JPH0513979A - Electromagnetic shielding body - Google Patents

Electromagnetic shielding body

Info

Publication number
JPH0513979A
JPH0513979A JP3193506A JP19350691A JPH0513979A JP H0513979 A JPH0513979 A JP H0513979A JP 3193506 A JP3193506 A JP 3193506A JP 19350691 A JP19350691 A JP 19350691A JP H0513979 A JPH0513979 A JP H0513979A
Authority
JP
Japan
Prior art keywords
conductor
magnet
electromagnetic shield
rod
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.)
Pending
Application number
JP3193506A
Other languages
Japanese (ja)
Inventor
Takashi Harada
高志 原田
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 JP3193506A priority Critical patent/JPH0513979A/en
Publication of JPH0513979A publication Critical patent/JPH0513979A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To provide an electromagnetic shielding body around the joint or the door of a metal case so as to prevent electromagnetic wave from leaking out of the metal case concerned. CONSTITUTION:An electromagnetic shielding body 1 is of integral structure composed of a conductor rod 5 provided with a groove U-shaped in cross section and a magnetic substance 2 formed of a rod-like magnetic substance 3 and a rod-like magnet 4 and filled into the groove provided to the conductor 5. As the rod-like magnet 4 is magnetized in a direction vertical to the lengthwise direction, the rod-like magnetic substance 3 kept in contact with the rod-like magnet 4 is magnetized in a crosssectional direction. Therefore, the shielding body 1 becomes high in magnetic permeability to a magnetic component in the lengthwise direction of the magnetic substance, so that it enables leakage electromagnetic waves possessed of a magnetic field component in the same direction to be much attenuated. Therefore, a metal case mounted with an electromagnetic shielding body of this design is not required to be equipped with a special structure so as to come into tight contact with the shielding body and has an enough shielding effect to a electromagnetic wave source of low impedance.

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、電子機器から放射され
る不要電磁波の抑制や電磁遮へい室に使用して電磁波の
漏洩,侵入を防止する電磁遮へい体に関し、特に金属筐
体の継目部や電磁遮へい室の扉部に使用して継目や扉の
周囲に生じた隙間から漏洩する電磁波を抑制する電磁遮
へい体に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an electromagnetic shield for suppressing unnecessary electromagnetic waves radiated from electronic equipment and for preventing electromagnetic waves from leaking or entering by being used in an electromagnetic shield room, and more particularly to a joint portion of a metal casing or The present invention relates to an electromagnetic shield that is used in a door portion of an electromagnetic shield room to suppress electromagnetic waves leaking from a seam or a gap around the door.

【0002】[0002]

【従来の技術】電磁遮へいに際し、一般に金属等の導体
同士が接触する箇所は部分的に導電率が低くなるため、
電磁波が漏洩しやすくなり、金属等の導体同士の接触部
に電磁遮へい体を設置して漏洩する電磁波を抑制する必
要がある。
2. Description of the Related Art When electromagnetic shielding is performed, the conductivity of a conductor such as a metal is generally low at a portion of the conductor.
Electromagnetic waves tend to leak, and it is necessary to install an electromagnetic shield at the contact portion between conductors such as metals to suppress the leaking electromagnetic waves.

【0003】従来のこの種の電磁遮へい体は、図14
(a)の断面図、(b)の斜視図に示すような金属片を
櫛形に構成したシールドフィンガー51、あるいは図1
5(a)の断面図、(b)の斜視図に示すような導電性
ゴムを管状にしたEMIガスケット52などの導電性電
磁遮へい材が知られている(“電磁シールドとアース系
の要点”、日本工業技術センター刊参照)。図14に示
す電磁遮へい体は、金属片のバネ作用を利用したもので
あり、図15に示す電磁遮へい体は、導電性ゴムの弾力
性を利用したものである。いずれも導体同士の接触部に
介装し、その導電率の向上に用いられる。
A conventional electromagnetic shield of this type is shown in FIG.
1A is a cross-sectional view and FIG. 1B is a perspective view.
A conductive electromagnetic shielding material such as an EMI gasket 52 in which a conductive rubber is tubular as shown in the sectional view of FIG. 5 (a) and the perspective view of (b) is known (“Key points of electromagnetic shield and earth system”). , See Japan Industrial Technology Center). The electromagnetic shield shown in FIG. 14 utilizes the spring action of a metal piece, and the electromagnetic shield shown in FIG. 15 utilizes the elasticity of conductive rubber. Both of them are interposed between the contact portions of the conductors and are used for improving the conductivity thereof.

【0004】[0004]

【発明が解決しようとする課題】ところが、図14,図
15に示す導電性の電磁遮へい材は、シールドフィンガ
ー51,ガスケット52と筐体,電磁遮へい室の取り付
け部、もしくはシールドフィンガー51,ガスケット5
2と接触する導体部との間の接触抵抗の大きさが電磁波
の漏洩効果に影響を与えるため、接触を強化するための
機構が必要であった。さらに、シールドフィンガー5
1,ガスケット52を用いた場合、バネ作用や弾力性の
経年変化が遮へい効果の低下を招くという問題がある。
However, the conductive electromagnetic shield material shown in FIGS. 14 and 15 is the shield finger 51, the gasket 52 and the housing, the mounting portion of the electromagnetic shield chamber, or the shield finger 51 and the gasket 5.
Since the magnitude of the contact resistance between the conductor portion 2 and the conductor portion that contacts 2 influences the leakage effect of electromagnetic waves, a mechanism for strengthening the contact was necessary. Furthermore, shield finger 5
1. When the gasket 52 is used, there is a problem that the secular change in spring action and elasticity causes a decrease in the shielding effect.

【0005】また、大電流小電圧形の低インピーダンス
の電磁波源に対して低周波帯において、遮へい効果が小
さくなる(電子情報通信学会技術研究報告,EMCJ9
0−48参照)という問題点があった。
Further, the shielding effect is reduced in the low frequency band with respect to the electromagnetic wave source of large current and small voltage type and low impedance (Technical Research Report of IEICE, EMCJ9).
0-48).

【0006】本発明の目的は、金属筐体の継目部や扉の
周囲に用いて電磁波の漏洩を抑制する電磁遮へい体、特
に接触を強化するために特別の機構を必要とせず、また
低インピーダンスの電磁波源に対しても低周波帯で十分
な遮へい効果を得る電磁遮へい体を提供することにあ
る。
An object of the present invention is to provide an electromagnetic shield for suppressing leakage of electromagnetic waves, which is used around a joint portion of a metal housing or a door, and in particular, does not require a special mechanism for strengthening the contact and has a low impedance. Another object of the present invention is to provide an electromagnetic shield that can sufficiently shield the electromagnetic wave source in the low frequency band.

【0007】[0007]

【課題を解決するための手段】上記目的を達成するた
め、第1の発明による電磁遮へい体においては、導体
と、磁性体とを有する電磁遮へい体であって、導体は、
棒状または板状であり、その長さ方向に溝が形成され、
磁性体は、前記導体の溝内に配置され、該溝の長さ方向
に垂直な方向の磁場が印加されるものである。
In order to achieve the above object, the electromagnetic shield according to the first invention is an electromagnetic shield having a conductor and a magnetic body, the conductor comprising:
It is rod-shaped or plate-shaped, with grooves formed in its lengthwise direction,
The magnetic body is arranged in the groove of the conductor, and a magnetic field in a direction perpendicular to the length direction of the groove is applied.

【0008】また、第2の発明においては、導体と磁性
体とを有する電磁遮へい体であって、導体と磁性体とは
棒状をなし、交互に並べて配置され、磁性体は、導体の
長さ方向に垂直な方向の磁場が印加されるものである。
In the second aspect of the invention, there is provided an electromagnetic shield having a conductor and a magnetic body, wherein the conductor and the magnetic body are rod-shaped and arranged alternately, and the magnetic bodies are the length of the conductor. A magnetic field in a direction perpendicular to the direction is applied.

【0009】また、第3の発明においては、導体と、磁
石と、磁性体とを有する電磁遮へい体であって、導体
は、棒状または板状であり、その長さ方向に溝が形成さ
れ、磁石及び磁性体は、構造体に組合されて前記導体の
溝内に埋め込まれて導体と一体化されたものであり、磁
石は、前記溝の長さ方向に垂直な向きに磁化されたもの
であり、磁性体は、前記磁石の磁化面に接して配設され
たものである。
According to the third aspect of the invention, there is provided an electromagnetic shield having a conductor, a magnet, and a magnetic body, wherein the conductor is rod-shaped or plate-shaped, and a groove is formed in the longitudinal direction thereof. The magnet and the magnetic body are combined with the structure, embedded in the groove of the conductor and integrated with the conductor, and the magnet is magnetized in a direction perpendicular to the length direction of the groove. The magnetic body is disposed in contact with the magnetized surface of the magnet.

【0010】また、第4の発明においては、導体と磁石
と磁性体とを有する電磁遮へい体であって、導体は、棒
状または板状であり、磁石と磁性体とは棒状または板状
の構造体に組合され、導体と構造体とは交互に並べて一
体化されたものであり、磁石は、導体の長さ方向に垂直
な向きに磁化されたものであり、磁性体は、前記磁石の
磁化面に接して配設されたものである。
According to a fourth aspect of the present invention, there is provided an electromagnetic shield having a conductor, a magnet and a magnetic body, wherein the conductor has a rod or plate shape, and the magnet and the magnetic body have a rod or plate structure. The magnet is magnetized in a direction perpendicular to the longitudinal direction of the conductor, and the magnet is magnetized by the magnet. It is arranged in contact with the surface.

【0011】また、第5の発明においては、前記第4の
発明の導体の一部もしくは全てが弾力性を有する電磁遮
へい材である。
In the fifth invention, part or all of the conductor of the fourth invention is an electromagnetic shielding material having elasticity.

【0012】また、第6の発明においては、導体と、磁
石と、磁性体とを有する電磁遮へい体であって、導体
は、少なくともその一部に弾力性を有する導電性電磁遮
へい材を有するものであり、導電性電磁遮へい材には、
その一部に一列もしくは複数列の溝を有し、磁石及び磁
性体は、構造体に組合されて前記導電性電磁遮へい材の
溝内に埋め込まれ、磁石は、前記溝の長さ方向に垂直な
向きに磁化されたものであり、磁性体は、前記磁石の磁
化面に接して配設されたものである。
Further, in the sixth invention, an electromagnetic shield having a conductor, a magnet, and a magnetic body, wherein the conductor has a conductive electromagnetic shield having elasticity in at least a part thereof. And the conductive electromagnetic shielding material is
Part of it has one or more rows of grooves, the magnet and magnetic body are combined with the structure and embedded in the groove of the conductive electromagnetic shielding material, and the magnet is perpendicular to the length direction of the groove. The magnetic body is magnetized in any direction, and the magnetic body is disposed in contact with the magnetized surface of the magnet.

【0013】また、第7の発明においては、導体と磁性
体とを有する電磁遮へい体であって、導体は、導電性を
有する磁石であり、磁性体は、棒状または板状をなし、
導電性を有する磁石は、磁性体をはさむように配置さ
れ、該磁性体をはさむ対向二面が互いに異なる極性に磁
化されたものである。
According to the seventh aspect of the invention, there is provided an electromagnetic shield having a conductor and a magnetic body, the conductor being a magnet having conductivity, and the magnetic body having a rod shape or a plate shape.
The magnet having conductivity is arranged so as to sandwich a magnetic body, and two opposing surfaces sandwiching the magnetic body are magnetized to have polarities different from each other.

【0014】また、第8の発明においては、導体と、磁
性体と、磁石とを有する電磁遮へい体であって、導体
は、棒状または板状であり、その長さ方向に溝を有し、
磁性体と磁石とは、構造体に組合されて前記導体の溝内
に埋め込まれ、磁石は、導電性を有する磁石であり、前
記溝の長さ方向に垂直な向きに磁化され、磁性体は、導
電性を有する磁石の磁化面に接触し、磁性体及び導電性
を有する磁石の一部の面は、導体表面に露出させたもの
である。
Further, in the eighth aspect of the present invention, there is provided an electromagnetic shield having a conductor, a magnetic body and a magnet, wherein the conductor is rod-shaped or plate-shaped, and has a groove in its lengthwise direction.
The magnetic body and the magnet are combined into a structure and embedded in the groove of the conductor, the magnet is a magnet having conductivity, and is magnetized in a direction perpendicular to the longitudinal direction of the groove, and the magnetic body is The magnetic body and a part of the surface of the magnet having conductivity are in contact with the magnetized surface of the magnet having conductivity, and are exposed on the surface of the conductor.

【0015】また、第9の発明においては、前記第8の
発明の導体もしくは、前記導体に電気的に接触する導電
性を有する磁石の一部に導電性電磁遮へい材を有し、前
記導体と前記導電性電磁遮へい材とは、直接もしくは前
記導電性を有する磁石を介して電気的に接触させたもの
である。
According to a ninth aspect of the invention, the conductor of the eighth aspect of the invention or a part of a magnet having electrical conductivity that electrically contacts the conductor has a conductive electromagnetic shielding material, The conductive electromagnetic shielding material is one that is electrically contacted directly or through the magnet having the conductivity.

【0016】本発明において、電磁遮へい体を構成する
棒状または板状の導体或いは磁性体の断面、また溝の断
面の形状は矩形,長方形,細長い長方形,円形,楕円
形,三角形,多角形等用途に応じて自由に設計できる。
例えばコの字やH字形,L字形の断面の導体を用いるこ
とができる。
In the present invention, the cross section of the rod-shaped or plate-shaped conductor or magnetic material constituting the electromagnetic shield and the cross section of the groove are rectangular, rectangular, elongated rectangular, circular, elliptical, triangular, polygonal, etc. Can be freely designed according to.
For example, a U-shaped, H-shaped, or L-shaped conductor can be used.

【0017】[0017]

【作用】図13(a)に示すように、棒状導体46と棒
状磁性体42とを交互に並べた構造44、もしくは、図
13(b)に示すような弾力性を有する導電性電磁遮へ
い材43に溝を設け、磁性体42を埋め込んだ構造41
の電磁遮へい体は、低インピーダンスな波源をもつ金属
筐体の隙間部用遮へい体として有効である。この種の電
磁遮へい体の遮へい効果は、埋め込んだ磁性体の透磁率
特性に大きく依存し、透磁率が大きいほど遮へい効果も
大きくなることが知られている(電子情報通信学会技術
研究報告,EMCJ90−48参照)。
As shown in FIG. 13A, a structure 44 in which rod-shaped conductors 46 and rod-shaped magnetic bodies 42 are alternately arranged, or a conductive electromagnetic shield having elasticity as shown in FIG. 13B. Structure 41 in which a groove is provided in 43 and a magnetic body 42 is embedded
The electromagnetic shield of (1) is effective as a shield for a gap in a metal casing having a low-impedance wave source. It is known that the shielding effect of this type of electromagnetic shield largely depends on the magnetic permeability characteristics of the embedded magnetic body, and the greater the magnetic permeability, the greater the shielding effect (Technical Research Report of IEICE, EMCJ90). -48).

【0018】一方、フェライト焼結体などの磁性体に直
流磁化を印加した場合、磁化と垂直な方向の磁界成分に
対応する高周波透磁率は大きくなる(電子情報通信学会
技術研究報告,EMCJ87−82参照)。
On the other hand, when DC magnetization is applied to a magnetic material such as a ferrite sintered body, the high frequency magnetic permeability corresponding to the magnetic field component in the direction perpendicular to the magnetization increases (Technical Research Report of the Institute of Electronics, Information and Communication Engineers, EMCJ87-82). reference).

【0019】したがって、図13(a)、または図13
(b)に示すような磁性体の断面方向に平行に直流磁界
47もしくは48を印加できれば、磁性体の長さ方向の
磁界に対する高周波透磁率が大きくなり、同方向の磁界
成分を有する漏洩電磁波49に対する遮へい効果を高め
ることができる。
Therefore, as shown in FIG.
If a DC magnetic field 47 or 48 can be applied parallel to the cross-sectional direction of the magnetic body as shown in (b), the high-frequency magnetic permeability with respect to the magnetic field in the longitudinal direction of the magnetic body becomes large, and the leakage electromagnetic wave 49 having a magnetic field component in the same direction 49. It is possible to enhance the shielding effect against.

【0020】[0020]

【実施例】以下に本発明の実施例を図面を参照して説明
する。
Embodiments of the present invention will be described below with reference to the drawings.

【0021】(実施例1)図1は、本発明の第1の実施
例を示す斜視図である。本実施例の電磁遮へい体1は、
断面がコの字形の棒状導体5において、その凹部に合致
するように棒状磁性体3と棒状磁石4とで構成された磁
性体部2を埋め込み一体化した構造である。
(Embodiment 1) FIG. 1 is a perspective view showing a first embodiment of the present invention. The electromagnetic shield 1 of this embodiment is
This is a structure in which a bar-shaped conductor 5 having a U-shaped cross section is embedded and integrated with a magnetic body portion 2 composed of a bar-shaped magnetic body 3 and a bar-shaped magnet 4 so as to match the recess.

【0022】棒状磁石4は、図2の断面図に示すよう
に、長さ方向に垂直に磁化されているため、棒状磁石4
に接触している棒状磁性体3も断面方向に磁化される。
したがって、磁性体の長さ方向の磁界成分に対する透磁
率は大きくなり、同方向の磁界成分を有する漏洩電磁波
の減衰を大きくできる。
As shown in the cross-sectional view of FIG. 2, the bar-shaped magnet 4 is magnetized perpendicularly to the longitudinal direction, so that the bar-shaped magnet 4 is
The rod-shaped magnetic body 3 in contact with is also magnetized in the cross-sectional direction.
Therefore, the magnetic permeability of the magnetic substance with respect to the magnetic field component in the length direction is increased, and the attenuation of the leaked electromagnetic wave having the magnetic field component in the same direction can be increased.

【0023】磁性体部2は、図3(a)の断面図に示す
ように複数の棒状磁性体3と複数の棒状磁石4を交互に
並べた構造としてもよい。この際、棒状磁石4は棒状磁
性体3が断面方向に磁化されるよう棒状磁性体3をはさ
んで対向する面の極性が互いに異なるように配置する。
また図3(b)のように磁性体部2は、棒状磁性体3と
棒状磁性体3との境界面が棒状導体5の凹部の底辺に垂
直になる構造としてもよい。あるいは境界面が図3
(c)のように斜めであってもよい。また棒状導体5
は、断面がL字形のものとしてもよく、さらにH字形の
ものとし双方の凹部に磁性体部2を埋め込んだ構造とし
てもよい。
The magnetic body portion 2 may have a structure in which a plurality of bar-shaped magnetic bodies 3 and a plurality of bar-shaped magnets 4 are alternately arranged as shown in the sectional view of FIG. At this time, the rod-shaped magnets 4 are arranged so that the rod-shaped magnetic bodies 3 are magnetized in the cross-sectional direction such that the surfaces of the rod-shaped magnetic bodies 3 facing each other have different polarities.
Further, as shown in FIG. 3B, the magnetic body portion 2 may have a structure in which the boundary surface between the rod-shaped magnetic bodies 3 is perpendicular to the bottom of the recessed portion of the rod-shaped conductor 5. Or the boundary surface is
It may be oblique as in (c). Also, the rod-shaped conductor 5
May have an L-shaped cross section, or may have an H-shaped cross section and have a structure in which the magnetic body portions 2 are embedded in both recesses.

【0024】図4は、磁性体部2と、棒状導体6とを交
互に並べた構造の電磁遮へい体の例である。複数の磁性
体部2と複数の棒状導体6とを交互に配置した構造とし
てもよい。棒状磁性体3には焼結フェライト材,フェラ
イト粉末を混入した高分子材,磁性アモルファス合金や
パーマロイ等の磁性合金により構成されるが、広帯域な
遮へい特性を得るためには高周波帯で透磁率の低下の小
さい焼結フェライト材が適当である。棒状磁石4は複数
の磁石を磁極の向きが一致するよう一列に並べ棒状構造
としてもよい。
FIG. 4 shows an example of an electromagnetic shield having a structure in which the magnetic material portions 2 and the rod-shaped conductors 6 are alternately arranged. A structure in which a plurality of magnetic body portions 2 and a plurality of rod-shaped conductors 6 are alternately arranged may be adopted. The rod-shaped magnetic body 3 is composed of a sintered ferrite material, a polymer material mixed with ferrite powder, or a magnetic alloy such as a magnetic amorphous alloy or permalloy. A sintered ferrite material with a small decrease is suitable. The rod-shaped magnet 4 may have a rod-shaped structure in which a plurality of magnets are arranged in a line so that the directions of the magnetic poles are the same.

【0025】図5は、棒状導体5の一部に弾力性を有す
る導電性電磁遮へい材7を設けた構造の電磁遮へい体8
の斜視図である。この構造では、導電性電磁遮へい材7
により導体間に生じた隙間を塞ぐことで高周波帯での遮
へい特性が改善され、広帯域な遮へい効果を得ることが
できる。導電性電磁遮へい材7は、導電性ゴムやポリウ
レタンフォーム材を銀コーティングした布で被覆した構
造の導電性ガスケット材、または導電フィンガーなど弾
力性のある導電材料にて構成する。
FIG. 5 shows an electromagnetic shield 8 having a structure in which a conductive electromagnetic shield 7 having elasticity is provided on a part of the rod-shaped conductor 5.
FIG. In this structure, the conductive electromagnetic shield 7
By closing the gap generated between the conductors, the shielding characteristics in the high frequency band are improved, and a wideband shielding effect can be obtained. The conductive electromagnetic shield 7 is made of a conductive gasket material having a structure in which conductive rubber or polyurethane foam material is coated with silver, or a conductive material having elasticity such as conductive fingers.

【0026】また、図4に示す構造において、一部もし
くはすべての棒状導体6を導電性電磁遮へい材と置き換
えた構造としても同様の効果が得られる。本電磁遮へい
体8は従来の導電性電磁遮へい材とは異なり、接触状態
の遮へい効果への影響が小さい。
Further, in the structure shown in FIG. 4, the same effect can be obtained even if some or all of the rod-shaped conductors 6 are replaced with a conductive electromagnetic shielding material. Unlike the conventional conductive electromagnetic shield material, the electromagnetic shield 8 has little influence on the shield effect in the contact state.

【0027】(実施例2)図6は、本発明の第2の実施
例を示す斜視図である。本実施例の電磁遮へい体11
は、断面形状がコの字形の弾力性を有する導電性電磁遮
へい材15において、その凹部に合致するように棒状磁
性体13と棒状磁石14からなる磁性体部12を組み込
み一体化した構造である。棒状磁石14は、長さ方向に
垂直に磁化されている。棒状磁性体13は、棒状磁石1
4の磁界面に接触して配置されるため、断面方向に磁化
している。そのため、長さ方向の磁界に対する透磁率が
大きくなり、同方向の磁界成分を有する漏洩電磁波は大
幅に減衰する。磁性体部12は、複数の棒状磁性体13
と複数の棒状磁石14とを交互に並べた構造としてもよ
い。この場合、棒状磁石14は、棒状磁性体13の磁化
の向きが断面方向になるよう棒状磁性体13をはさんで
対向する面の磁極が互いに異なるように配置する。
(Second Embodiment) FIG. 6 is a perspective view showing a second embodiment of the present invention. Electromagnetic shield 11 of this embodiment
Is a structure in which a magnetic material portion 12 composed of a rod-shaped magnetic body 13 and a rod-shaped magnet 14 is incorporated and integrated in a conductive electromagnetic shield 15 having a U-shaped cross-section and having elasticity so as to match the recess. . The bar magnet 14 is magnetized perpendicularly to the length direction. The rod-shaped magnetic body 13 is the rod-shaped magnet 1
Since it is arranged in contact with the magnetic field surface of No. 4, it is magnetized in the cross-sectional direction. Therefore, the magnetic permeability with respect to the magnetic field in the length direction increases, and the leaked electromagnetic wave having the magnetic field component in the same direction is significantly attenuated. The magnetic body portion 12 includes a plurality of rod-shaped magnetic bodies 13
And a plurality of bar-shaped magnets 14 may be alternately arranged. In this case, the rod-shaped magnets 14 are arranged such that the magnetic poles on the surfaces facing each other sandwiching the rod-shaped magnetic body 13 are different from each other so that the magnetization direction of the rod-shaped magnetic body 13 is the cross-sectional direction.

【0028】また、図7に示すように、棒状磁性体13
と棒状磁石14との境界面が導電性電磁遮へい材15の
凹部の底辺に垂直になるような配置としてもよい。導電
性電磁遮へい材15は、断面がHの字形のものを利用
し、それぞれの凹部に磁性体部12を埋め込んだ構造と
してもよい。本実施例による電磁遮へい体11は、金属
や良導体で構成された筐体等の隙間部に適用する際、隙
間を構成する導体壁面との接触部と磁性体部12が埋め
込まれている部分とが一致するように配置することで磁
性体の作用により低周波帯、導電性の接触の効果により
高周波帯が遮へいできるため、広帯域な遮へい効果を得
ることができる。
Further, as shown in FIG. 7, the rod-shaped magnetic body 13
The boundary surface between the bar magnet 14 and the bar-shaped magnet 14 may be arranged so as to be perpendicular to the bottom of the recess of the conductive electromagnetic shield 15. The conductive electromagnetic shielding material 15 may be one having an H-shaped cross section, and the magnetic material portion 12 may be embedded in each recess. When the electromagnetic shield 11 according to the present embodiment is applied to a gap portion such as a case made of metal or a good conductor, it has a contact portion with a conductor wall surface forming the gap and a portion in which the magnetic body portion 12 is embedded. By arranging so that they coincide with each other, a low frequency band can be shielded by the action of the magnetic material, and a high frequency band can be shielded by the effect of conductive contact, so that a broadband shielding effect can be obtained.

【0029】(実施例3)図8は、本発明の第3の実施
例を示す斜視図である。本実施例の電磁遮へい体21
は、棒状磁性体22を導電性を有する棒状磁石23の対
間に挾み、一体化した構造である。棒状磁石23は、導
電性を有しているため、低インピーダンス波源に対する
低周波帯の電磁遮へい体として有効である。
(Third Embodiment) FIG. 8 is a perspective view showing a third embodiment of the present invention. The electromagnetic shield 21 of this embodiment
Is a structure in which the rod-shaped magnetic body 22 is sandwiched between a pair of conductive rod-shaped magnets 23 and integrated. Since the bar-shaped magnet 23 has conductivity, it is effective as a low-frequency electromagnetic shield for a low-impedance wave source.

【0030】さらに図9の断面図に示すように、棒状磁
性体22をはさむ二つの棒状磁石23は、長さ方向に垂
直に磁化されており、かつ、互いに極性の異なる面が対
向するように配置されているため、棒状磁石23は、断
面方向に磁化され、長さ方向の磁界に対する透磁率が大
きくなり、同方向の磁界成分を有する漏洩電磁波の遮へ
い特性を大幅に改善できる。棒状磁石23は、複数の磁
石を互いに磁極の向きが一致するように並べ棒状に構成
してもよい。棒状磁石23は、サマリウムコバルト磁石
のように導電性を有する磁石で構成するが、非導電性の
磁石に金属メッキなどの導電メッキを施したものを用い
ても良い。
Further, as shown in the sectional view of FIG. 9, the two bar-shaped magnets 23 sandwiching the bar-shaped magnetic body 22 are magnetized perpendicularly to the longitudinal direction, and the surfaces having different polarities face each other. Since the bar-shaped magnets 23 are arranged, the bar-shaped magnets 23 are magnetized in the cross-sectional direction, the magnetic permeability in the longitudinal direction is increased, and the shielding property of the leaked electromagnetic wave having the magnetic field component in the same direction can be significantly improved. The rod-shaped magnet 23 may be formed by arranging a plurality of magnets in a rod shape so that the directions of the magnetic poles thereof are aligned with each other. The rod-shaped magnet 23 is made of a conductive magnet such as a samarium-cobalt magnet, but a non-conductive magnet having conductive plating such as metal plating may be used.

【0031】また導電性を有する棒状磁石23の一部に
図10の斜視図に示すように、導電性電磁遮へい材25
を設け、導電性を有する棒状磁石23と導電性電磁遮へ
い材25とが電気的に接触した構造の電磁遮へい体24
は、導電性電磁遮へい材25により導体間に生じた隙間
を塞ぐように配置することで、高周波特性が改善され、
広帯域な遮へい特性を得ることができる。本電磁遮へい
体24は、従来の導電性電磁遮へい材とは異なり、接触
状態の遮へい効果への影響が小さい。
Further, as shown in the perspective view of FIG. 10, a part of the conductive bar magnet 23 has a conductive electromagnetic shield 25.
The electromagnetic shield 24 having a structure in which the bar-shaped magnet 23 having conductivity and the conductive electromagnetic shield 25 are in electrical contact with each other.
Is arranged so as to close the gap generated between the conductors by the conductive electromagnetic shielding material 25, so that the high frequency characteristics are improved,
Wideband shielding characteristics can be obtained. Unlike the conventional conductive electromagnetic shield material, the electromagnetic shield 24 has little influence on the shielding effect in the contact state.

【0032】(実施例4)図11は、本発明の第4の実
施例を示す斜視図である。本実施例の電磁遮へい体31
は、断面形状がコの字形を有する棒状導体35の凹部
に、その凹部に合致する断面を有し、かつ長さ方向に垂
直な向きに磁化した導電性を有する棒状磁石34と、こ
の棒状磁石34の磁化面に接触する棒状磁性体33とを
交互に並べて一体化してなる磁性体部32を組み込んだ
構造である。棒状磁性体33と導電性を有する棒状磁石
34との境界面は、棒状導体35の凹部の底辺に垂直と
する。棒状磁石34は、棒状磁性体33をはさんで対向
する二つの面の極性が互いに異なるように配置し、棒状
磁性体33を長さ方向に垂直な向きに磁化する。そのた
め棒状磁性体33の長さ方向の磁界に対する透磁率が大
きくなり、同方向の磁界成分を有する漏洩電磁波の遮へ
い効果が大きくなる。棒状磁性体33は、断面積が小さ
くなるように細く多数に分割し、棒状磁石34と交互に
並べることで反磁界の影響を小さくし、実効的な透磁率
の低下を抑え、良好な遮へい効果を保つことができる。
導電性を有する棒状磁石34は、サマリウムコバルト磁
石のように導電性を有する磁石で構成するが、非導電性
の磁石に金属メッキなどの導電メッキを施したものを用
いても良い。また導電性磁石を磁極の向きが一致するよ
うに多数並べ、棒状としたものを用いてもよい。
(Fourth Embodiment) FIG. 11 is a perspective view showing a fourth embodiment of the present invention. Electromagnetic shield 31 of this embodiment
Is a rod-shaped magnet 34 having a U-shaped cross-section in the concave portion of the rod-shaped conductor 35, having a cross-section that matches the concave portion, and magnetized in a direction perpendicular to the longitudinal direction, and the rod-shaped magnet 34. This is a structure in which a magnetic body portion 32 formed by alternately arranging and integrating rod-shaped magnetic bodies 33 contacting the magnetized surface of 34 is incorporated. The boundary surface between the rod-shaped magnetic body 33 and the rod-shaped magnet 34 having conductivity is perpendicular to the bottom of the recess of the rod-shaped conductor 35. The rod-shaped magnet 34 is arranged such that two surfaces facing each other with the rod-shaped magnetic body 33 sandwiched therebetween have polarities different from each other, and magnetizes the rod-shaped magnetic body 33 in a direction perpendicular to the longitudinal direction. Therefore, the magnetic permeability of the rod-shaped magnetic body 33 with respect to the magnetic field in the longitudinal direction increases, and the effect of shielding leaked electromagnetic waves having a magnetic field component in the same direction increases. The rod-shaped magnetic body 33 is divided into a number of small pieces so as to have a small cross-sectional area, and the rod-shaped magnets 34 are alternately arranged to reduce the effect of the demagnetizing field, suppress the effective decrease in magnetic permeability, and provide a good shielding effect. Can be kept.
The conductive bar-shaped magnet 34 is composed of a conductive magnet such as a samarium-cobalt magnet, but a non-conductive magnet plated with conductive material such as metal plating may be used. Further, a large number of conductive magnets may be arranged so that the directions of the magnetic poles are aligned to form a rod shape.

【0033】図12は、棒状導体35もしくは導電性を
有する棒状磁石34の一部に弾力性のある導電性電磁遮
へい材37を設け、前記棒状導体35もしくは前記導電
性を有する棒状磁石34と導電性電磁遮へい材37とが
電気的に接触した構造の電磁遮へい体36の斜視図であ
る。この電磁遮へい体36を、筐体隙間に適用した際、
導電性電磁遮へい材37により導体間の隙間を塞ぐよう
に配置すれば、高周波特性が改善され、広帯域な遮へい
特性が得られる。本電磁遮へい体36は、従来の導電性
電磁遮へい材と異なり接触状態の遮へい効果への影響が
小さい。
In FIG. 12, a conductive conductive electromagnetic shield 37 having elasticity is provided on a part of the bar-shaped conductor 35 or the bar-shaped magnet 34 having conductivity, and the bar-shaped conductor 35 and the bar-shaped magnet 34 having conductivity are electrically connected to each other. 3 is a perspective view of an electromagnetic shield 36 having a structure in which a conductive electromagnetic shield 37 is in electrical contact with the electromagnetic shield 36. FIG. When this electromagnetic shield 36 is applied to the gap of the housing,
If the conductive electromagnetic shielding material 37 is arranged so as to close the gap between the conductors, the high frequency characteristic is improved and the broadband shielding characteristic is obtained. Unlike the conventional conductive electromagnetic shield material, the electromagnetic shield 36 has little influence on the shielding effect in the contact state.

【0034】本実施例では、磁性体に磁場を印加する手
段として棒状磁石等を用いたが電磁石を用いてもよい。
また磁性体と磁石の間にスペーサをはさんだ構造であっ
てよく、両者が接している必要はない。
In this embodiment, a bar magnet or the like is used as a means for applying a magnetic field to the magnetic material, but an electromagnet may be used.
Further, the structure may be such that a spacer is sandwiched between the magnetic body and the magnet, and it is not necessary that both are in contact with each other.

【0035】本発明はコンピュータや交換機,通信機器
のラック,キャビネ等の圧体や電子部品モジュールやシ
ャーシ等、電子機器全般に適用できる。
The present invention can be applied to general electronic equipment such as computers, exchanges, communication equipment racks, pressure bodies such as cabinets, electronic component modules and chassis.

【0036】[0036]

【発明の効果】以上説明したように本発明による電磁遮
へい体によれば、接触の影響が小さいため、金属筐体の
隙間,継目部などに応用した際に、接触を強化するため
の機構を必要とせず、効率的な遮へい対策を行える効果
を有する。また、本発明による遮へい体は、従来の導電
性電磁遮へい材に比して漏洩電流の抑制効果が大きいた
め、誘起電流の生じやすい低インピーダンス波源の遮へ
いに対し大幅な改善が図られる。
As described above, according to the electromagnetic shield according to the present invention, the influence of the contact is small. Therefore, a mechanism for strengthening the contact when applied to a gap or a joint portion of a metal housing is provided. It has the effect that effective shielding measures can be taken without the need. Further, the shield according to the present invention has a greater effect of suppressing the leakage current as compared with the conventional conductive electromagnetic shield material, so that the shield of the low impedance wave source where an induced current is likely to occur is significantly improved.

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

【図1】本発明の第1の実施例を示す斜視図である。FIG. 1 is a perspective view showing a first embodiment of the present invention.

【図2】第1の実施例の断面図である。FIG. 2 is a sectional view of the first embodiment.

【図3】(a),(b),(c)は、磁性体の配置例を
示す図である。
3 (a), (b) and (c) are diagrams showing an arrangement example of magnetic bodies.

【図4】磁性体部と、棒状導体との組合せ構造の他の例
を示す図である。
FIG. 4 is a diagram showing another example of a combined structure of a magnetic body portion and a rod-shaped conductor.

【図5】棒状導体の一部に弾力性を有する導電性遮へい
材を設けた例を示す図である。
FIG. 5 is a diagram showing an example in which a conductive shield having elasticity is provided on a part of a rod-shaped conductor.

【図6】第2の実施例を示す斜視図である。FIG. 6 is a perspective view showing a second embodiment.

【図7】棒状磁性体と棒状磁石との組合せの他の例を示
す図である。
FIG. 7 is a diagram showing another example of a combination of a rod-shaped magnetic body and a rod-shaped magnet.

【図8】第3の実施例を示す図である。FIG. 8 is a diagram showing a third embodiment.

【図9】第3の実施例の断面図である。FIG. 9 is a sectional view of a third embodiment.

【図10】導電性電磁遮へい材を付設した例を示す図で
ある。
FIG. 10 is a diagram showing an example in which a conductive electromagnetic shielding material is attached.

【図11】第4の実施例を示す図である。FIG. 11 is a diagram showing a fourth embodiment.

【図12】弾力性のある導電性電磁遮へい材を付設した
例を示す図である。
FIG. 12 is a view showing an example in which an elastic conductive electromagnetic shield material is attached.

【図13】本発明の作用を示す図である。FIG. 13 is a diagram showing the operation of the present invention.

【図14】従来の電磁遮へい体を示す図である。FIG. 14 is a diagram showing a conventional electromagnetic shield.

【図15】従来の電磁遮へい体を示す図である。FIG. 15 is a view showing a conventional electromagnetic shield.

【符号の説明】[Explanation of symbols]

1 電磁遮へい体 2 磁性体部 3 磁性体部を構成する棒状磁性体 4 磁性体部を構成する棒状磁石 5 断面形状がコの字形の棒状導体 6 棒状導体 7 導電性電磁遮へい材 11 電磁遮へい体 12 磁性体部 13 磁性体部を構成する棒状磁性体 14 磁性体部を構成する棒状磁石 15 弾力性を有する導電性電磁遮へい材 21 電磁遮へい体 22 棒状磁性体 23 導電性を有する棒状磁石 24 電磁遮へい体 25 導電性電磁遮へい材 31 電磁遮へい体 32 磁性体部 33 磁性体部を構成する棒状磁性体 34 磁性体部を構成する導電性を有する棒状磁石 35 断面形状がコの字形をなす棒状導体 36 電磁遮へい体 37 導電性電磁遮へい材 41 電磁遮へい体 42 棒状磁性体 43 溝を設けた弾力性を有する導電性電磁遮へい材 44 電磁遮へい体 46 棒状導体 47,48 磁化の方向 49 漏洩電磁波 1 Electromagnetic shield 2 Magnetic part 3 Rod-shaped magnetic material that constitutes the magnetic material part 4 Bar-shaped magnets that make up the magnetic body 5 Bar-shaped conductor with a U-shaped cross section 6 Rod-shaped conductor 7 Conductive electromagnetic shielding material 11 Electromagnetic shield 12 Magnetic part 13 Rod-shaped magnetic material that constitutes the magnetic material part 14 Rod-shaped magnets that form the magnetic body 15 Conductive electromagnetic shielding material with elasticity 21 Electromagnetic shield 22 Rod-shaped magnetic body 23 Conductive bar magnet 24 Electromagnetic shield 25 Conductive electromagnetic shielding material 31 Electromagnetic shield 32 Magnetic part 33 Rod-shaped magnetic body that constitutes the magnetic body part 34 Conductive bar-shaped magnet that constitutes the magnetic body 35 Rod-shaped conductor with U-shaped cross-section 36 Electromagnetic shield 37 Conductive electromagnetic shielding material 41 Electromagnetic shield 42 Rod-shaped magnetic body 43 Elastic Conductive Electromagnetic Shielding Material with Grooves 44 Electromagnetic shield 46 Bar conductor 47,48 Magnetization direction 49 Leaked electromagnetic wave

Claims (9)

【特許請求の範囲】[Claims] 【請求項1】 導体と、磁性体とを有する電磁遮へい体
であって、 導体は、棒状または板状であり、その長さ方向に溝が形
成され、 磁性体は、前記導体の溝内に配置され、該溝の長さ方向
に垂直な方向の磁場が印加されるものであることを特徴
とする電磁遮へい体。
1. An electromagnetic shield having a conductor and a magnetic body, wherein the conductor is rod-shaped or plate-shaped, and a groove is formed in a longitudinal direction thereof. The magnetic body is provided in the groove of the conductor. An electromagnetic shield, which is arranged and to which a magnetic field in a direction perpendicular to the longitudinal direction of the groove is applied.
【請求項2】 導体と磁性体とを有する電磁遮へい体で
あって、 導体と磁性体とは棒状をなし、交互に並べて配置され、 磁性体は、導体の長さ方向に垂直な方向の磁場が印加さ
れるものであることを特徴とする電磁遮へい体。
2. An electromagnetic shield having a conductor and a magnetic body, wherein the conductor and the magnetic body are rod-shaped and are alternately arranged. The magnetic bodies are magnetic fields in a direction perpendicular to the length direction of the conductor. An electromagnetic shield characterized by being applied.
【請求項3】 導体と、磁石と、磁性体とを有する電磁
遮へい体であって、 導体は、棒状または板状であり、その長さ方向に溝が形
成され、 磁石及び磁性体は、構造体に組合されて前記導体の溝内
に埋め込まれて導体と一体化されたものであり、 磁石は、前記溝の長さ方向に垂直な向きに磁化されたも
のであり、 磁性体は、前記磁石の磁化面に接して配設されたもので
あることを特徴とする電磁遮へい体。
3. An electromagnetic shield having a conductor, a magnet, and a magnetic body, wherein the conductor has a rod shape or a plate shape, and a groove is formed in a length direction thereof, and the magnet and the magnetic body have a structure. The magnet is combined with the body and embedded in the groove of the conductor to be integrated with the conductor, the magnet is magnetized in a direction perpendicular to the length direction of the groove, and the magnetic body is An electromagnetic shield, which is arranged in contact with a magnetized surface of a magnet.
【請求項4】 導体と磁石と磁性体とを有する電磁遮へ
い体であって、 導体は、棒状または板状であり、 磁石と磁性体とは棒状または板状の構造体に組合され、
導体と構造体とは交互に並べて一体化されたものであ
り、 磁石は、導体の長さ方向に垂直な向きに磁化されたもの
であり、 磁性体は、前記磁石の磁化面に接して配設されたもので
あることを特徴とする電磁遮へい体。
4. An electromagnetic shield having a conductor, a magnet and a magnetic body, wherein the conductor has a rod shape or a plate shape, and the magnet and the magnetic body are combined in a rod shape or a plate shape structure,
The conductor and the structure are alternately arranged and integrated, the magnet is magnetized in a direction perpendicular to the length direction of the conductor, and the magnetic body is arranged in contact with the magnetized surface of the magnet. An electromagnetic shield characterized by being installed.
【請求項5】 前記導体の一部もしくは全てが弾力性を
有する電磁遮へい材である請求項4に記載の電磁遮へい
体。
5. The electromagnetic shield according to claim 4, wherein a part or all of the conductor is an elastic electromagnetic shield material.
【請求項6】 導体と、磁石と、磁性体とを有する電磁
遮へい体であって、 導体は、少なくともその一部に弾力性を有する導電性電
磁遮へい材を有するものであり、 導電性電磁遮へい材には、その一部に一列もしくは複数
列の溝を有し、 磁石及び磁性体は、構造体に組合されて前記導電性電磁
遮へい材の溝内に埋め込まれ、 磁石は、前記溝の長さ方向に垂直な向きに磁化されたも
のであり、 磁性体は、前記磁石の磁化面に接して配設されたもので
あることを特徴とする電磁遮へい体。
6. An electromagnetic shield including a conductor, a magnet and a magnetic body, wherein the conductor has a conductive electromagnetic shield having elasticity at least in a part thereof. The material has one or more rows of grooves in a part thereof, the magnet and the magnetic body are combined with the structure and embedded in the groove of the conductive electromagnetic shielding material, and the magnet has the length of the groove. An electromagnetic shield, wherein the magnetic body is magnetized in a direction perpendicular to the vertical direction, and the magnetic body is arranged in contact with the magnetized surface of the magnet.
【請求項7】 導体と磁性体とを有する電磁遮へい体で
あって、 導体は、導電性を有する磁石であり、 磁性体は、棒状または板状をなし、 導電性を有する磁石は、磁性体をはさむように配置さ
れ、該磁性体をはさむ対向二面が互いに異なる極性に磁
化されたものであることを特徴とする電磁遮へい体。
7. An electromagnetic shield having a conductor and a magnetic material, wherein the conductor is a magnet having conductivity, the magnetic material has a rod shape or a plate shape, and the magnet having conductivity is a magnetic material. An electromagnetic shield, wherein the two opposing surfaces sandwiching the magnetic material are magnetized to have polarities different from each other.
【請求項8】 導体と、磁性体と、磁石とを有する電磁
遮へい体であって、 導体は、棒状または板状であり、その長さ方向に溝を有
し、 磁性体と磁石とは、構造体に組合されて前記導体の溝内
に埋め込まれ、 磁石は、導電性を有する磁石であり、前記溝の長さ方向
に垂直な向きに磁化され、 磁性体は、導電性を有する磁石の磁化面に接触し、磁性
体及び導電性を有する磁石の一部の面は、導体表面に露
出させたものであることを特徴とする電磁遮へい体。
8. An electromagnetic shield having a conductor, a magnetic body, and a magnet, wherein the conductor is rod-shaped or plate-shaped, and has a groove in its lengthwise direction. Embedded in the groove of the conductor combined with the structure, the magnet is a magnet having conductivity, magnetized in a direction perpendicular to the length direction of the groove, the magnetic body of the magnet having conductivity. An electromagnetic shield, which is in contact with a magnetized surface, and a part of the surface of a magnet having a magnetic substance and conductivity is exposed on the surface of a conductor.
【請求項9】 前記導体もしくは、前記導体に電気的に
接触する導電性を有する磁石の一部に導電性電磁遮へい
材を有し、 前記導体と前記導電性電磁遮へい材とは、直接もしくは
前記導電性を有する磁石を介して電気的に接触させたも
のであることを特徴とする請求項8に記載の電磁遮へい
体。
9. A conductive electromagnetic shielding material is provided on a part of the conductor or a magnet having electrical conductivity that electrically contacts the conductor, and the conductor and the conductive electromagnetic shielding material are directly or The electromagnetic shield according to claim 8, which is electrically contacted through a magnet having conductivity.
JP3193506A 1991-07-08 1991-07-08 Electromagnetic shielding body Pending JPH0513979A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP3193506A JPH0513979A (en) 1991-07-08 1991-07-08 Electromagnetic shielding body

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP3193506A JPH0513979A (en) 1991-07-08 1991-07-08 Electromagnetic shielding body

Publications (1)

Publication Number Publication Date
JPH0513979A true JPH0513979A (en) 1993-01-22

Family

ID=16309189

Family Applications (1)

Application Number Title Priority Date Filing Date
JP3193506A Pending JPH0513979A (en) 1991-07-08 1991-07-08 Electromagnetic shielding body

Country Status (1)

Country Link
JP (1) JPH0513979A (en)

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH08288685A (en) * 1995-04-12 1996-11-01 Nec Corp Electromagnetic shielding material
WO2004045265A1 (en) * 2002-11-11 2004-05-27 Nec Tokin Corporation Counter emi component and counter emi method
JP2012227390A (en) * 2011-04-20 2012-11-15 Toyota Motor Corp Shield material
JP2017092145A (en) * 2015-11-05 2017-05-25 株式会社竹中工務店 Electromagnetic shield structure
CN111590804A (en) * 2020-05-11 2020-08-28 诺兰特新材料(北京)有限公司 Method and system for preparing electromagnetic shielding sealing strip

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6413197U (en) * 1987-07-10 1989-01-24
JPH01138799A (en) * 1987-08-31 1989-05-31 Inax Corp Thin layer electromagnetic wave absorbing body
JPH0410499A (en) * 1989-11-29 1992-01-14 Nec Corp Electromagnetic shield and case for electromagnetic shielding

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6413197U (en) * 1987-07-10 1989-01-24
JPH01138799A (en) * 1987-08-31 1989-05-31 Inax Corp Thin layer electromagnetic wave absorbing body
JPH0410499A (en) * 1989-11-29 1992-01-14 Nec Corp Electromagnetic shield and case for electromagnetic shielding

Cited By (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH08288685A (en) * 1995-04-12 1996-11-01 Nec Corp Electromagnetic shielding material
WO2004045265A1 (en) * 2002-11-11 2004-05-27 Nec Tokin Corporation Counter emi component and counter emi method
EP1511370A1 (en) * 2002-11-11 2005-03-02 Nec Tokin Corporation Counter emi component and counter emi method
EP1511370A4 (en) * 2002-11-11 2005-10-26 Nec Tokin Corp Counter emi component and counter emi method
JP2012227390A (en) * 2011-04-20 2012-11-15 Toyota Motor Corp Shield material
JP2017092145A (en) * 2015-11-05 2017-05-25 株式会社竹中工務店 Electromagnetic shield structure
CN111590804A (en) * 2020-05-11 2020-08-28 诺兰特新材料(北京)有限公司 Method and system for preparing electromagnetic shielding sealing strip
CN111590804B (en) * 2020-05-11 2022-03-01 诺兰特新材料(北京)有限公司 Method and system for preparing electromagnetic shielding sealing strip

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