JPS6242498A - Radio wave absorbing body - Google Patents

Radio wave absorbing body

Info

Publication number
JPS6242498A
JPS6242498A JP18235185A JP18235185A JPS6242498A JP S6242498 A JPS6242498 A JP S6242498A JP 18235185 A JP18235185 A JP 18235185A JP 18235185 A JP18235185 A JP 18235185A JP S6242498 A JPS6242498 A JP S6242498A
Authority
JP
Japan
Prior art keywords
radio wave
molded body
ferrite
pyramid
frequency band
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
JP18235185A
Other languages
Japanese (ja)
Inventor
賢一 畠山
高志 原田
乾 哲司
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.)
NEC Corp
Original Assignee
NEC 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 NEC Corp filed Critical NEC Corp
Priority to JP18235185A priority Critical patent/JPS6242498A/en
Publication of JPS6242498A publication Critical patent/JPS6242498A/en
Pending legal-status Critical Current

Links

Abstract

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は電磁波の不要な反射、散乱を抑制するための電
波吸収体に関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a radio wave absorber for suppressing unnecessary reflection and scattering of electromagnetic waves.

〔従来の技術〕[Conventional technology]

主として電波暗室等の屋内で使用される電波吸収体にお
いて、電波吸収特性として周波数帯域の広いことが要求
される場合には、電波吸収体の形態として第4図に示す
様にピラミッド形、或いは模形に成形加工したものが良
く用いられる。
When a radio wave absorber used indoors, such as an anechoic chamber, is required to have a wide frequency band as its radio wave absorption characteristics, the shape of the radio wave absorber may be pyramid-shaped or patterned as shown in Figure 4. It is often used after being molded into a shape.

従来より電波吸収棒金構成する吸収材料には、カーlン
、グラファイト、或いは全品粉末等を混合して誘電損失
を増加させた発泡樹脂、又は、磁性損失の大きいフェラ
イトが用いられていた。
Conventionally, the absorbing material constituting the radio wave absorbing bar has been a foamed resin mixed with carbon, graphite, whole powder, etc. to increase dielectric loss, or ferrite with large magnetic loss.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

ところが、発泡樹脂に訪邂損失材を混合し九電波吸収体
では、機械的強度が弱く又、低周波帯になるほど、ピラ
ミッドを大形化しなければならない。一方、フェライト
ttJ1.吸収体によれば、低周波帯で大きな磁気的損
失を利用できるので比較的小形のピラミッドでよいが高
価であり、又、硬度は大きいが脆いという欠点がある。
However, the nine radio wave absorbers made of a foamed resin mixed with a visiting loss material have weak mechanical strength, and the pyramid must be made larger as the frequency band becomes lower. On the other hand, ferrite ttJ1. According to the absorber, since a large magnetic loss can be utilized in a low frequency band, a relatively small pyramid can be used, but it is expensive, and although it has high hardness, it has the disadvantage of being brittle.

本発明の目的は、を波吸収特性に優れ、しかも邦集材と
して使用できる様な強度を有する電波吸収体を提供する
ことにある。
An object of the present invention is to provide a radio wave absorber that has excellent wave absorption properties and is strong enough to be used as a Japanese timber.

〔問題点、を解決するための手段〕[Means to solve the problem]

本発明にコンクリート、モルタルなどの基材中にカー?
ン、グラファイト、金属粉末等のg E 損失材を混入
してピラミッド状又は種形状に成形した成形体において
、該成形体の組織の一部をフェライト等の磁性損失、(
イ゛にて置き替え九ことを特徴とする電波吸収体である
The present invention does not contain cartilage in base materials such as concrete and mortar.
In a molded body formed into a pyramid shape or seed shape by mixing G E loss material such as carbon, graphite, metal powder, etc., a part of the structure of the molded body is mixed with magnetic loss material such as ferrite, etc.
This is a radio wave absorber characterized by being replaced with (9).

〔実施例〕〔Example〕

以下に本発明の実施例を図によって説明する。 Embodiments of the present invention will be described below with reference to the drawings.

一般に建築材として用いられているコンクIJ−ト材モ
ルタル、その他の基材にカーゲン、グラファイト、或い
は金属粉末等を混合して誘電損失を太きくし、これをピ
ラミッド状、又は楔形状の成形体に成形する。これを第
4図に示した様に空間的に配置した面は、電波吸収壁と
して働らき、かつ、機械的強度も強く、建築用壁材とし
て用いることができる。但し、誘電損失のみを利用した
吸収材では低周波帯になるほど大形化する必要がある。
Concrete IJ mortar, which is generally used as a construction material, and other base materials are mixed with cargen, graphite, metal powder, etc. to increase dielectric loss, and this is made into a pyramid-shaped or wedge-shaped molded body. Shape. The surface where these are spatially arranged as shown in FIG. 4 functions as a radio wave absorbing wall and has strong mechanical strength, so that it can be used as a wall material for construction. However, an absorber using only dielectric loss needs to be made larger as the frequency band becomes lower.

発泡樹脂を母材として実用化されているものでは、例え
ば30FvlHz用ではピラミッドの高さは2m以上に
も達する。本発明では低周波帯での大形化を避けるため
、上記のピラミッド形、或い#−1t楔形に成形した成
形体1の組織の一部を第1図。
In the case where the base material is made of foamed resin and has been put into practical use, for example, the height of the pyramid reaches 2 m or more in the case of 30 FvlHz. In the present invention, in order to avoid increasing the size in the low frequency band, FIG. 1 shows a part of the structure of the molded body 1, which is molded into the above pyramid shape or #-1t wedge shape.

第2図、第3図に示すように低周波帯で磁気損失の大き
いフェライト成形体2にて置き替えたものである。
As shown in FIGS. 2 and 3, the ferrite molded body 2 has been replaced with a ferrite molded body 2 which has a large magnetic loss in the low frequency band.

この様な構成にすると、低周波帯ではフェライトの磁気
損失が効率良く働らいてコンクリート材の大きさを縮少
することができる。
With such a configuration, the magnetic loss of the ferrite works efficiently in the low frequency band, and the size of the concrete material can be reduced.

ピラミッド状、あるいVi、PA形状成形体を用いた誘
電損失材が艮好な電波吸収特性を得られるのは。
The dielectric loss material using a pyramid-shaped, Vi, or PA-shaped molded body can obtain excellent radio wave absorption characteristics.

電磁波が入射するにつれてピラミッド状、或いは楔形状
の損失材の空間に占める体積率が徐々に変化するため、
空間的なインピーダンスの変化がゆるやかであることに
起因する。第1図に示す様に♂ラミラド型底形体1の低
面側の組織の一部を同形のフェライト成形体2で置き替
えた構造では、コンクリート材からフェライトに電磁波
が入射する場合にも、インピーダンスの変化はゆるやか
である。又、高周波帯ではフェライトの磁気的損失が小
さくなって、コンクリート材と同等の誘電率全有する誘
電体の性質2有する。従って、高周波帯では通常の誘電
損失を用いたピラミッド状の電波吸収体と等価である。
As the electromagnetic waves are incident, the volume ratio of the pyramid-shaped or wedge-shaped lossy material in the space gradually changes.
This is due to the gradual change in spatial impedance. As shown in Fig. 1, in a structure in which a part of the structure on the lower surface side of the female Lamirado bottom body 1 is replaced with a ferrite molded body 2 of the same shape, even when electromagnetic waves are incident on the ferrite from the concrete material, the impedance changes are gradual. In addition, in the high frequency band, the magnetic loss of ferrite becomes small, and it has properties 2 of a dielectric material having a dielectric constant equivalent to that of concrete material. Therefore, in the high frequency band, it is equivalent to a pyramid-shaped radio wave absorber using normal dielectric loss.

低周波帯ではフェライトの有する磁気損失が効果的に作
用し、良好な電波吸収特性が得られる。
In the low frequency band, the magnetic loss of ferrite acts effectively and good radio wave absorption characteristics can be obtained.

コンクリート成形体へのフェライトの挿入による他の実
施例第2図、第3図に示す。第3図は円柱又は角柱状の
フェライト成形体2をコンクリート成形体1に挿入した
場合である。この構成では、フェライト成形体2の断面
積を調整して、電磁波Wが入射する面での等価的な銹を
率と透磁率とを等しくして、表面反射の成分を小さくす
ることが必要となる。従って、フェライトの透磁率をμ
とし、入射面の面積6s、フェライト成形体の断面調整
する。但し、1はフェライト、およびコンクリートの誘
電率である。この構成に於ても、フェライトは低周波帯
の電波吸収特性を改良する効果金与える。
Another embodiment in which ferrite is inserted into a concrete molded body is shown in FIGS. 2 and 3. FIG. 3 shows a case where a cylindrical or prismatic ferrite molded body 2 is inserted into a concrete molded body 1. In this configuration, it is necessary to adjust the cross-sectional area of the ferrite molded body 2 to equalize the equivalent rust rate and magnetic permeability on the surface where the electromagnetic wave W is incident, and to reduce the surface reflection component. Become. Therefore, the magnetic permeability of ferrite is μ
The area of the incident surface is 6s, and the cross section of the ferrite molded body is adjusted. However, 1 is the dielectric constant of ferrite and concrete. Even in this configuration, ferrite has the effect of improving the radio wave absorption characteristics in the low frequency band.

第3図はフェライト成形体2をピラミッド形としてこれ
をコンクリート成形体1の頂部に逆向きの方向に挿入し
た構成である。この場合も第3図に述べた如く、電磁波
の入射面で等価的な誘電率と透磁率が等しくなるように
、ΔSとSを調整する。
FIG. 3 shows a configuration in which the ferrite molded body 2 is pyramid-shaped and inserted into the top of the concrete molded body 1 in the opposite direction. In this case as well, as described in FIG. 3, ΔS and S are adjusted so that the equivalent permittivity and magnetic permeability are equal on the plane of incidence of electromagnetic waves.

フェライト成形体の形状挿入方法の設定は実際の使用に
応じて自由に選定すればよい。
The method for inserting the shape of the ferrite molded body may be freely selected depending on the actual use.

〔発明の効果〕〔Effect of the invention〕

本発明によれば、本電波吸収体の体積の殆んどをコンク
リート材が占めるので機械的強度が大きく、建築材とし
て使用でき、しかもその組織の一部をフェライトにて置
き替えたために、低周波帯の吸収特性を改善できる効果
2有するものである。
According to the present invention, since the concrete material occupies most of the volume of the radio wave absorber, it has high mechanical strength and can be used as a building material.Moreover, since a part of the structure is replaced with ferrite, it has a low It has the effect 2 of improving the absorption characteristics of the frequency band.

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

第1図は本発明の一実施例を示す断面図、第2図、第3
図はそれぞれ他の実施例を示す断面図、第4図は電波吸
収体の基本型を示す断面図である。 1・・・誘電損失材を含む成形体、2・・・フェライト
成形体 W・・・電磁波、S・・・成形体への電磁波の
入射面積、ΔS・・・フェライト成形体の断面積。
Figure 1 is a sectional view showing one embodiment of the present invention, Figures 2 and 3 are
The figures are sectional views showing other embodiments, and FIG. 4 is a sectional view showing a basic type of radio wave absorber. 1... Molded body containing dielectric loss material, 2... Ferrite molded body W... Electromagnetic wave, S... Area of incidence of electromagnetic waves on the molded body, ΔS... Cross-sectional area of ferrite molded body.

Claims (1)

【特許請求の範囲】[Claims] (1)コンクリート、モルタルなどの基材中にカーボン
、グラファイト、金属粉末等の誘電損失材を混入してピ
ラミッド状又は楔形状に成形した成形体において、該成
形体の組織の一部をフェライト等の磁性損失材にて置き
替えたことを特徴とする電波吸収体。
(1) In a molded body formed into a pyramid or wedge shape by mixing a dielectric loss material such as carbon, graphite, or metal powder into a base material such as concrete or mortar, a part of the structure of the molded body may be ferrite, etc. A radio wave absorber characterized by replacing the magnetic loss material with a magnetic loss material.
JP18235185A 1985-08-19 1985-08-19 Radio wave absorbing body Pending JPS6242498A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP18235185A JPS6242498A (en) 1985-08-19 1985-08-19 Radio wave absorbing body

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP18235185A JPS6242498A (en) 1985-08-19 1985-08-19 Radio wave absorbing body

Publications (1)

Publication Number Publication Date
JPS6242498A true JPS6242498A (en) 1987-02-24

Family

ID=16116791

Family Applications (1)

Application Number Title Priority Date Filing Date
JP18235185A Pending JPS6242498A (en) 1985-08-19 1985-08-19 Radio wave absorbing body

Country Status (1)

Country Link
JP (1) JPS6242498A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6467997A (en) * 1987-09-08 1989-03-14 Yasutaka Shimizu Radio wave absorber containing ferrite
EP0689262A1 (en) 1994-06-23 1995-12-27 Takenaka Corporation Wave absorber composition, radio wave absorber member, radio wave absorber and method for producing wave absorber member

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6467997A (en) * 1987-09-08 1989-03-14 Yasutaka Shimizu Radio wave absorber containing ferrite
EP0689262A1 (en) 1994-06-23 1995-12-27 Takenaka Corporation Wave absorber composition, radio wave absorber member, radio wave absorber and method for producing wave absorber member

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