JPH025033B2 - - Google Patents

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Publication number
JPH025033B2
JPH025033B2 JP58032873A JP3287383A JPH025033B2 JP H025033 B2 JPH025033 B2 JP H025033B2 JP 58032873 A JP58032873 A JP 58032873A JP 3287383 A JP3287383 A JP 3287383A JP H025033 B2 JPH025033 B2 JP H025033B2
Authority
JP
Japan
Prior art keywords
plate
ribbon
electromagnetic
shielding
magnetic
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.)
Expired - Lifetime
Application number
JP58032873A
Other languages
Japanese (ja)
Other versions
JPS59159598A (en
Inventor
Toshihiko Asada
Yasushi Shirota
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.)
ASAOKA KK
Original Assignee
ASAOKA 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 ASAOKA KK filed Critical ASAOKA KK
Priority to JP3287383A priority Critical patent/JPS59159598A/en
Publication of JPS59159598A publication Critical patent/JPS59159598A/en
Publication of JPH025033B2 publication Critical patent/JPH025033B2/ja
Granted legal-status Critical Current

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

Description

【発明の詳細な説明】 この発明は電磁障害や磁気障害を防止する電磁
波シールド装置に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an electromagnetic shielding device for preventing electromagnetic interference and magnetic interference.

従来、公害としての不要電磁波汚染防止の立場
から、この種の妨害は雑音、電気雑音、静電雑
音、無線周波妨害等として取扱われてきたが、近
年電子機器の電磁障害が大きな問題となり、その
発生源に関する周波数成分と特性に分類されて論
議され、その大きさはその電界、磁界、電磁界の
強度あるいは特定周波数又は周波数帯に関する振
幅といつた形で測定され記述されるようになつ
た。
Traditionally, this type of interference has been treated as noise, electrical noise, static noise, radio frequency interference, etc. from the standpoint of preventing unnecessary electromagnetic wave pollution, but in recent years electromagnetic interference from electronic devices has become a major problem, and The frequency components and characteristics of sources have been classified and discussed, and their magnitudes have come to be measured and described in terms of electric fields, magnetic fields, the strength of electromagnetic fields, or the amplitudes of specific frequencies or frequency bands.

一般にシールドには静電シールド、電磁シール
ド、磁気シールドの3種類があるが、静電シール
ドは静電気結合による干渉を防止するもので、比
較的抵抗でも電流を通しアースすることにより効
果が得られる。また電磁シールドの対称となる周
波数は10kHz〜1000MHzの主として高周波であつ
て、低抵抗の金属を用いその中に電流が流れるこ
とを利用して磁束の干渉を防止するもので、電波
規制の対象となつている。さらに磁気シールドは
主として低周波に用いられ、導磁率の高い材料を
使用して磁束の誘導を防止するが、これは電波規
制の対象外となつている。
Generally, there are three types of shields: electrostatic shields, electromagnetic shields, and magnetic shields. Electrostatic shields prevent interference due to electrostatic coupling, and can be effective by passing current through and grounding even with a relatively high resistance. In addition, the frequency that electromagnetic shielding is symmetrical is mainly high frequency from 10kHz to 1000MHz, and it prevents magnetic flux interference by using low-resistance metal and using current flowing through it, and is subject to radio wave regulations. It's summery. Furthermore, magnetic shielding is mainly used for low frequencies and uses materials with high magnetic permeability to prevent the induction of magnetic flux, but this is not subject to radio wave regulations.

又一般に電子機器間で電磁障害の伝達は、空間
に放射される電磁波の形で伝達される「放射性電
磁障害」と称され、これには金属材料によるシー
ルド手法は古くから確立されていたが、近年デザ
イン化、軽量化、経済性などから金属材料からプ
ラスチツクへの移行が著しく、従つてプラスチツ
クハウジングにシールド処理を行わないと、電気
的技術基準をを満足できないようになつてきた。
Furthermore, the transmission of electromagnetic interference between electronic devices is generally referred to as ``radiated electromagnetic interference,'' which is transmitted in the form of electromagnetic waves radiated into space, and shielding methods using metal materials have been established for a long time. In recent years, there has been a significant shift from metal materials to plastics due to design, weight reduction, economic efficiency, etc., and it has become impossible to meet electrical technical standards unless a plastic housing is shielded.

現在行われているシールド手法は、亜鉛溶射を
プラスチツク面に行うか、導電性塗料をスプレー
又はハケ塗りする方法が90%を占める主流をな
し、その他の技術は開発研究の段階である。例え
ば、超微粒子金属粉等を板状や箱状体に塗布して
電磁波を部分的に吸収させるとか、又アメリカで
鉄−コバルト−ニツケル系の合金を超急冷技術で
処理・製造されたアモルフアス金属によるリボン
状の材料が開発されて以来、これを単体もしくは
網目状に織成して可とう性を有する円筒状体を作
り、電磁波を吸収させるというものが公知になつ
ている。これらのいづれの場合にも電磁波シール
ド効果は、デシベル(dB)で表わされる数値で
示されており、一般的に言われる30〜40dB程度
の効果で実用化されている。シールド効果のレベ
ル区分としては、0〜10dB:ほとんど効果なし、
10〜30dB:最小限度の効果が認められる、更に
30〜60dBは平均、60〜90dB平均以上、90dB以上
が最高の技術によるシールドで表わされている。
90% of the current shielding methods are spraying zinc on plastic surfaces or spraying or brushing conductive paint, and other techniques are still at the development and research stage. For example, applying ultrafine metal powder to a plate or box-like body to partially absorb electromagnetic waves, or amorphous metal produced by processing iron-cobalt-nickel alloy using ultra-quenching technology in the United States. Since the development of a ribbon-like material, it has become known to fabricate a flexible cylindrical body by weaving it singly or in a mesh to absorb electromagnetic waves. In any of these cases, the electromagnetic shielding effect is expressed in decibels (dB), and is generally put into practical use with an effect of about 30 to 40 dB. The level classification of the shielding effect is as follows: 0 to 10 dB: Almost no effect;
10-30dB: minimal effect is observed, and
30 to 60 dB is average, 60 to 90 dB above average, and 90 dB or more is represented by shielding with the best technology.

また一般に、アモルフアス金属には成分の組成
域によつて種々の材料特性があるが、その中でも
磁歪が10×10-6程度の合金は主に磁気シールド材
料として、又磁歪零の合金は主に磁気ヘツド材料
として使用されている。これは現用の結晶系金属
即ち金属高透磁率材料で幅広い用途を持つている
例えばパーマロイ合金に匹敵し、あるいはそれよ
りも更に高い実効透磁率と飽和磁束密度、低い保
磁力を持つ優れた材料だからであるが、いづれの
場合でも金属単体での使用又は網目状に織成した
素材としての利用の枠内の域を出なかつた。
In general, amorphous metals have various material properties depending on the composition range of their components, but alloys with a magnetostriction of about 10×10 -6 are mainly used as magnetic shielding materials, and alloys with zero magnetostriction are mainly used as magnetic shielding materials. Used as a magnetic head material. This is a current crystalline metal, i.e., a metallic high magnetic permeability material that has a wide range of applications.It is an excellent material with effective magnetic permeability, saturation magnetic flux density, and low coercive force that is comparable to, or even higher than, permalloy alloys. However, in either case, it was limited to use as a single metal or as a material woven into a mesh.

本発明はこれらの問題点を究明し解決すると共
に、低周波から高周波帯に至るあらゆる電磁波や
その方向・角度に対して、90dB以上等の極めて
高いシールド効果で吸収し悪影響をなくすとい
う、アモルフアス金属を利用した板状体を提供す
るものである。
The present invention has investigated and solved these problems, and has developed an amorphous amorphous metal that absorbs all electromagnetic waves from low frequencies to high frequencies, their directions and angles, with an extremely high shielding effect of 90 dB or more, eliminating any negative effects. The present invention provides a plate-like body that utilizes.

本発明を図面に基づいて説明すると、連続融体
急冷法によつて製造した鉄−コバルト−ニツケル
を主成分とする軟磁性を有する一定形状のアモル
フアス合金リボン、即ち第1図のように適宜の大
きさに巻かれたコイル状リボン1において、先端
をαとし任意の長さに切断した短冊状リボン片2
の長手方向の後端をβとすると、このリボン片2
を第2図に示すように先端αと後端βとを夫々同
方向にそろえて複数枚並列し、隣接するリボン片
2の側方端部を互に一部重ね合せ、かつ一体化し
て一枚の板状体11に形成する。尚、この場合複
数枚のリボン片2を一枚の板状体11に形成する
方法は、プラスチツクで全体を被ふくしたり、プ
ラスチツクテープで一体化したり、接着剤で互に
接着させたりなど種々の方法をとることができ
る。
To explain the present invention based on the drawings, an amorphous alloy ribbon having a certain shape and having soft magnetic properties mainly composed of iron-cobalt-nickel manufactured by a continuous melt quenching method, that is, an appropriate ribbon as shown in FIG. A rectangular ribbon piece 2 whose tip is set at α and cut into an arbitrary length from a coiled ribbon 1 wound to a size.
If the rear end in the longitudinal direction is β, then this ribbon piece 2
As shown in FIG. 2, a plurality of ribbon pieces 2 are arranged in parallel with their leading ends α and rear ends β aligned in the same direction, and the side ends of adjacent ribbon pieces 2 are partially overlapped with each other, and are integrated into one piece. A sheet of plate-like body 11 is formed. In this case, there are various methods for forming the plurality of ribbon pieces 2 into a single plate-like body 11, such as covering the entire ribbon with plastic, integrating them with plastic tape, and bonding them together with adhesive. method can be taken.

ところが、この板状体11と形成するリボン片
2の長手方向の向きA−A′とこれと直角に交さ
するB−B′に沿つて高周波電流発生装置を一定
出力の高周波電流に基づく電磁波を発生させなが
ら移動させたところ、この電磁波の移動方向がA
−A′方向では吸収作用即ち電磁波減衰作用が発
生しないが、B−B′方向では吸収作用即ち電磁
波減衰作用が発生することが判明した。
However, the high-frequency current generator generates electromagnetic waves based on a high-frequency current of a constant output along the longitudinal direction A-A' of the ribbon piece 2 formed with this plate-like body 11 and the B-B' that intersects at right angles with this direction. When the electromagnetic wave is moved while generating, the direction of movement of this electromagnetic wave is A.
It has been found that in the -A' direction, no absorption effect, ie, electromagnetic wave attenuation effect occurs, but in the BB' direction, an absorption effect, ie, electromagnetic wave attenuation effect, occurs.

また、マグネツトの有するN〜S磁界の下に鉄
粉等の磁性粉を置き、マグネツトを近づけて磁性
粉が吸着される距離において、その中間に任意の
大きさを有する第3図Aに如く、第2図に示した
同一方向を向いた複数枚のリボン片2からなる板
状体11を、例えばα〜βの方向をそろえて三段
重ねたものと、第3図Bに10として示す如く、
板状体11を二段α〜βの方向を直角にして重ね
たものとを比較したところ、板状体11の段数が
少なくても直角に重ねた場合の方が磁性粉が吸着
されないという減衰効果が得られた。この結果か
ら第3図Aのように同一方向を向いた板状体11
を更に重ねても減衰効果がほとんど得られないと
いう基本現象を確認し、一般に言われている厚さ
を厚くすれば良いというものではないことも解明
した。これによつて電磁波のシールドには、従来
のように単に平面的な網目状などにするのみでは
シールド効果が少なく、電磁波即ち放射性電磁障
害等に対してはこのリボン片2のα〜β方向の方
向性の組合せが極めて重要であり、第3図Bに示
すような組合せが特に顕著な電磁波シールド効果
を表わすことがわかつた。
Also, magnetic powder such as iron powder is placed under the N to S magnetic field of the magnet, and the magnet is brought close to the magnetic powder at a distance where the magnetic powder is attracted, and the magnetic powder has an arbitrary size in the middle, as shown in FIG. 3A. For example, the plate-shaped body 11 consisting of a plurality of ribbon pieces 2 facing the same direction shown in FIG. ,
A comparison of two plate-like bodies 11 stacked with the directions α and β at right angles revealed that magnetic powder is not adsorbed better when the plate-like bodies 11 are stacked at right angles even if the number of stages is small. It worked. From this result, as shown in FIG. 3A, the plate-like bodies 11 facing the same direction
We confirmed the basic phenomenon that even if layers are layered, little damping effect can be obtained, and also clarified that simply increasing the thickness is not the answer, as is generally said. As a result, for electromagnetic wave shielding, simply forming a planar mesh shape as in the past has little shielding effect, and for electromagnetic waves, that is, radioactive electromagnetic interference, etc., the α to β direction of this ribbon piece 2 is It has been found that the combination of directions is extremely important, and the combination shown in FIG. 3B exhibits a particularly remarkable electromagnetic shielding effect.

以上のように、本発明の高周波用電磁波シール
ド板10は、アモルフアス金属リボン1を切断し
て作成した短冊状リボン片2を、切断時の先端α
及び後端βを夫々同方向にそろえて複数枚並列
し、隣接するリボン片2の側方端部を互に一部重
ね合せ、かつ一体化して一枚の板状体11に形成
し、更に2枚の前記板状体11を夫々の板状体を
形成する短冊状リボン片2の長手方向の向きが互
にほぼ直交するように、重複・一体化して構成し
たものである。
As described above, the high-frequency electromagnetic wave shielding plate 10 of the present invention has a rectangular ribbon piece 2 created by cutting an amorphous metal ribbon 1.
A plurality of ribbon pieces 2 are arranged in parallel with their rear ends β aligned in the same direction, and the side ends of adjacent ribbon pieces 2 are partially overlapped and integrated to form a single plate-shaped body 11. The two plate-shaped bodies 11 are overlapped and integrated so that the longitudinal directions of the strip-shaped ribbon pieces 2 forming each plate-shaped body are substantially orthogonal to each other.

次に、本発明の電磁波シールド板10を利用し
たシールド装置12について説明する。
Next, a shielding device 12 using the electromagnetic wave shielding plate 10 of the present invention will be explained.

このシールド装置12は、第4図の上面図、第
5図の断面図で示すように、合成樹脂製の六角柱
状ユニツト3の集合からなるハニカム状板体をな
し、下面を一体の板状プラスチツク架台8で連結
したものを基台とし、そのユニツトに対してそれ
ぞれ一つの壁面4と、それに隣接する壁面5に、
リボン片2の方向が互に直交するように、各壁面
4,5、に本発明のシールド板10を接着した
り、又は板状体11を接着して六角柱状ユニツト
3の連続集合板状物を形成し、更に第5図に示す
ように上面6と下面6′とにシールド板10を配
設し、又夫々のユニツト3の中にはリボン片2か
らなる六角形状(五角形状や四角形状等でもよ
い))をした多角形状体7を夫々図示するように
角度及び方向を変えて斜めに交互に装入し、両面
接着テープ等で第6図に示すように固定する。第
4図及び第6図中の矢印は多角形板状体7等を構
成するリボン片2のα〜β方向の一例を示してい
る。
As shown in the top view of FIG. 4 and the cross-sectional view of FIG. The units connected by the frame 8 are used as a base, and each unit has one wall surface 4 and an adjacent wall surface 5,
The shield plate 10 of the present invention is adhered to each wall surface 4, 5 so that the directions of the ribbon pieces 2 are perpendicular to each other, or the plate-like body 11 is adhered to form a continuous plate-like assembly of hexagonal columnar units 3. Furthermore, as shown in FIG. etc.) The polygonal bodies 7 are alternately inserted obliquely at different angles and directions as shown, and fixed with double-sided adhesive tape or the like as shown in FIG. 6. The arrows in FIGS. 4 and 6 indicate an example of the α to β directions of the ribbon pieces 2 constituting the polygonal plate-shaped body 7 and the like.

このようなシールド装置は、あらゆる角度及び
方向からの放射性電磁波に対しても顕著な効果を
有するものである。身近な例としてドライヤー、
回転歯ブラシ、回転消しゴム等の回転体をテレビ
に近づけると画面が変動するが、これらを夫々上
記装置からなる箱状体に入れて発信源を密閉する
ことにより、テレビ画面は静止した。
Such a shield device has a remarkable effect against radiated electromagnetic waves from all angles and directions. A familiar example is a hair dryer,
When a rotating object such as a rotating toothbrush or a rotating eraser is brought close to the television, the screen changes; however, by placing each of these objects in a box-like body made of the above-mentioned device and sealing the source, the television screen becomes stationary.

即ち、ノイズの悪影響を完全に防止できる電磁
波シードル装置として極めて効果の高いものであ
る。例えばこの装置内の合成樹脂材料に軟質塩ビ
等を使用するときは、可とう性と有する電磁波シ
ールド装置となり、又ガラス繊維強化プラスチツ
ク等で固めることにより堅ろうで防錆・耐候性等
の特徴を具備した電磁波シールド装置となる。
In other words, it is extremely effective as an electromagnetic wave shielding device that can completely prevent the adverse effects of noise. For example, when soft PVC is used as the synthetic resin material in this device, it becomes a flexible electromagnetic shielding device, and when it is hardened with glass fiber reinforced plastic, it has features such as robustness, rust prevention, and weather resistance. It becomes an electromagnetic shielding device.

この電磁波シールド装置12の作用を図につい
て簡単に説明すると、シールドとは電磁波のエネ
ルギーを吸収したり反射させたりして、表面から
内部へのエネルギーが伝わつていくのを妨げるこ
とであつて、その電磁波のエネルギーをどの程度
減衰させることができるかということがシールド
効果である。
To briefly explain the function of this electromagnetic wave shielding device 12 with reference to the diagram, shielding absorbs or reflects the energy of electromagnetic waves and prevents the energy from being transmitted from the surface to the inside. The shielding effect is the degree to which the energy of electromagnetic waves can be attenuated.

第7図は本発明の電磁波シールド板10を利用
した前記シールド装置12の六角柱状ユニツト3
におけるを断面構造をアモルフアス金属リボンで
の電磁波減衰の作用を説明した図である。電磁エ
ネルギー9が上面6のシールド板10に衝突する
と一部は反射され他は入射し、減衰されて放射成
分として六角柱状ユニツト3内に放出される。こ
こで反射効率を高めるため斜めに設置した多角形
板状体7によつて大部分のエネルギーは反射し、
次にユニツト内の例えばリボン片2の方向が異な
る壁面4,5等によつて著しい減衰状態を生ず
る。更に反射した一部のエネルギーが隣のユニツ
ト内に入射しても、方向の異なる壁面と方向の異
なる多角形板状体7によつてほとんど減衰されて
しまう。ここで多角形板状体7を通過し弱まつた
エネルギーは、同じ方向の異なる壁面で減衰し、
残部がプラスチツク架台8を通過して下面6′の
シールド板10に到達する。上面6のシールド板
10と同様に第3図Bについて説明したような減
衰効果により反対側に放出されるエネルギーはほ
とんどなくなり、従つて低周波から高周波帯に至
るあらゆる電磁波をその方向・入射角度にかかわ
らず、90dB以上のシールド効果で吸収し悪影響
をなくすことができた。このシールド装置12は
本発明のシールド板10を利用した一例であつ
て、シールド板10を利用することにより平面的
あるいは立体的な構成によつて、程度の差はある
がすべて同様の優れた効果を奏するものである。
FIG. 7 shows a hexagonal columnar unit 3 of the shielding device 12 using the electromagnetic wave shielding plate 10 of the present invention.
FIG. 2 is a diagram illustrating the effect of electromagnetic wave attenuation in an amorphous metal ribbon whose cross-sectional structure is shown in FIG. When the electromagnetic energy 9 collides with the shield plate 10 on the upper surface 6, part of it is reflected while the other part is incident, attenuated, and emitted into the hexagonal columnar unit 3 as a radiation component. Here, most of the energy is reflected by the polygonal plate-shaped body 7 installed diagonally to increase the reflection efficiency.
A significant damping condition then occurs due to walls 4, 5, etc. in which the ribbon pieces 2 are directed in different directions, for example, within the unit. Furthermore, even if a part of the reflected energy enters the adjacent unit, it is almost attenuated by the wall surface in a different direction and the polygonal plate-shaped body 7 in a different direction. Here, the energy that passes through the polygonal plate-shaped body 7 and weakens is attenuated by different wall surfaces in the same direction,
The remainder passes through the plastic frame 8 and reaches the shield plate 10 on the lower surface 6'. As with the shield plate 10 on the top surface 6, almost no energy is emitted to the opposite side due to the attenuation effect explained with reference to FIG. However, we were able to absorb it with a shielding effect of over 90dB and eliminate any negative effects. This shield device 12 is an example of using the shield plate 10 of the present invention, and by using the shield plate 10, depending on the planar or three-dimensional configuration, the same excellent effects can be obtained although there are differences in degree. It is something that plays.

このように本発明の高周波用電磁波シールド板
は、アモルフアス金属リボンを切断して作成した
短冊状リボン片2を、切断時の先端及び後端を
夫々同方向にそろえて複数枚並列し、隣接するリ
ボン片の側方端部を互に一部重ね合せ、かつ一体
化して一枚の板状体に形成し、更に2枚の前記板
状体を夫々の板状体を形成する短冊状リボン片の
長手方向の向きが互にほぼ直交するように、重
複、一体化して構成したものであるので、リボン
片とリボン片のすき間から電磁波が漏えいするよ
うなことがなく、又一枚の板状体を形成する各リ
ボン片の先後端の方向が同一で、かつ重複される
二枚の板状体のリボン片の方向が互にほぼ直交す
ることにより、極めて薄層であるにもかかわらず
優れたシールド効果を奏することができる。
In this way, the high-frequency electromagnetic wave shielding plate of the present invention has a plurality of strip-shaped ribbon pieces 2 created by cutting an amorphous metal ribbon, arranged in parallel with the leading and trailing ends at the time of cutting aligned in the same direction, and adjacent to each other. A strip-shaped ribbon piece in which the side ends of the ribbon pieces are partially overlapped and integrated to form one plate-shaped body, and the two plate-shaped bodies are further formed to form each plate-shaped body. Since the ribbons are overlapped and integrated so that their longitudinal directions are almost perpendicular to each other, electromagnetic waves do not leak from the gaps between the ribbon pieces, and the ribbon-like The front and rear ends of each ribbon piece that forms the body are in the same direction, and the ribbon pieces of the two overlapping plate-like bodies are almost perpendicular to each other. It can provide a shielding effect.

従つて、本発明の電磁波シールド板は、これを
有効に利用することによつて、今後の産業界で大
きな効果を発揮すると共に、電波障害防止の規制
上からも、我々の生活面に寄与することは、はか
り知れないものがある。
Therefore, by making effective use of the electromagnetic shielding plate of the present invention, it will not only be highly effective in the future industry, but also contribute to our lives in terms of regulations for preventing radio interference. There is something immeasurable about this.

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

第1図はアモルフアス金属リボンの斜視図、第
2図は同一方向のリボン片からなる板状体の説明
図、第3図Aは同一方向のリボン片を有する板状
体を複数重ね合せた説明図、同Bは本発明の実施
例の説明図、第4図は本発明を利用した電磁波シ
ールド装置の上面図、第5図はその断面図、第6
図はその装置内の一ユニツトの構成図、第7図は
同装置における電磁波減衰状態の説明図である。 1……アモルフアス金属リボン、2……リボン
片、10……電磁波シールド板、11……板状
体、α……先端、β……後端。
Fig. 1 is a perspective view of an amorphous metal ribbon, Fig. 2 is an explanatory diagram of a plate-like body made up of ribbon pieces oriented in the same direction, and Fig. 3A is an illustration of a plurality of plate-like bodies having ribbon pieces oriented in the same direction stacked together. Fig. 4B is an explanatory diagram of an embodiment of the present invention, Fig. 4 is a top view of an electromagnetic shielding device using the present invention, Fig. 5 is a cross-sectional view thereof, and Fig. 6 is an explanatory diagram of an embodiment of the present invention.
The figure is a configuration diagram of one unit in the device, and FIG. 7 is an explanatory diagram of the electromagnetic wave attenuation state in the device. DESCRIPTION OF SYMBOLS 1... Amorphous metal ribbon, 2... Ribbon piece, 10... Electromagnetic shielding plate, 11... Plate-shaped body, α... Tip, β... Back end.

Claims (1)

【特許請求の範囲】[Claims] 1 アモルフアス金属リボン1を切断して作成し
た短冊状リボン片2を、切断時の先端α及び後端
βをそれぞれ同方向にそろえて複数枚並列し、隣
接するリボン片2の側方端部を互に一部重ね合
せ、かつ一体化して一枚の板状体11に形成し、
さらに2枚の前記板状体11をそれぞれの板状体
を形成する短冊状リボン片2の長手方向の向きが
互にほぼ直交するように、重複、一体化して構成
したことを特徴とする高周波用電磁波シールド
板。
1. A plurality of strip-shaped ribbon pieces 2 made by cutting an amorphous metal ribbon 1 are arranged in parallel with the cutting ends α and rear ends β aligned in the same direction, and the lateral ends of the adjacent ribbon pieces 2 are aligned. Partially overlapped with each other and integrated to form a single plate-shaped body 11,
Further, the two plate-like bodies 11 are overlapped and integrated so that the longitudinal directions of the strip-shaped ribbon pieces 2 forming each plate-like body are substantially perpendicular to each other. Electromagnetic shield plate for use.
JP3287383A 1983-03-02 1983-03-02 High frequency electromagnetic shielding device with all directivity Granted JPS59159598A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP3287383A JPS59159598A (en) 1983-03-02 1983-03-02 High frequency electromagnetic shielding device with all directivity

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP3287383A JPS59159598A (en) 1983-03-02 1983-03-02 High frequency electromagnetic shielding device with all directivity

Publications (2)

Publication Number Publication Date
JPS59159598A JPS59159598A (en) 1984-09-10
JPH025033B2 true JPH025033B2 (en) 1990-01-31

Family

ID=12370982

Family Applications (1)

Application Number Title Priority Date Filing Date
JP3287383A Granted JPS59159598A (en) 1983-03-02 1983-03-02 High frequency electromagnetic shielding device with all directivity

Country Status (1)

Country Link
JP (1) JPS59159598A (en)

Families Citing this family (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6335207A (en) * 1986-07-30 1988-02-15 平岡織染株式会社 Carpet having electromagnetic wave shield property
JP2765826B2 (en) * 1987-03-25 1998-06-18 平岡織染株式会社 Amorphous metal thin film laminated composite sheet
JP2723442B2 (en) * 1987-03-25 1998-03-09 平岡織染株式会社 Electromagnetic wave shielding amorphous metal thin film laminated sheet
JPH02215197A (en) * 1989-02-16 1990-08-28 Tokyu Constr Co Ltd Magnetic shielding panel
JPH0770855B2 (en) * 1990-11-06 1995-07-31 平岡織染株式会社 Method for forming electromagnetic wave shielding wall covering material on wall surface

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS558318U (en) * 1978-07-04 1980-01-19

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS558318U (en) * 1978-07-04 1980-01-19

Also Published As

Publication number Publication date
JPS59159598A (en) 1984-09-10

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