸収シート)を提供することを課題とする。
【0007】
【課題を解決するための手段】
本発明者らは、上記課題を達成するために、フェライトなどの合金粉末に比べ安価な鉄粉を選択し、粒径、純度等の異なる種々の鉄粉にて試作検討を繰り返した結果、鉄粉の平均粒径と比表面積を限定すること等により、GHz帯にて高い電波吸収性能を得ることができ、本発明に至ったものである。
【0008】
本発明は、合成樹脂に海綿状鉄粉を分散混合してなる電波吸収シートである。平均粒径が10〜150μm、比表面積が0.05m2/g以上の海綿状鉄粉を用いることが特徴である。合成樹脂にはポリオレフィン系、ポリスチレン系、ポリウレタン系あるいはポリエステル系の熱可塑性エラストマーを用いることが望ましい。また、耐熱性や強度等から、ポリオレフィン樹脂、ポリスチレン樹脂、ポリウレタン樹脂あるいはポリエステル樹脂を一定量添加しても良い。
【0009】
本発明の電波吸収シートは、海綿状鉄粉を70〜85重量%分散混合し、厚みが0.05〜1.5mmであることが望ましい。耐食性等を考慮して、表面を金属や樹脂でコーティングした海綿状鉄粉を使用することも好ましい。
【0010】
また、本発明の電波吸収シートは、電波反射板として、片面(背面となる側)に金属板、金属箔あるいは表面処理鋼板を積層することが望ましい。これにより、40〜80GHzのミリ波帯の電波に対する反射減衰量を20dB以上得ることが可能となる。
【0011】
【発明の実施の形態】
以下、本発明の実施の形態について詳細に説明する。
【0012】
一般に電波吸収体において、使用する粉末の種類、形状、粒径やその含有量等が異なると、それに応じて電波吸収性能も異なってくる。本発明者らは、フェライトなどの合金粉末に比べると安価な鉄粉を使用し、目標のGHz帯にて高い電波吸収性能を有する電波吸収シートの開発を行った。
【0013】
本発明の電波吸収シートは、平均粒径および比表面積を限定し、海綿状鉄粉を用いることが特徴である。ここで言う海綿状鉄粉とは、酸化鉄などの酸化されている鉄粉から、気体あるいは固体の還元剤によって還元して製造される気孔を多く含んだ多孔質の鉄粉(例えば海綿鉄粉など)のこと全般を指すものである。この鉄粉は数μm程度の単一粒子が連結したスポンジ状の凝集粒子をなしたもので、通常のアトマイズ鉄粉やカーボニル鉄粉に比べると比表面積が大きいことが特徴である。合成樹脂に分散混合する海綿状鉄粉の平均粒径を10〜150μm、比表面積を0.05m2/g以上と限定することにより、電波吸収性能の高い電波吸収シートを得ることができる。
【0014】
次に本発明の電波吸収シートでは、海綿状鉄粉を70〜85重量%分散混合し、厚さを0.05〜1.5mmの範囲とする。含有量については、シート成型時の作業性やシートの耐久性や柔軟性等を考慮すると、70〜85重量%の範囲が実用的であり好ましい。海綿状鉄粉の添加量が少なすぎると十分な電波吸収性能が得られず、多すぎると粒子同士が接触し電波を反射しやすくなり、電波吸収性能は低下するうえ、また経済性も損なう。海綿状鉄粉の平均粒径、比表面積、シート中の含有量やシート厚さと電波吸収性能とは相関があり、これらを適切にコントロールすることにより、目的の周波数や用途に叶った優れた電波吸収性能を得ることが可能である。目的の周波数、電波吸収量に応じて、主にシート中の海綿状鉄粉の含有量およびシート厚さを選定する。
【0015】
ここで、耐食性等が要求される用途には、使用する海綿状鉄粉の表面に金属又は樹脂のコーティングを行う。金属コーティングの場合は、海綿状鉄粉の表面に電気Niメッキもしくは無電解Ni−Pメッキ等を行うことが好ましい。また、樹脂コーティングの場合は、海綿状鉄粉の表面にポリエチレン、ポリエステル、ナイロン、エポキシ、フッ素等の樹脂をコーティングすることが好ましい。
【0016】
次に本発明に用いられる合成樹脂に関しては、柔軟性、耐薬品性、耐熱性や経時安定性等に優れるポリエチレン−ブテン共重合体エラストマー、ポリプロピレン−ポリエチレン共重合体エラストマー等のポリオレフィン系熱可塑性エラストマー、ポリスチレン−ブタジエン共重合体エラストマー等のポリスチレン系熱可塑性エラストマー、ポリウレタン系熱可塑性エラストマーあるいはポリブチレンテレフタレート−ポリブタジオール共重合体エラストマー等のポリエステル系熱可塑性エラストマーが適する。これらの熱可塑性エラストマーを用いることにより、70〜85%海綿状鉄粉を分散混合した後も可撓性を有する。
【0017】
さらに、本発明の電波吸収シートは、電波反射板として、片面(背面となる側)に、亜鉛,亜鉛−ニッケル合金、亜鉛−コバルト−モリブデンあるいはニッケルなどのメッキを施した表面処理鋼板、、鉄板、鋼板、銅板、ステンレス板やアルミニウム等の公知金属板を積層するのが望ましい。また、亜鉛メッキ、ニッケルメッキ、錫メッキや電解クロム酸処理などの公知表面処理を行った電解鉄箔、ニッケル箔、銅箔、ステンレス箔などの公知の金属箔を積層しても良い。これにより、電波吸収性能が向上し、40〜80GHzのミリ波帯の電波に対する反射減衰量が20dB以上と優れた電波吸収性能を安定して保つことが可能となり、またシートの支持の役割も兼ね備えることができる。
【0018】
【実施例】
平均粒径および比表面積の異なる数種類の海面状鉄粉を使用した。ここで使用粉末の比表面積は、固体表面に吸着した分子の数から表面積を算出する方法である気相吸着法(BET法)で行い、3回測定による平均値を用いた。試料No1〜22の熱可塑性樹脂(合成樹脂)としては、混練容易性より、ポリオレフィン系エラストマーであるポリプロピレン−ポリエチレン共重合体エラストマーを使用した。これらの鉄粉と合成樹脂とを所定の割合で配合し、ゾル形成後、ロール混練機により厚さが0.05〜1.5mm、150mm×150mmの電波吸収シートを作製した。そして、これらシートの片面に、電波反射板として厚さ30μmの鉄箔を接着し、評価に用いた。
【0019】
〔試料No.1〜6〕
表1に示すように、実施例として、平均粒径が100μm、比表面積が0.072m2/g、嵩密度が1.72g/cm3の海面状鉄粉を使用した。表1の試料No.1〜6に海面状鉄粉の含有量が70、80、85重量%の場合の測定結果を示す。
【0020】
〔試料No.7〜12〕
表1に示すように実施例として、平均粒径が45μm、比表面積が0.085m2/g、嵩密度が2.97g/cm3の海面状鉄粉を使用した。表1の試料No.7〜12に海面状鉄粉の含有量が70、80、85重量%の場合の測定結果を示す。
【0021】
〔試料No.13〜18〕
表1に示すように、実施例として、平均粒径が75μm、比表面積が0.272m2/g、嵩密度が1.94g/cm3の海面状鉄粉を使用した。表1の試料No.13〜18に海面状鉄粉の含有量が70、80、85重量%の場合の測定結果を示す。
【0022】
〔比較例〕
表1に示すように、比較例には、粉末冶金にてアトマイズ法で製造される球状のアトマイズ鉄粉を使用した。平均粒径100μm、比表面積0.043m2/g、嵩密度3.21g/cm3のアトマイズ鉄粉を使用した。表1の試料No.19〜22に比較例としてアトマイズ鉄粉の含有量が70、80重量%の場合の測定結果を示す。
【0023】
〔電波吸収性能の測定方法〕
以上の試料の電波吸収性能については、測定範囲をミリ波帯とし、ネットワークアナライザーを用い、各周波数における反射減衰量(dB)を測定した。表1に、40〜80GHzの範囲において、最大となる反射減衰量(dB)の値、すなわち最大反射減衰量(dB)とそのときの周波数を記す。また、図1には、40〜80GHzの範囲における、試料No.4、No.10、No.22の反射減衰曲線の結果を示すグラフの例を示す。
【0024】
表1および図1に示す結果より、試料No.1〜18に用いた海面状鉄粉は、40〜80GHzのミリ波帯において、反射減衰量のピークを有し、その値は20dB以上と優れた電波吸収性能を示した。比較例として用いたアトマイズ鉄粉は、平均粒径は試料No.1〜6の海綿状鉄粉と同じではあるが、最大反射減衰量は小さなものとなり、良好な電波吸収性能が得られない。
【0025】
【表1】
【0026】
【発明の効果】
本発明の電波吸収シートは、合成樹脂に、平均粒径が10〜150μm以下、比表面積が0.05m2/g以上の海綿状鉄粉を分散混合してなることを特徴とする。海綿状鉄粉の含有量を70〜85重量%、厚さを0.05〜1.5mmとし、必要に応じ、その片面(背面となる側)に反射板として金属板や金属箔あるいは表面処理鋼板を積層した構造とすることにより、ミリ波の高周波数帯域(40〜80GHz)で、薄型でかつ減衰量20dB以上(99%以上吸収)の高い電波吸収性能を有する。
【図面の簡単な説明】
【図1】本発明の実施例と比較例におけるミリ波帯(40〜80GHz)での電波吸収性能を示すグラフ。[0001]
TECHNICAL FIELD OF THE INVENTION
The present invention relates to a sheet-like radio wave absorber (radio wave absorption sheet) obtained by dispersing and mixing spongy iron powder in a synthetic resin.
[0002]
[Prior art]
In recent years, electric and electronic devices using radio waves in the GHz band, such as mobile communication and wireless LAN, have been widely used. The expressway automatic toll collection system (ETC) uses a microwave band near 5.8 GHz, and technology development using a high frequency band such as a millimeter wave is being actively promoted as a new field. . The millimeter wave band refers to a region of 30 to 300 GHz, and particularly, a frequency in the vicinity of 60 to 80 GHz is being considered for application to an intelligent transportation system (ITS) such as inter-vehicle radar and inter-vehicle communication of an automobile. There is a need for a radio wave absorber that can efficiently absorb radio noise (unwanted radio waves).
[0003]
Radio wave absorbers absorb incident radio waves and convert radio wave energy into heat energy, etc., and should be attached to electrical and electronic devices and their surroundings where unwanted radio wave reflection, scattering, and interference occur. This suppresses various troubles. Conventionally, radio wave absorbers are generally made of kneaded ferrite powder, carbon powder, carbonyl iron powder, etc. in an insulator such as urethane foam, rubber, resin, plastic, etc. Has not progressed.
[0004]
Conventionally, a three-layer structure (for example, see Patent Literature 1), one using a coupling material (for example, Patent Literature 2), one using fiber-reinforced plastic (see Patent Literature 3), and one using carbon (See, for example, Patent Document 4), a device using an Fe—Cr alloy (see, for example, Patent Document 5), and a device using a soft magnetic metal powder (see, for example, Patent Document 6).
However, these are all expensive.
In the future, problems of radio interference such as malfunction of devices due to unnecessary radio waves will become more severe due to higher performance and higher functionality of electronic devices and communication devices, an increase in the number of devices, and an increase in the frequency band used. For this reason, a radio wave absorber that has high radio wave absorption performance in the GHz band, especially in the high frequency band of millimeter waves, and is excellent in economy is desired.
[0005]
Prior art document information relating to the invention of this application includes, for example, the following.
[Patent Document 1]
JP-A-9-51190 [Patent Document 2]
JP-A-11-45804 [Patent Document 3]
JP 2000-31685 A [Patent Document 4]
JP 2000-165087 A [Patent Document 5]
Japanese Patent Application Laid-Open No. 2000-200990 [Patent Document 6]
JP, 2002-118008, A
[Problems to be solved by the invention]
In accordance with the social situation regarding such radio waves, the present invention is excellent in the economics of a thin, high-wave-absorbing sheet-shaped sheet in the GHz band, especially in the millimeter-wave band where there is a strong demand for technical development of radio wave absorbers. It is an object to provide a radio wave absorber (a radio wave absorption sheet).
[0007]
[Means for Solving the Problems]
The present inventors have selected iron powder that is inexpensive compared to alloy powders such as ferrite in order to achieve the above-described object, and as a result of repeatedly examining prototypes with various iron powders having different particle diameters and purities, as a result, By limiting the average particle size and specific surface area of the powder, high radio wave absorption performance in the GHz band can be obtained, and the present invention has been achieved.
[0008]
The present invention is a radio wave absorbing sheet obtained by dispersing and mixing spongy iron powder in a synthetic resin. It is characterized by using spongy iron powder having an average particle size of 10 to 150 μm and a specific surface area of 0.05 m 2 / g or more. It is desirable to use a polyolefin-based, polystyrene-based, polyurethane-based or polyester-based thermoplastic elastomer as the synthetic resin. In addition, a certain amount of a polyolefin resin, a polystyrene resin, a polyurethane resin or a polyester resin may be added from the viewpoint of heat resistance and strength.
[0009]
It is desirable that the radio wave absorbing sheet of the present invention has a thickness of 0.05 to 1.5 mm in which spongy iron powder is dispersed and mixed in an amount of 70 to 85% by weight. In consideration of corrosion resistance and the like, it is also preferable to use spongy iron powder whose surface is coated with metal or resin.
[0010]
Further, in the radio wave absorbing sheet of the present invention, it is desirable that a metal plate, a metal foil, or a surface-treated steel sheet is laminated on one side (the back side) as a radio wave reflecting plate. As a result, it is possible to obtain a return loss of 20 dB or more for radio waves in the millimeter wave band of 40 to 80 GHz.
[0011]
BEST MODE FOR CARRYING OUT THE INVENTION
Hereinafter, embodiments of the present invention will be described in detail.
[0012]
In general, when the type, shape, particle size, content and the like of the powder used in the radio wave absorber are different, the radio wave absorption performance also changes accordingly. The present inventors have developed a radio wave absorption sheet having high radio wave absorption performance in a target GHz band using iron powder which is less expensive than alloy powder such as ferrite.
[0013]
The radio wave absorption sheet of the present invention is characterized in that the average particle size and the specific surface area are limited, and spongy iron powder is used. The spongy iron powder referred to here is a porous iron powder containing many pores (eg, sponge iron powder) produced by reducing an oxidized iron powder such as iron oxide with a gas or solid reducing agent. Etc.) in general. This iron powder is formed as sponge-like aggregated particles in which single particles of about several μm are connected, and is characterized by having a larger specific surface area than ordinary atomized iron powder or carbonyl iron powder. By limiting the average particle size of the spongy iron powder dispersed and mixed in the synthetic resin to 10 to 150 μm and the specific surface area to 0.05 m 2 / g or more, a radio wave absorbing sheet having high radio wave absorbing performance can be obtained.
[0014]
Next, in the radio wave absorption sheet of the present invention, spongy iron powder is dispersed and mixed in an amount of 70 to 85% by weight, and the thickness is set to a range of 0.05 to 1.5 mm. The content is practically preferable in the range of 70 to 85% by weight in consideration of workability during sheet molding, durability and flexibility of the sheet, and the like. If the added amount of spongy iron powder is too small, sufficient radio wave absorption performance cannot be obtained, and if it is too large, the particles come into contact with each other to easily reflect radio waves, resulting in reduced radio wave absorption performance and reduced economic efficiency. There is a correlation between the average particle size, specific surface area of the spongy iron powder, the content in the sheet and the sheet thickness and the radio wave absorption performance, and by appropriately controlling these, excellent radio waves that meet the target frequency and application It is possible to obtain absorption performance. The content of spongy iron powder in the sheet and the sheet thickness are mainly selected according to the target frequency and the amount of radio wave absorption.
[0015]
Here, for applications requiring corrosion resistance or the like, the surface of the spongy iron powder to be used is coated with a metal or resin. In the case of metal coating, it is preferable to perform electric Ni plating or electroless Ni-P plating on the surface of spongy iron powder. In the case of resin coating, the surface of spongy iron powder is preferably coated with a resin such as polyethylene, polyester, nylon, epoxy, or fluorine.
[0016]
Next, regarding the synthetic resin used in the present invention, a polyolefin-based thermoplastic elastomer such as a polyethylene-butene copolymer elastomer and a polypropylene-polyethylene copolymer elastomer having excellent flexibility, chemical resistance, heat resistance, and stability over time, etc. Polystyrene-based thermoplastic elastomers such as polystyrene-butadiene copolymer elastomers, polyurethane-based thermoplastic elastomers, and polyester-based thermoplastic elastomers such as polybutylene terephthalate-polybutadiol copolymer elastomers are suitable. By using these thermoplastic elastomers, they have flexibility even after 70-85% spongy iron powder is dispersed and mixed.
[0017]
Further, the radio wave absorbing sheet of the present invention may be used as a radio wave reflecting plate, a surface-treated steel sheet having one surface (a back surface side) plated with zinc, zinc-nickel alloy, zinc-cobalt-molybdenum, nickel, or the like; It is desirable to laminate a known metal plate such as a steel plate, a copper plate, a stainless plate, and aluminum. Further, a known metal foil such as an electrolytic iron foil, a nickel foil, a copper foil, and a stainless steel foil which has been subjected to a known surface treatment such as zinc plating, nickel plating, tin plating, or electrolytic chromic acid treatment may be laminated. As a result, the radio wave absorption performance is improved, and the reflection attenuation for radio waves in the millimeter wave band of 40 to 80 GHz can be stably maintained at an excellent level of 20 dB or more, and also has a role of supporting the sheet. be able to.
[0018]
【Example】
Several kinds of sea-like iron powders having different average particle sizes and specific surface areas were used. Here, the specific surface area of the powder used was determined by a gas phase adsorption method (BET method) which is a method of calculating the surface area from the number of molecules adsorbed on the solid surface, and an average value obtained by three measurements was used. As the thermoplastic resin (synthetic resin) of Sample Nos. 1 to 22, a polypropylene-polyethylene copolymer elastomer, which is a polyolefin-based elastomer, was used because of easiness of kneading. These iron powders and synthetic resin were mixed at a predetermined ratio, and after forming the sol, a radio wave absorbing sheet having a thickness of 0.05 to 1.5 mm and 150 mm × 150 mm was produced by a roll kneader. Then, an iron foil having a thickness of 30 μm was adhered to one surface of these sheets as a radio wave reflection plate, and used for evaluation.
[0019]
[Sample No. 1-6)
As shown in Table 1, as an example, sea-surface iron powder having an average particle size of 100 μm, a specific surface area of 0.072 m 2 / g, and a bulk density of 1.72 g / cm 3 was used. Sample No. 1 in Table 1. 1 to 6 show measurement results when the content of sea-surface iron powder is 70, 80, and 85% by weight.
[0020]
[Sample No. 7-12]
As shown in Table 1, as an example, a sea-surface iron powder having an average particle size of 45 μm, a specific surface area of 0.085 m 2 / g, and a bulk density of 2.97 g / cm 3 was used. Sample No. 1 in Table 1. 7 to 12 show measurement results when the content of sea-surface iron powder is 70, 80, and 85% by weight.
[0021]
[Sample No. 13-18)
As shown in Table 1, as an example, sea-surface iron powder having an average particle size of 75 μm, a specific surface area of 0.272 m 2 / g, and a bulk density of 1.94 g / cm 3 was used. Sample No. 1 in Table 1. 13 to 18 show the measurement results when the content of the sea-surface iron powder is 70, 80, and 85% by weight.
[0022]
(Comparative example)
As shown in Table 1, a spherical atomized iron powder produced by an atomizing method in powder metallurgy was used in Comparative Examples. Atomized iron powder having an average particle size of 100 μm, a specific surface area of 0.043 m 2 / g, and a bulk density of 3.21 g / cm 3 was used. Sample No. 1 in Table 1. 19 to 22 show the measurement results when the content of the atomized iron powder was 70 or 80% by weight as a comparative example.
[0023]
(Method of measuring radio wave absorption performance)
Regarding the radio wave absorption performance of the above samples, the measurement range was set to the millimeter wave band, and the return loss (dB) at each frequency was measured using a network analyzer. Table 1 shows the value of the maximum return loss (dB) in the range of 40 to 80 GHz, that is, the maximum return loss (dB) and the frequency at that time. FIG. 1 shows the sample No. in the range of 40 to 80 GHz. 4, no. 10, no. 22 shows an example of a graph showing the results of the 22 return loss curves.
[0024]
From the results shown in Table 1 and FIG. The sea-surface iron powder used in Nos. 1 to 18 had a peak of the return loss in the millimeter wave band of 40 to 80 GHz, and the value showed an excellent radio wave absorption performance of 20 dB or more. The atomized iron powder used as a comparative example has an average particle size of Sample No. Although the same as the spongy iron powders Nos. 1 to 6, the maximum return loss is small, and good radio wave absorption performance cannot be obtained.
[0025]
[Table 1]
[0026]
【The invention's effect】
The radio wave absorbing sheet of the present invention is characterized in that a spongy iron powder having an average particle size of 10 to 150 μm or less and a specific surface area of 0.05 m 2 / g or more is dispersed and mixed in a synthetic resin. The content of spongy iron powder is 70 to 85% by weight, the thickness is 0.05 to 1.5 mm, and if necessary, a metal plate, a metal foil or a surface treatment is provided on one side (the back side) as a reflection plate. By having a structure in which steel sheets are laminated, the thin film has high electromagnetic wave absorption performance with an attenuation of 20 dB or more (absorbs 99% or more) in a high frequency band of millimeter waves (40 to 80 GHz).
[Brief description of the drawings]
FIG. 1 is a graph showing radio wave absorption performance in a millimeter wave band (40 to 80 GHz) in an example of the present invention and a comparative example.
Claims (6)
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
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| JP2002343706A JP2004179385A (en) | 2002-11-27 | 2002-11-27 | Radio wave absorbing sheet |
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| JP2002343706A JP2004179385A (en) | 2002-11-27 | 2002-11-27 | Radio wave absorbing sheet |
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| JP2004179385A true JP2004179385A (en) | 2004-06-24 |
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Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| WO2008029861A1 (en) | 2006-09-01 | 2008-03-13 | The University Of Tokyo | Magnetic crystal for radio wave absorbing material and radio wave absorbent |
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2002
- 2002-11-27 JP JP2002343706A patent/JP2004179385A/en active Pending
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| WO2008029861A1 (en) | 2006-09-01 | 2008-03-13 | The University Of Tokyo | Magnetic crystal for radio wave absorbing material and radio wave absorbent |
| US8072365B2 (en) | 2006-09-01 | 2011-12-06 | The University Of Tokyo | Magnetic crystal for electromagnetic wave absorbing material and electromagnetic wave absorber |
| EP2410832A2 (en) | 2006-09-01 | 2012-01-25 | The University of Tokyo | Magnetic crystal for electromagnetic wave absorbing material and electromagnetic wave absorber |
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