JPH05183331A - Radio wave absorbing wall for tv frequency band - Google Patents

Radio wave absorbing wall for tv frequency band

Info

Publication number
JPH05183331A
JPH05183331A JP3288024A JP28802491A JPH05183331A JP H05183331 A JPH05183331 A JP H05183331A JP 3288024 A JP3288024 A JP 3288024A JP 28802491 A JP28802491 A JP 28802491A JP H05183331 A JPH05183331 A JP H05183331A
Authority
JP
Japan
Prior art keywords
cement
radio wave
wall
thickness
field direction
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.)
Withdrawn
Application number
JP3288024A
Other languages
Japanese (ja)
Inventor
Takeshi Yamamoto
毅 山本
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.)
Taisei Corp
DIC Corp
Nippon Steel Corp
Showa Kogyo KK
Original Assignee
Taisei Corp
Nippon Steel Corp
Dainippon Ink and Chemicals Co Ltd
Showa Kogyo KK
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 Taisei Corp, Nippon Steel Corp, Dainippon Ink and Chemicals Co Ltd, Showa Kogyo KK filed Critical Taisei Corp
Priority to JP3288024A priority Critical patent/JPH05183331A/en
Publication of JPH05183331A publication Critical patent/JPH05183331A/en
Withdrawn legal-status Critical Current

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

Abstract

PURPOSE:To facilitate the installation and to absorb a radio wave over a wide TV frequency band by forming the wall with cement and magnetic particles, providing a specific shape and selecting the length of the wall in the magnetic field direction of the TV radio wave to be a required absorbing wavelength or over. CONSTITUTION:A groove 12 whose depth is (d2-d1) is provided to the wall in the electric field direction of a TV radio wave, a thickness d1 of a recessed part of a forming and a thickness d2 of a projection of a forming are selected to be 0<d1<=50mm and d2<d2<=50mm and 0.2<=(d2-d1)/d2<=1.0. Then the wall is made of major components as 5-20% of cement and 80-95% of magnetic particles in the dry weight ratio, and the length of the wall in the magnetic field direction of the TV radio wave is selected to be the required absorbing wave or over. In this case a cement called generally a cement such as hydraulic cement, air setting cement, and special cement is enough for the purpose. Furthermore, the magnetic particles are oxide magnetic particles and metallic magnetic particles. Then a gap being a groove 12 is provided in the direction of the electric field and a substance with a low dielectric constant is used inbetween, then the substantial induction rate is reduced and the absorbing performance is improved.

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、セメントと磁性粉粒物
を主原料とした、TV周波数帯域用電波吸収壁に関する
ものである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a radio wave absorption wall for TV frequency band, which is mainly composed of cement and magnetic powder particles.

【0002】[0002]

【従来の技術】TV電波は、100MHz 近傍、波長約3
mを使用周波数にもつ1ch〜3ch、200MHz 近傍、波
長約1.5mを使用周波数にもつ4ch〜12ch、600
MHz 近傍、波長として約0.5mを使用周波数にもつ1
3ch〜62chまで、実に最大8倍強の異なる周波数(波
長)の電波が使用されている。
2. Description of the Related Art TV radio waves have a wavelength of about 3 and a wavelength of about 3 MHz.
1ch to 3ch with m as the operating frequency, around 200MHz, 4ch to 12ch with 600nm as the operating frequency, 600
Around 1 MHz with a frequency of about 0.5 m as a wavelength
From 3ch to 62ch, radio waves with different frequencies (wavelengths) of up to 8 times are actually used.

【0003】したがって、固有の厚みを有する電波吸収
体で、広帯域かつ波長差が2mを超えるTV電波を吸収
し、偽像(ゴースト)を防止する電波吸収体の種類は少
ない。このため高層建築物が乱立する都市部において
は、テレビ画面上の像が2重、3重に見られることも珍
しくはない。
Therefore, there are few types of radio wave absorbers having a unique thickness and capable of absorbing TV radio waves with a wavelength difference of more than 2 m and preventing false images (ghosts). For this reason, it is not uncommon to see double or triple images on the TV screen in urban areas where high-rise buildings are scattered.

【0004】現在知られている解決手段は、主に2つ存
在し、焼結フェライトタイル材を用いる方法と、カーボ
ン粉と発泡スチロール複合体からなるピラミッド型ブロ
ック材を用いる方法とがある。
There are mainly two currently known solutions, and there are a method of using a sintered ferrite tile material and a method of using a pyramid type block material composed of carbon powder and a styrofoam composite.

【0005】しかしながら、焼結フェライトタイル材
は、1000℃以上の高温で焼成する工程が不可避であ
るため、焼きむらや焼成中のタイルのそり等の変形が生
ずる。この焼成条件の不均一さを軽減する目的上、タイ
ルの形状には大きさに制約があり、その寸法は10cm×
10cm程度となる。この値は、1ch波長の約1/30、
8ch波長の1/15であり、良好な吸収特性を獲得する
ためには、フェライトタイルを連続的に最低限15枚か
ら30枚列べる必要があり、寸法精度確保のために、接
合面を研磨する等の非常にめんどうな工程が施工能率を
低下させている。またピラミッド型ブロック材の場合、
現在知られているTV吸収体の厚みは1〜2mであり、
ビルの外壁に採用するには、空間的な問題が多く、電波
暗室等に使用する場合にも、部屋の空間を大きく占有す
るといった問題点がある。
However, since the step of firing the sintered ferrite tile material at a high temperature of 1000 ° C. or more is inevitable, uneven firing or warping of the tile during firing occurs. For the purpose of reducing the unevenness of the firing conditions, the shape of the tile is limited in size, and its size is 10 cm ×
It will be about 10 cm. This value is about 1/30 of 1ch wavelength,
It is 1/15 of 8ch wavelength, and it is necessary to row at least 15 to 30 ferrite tiles continuously in order to obtain good absorption characteristics. Very laborious processes such as polishing reduce the construction efficiency. In the case of pyramid type block material,
Currently known TV absorbers have a thickness of 1-2 m,
There are many spatial problems when it is used for the outer wall of a building, and when it is used in an anechoic chamber, etc., it occupies a large space in the room.

【0006】特公昭55−49798号公報には、軽量
化ならびに低コスト化のため、フェライト板を磁界方向
に連続して、電界方向に不連続となる如く間隔をあけ、
列べることを特徴とする電波吸収壁が開示されている。
また、特公昭55−29599号公報においては、錘体
状のフェライト部材を用いて、電波吸収体の厚さを連続
して変化させる方法が開示されている。
In Japanese Patent Publication No. 55-49798, in order to reduce the weight and the cost, the ferrite plates are continuous in the magnetic field direction and are spaced so as to be discontinuous in the electric field direction.
There is disclosed a radio wave absorption wall characterized by being lined up.
In addition, Japanese Patent Publication No. 55-29599 discloses a method of continuously changing the thickness of a radio wave absorber by using a weight-shaped ferrite member.

【0007】しかしながら、両者とも使用の際には、1
0×10cm程度の大きさのフェライトタイルを多数個列
べて、使用しなければならない欠点があり、一般のフェ
ライトタイル材同様、広く一般建築物に普及していな
い。
However, when both are used, 1
There is a drawback that a large number of ferrite tiles with a size of about 0 × 10 cm must be lined up and used, and like general ferrite tile materials, they are not widely used in general buildings.

【0008】次に、形状の欠点を克服し、大型電波吸収
体を作成する方法としては、現在下記の方法が開示され
ている。
Next, as a method for overcoming the shape defect and producing a large-sized electromagnetic wave absorber, the following method is currently disclosed.

【0009】粗骨材及び細骨材としてフェライトを使用
し、コンクリートよりなる電波吸収層を設けたことを特
徴とする電波吸収壁体が報告されている(特開昭63−
66999号公報)。他にも、磁性粉粒物とセメントも
しくはゴム等の非磁性体との混合物を使用した複合電波
吸収体について、反射減衰量が報告されているものとし
ては、例えば特開昭50−155999号公報、同51
−121200号公報、同51−110951号公報、
同52−67945号公報、同54−41495号公
報、同60−89902号公報がある。
A radio wave absorbing wall body has been reported which is characterized by using a ferrite as a coarse aggregate and a fine aggregate and providing an electric wave absorbing layer made of concrete.
No. 66999). In addition, regarding a composite electromagnetic wave absorber using a mixture of magnetic powder particles and a non-magnetic substance such as cement or rubber, Japanese Patent Laid-Open Publication No. 50-155999 discloses that the return loss is reported. , The same 51
No. 121200, No. 51-110951.
No. 52-67945, No. 54-41495, and No. 60-89902.

【0010】しかしながら、上記記載の電波吸収体にお
いて、TV周波数の特に低周波側(90〜230MHz 、
1〜12chに対応)を吸収周波数領域にもつ吸収体の記
載はなく、比較のため強いて述べれば、特開昭52−6
7945号公報記載の電波吸収体(厚み150mm)が、
300MHz 以上の周波数領域において良好な特性を示し
ているに過ぎず、磁性粉粒物と非磁性体とを混合した電
波吸収体の多くは、500MHz 〜1GHz 以上の周波数領
域を電波吸収領域としている。
However, in the radio wave absorber described above, in the low frequency side of TV frequency (90 to 230 MHz,
There is no description of an absorber having an absorption frequency region (corresponding to 1 to 12 channels), and if it is stated strongly for comparison, it is disclosed in Japanese Patent Laid-Open No. 52-6.
The electromagnetic wave absorber (thickness 150 mm) described in 7945 is
It only shows good characteristics in the frequency range of 300 MHz or higher, and most of the radio wave absorbers in which magnetic powder particles and non-magnetic materials are mixed have the radio wave absorption region in the frequency range of 500 MHz to 1 GHz or higher.

【0011】[0011]

【発明が解決しようとする課題】本発明は、既存電波吸
収体の経済的・形状的・空間的欠点を克服し、施工が容
易で、しかも広帯域にわたるTV周波数帯域電波の吸収
を可能とする成形体の吸収特性改善を目的としている。
DISCLOSURE OF THE INVENTION The present invention overcomes the economical, shape and spatial drawbacks of existing electromagnetic wave absorbers, is easy to construct, and is capable of absorbing radio waves in the TV frequency band over a wide band. The purpose is to improve the absorption characteristics of the body.

【0012】[0012]

【課題を解決するための手段】本発明は、TV電波の電
界方向に深さ(d2 −d1 )の溝を有し、成形体凹部厚
みd1 ならびに、成形体凸部厚みd2 が、0<d1 ≦5
0mm、かつd1 <d2 ≦50mm、かつ0.2≦(d2
1 )/d2 ≦1.0を特徴とし、乾燥重量比でセメン
ト5〜20%、磁性粉粒物80〜95%の主成分から構
成されたTV電波の磁界方向長さが、要求吸収波長以上
であることを特徴とするTV周波数帯域用電波吸収壁、
または、TV電波の電界方向に深さ(dn+1 −dn )の
溝を有し、成形体厚みdn ならびに、成形体厚みdn+1
(n=1,2,3…)が、0<dn ≦50mm、かつdn
<dn+1 ≦50mm、かつ0.2≦(dn −d1 )/dn
≦1.0を特徴とし、乾燥重量比でセメント5〜20
%、磁性粉粒物80〜95%の主成分から構成されたT
V電波の磁界方向長さが、要求吸収波長以上であること
を特徴とするTV周波数帯域用電波吸収壁、または、T
V電波の電界方向に隙間を有し、成形体の厚みdが、1
0≦d≦50mmを特徴とする、乾燥重量比でセメント5
〜20%、磁性粉粒物80〜95%の主成分から構成さ
れたTV電波の磁界方向長さが、要求吸収波長以上であ
ることを特徴とするTV周波数帯域用電波吸収壁であ
る。
The present invention has a groove having a depth (d 2 −d 1 ) in the electric field direction of TV radio waves, and the molded body concave portion thickness d 1 and the molded body convex portion thickness d 2 are , 0 <d 1 ≦ 5
0 mm, d 1 <d 2 ≦ 50 mm, and 0.2 ≦ (d 2
d 1 ) / d 2 ≦ 1.0, the length of the TV radio wave in the magnetic field direction is the required absorption, composed of the main components of 5 to 20% of cement and 80 to 95% of magnetic powder granules in the dry weight ratio. A radio wave absorption wall for TV frequency band, which is characterized by being equal to or more than the wavelength
Or has a groove depth in the direction of the electric field of the TV radio wave (d n + 1 -d n) , the molded body thickness d n and moldings thickness d n + 1
(N = 1, 2, 3 ...) is 0 <d n ≦ 50 mm, and d n
<D n + 1 ≦ 50mm and 0.2 ≦ (d n -d 1) , / d n
≤1.0, characterized by dry weight ratio of cement 5-20
%, Magnetic powder granules 80-95%
The electromagnetic wave absorption wall for TV frequency band, characterized in that the magnetic field length of V electric wave is equal to or longer than the required absorption wavelength, or T
There is a gap in the electric field direction of V radio waves, and the thickness d of the molded body is 1
Cement 5 by dry weight ratio, characterized by 0 ≦ d ≦ 50 mm
The electromagnetic wave absorption wall for the TV frequency band is characterized in that the magnetic field length of the TV radio wave in the magnetic field direction, which is composed of the main components of ˜20% and magnetic powder granules 80 to 95%, is not less than the required absorption wavelength.

【0013】[0013]

【作用】以下に本発明を詳細に説明する。本発明でいう
セメントとは、水硬性セメント(例えば、ポルトランド
セメント、白色ポルトランドセメント、アルミナセメン
ト、ポゾランセメント、トラスセメント、サントリンセ
メント、石灰スラグセメント、ポゾランポルトランドセ
メント、シリカセメント、トラスポルトランドセメン
ト、高炉セメント、鉄ポルトランドセメント、フライア
ッシュセメント、ソリジットセメント、頁岩灰ポルトラ
ンドセメント)、気硬性セメント(マグネシアセメン
ト)、特殊セメント(耐火セメント、耐酸セメント、水
ガラスセメント、高硫酸塩スラグセメント)等、一般に
セメントと呼ばれているセメント類であれば特に限定さ
れない。
The present invention will be described in detail below. The cement referred to in the present invention is a hydraulic cement (for example, Portland cement, white Portland cement, alumina cement, pozzolan cement, truss cement, santorin cement, lime slag cement, pozzolan Portland cement, silica cement, trasportland cement, blast furnace Cement, iron Portland cement, fly ash cement, solidit cement, shale ash Portland cement), air-hardening cement (magnesia cement), special cement (fire resistant cement, acid resistant cement, water glass cement, high sulfate slag cement), etc. The cement is not particularly limited as long as it is called cement.

【0014】その配合比は、乾燥重量比で全体の5wt%
以上ないし25wt%以下の範囲であり、5wt%未満の範
囲では成形物が凝結しにくく、また、25wt%を超える
範囲では、電波吸収材としての本来の機能が劣る。
The blending ratio is 5 wt% of the total dry weight ratio.
It is in the range of not less than 25 wt% and not more than 25 wt%, and the molded product is hard to congeal in the range of less than 5 wt%, and the original function as a radio wave absorber is inferior in the range of more than 25 wt%.

【0015】磁性粉粒物とは、酸化物磁性体ならびに金
属磁性体であり、例えば(FeO−Fe2 3 ,γ−F
2 3 ,MnO−Fe2 3 ,MnO−ZnO−Fe
2 3 ,CuO−ZnO−Fe2 3 ,CuO−MnO
−Fe2 3 ,NiO−ZnO−Fe2 3 ,NiO−
CuO−ZnO−Fe2 3 ,MgO−Fe2 3 ,M
gO−ZnO−Fe2 3 ,MgO−MnO−Fe2
3 ,LiO−ZnO−Fe2 3 などの酸化物磁性体
と、鉄粉、ケイ素鋼粉、パーマロイ粉、センダスト粉な
どの金属磁性体とがある。
[0015] The magnetic powder and granular material is an oxide magnetic material and the metallic magnetic, for example (FeO-Fe 2 O 3, γ-F
e 2 O 3, MnO-Fe 2 O 3, MnO-ZnO-Fe
2 O 3, CuO-ZnO- Fe 2 O 3, CuO-MnO
-Fe 2 O 3, NiO-ZnO -Fe 2 O 3, NiO-
CuO-ZnO-Fe 2 O 3 , MgO-Fe 2 O 3, M
gO-ZnO-Fe 2 O 3 , MgO-MnO-Fe 2 O
3 , there are oxide magnetic materials such as LiO—ZnO—Fe 2 O 3 and metal magnetic materials such as iron powder, silicon steel powder, permalloy powder and Sendust powder.

【0016】なお、酸化物磁性体に限定すれば、磁気特
性の改善、焼結反応の促進、結晶粒内・粒界抵抗の制御
などを目的として微量元素(例えば、CaO,SiO2
等)を焼成前に添加することが望ましい。
If the oxide magnetic material is limited, trace elements (for example, CaO, SiO 2) are used for the purpose of improving magnetic properties, accelerating the sintering reaction, controlling the resistance of crystal grains and grain boundaries.
Etc.) is preferably added before firing.

【0017】さらに、現在入手が比較的容易で、大量、
安価に市場に出回っている磁性体で、しかも吸収特性に
も優れている材料としては、Mn−Zn系ならびにMn
−Mg系などのMn基フェライトや、Ni−Zn系フェ
ライトが適当である。
Further, it is relatively easy to obtain at present, and a large amount of
Magnetic materials that are inexpensively available on the market and have excellent absorption characteristics include Mn—Zn-based materials and Mn-based materials.
A Mn-based ferrite such as -Mg-based ferrite or a Ni-Zn-based ferrite is suitable.

【0018】磁性粉粒物の大きさや粒径分布について
は、特に規定はしないが、本発明の磁性粉粒物のセメン
トに対する混練量がかなり高いという理由により、ま
た、磁性粉粒物をセメント骨材の代用と見なすことよ
り、成形時の簡便さを粒径サイズの目安とすることが妥
当と考えられる。
The size and particle size distribution of the magnetic powder granules are not particularly specified, but because the amount of the magnetic powder granules of the present invention to be kneaded with the cement is considerably high, the magnetic powder granules are also mixed with the cement bone. By considering it as a substitute for the material, it is considered appropriate to use the ease of molding as a guide for the particle size.

【0019】粉粒物の粒系分布については、例えば、F
ullerおよびThompsonによるフルイ分布曲
線や、Grafが提唱した細骨材のドイツ規格(DIN
1045)を参考にしても良いし、また上記提唱者の値
を必ずしも、完全に満足する必要もない。
Regarding the grain-based distribution of the powder or granular material, for example, F
Fluler distribution curve by uller and Thompson, and German standard for fine aggregate proposed by Graf (DIN
1045) may be referred to, and it is not always necessary to completely satisfy the values of the above-mentioned proponents.

【0020】磁性粉粒物の配合比は、乾燥重量比で全体
の75%以上ないし95wt%以下の範囲であり、95wt
%を超える範囲では成形体が凝固しにくく、また、75
wt%未満の範囲では電波吸収体としての本来の性能が劣
る。
The compounding ratio of the magnetic powder particles is in the range of 75% to 95% by weight in terms of dry weight ratio, and 95% by weight.
%, The molded body is hard to solidify,
In the range of less than wt%, the original performance as a radio wave absorber is poor.

【0021】以上、本文で述べた材料すなわち、セメン
ト、磁性粉粒物を本発明では主成分と呼び、成形にあた
っては水分や混和材料(例えば、AE材、分散材、凝結
・硬化促進材、防水材、防凍材、発泡材、着色材、混合
材、耐火性促進材等)を適宜添加する。また、長繊維状
もしくは短繊維状のカーボンファイバーをコンクリート
中に1種類以上混凍することにより、成形体の複素誘電
率を微調整し、吸収特性を改善しても良い。
In the present invention, the materials described above, that is, cement and magnetic powder granules are referred to as the main components, and water and admixtures (eg, AE material, dispersion material, setting / hardening accelerator, waterproofing) are used for molding. Materials, anti-freezing materials, foaming materials, coloring materials, mixing materials, fire resistance promoting materials, etc.) are appropriately added. Further, the absorption permittivity may be improved by finely adjusting the complex dielectric constant of the molded body by freeze-drying one or more kinds of long fiber-shaped or short fiber-shaped carbon fibers in concrete.

【0022】電波吸収特性は、透磁率の実数成分・虚数
成分ならびに、誘電率の実数成分・虚数成分の値に依存
する。このうち、本発明において特に重要なのが虚数透
磁率と実数誘電率である。
The electromagnetic wave absorption characteristics depend on the values of the real number component / imaginary number component of magnetic permeability and the real number component / imaginary number component of permittivity. Of these, the imaginary permeability and the real permittivity are particularly important in the present invention.

【0023】虚数透磁率を増大させることは、電波吸収
体の厚みを低減させるために不可欠な要素であり、実数
誘電率を低減させることは、電波吸収特性を広帯域化さ
せるために不可欠である。
Increasing the imaginary magnetic permeability is an essential factor for reducing the thickness of the electromagnetic wave absorber, and decreasing the real number dielectric constant is essential for widening the electromagnetic wave absorption characteristics.

【0024】しかしながら、虚数透磁率を増大させるた
めには、図3に示すように、主成分中の磁性粉粒物比を
増大させなければならず、磁性粉粒物比の増大は実数誘
電率を増大させる。
However, in order to increase the imaginary magnetic permeability, as shown in FIG. 3, the ratio of the magnetic powder particles in the main component must be increased. Increase.

【0025】この矛盾した要求を解消するため、電界方
向に隙間もしくは、溝を設け、低誘電率の物質(例え
ば、空気、コンクリート、モルタル等)を間に挟むこと
で、見かけ上、実数誘電率が低減でき、吸収特性が改善
される。
In order to solve this contradictory requirement, a gap or groove is provided in the direction of the electric field, and a substance having a low dielectric constant (for example, air, concrete, mortar, etc.) is sandwiched between them, so that the real dielectric constant is apparent. Can be reduced and absorption characteristics can be improved.

【0026】図4は、隙間ならびに溝を有する本発明吸
収壁の見かけの実数誘電率変化量、ならびに見かけの虚
数透磁率変化量を、隙間ならびに溝深さとの関係で示し
た。ここで、見かけの実数誘電率ならびに、見かけの虚
数透磁率は、試験片の凸凹を平均化した平均厚みの値を
用いて算出した。
FIG. 4 shows the apparent real number permittivity change amount and the apparent imaginary permeability change amount of the absorbing wall of the present invention having a gap and a groove in relation to the gap and the groove depth. Here, the apparent real number dielectric constant and the apparent imaginary number magnetic permeability were calculated using the average thickness values obtained by averaging the irregularities of the test piece.

【0027】また、横軸の隙間ならびに溝深さについて
も、平均厚みで除した値(%)で整理を行った。
The gaps and groove depths on the horizontal axis were also organized by the value (%) divided by the average thickness.

【0028】図において、Δμ″の値は、電界方向の隙
間ならびに溝の有無にかかわらず、ほぼ変化量ゼロを示
す。このことは、磁界方向に隙間もしくは溝が無い本発
明における特徴であり、形状の変化により、磁気特性
(μ″)は影響しない。
In the figure, the value of Δμ ″ shows almost zero variation regardless of the presence or absence of a gap and a groove in the electric field direction. This is a feature of the present invention in which there is no gap or groove in the magnetic field direction, Due to the change in shape, the magnetic characteristics (μ ″) are not affected.

【0029】Δε′については、電界方向の隙間ならび
に溝深さの増大に伴い減少し、見かけの実数誘電率は、
10%〜60%程度まで低減できる。このことは先に述
べたように、高い磁性粉粒物の配合比率においても、高
μ″かつ低ε′化でき、広い周波数範囲で良好な吸収条
件を得易くする。
Regarding Δε ′, it decreases as the gap in the electric field direction and the groove depth increase, and the apparent real number dielectric constant is
It can be reduced to about 10% to 60%. As described above, this makes it possible to obtain a high μ ″ and a low ε ′ even at a high mixing ratio of the magnetic powder particles, and it becomes easy to obtain a good absorption condition in a wide frequency range.

【0030】すなわち、本発明記載の形状上の特徴は、
流し込み成形等で容易に隙間や溝が作成できる本発明記
載の構成成分の特徴と組合せることにより、最も効果的
かつ経済的にTV電波を吸収する。
That is, the geometrical features described in the present invention are as follows.
By combining with the features of the constituent components according to the present invention that can easily form gaps and grooves by casting or the like, TV waves are most effectively and economically absorbed.

【0031】図1ならびに図2には、本発明の概略図を
示す。図において、d1 ,d2 ならびにdは電波吸収体
の厚みである。
1 and 2 show a schematic diagram of the present invention. In the figure, d 1 , d 2 and d are the thickness of the electromagnetic wave absorber.

【0032】本発明で述べる電波吸収壁の裏面には、短
絡板とよばれる導電体が施工される。この板は、鉄板、
銅板などの金属製板の他、金網や鉄筋などでも代用が可
能である。図において10:鉄筋、11:電波吸収コン
クリートパネル、12:溝、13:表面層(タイル、モ
ルタル、岩石、ボード)を示す。
On the back surface of the electromagnetic wave absorbing wall described in the present invention, a conductor called a short circuit plate is installed. This plate is an iron plate,
In addition to metal plates such as copper plates, wire mesh and reinforcing bars can be used instead. In the figure, 10: rebar, 11: radio wave absorption concrete panel, 12: groove, 13: surface layer (tile, mortar, rock, board) are shown.

【0033】また、図5(a)には、2段厚み(d1
2 )の場合、図5(b)には、3段厚み(d1
2 ,d3 )の場合を、図5(c)には、4段厚みの場
合(d1 ,d2 ,d3 ,d4 )を示す。
Further, in FIG. 5 (a), the two-step thickness (d 1 ,
For d 2), in FIG. 5 (b), 3 Dan'atsumi (d 1,
FIG. 5C shows the case of d 2 , d 3 ), and the case of 4 steps thickness (d 1 , d 2 , d 3 , d 4 ).

【0034】複数の厚みで吸収壁を構成することによ
り、吸収できる周波数帯域をより広帯域化できる。溝の
深さは吸収体の平均厚みの20%程度でも効果があり、
さらに望ましくは、平均厚みの50%以上が良い。
By forming the absorption wall with a plurality of thicknesses, the frequency band that can be absorbed can be broadened. Even if the depth of the groove is about 20% of the average thickness of the absorber, it is effective,
More preferably, it is 50% or more of the average thickness.

【0035】溝もしくは隙間の割合は、幅全体の1/3
以上、3倍以下が望ましく、さらに望ましくは、1/2
以上、2倍以下が望ましい。この電界方向の溝ならびに
隙間により、見かけ上実数誘電率が低減し、吸収特性が
改善される。図6及び図7は本発明の他の例の説明図で
ある。
The ratio of grooves or gaps is 1/3 of the entire width.
It is desirable to be 3 times or more, and more desirably 1/2
It is desirable to be 2 times or less. The grooves and gaps in the direction of the electric field apparently reduce the real number dielectric constant and improve the absorption characteristics. 6 and 7 are explanatory views of another example of the present invention.

【0036】本発明でいう要求吸収波長とは、TVチャ
ンネルの1ch(90〜96MHz)で3.2m、4ch(17
0〜176MHz)で1.7m、12ch(216〜222MH
z)で1.4m、13ch(470〜476MHz)で0.6m
であり、吸収壁寸法に関しては、この要求吸収波長以上
の大きさに磁界方向長さを成形することで、電波吸収材
と電波吸収材との隙間による電波吸収性能の低下が軽減
できる。
The required absorption wavelength in the present invention means 3.2 m for 1 channel (90 to 96 MHz) of TV channel and 4 channels (17 channels).
1.7m at 0 to 176MHz, 12ch (216 to 222MH)
z) 1.4m, 13ch (470-476MHz) 0.6m
With respect to the size of the absorption wall, by molding the length in the magnetic field direction to a size that is equal to or larger than the required absorption wavelength, it is possible to reduce the deterioration of the electromagnetic wave absorption performance due to the gap between the electromagnetic wave absorber and the electromagnetic wave absorber.

【0037】例えば、10階建てのビルの4階以上の面
積(1000m2 と想定)が電波障害となる場合、10
cm角タイルを全面に取り付けると、約10万枚分の作業
が必要となる。しかも、電波吸収材と電波吸収材との磁
界方向隙間が1mmずつ存在すると電波(100MHz)の反
射率は約33倍増加し、吸収特性は激減する(日本放送
協会編:電波吸収体による電波障害対策ガイドブック昭
和56年7月6頁)。
For example, if the area of the fourth floor or above of a 10-story building (assuming 1000 m 2 ) causes radio interference, 10
If you attach cm square tiles to the entire surface, you will need to work for about 100,000 sheets. Moreover, if there is a gap of 1 mm between the electromagnetic wave absorber and the electromagnetic wave absorber in the magnetic field direction, the reflectance of radio waves (100 MHz) will increase about 33 times, and the absorption characteristics will drastically decrease. Countermeasure guidebook, July 6, 1981).

【0038】ところが、本発明に述べる電波吸収壁を、
磁界方向の長さが要求吸収波長以上(例えば3m×1
m)に成形することにより、取り付け総数は約330枚
分・工数は約1/300に簡素化でき、また隙間の問題
も解消可能となる。
However, the electromagnetic wave absorption wall described in the present invention is
The length in the magnetic field direction is greater than or equal to the required absorption wavelength (for example, 3m x 1
By molding into m), the total number of attachments can be reduced to about 330 and the man-hours can be simplified to about 1/300, and the problem of gaps can be solved.

【0039】[0039]

【実施例】実施例1 本発明TV周波数帯域用電波吸収壁の特性例を示す。成
形体の配合比は、乾燥重量比で、Mn−Znフェライト
粉粒物87.5%(コンクリート重量の約7倍)、残部
白色ポルトランドセメントであり、測定周波数は、TV
電波の全域に相当する90MHz から770MHz とした。
EXAMPLE 1 An example of the characteristics of the radio wave absorption wall for the TV frequency band of the present invention will be shown. The compounding ratio of the molded product was 87.5% of Mn-Zn ferrite powder granules (about 7 times the weight of concrete) and the balance white Portland cement in dry weight ratio, and the measurement frequency was TV.
The frequency was changed from 90MHz to 770MHz, which corresponds to the entire radio wave.

【0040】本発明材の電波吸収測定値は、図8に示す
ように例えば、厚みd1 =27mm、d2 =43mmにおい
て19.4dB(100MHz)であった。この値は、現在使
用されているフェライト焼結タイル材(厚み約7mm前
後)の電波吸収量(20dBとして比較)の約99.8%
に相当するTV電波を吸収する。
As shown in FIG. 8, the radio wave absorption measurement value of the material of the present invention was 19.4 dB (100 MHz) at a thickness d 1 = 27 mm and a thickness d 2 = 43 mm, for example. This value is about 99.8% of the electromagnetic wave absorption amount (compared to 20 dB) of the currently used ferrite sintered tile material (thickness about 7 mm).
Absorb TV radio waves equivalent to.

【0041】同様に200MHz ならびに600MHz にお
いても、それぞれ17.4dB,14.5dBと、20dB換
算値の99.2%、97.4%に相当する電波を吸収で
きる。
Similarly, at 200 MHz and 600 MHz, it is possible to absorb radio waves of 17.4 dB and 14.5 dB, which correspond to 99.2% and 97.4% of the 20 dB converted value, respectively.

【0042】この値は、実装状態(窓・サッシ枠・バル
コニー等、電波を反射し易い物質が表面に露呈される場
合が多い)を考慮すると、焼結フェライトタイル材と比
較しても、十分使用可能となる吸収特性と考えられる。
This value is sufficient even when compared with a sintered ferrite tile material in consideration of the mounting state (often a material that easily reflects radio waves such as windows, sash frames, balconies, etc. is exposed on the surface). It is considered to be the absorption characteristics that make it usable.

【0043】ここで、10dBとは、電波の90%を吸収
することに相当し、20dBとは99%の電波を吸収する
ことに相当する。
Here, 10 dB corresponds to absorbing 90% of the electric wave, and 20 dB corresponds to absorbing 99% of the electric wave.

【0044】ところが、図8で示す比較材(乾燥重量比
で、Mn−Znフェライト粉粒物87.5%、残部白色
ポルトランドセメントを主成分とする、厚み30mmの電
波吸収壁1段)の電波吸収測定値においては、100MH
z で15.1dB、200MHzで13.2dB、600MHz
で7.3dBと、本発明例に対する比較例の反射量は、1
00MHz で2.7倍、200MHz で2.6倍、600MH
z で5.2倍と大きく、特に高周波側で明瞭な違いとな
って現れる。
However, the radio wave of the comparative material shown in FIG. 8 (1 step of the radio wave absorption wall having a thickness of 30 mm, which is composed mainly of Mn-Zn ferrite powder particles 87.5% by dry weight and the balance white Portland cement). Absorption measurement value is 100MH
15.1dB at z, 13.2dB at 200MHz, 600MHz
Is 7.3 dB, and the reflection amount of the comparative example with respect to the present invention example is 1
2.7 times at 00MHz, 2.6 times at 200MHz, 600MH
It is as large as 5.2 times z, and it appears as a clear difference especially on the high frequency side.

【0045】実施例2 表1には、乾燥重量比における主原料の配合比ならび
に、厚みd1 ,d2 ,d及び隙間ならびに溝の幅割合
(%)、反射減衰量(dB値)を示す。
Example 2 Table 1 shows the blending ratio of the main raw materials in the dry weight ratio, the thicknesses d 1 , d 2 , d and the gap and groove width ratio (%), and the return loss (dB value). .

【0046】[0046]

【表1】 [Table 1]

【0047】[0047]

【表2】 [Table 2]

【0048】[0048]

【発明の効果】従来使用されていた電波吸収タイル材
(10cm×10cm)にかわり、本発明の電波吸収壁を使
用することにより、形状の自由が与えられ、施工工程が
簡素化・量産することが可能となる。
EFFECTS OF THE INVENTION By using the radio wave absorbing wall of the present invention in place of the radio wave absorbing tile material (10 cm × 10 cm) which has been used conventionally, the shape is given freely and the construction process is simplified and mass produced. Is possible.

【0049】従来ε′は、磁性粉粒物の含有量で決定さ
れ、この磁性粉粒物の配合量により、μ′ならびにμ″
の値も、電波吸収特性も、ほぼ決定されてしまう欠点が
あった。本発明に記載する形状上の変更により、ε′と
フェライト配合比を、それぞれ別々に決定でき、低い見
かけの誘電率とすることで、広い周波数範囲において
も、良好な吸収特性が得られる。
Conventionally, ε'is determined by the content of the magnetic powder particles, and μ'and μ "are determined depending on the compounding amount of the magnetic powder particles.
There is a drawback that both the value of and the electromagnetic wave absorption characteristics are almost determined. By changing the shape described in the present invention, ε'and the ferrite compounding ratio can be determined separately, and by setting a low apparent dielectric constant, good absorption characteristics can be obtained even in a wide frequency range.

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

【図1】本発明によるTV周波数帯域電波吸収体の斜視
図である。
FIG. 1 is a perspective view of a TV frequency band electromagnetic wave absorber according to the present invention.

【図2】本発明の他の実施例を示す斜視図である。FIG. 2 is a perspective view showing another embodiment of the present invention.

【図3】磁性粉粒物配合比の変化に伴う、μ″ならびに
ε′の図表である。
FIG. 3 is a chart of μ ″ and ε ′ according to a change in the mixing ratio of magnetic powder particles.

【図4】本発明吸収体の隙間または溝深さ変化に伴う見
かけの虚数透磁率ならびに、見かけの実数誘電率変化の
図表である。
FIG. 4 is a table showing changes in apparent imaginary permeability and changes in apparent real permittivity with changes in the gap or groove depth of the absorber of the present invention.

【図5】(a),(b),(c)は、本発明例の部分断
面図である。
5 (a), (b), (c) are partial cross-sectional views of an example of the present invention.

【図6】(a),(b),(c),(d)は、本発明の
他の例の部分断面図である。
6 (a), (b), (c) and (d) are partial cross-sectional views of another example of the present invention.

【図7】(e),(f),(g)は、図6と同様に本発
明の他の例の部分断面図である。
7 (e), (f), and (g) are partial cross-sectional views of another example of the present invention, similar to FIG.

【図8】電波吸収体の測定例の図表である。FIG. 8 is a chart of a measurement example of a radio wave absorber.

───────────────────────────────────────────────────── フロントページの続き (71)出願人 000002886 大日本インキ化学工業株式会社 東京都板橋区坂下3丁目35番58号 (72)発明者 山本 毅 神奈川県川崎市中原区井田1618番地 新日 本製鐵株式会社先端技術研究所内 ─────────────────────────────────────────────────── ─── Continuation of the front page (71) Applicant 000002886 Dainippon Ink and Chemicals, Inc. 3-35-58 Sakashita, Itabashi-ku, Tokyo (72) Inventor Takeshi Yamamoto 1618 Ida, Nakahara-ku, Kawasaki-shi, Kanagawa Shin-Nihon Steel Engineering Co., Ltd.

Claims (3)

【特許請求の範囲】[Claims] 【請求項1】 TV電波の電界方向に深さ(d2
1 )の溝を有し、成形体凹部厚みd1 ならびに成形体
凸部厚みd2 が、0<d1 ≦50mm、かつd1 <d2
50mm、かつ0.2≦(d2 −d1 )/d2 ≦1.0を
満足し、乾燥重量比でセメント5〜20%、磁性粉粒物
80〜95%の主成分から構成されたTV電波の磁界方
向長さが、要求吸収波長以上であることを特徴とするT
V周波数帯域用電波吸収壁。
1. A depth (d 2 −) in the electric field direction of TV radio waves.
d 1 ), and the thickness d 1 of the concave portion of the molded body and the thickness d 2 of the convex portion of the molded body are 0 <d 1 ≦ 50 mm and d 1 <d 2
50 mm and 0.2 ≦ (d 2 −d 1 ) / d 2 ≦ 1.0 were satisfied, and it was composed of the main components of cement 5 to 20% and magnetic powder granules 80 to 95% in dry weight ratio. The length of the TV radio wave in the magnetic field direction is equal to or longer than the required absorption wavelength.
Electromagnetic wave absorption wall for V frequency band.
【請求項2】 TV電波の電界方向に深さ(dn+1 −d
n )の溝を有し、成形体厚みdn ならび、に成形体厚み
n+1 (n=1,2,3…)が、0<dn ≦50mm、か
つdn <dn+1 ≦50mm、かつ0.2≦(dn −d1
/dn ≦1.0を満足することを特徴とする請求項1記
載のTV周波数帯域用電波吸収壁。
2. A depth (dn + 1- d) in the electric field direction of TV radio waves.
n ), the molded body thickness d n and the molded body thickness d n + 1 (n = 1, 2, 3 ...) Are 0 <d n ≦ 50 mm and d n <d n + 1. ≦ 50 mm, and 0.2 ≦ (d n -d 1)
The electromagnetic wave absorption wall for TV frequency band according to claim 1, wherein / d n ≦ 1.0 is satisfied.
【請求項3】 TV電波の電界方向に隙間を有し、成形
体の厚みdが、10≦d≦50mmを満足することを特徴
とする請求項1記載のTV周波数帯域用電波吸収壁。
3. The radio wave absorption wall for a TV frequency band according to claim 1, wherein there is a gap in the electric field direction of TV radio waves, and the thickness d of the molded body satisfies 10 ≦ d ≦ 50 mm.
JP3288024A 1991-11-01 1991-11-01 Radio wave absorbing wall for tv frequency band Withdrawn JPH05183331A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP3288024A JPH05183331A (en) 1991-11-01 1991-11-01 Radio wave absorbing wall for tv frequency band

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP3288024A JPH05183331A (en) 1991-11-01 1991-11-01 Radio wave absorbing wall for tv frequency band

Publications (1)

Publication Number Publication Date
JPH05183331A true JPH05183331A (en) 1993-07-23

Family

ID=17724831

Family Applications (1)

Application Number Title Priority Date Filing Date
JP3288024A Withdrawn JPH05183331A (en) 1991-11-01 1991-11-01 Radio wave absorbing wall for tv frequency band

Country Status (1)

Country Link
JP (1) JPH05183331A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0767578A (en) * 1993-06-30 1995-03-14 Nisshin Oil Mills Ltd:The Production of daily dishes

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0767578A (en) * 1993-06-30 1995-03-14 Nisshin Oil Mills Ltd:The Production of daily dishes

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