JPH04275403A - Complex sintered material for electromagnetic wave absorption - Google Patents

Complex sintered material for electromagnetic wave absorption

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Publication number
JPH04275403A
JPH04275403A JP3061007A JP6100791A JPH04275403A JP H04275403 A JPH04275403 A JP H04275403A JP 3061007 A JP3061007 A JP 3061007A JP 6100791 A JP6100791 A JP 6100791A JP H04275403 A JPH04275403 A JP H04275403A
Authority
JP
Japan
Prior art keywords
electromagnetic wave
ferrite
sintered material
frequency band
composite sintered
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
JP3061007A
Other languages
Japanese (ja)
Inventor
Hiroyoshi Ishii
石井博義
Yukio Toda
戸田幸生
Hiroshi Kawamoto
河本博
Toshikatsu Hayashi
林利勝
Kenzo Suzuki
鈴木賢造
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.)
Riken Corp
Original Assignee
Riken 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 Riken Corp filed Critical Riken Corp
Priority to JP3061007A priority Critical patent/JPH04275403A/en
Publication of JPH04275403A publication Critical patent/JPH04275403A/en
Pending legal-status Critical Current

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  • Hard Magnetic Materials (AREA)
  • Soft Magnetic Materials (AREA)
  • Shielding Devices Or Components To Electric Or Magnetic Fields (AREA)

Abstract

PURPOSE:To obtain a ferrite complex sintering material which has electromagnetic wave absorbing properies excellent in a wide frequency band, especially, in the TV frequency band. CONSTITUTION:The complex sintering material is constituted as complex ceramics where conductive particles having the shape that the electric resistivity is 1X10-2-10OMEGA.cm and that the anti-electric-field coefficient becomes 0.2 or below are mixed 5-30% by volume ratio in the oxide magnetic substances of ferrite and are sintered.

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、高周波帯域での電磁波
吸収材として使用される複合焼結材に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a composite sintered material used as an electromagnetic wave absorbing material in a high frequency band.

【0002】0002

【従来の技術】高周波帯域での電磁波吸収材として、フ
ェライト系の磁性体、例えばNi−Zn系フェライトや
、Mn−Zn系フェライト磁性体等が実用され、あるい
は提案されている。これらのフェライト系磁性体はいず
れもフェリ磁性の非金属系磁性材料で、セラミックス焼
結体として、多くはタイル状で使用されている。
2. Description of the Related Art Ferrite-based magnetic materials, such as Ni--Zn ferrite and Mn--Zn ferrite magnetic materials, have been put into practice or proposed as electromagnetic wave absorbing materials in high frequency bands. All of these ferrite-based magnetic materials are ferrimagnetic non-metallic magnetic materials, and are used as ceramic sintered bodies, often in the form of tiles.

【0003】これらの焼結体の電磁波吸収効果は、いず
れもフェライトの磁気損失を利用するものであるが、充
分な吸収特性を有するものとは云えない。そこで、吸収
特性を向上させるため、金属反射層をタイルに裏張りし
たり、入射波と反射波の干渉を利用する等の手段を併用
することが試みられている。しかし、吸収特性に誘電損
失を利用していないので、有効な周波数帯域が限定され
、かつ、吸収特性も充分とは云えない。
The electromagnetic wave absorption effect of these sintered bodies utilizes the magnetic loss of ferrite, but it cannot be said that they have sufficient absorption characteristics. Therefore, in order to improve the absorption characteristics, attempts have been made to use a combination of measures such as lining the tiles with a metal reflective layer and utilizing interference between incident waves and reflected waves. However, since dielectric loss is not utilized for absorption characteristics, the effective frequency band is limited, and the absorption characteristics cannot be said to be sufficient.

【0004】又、電磁波吸収材としては、ゴムにフェラ
イト粉末、あるいはフェライトとカーボンの粉末を混合
した複合材料も実用、あるいは提案されているが、TV
帯域(約100MHz/1,000MHz帯域)での吸
収特性は全く不充分で、一部レーダー対策用として橋梁
等に実用化されているのみで、広帯域の周波数には対応
できない。
[0004] Also, as electromagnetic wave absorbing materials, composite materials made by mixing rubber with ferrite powder or ferrite and carbon powder have been put into practical use or have been proposed.
The absorption characteristics in the band (approximately 100 MHz/1,000 MHz band) are completely inadequate, and it has only been put to practical use in bridges and the like as part of radar countermeasures, and is not compatible with a wide band of frequencies.

【0005】[0005]

【発明が解決しようとする課題】本発明は、従来実用さ
れ、あるいは提案されているフェライト系の電磁波吸収
用焼結体の上記の実情にかんがみ、広帯域の周波数帯域
、特にTV周波数帯域で、優れた電磁波吸収特性を示す
フェライト系複合焼結材を提供することを課題とする。
Problems to be Solved by the Invention In view of the above-mentioned circumstances of the ferrite-based electromagnetic wave absorbing sintered bodies that have been put into practical use or have been proposed, the present invention has been made to provide excellent performance in a wide frequency band, particularly in the TV frequency band. An object of the present invention is to provide a ferrite-based composite sintered material that exhibits electromagnetic wave absorption characteristics.

【0006】[0006]

【課題を解決するための手段】本発明の複合焼結材は、
上記の課題を解決させるため、フェライトの酸化物磁性
体に、電気抵抗率が1×10−2Ω・cm〜10Ω・c
mで、かつ、反電界係数が0.02以下になる形状を有
する導電体粒子を、容積比で5%〜30%混合し焼結し
た複合セラミックとして成ることを特徴とする。
[Means for solving the problems] The composite sintered material of the present invention is
In order to solve the above problems, we developed a ferrite oxide magnetic material with an electrical resistivity of 1 x 10-2 Ω・cm to 10 Ω・c.
The present invention is characterized in that it is made into a composite ceramic in which 5% to 30% by volume of conductive particles having a shape with a diameter of m and an anti-electric field coefficient of 0.02 or less are mixed and sintered.

【0007】上記の導電体粒子としては、SiC又はS
iCウィスカーが利用可能である。
[0007] As the above-mentioned conductor particles, SiC or S
iC whiskers are available.

【0008】[0008]

【作用】一般に、物質の高周波域における電磁波吸収特
性は、その物質の基礎特性である複合透磁率μ* =μ
′−jμ″や、損失角tanδ=μ″/μ′、並びに複
素誘電率ε* =ε′−jε″や、その損失角tanδ
=ε″/ε′で表わされることはよく知られている。前
者の複素透磁率は磁気損失に、後者の複素誘電率は誘電
損失と直接関係し、吸収特性を決定する。
[Operation] Generally, the electromagnetic wave absorption characteristics of a material in the high frequency range are determined by the composite magnetic permeability μ* = μ, which is the basic property of the material.
'-jμ'', loss angle tanδ=μ''/μ', complex permittivity ε* =ε'-jε'', and its loss angle tanδ
It is well known that the complex magnetic permeability of the former is directly related to the magnetic loss, and the complex dielectric constant of the latter is directly related to the dielectric loss, and determines the absorption characteristics.

【0009】在来のフェライトを用いた吸収体用焼結材
は、目的とするTV周波数帯域での磁気損失が大きい材
料で、特に磁気損失を示すμ″(又はtanδ)の値が
大きい材料が使用されているが、本発明の複合焼結体で
は、フェライトが有する優れた磁気損失に加えて、非金
属導電体が絶縁体中に存在することにより生ずる誘電損
失が加わり、吸収特性が向上する。又、フェライトの粉
末とカーボン粉末や短繊維をゴム等で固めた複合材に比
して、本発明の複合焼結材は、フェライトを焼結してセ
ラミックとしたので、磁気損失も大きくなり、この点か
らも吸収特性は改善される。
[0009] Conventional sintered materials for absorbers using ferrite are materials that have a large magnetic loss in the target TV frequency band, and in particular, materials that have a large value of μ'' (or tan δ), which indicates magnetic loss. However, in the composite sintered body of the present invention, in addition to the excellent magnetic loss possessed by ferrite, dielectric loss caused by the presence of a nonmetallic conductor in the insulator is added, and the absorption properties are improved. In addition, compared to composite materials made by hardening ferrite powder, carbon powder, or short fibers with rubber, etc., the composite sintered material of the present invention has a larger magnetic loss because the ferrite is sintered to form a ceramic. , the absorption characteristics are improved from this point as well.

【0010】本発明者の多くの実験を含む研究によれば
、上記のμ′、μ″は、電磁波の周波数を定めれば、導
電体粒子の容積比率V、電気抵抗率R並びに導電体粒子
の長軸/短軸比kにより定まる反電界係数Nに依存する
。換言すれば、複合焼結材構成に際して、これらの値を
制御することにより、μ′、μ″の値を定めることがで
きる。
According to research including many experiments conducted by the present inventor, the above μ' and μ'' can be determined by determining the frequency of electromagnetic waves, the volume ratio V of the conductor particles, the electrical resistivity R, and the conductor particles. It depends on the anti-electric field coefficient N, which is determined by the major axis/minor axis ratio k of .

【0011】多数の実験結果によれば、導電体粒子の電
気抵抗率は、10−2Ω・cm以下では所望のμ″やt
anδが得られず、望ましい磁気損失が得られず、又、
10Ω・cm以上になると、導電性材料としての特長が
失なわれるので好ましくない。したがって、電気抵抗率
Rの望ましい範囲は1×10−2Ω・cm〜10Ω・c
mである。 又、導電体粒子の混合比は容積比で5〜30%が適当で
ある。又、反電界係数Nは0.2以下であることが望ま
しい。なお、代表的な粒子形状の寸法比と反電界係数の
値を表1に示す。
According to a large number of experimental results, when the electrical resistivity of conductive particles is 10-2 Ω·cm or less, the desired μ″ and t
anδ cannot be obtained, desired magnetic loss cannot be obtained, and
If it exceeds 10 Ω·cm, it is not preferable because it loses its characteristics as a conductive material. Therefore, the desirable range of electrical resistivity R is 1×10-2 Ω・cm to 10 Ω・c
It is m. Further, the appropriate mixing ratio of the conductor particles is 5 to 30% by volume. Further, it is desirable that the anti-electric field coefficient N is 0.2 or less. Note that Table 1 shows the size ratio of typical particle shapes and the values of anti-electric field coefficients.

【0012】0012

【表1】[Table 1]

【0013】Nの値が0.2以下となるようなKは、表
1より、長軸l1 と短軸l2 の比l1 /l2 が
略々5以上であればよい。
According to Table 1, K such that the value of N is 0.2 or less is determined as long as the ratio l1 /l2 of the major axis l1 to the minor axis l2 is approximately 5 or more.

【0014】以上のことより、望ましい導体の材料とし
ては、電気抵抗率Rが2×10−1Ω・cmのSiCの
短繊維やウィスカーが最も適している。SiCの塊状の
粒子は電気抵抗率は満足するが、Nの値の点で不適であ
る。 又、カーボンの粉末や短繊維は電気抵抗率がほぼ10−
3Ω・cmであり、好ましい結果は得られなかった。
From the above, the most suitable conductor material is SiC short fibers or whiskers having an electrical resistivity R of 2×10 −1 Ω·cm. Although bulk particles of SiC satisfy the electrical resistivity, they are unsuitable in terms of the N value. Also, carbon powder and short fibers have an electrical resistivity of approximately 10-
3Ω·cm, and no favorable results were obtained.

【0015】[0015]

【実施例】以下に、本発明の実施例としての電磁波吸収
用複合焼結材を、現用されている電磁波吸収材と比較し
て、その特性を表2及び表4に示す。
[Example] Below, a composite sintered material for absorbing electromagnetic waves as an example of the present invention will be compared with a currently used electromagnetic wave absorbing material, and its properties will be shown in Tables 2 and 4.

【0016】表2は、Ni−Zn系フェライトに各種導
電体粒子を容積比で15%混合して焼結した複合焼結材
の電磁波吸収特性を、周波数200MHzについて示す
表である。
Table 2 shows the electromagnetic wave absorption characteristics of a composite sintered material obtained by mixing Ni--Zn ferrite with various conductive particles at a volume ratio of 15% at a frequency of 200 MHz.

【0017】[0017]

【表2】[Table 2]

【0018】表2中の各種導電性粒子の寸法形状、Nの
値、電気抵抗率は表3のとおりである。
The dimensions, shapes, N values, and electrical resistivities of the various conductive particles in Table 2 are as shown in Table 3.

【0019】[0019]

【表3】[Table 3]

【0020】又、表4に、種々の組成のNi−Zn系フ
ェライトに導電体粒子としてSiCウィスカーを容積比
で10%混合した複合焼結材の電磁波吸収特性を周波数
200MHzについての値を示す。なお、混合するSi
Cウィスカーの寸法形状、Nの値、電気抵抗率は表3と
同じである。表2の2、3及び4欄、表4の5及び6欄
の電磁波吸収材は比較材である。又、電磁波吸収層の厚
さ(skin  depth  S)は、電磁波強度が
l/eに減衰するための吸収層の厚みで表わされている
Table 4 also shows the electromagnetic wave absorption characteristics at a frequency of 200 MHz of composite sintered materials prepared by mixing Ni--Zn ferrite of various compositions with SiC whiskers as conductive particles at a volume ratio of 10%. In addition, Si to be mixed
The dimensions, shape, N value, and electrical resistivity of the C whiskers are the same as in Table 3. The electromagnetic wave absorbing materials in columns 2, 3 and 4 of Table 2 and columns 5 and 6 of Table 4 are comparative materials. Further, the thickness of the electromagnetic wave absorption layer (skin depth S) is expressed as the thickness of the absorption layer for attenuating the electromagnetic wave intensity to 1/e.

【0021】[0021]

【表4】[Table 4]

【0022】表2及び表4より見られる如く、本発明材
は比較材に比して電磁波の反射率が小さく、吸収層の厚
みも小さくなる。
As seen from Tables 2 and 4, the material of the present invention has a lower electromagnetic wave reflectance and a smaller thickness of the absorption layer than the comparative material.

【0023】[0023]

【効果】以上の如く、本発明によれば、広帯域の周波数
帯域、特にTV周波数帯域で、優れた吸収特性を有し、
吸収層の厚みを小さくすることのできるフェライト系複
合焼結材を得ることができる。
[Effects] As described above, the present invention has excellent absorption characteristics in a wide frequency band, especially in the TV frequency band,
A ferritic composite sintered material that can reduce the thickness of the absorption layer can be obtained.

Claims (3)

【特許請求の範囲】[Claims] 【請求項1】  高周波帯域での電磁波吸収材として使
用される複合焼結材において、フェライトの酸化物磁性
体に、電気抵抗率が1×10−2Ω・cm〜10Ω・c
mで、かつ、反電界係数が0.02以下になる形状の導
電体粒子を、容積比で5%〜30%混合し、焼結した複
合セラミックとして成ることを特徴とする複合焼結材。
Claim 1: In a composite sintered material used as an electromagnetic wave absorbing material in a high frequency band, the ferrite oxide magnetic material has an electrical resistivity of 1 x 10-2 Ω·cm to 10 Ω·c.
1. A composite sintered material, characterized in that it is made of a composite ceramic obtained by mixing 5% to 30% by volume of conductive particles having a shape of m and an anti-electric field coefficient of 0.02 or less and sintering the mixture.
【請求項2】  上記の導電体粒子がSiCであること
を特徴とする請求項1に記載の複合焼結材。
2. The composite sintered material according to claim 1, wherein the conductor particles are SiC.
【請求項3】  上記の導電体粒子がSiCウィスカー
であることを特徴とする請求項1に記載の複合焼結材。
3. The composite sintered material according to claim 1, wherein the conductor particles are SiC whiskers.
JP3061007A 1991-03-04 1991-03-04 Complex sintered material for electromagnetic wave absorption Pending JPH04275403A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP3061007A JPH04275403A (en) 1991-03-04 1991-03-04 Complex sintered material for electromagnetic wave absorption

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP3061007A JPH04275403A (en) 1991-03-04 1991-03-04 Complex sintered material for electromagnetic wave absorption

Publications (1)

Publication Number Publication Date
JPH04275403A true JPH04275403A (en) 1992-10-01

Family

ID=13158855

Family Applications (1)

Application Number Title Priority Date Filing Date
JP3061007A Pending JPH04275403A (en) 1991-03-04 1991-03-04 Complex sintered material for electromagnetic wave absorption

Country Status (1)

Country Link
JP (1) JPH04275403A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US8138959B2 (en) * 2006-10-19 2012-03-20 Hitachi Metals, Ltd. Radio wave absorption material and radio wave absorber

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US8138959B2 (en) * 2006-10-19 2012-03-20 Hitachi Metals, Ltd. Radio wave absorption material and radio wave absorber

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