JPH04317399A - Electromagnetic shield - Google Patents
Electromagnetic shieldInfo
- Publication number
- JPH04317399A JPH04317399A JP3111054A JP11105491A JPH04317399A JP H04317399 A JPH04317399 A JP H04317399A JP 3111054 A JP3111054 A JP 3111054A JP 11105491 A JP11105491 A JP 11105491A JP H04317399 A JPH04317399 A JP H04317399A
- Authority
- JP
- Japan
- Prior art keywords
- conductor
- electromagnetic
- contact
- shielding
- conductive
- 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
Links
- 239000004020 conductor Substances 0.000 claims abstract description 30
- 239000000463 material Substances 0.000 claims abstract description 30
- 230000000694 effects Effects 0.000 abstract description 14
- 229910052751 metal Inorganic materials 0.000 abstract description 8
- 239000002184 metal Substances 0.000 abstract description 8
- 230000005686 electrostatic field Effects 0.000 abstract 1
- 239000000696 magnetic material Substances 0.000 description 6
- 238000010586 diagram Methods 0.000 description 4
- 229910000859 α-Fe Inorganic materials 0.000 description 3
- 229920001971 elastomer Polymers 0.000 description 2
- 229920005830 Polyurethane Foam Polymers 0.000 description 1
- NMFHJNAPXOMSRX-PUPDPRJKSA-N [(1r)-3-(3,4-dimethoxyphenyl)-1-[3-(2-morpholin-4-ylethoxy)phenyl]propyl] (2s)-1-[(2s)-2-(3,4,5-trimethoxyphenyl)butanoyl]piperidine-2-carboxylate Chemical compound C([C@@H](OC(=O)[C@@H]1CCCCN1C(=O)[C@@H](CC)C=1C=C(OC)C(OC)=C(OC)C=1)C=1C=C(OCCN2CCOCC2)C=CC=1)CC1=CC=C(OC)C(OC)=C1 NMFHJNAPXOMSRX-PUPDPRJKSA-N 0.000 description 1
- 229910000808 amorphous metal alloy Inorganic materials 0.000 description 1
- 230000006866 deterioration Effects 0.000 description 1
- 230000007613 environmental effect Effects 0.000 description 1
- 239000004744 fabric Substances 0.000 description 1
- 229920001821 foam rubber Polymers 0.000 description 1
- 229910001004 magnetic alloy Inorganic materials 0.000 description 1
- 150000002739 metals Chemical class 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 229910000889 permalloy Inorganic materials 0.000 description 1
- 230000035699 permeability Effects 0.000 description 1
- 239000002861 polymer material Substances 0.000 description 1
- 239000011496 polyurethane foam Substances 0.000 description 1
- 239000000843 powder Substances 0.000 description 1
Abstract
Description
【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、侵入を防止するための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た
めの電磁遮へい体に関する。[Industrial Application Field] The present invention relates to an electromagnetic shield for suppressing unnecessary electromagnetic waves emitted from electronic equipment and for use in electromagnetic shielding rooms to prevent leakage and intrusion of electromagnetic waves, particularly at joints of metal casings. The present invention relates to an electromagnetic shielding body that is used in the door of an electromagnetic shielding room to suppress electromagnetic waves leaking from joints or gaps 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。[Prior Art] When providing electromagnetic shielding, generally conductors such as metals have low conductivity in some areas where they come into contact with each other.
Electromagnetic waves tend to leak, and it is necessary to install electromagnetic shields at the contact points between conductors such as metal to suppress leaking electromagnetic waves.
【0003】従来、この種の電磁遮へい体は、図6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1
1、あるいは図7に示すような導電性ゴムを管状にした
EMIガスケット12などの導電性遮へい材が用いられ
ていた(“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6に示すような電磁遮へい体
は、金属片のバネ作用を利用し、図7に示すような電磁
遮へい体は、導電性ゴムの弾力性を利用して、それぞれ
導体同士の接触部に介装し、その導電率の向上を図って
いた。Conventionally, this type of electromagnetic shielding body has a shielding finger 1 formed of a comb-shaped metal piece as shown in FIG.
1, or a conductive shielding material such as an EMI gasket 12 made of conductive rubber in the form of a tube as shown in FIG. The electromagnetic shield shown in Fig. 6 uses the spring action of a metal piece, and the electromagnetic shield shown in Fig. 7 uses the elasticity of conductive rubber to connect the conductors to each other. The aim was to improve its electrical conductivity.
【0004】0004
【発明が解決しようとする課題】ところが、図6、図7
に示す導電性の電磁遮へい体は、シールドフィンガー1
1、ガスケット12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11、ガスケット12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。[Problem to be solved by the invention] However, FIGS. 6 and 7
The conductive electromagnetic shield shown in FIG.
1. The contact resistance between the gasket 12 and the housing, the attachment part of the electromagnetic shielding room, or the shield finger 11 or the conductor part that comes into contact with the gasket 12 affects the electromagnetic wave leakage effect, so the contact is strengthened. A mechanism was needed to do so.
【0005】さらに、シールドフィンガー11、ガスケ
ット12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いていた。Furthermore, when the shield fingers 11 and gaskets 12 are used, changes in spring action and elasticity over time have led to a decrease in the shielding effect.
【0006】また大電流小電圧形の低インピーダンスな
電磁波源を有する場合には、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、環境電磁工学研究
会技術研究報告、EMCJ90−48参照)などの問題
点があった。[0006] Furthermore, when a low-impedance electromagnetic wave source of a large current and low voltage type is used, the shielding effect becomes smaller in the low frequency band (see Institute of Electronics, Information and Communication Engineers, Environmental Electromagnetic Engineering Research Group Technical Research Report, EMCJ90-48). There were problems such as:
【0007】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ための電磁遮へい体
であって、接触を強化するための特別な機構を必要とせ
ず、また低インピーダンスな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ための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 use around the joints and doors of metal casings to suppress leakage of electromagnetic waves, which does not require any special mechanism to strengthen contact. Another object of the present invention is to provide an electromagnetic shielding body capable of obtaining a sufficient shielding effect in a low frequency band even against a low-impedance electromagnetic wave source.
【0008】[0008]
【課題を解決するための手段】上記目的を達成するため
、本発明に係る電磁遮へい体においては、導電性遮へい
材と、棒状の磁性体とを有する電磁遮へい体であって、
導電性遮へい材は、弾力性を有し、導体同士間に形成さ
れる隙間内に設置されるものであり、棒状の磁性体は、
導体と接触する導電性遮へい材の接触部に一体に設けら
れ、該接触部を表面インピーダンスが装荷された状態と
するものである。[Means for Solving the Problems] In order to achieve the above object, an electromagnetic shielding body according to the present invention is an electromagnetic shielding body having a conductive shielding material and a rod-shaped magnetic body, the electromagnetic shielding body comprising:
The conductive shielding material has elasticity and is installed in the gap formed between the conductors, and the rod-shaped magnetic material is
It is provided integrally with a contact portion of a conductive shielding material that comes into contact with a conductor, and places the contact portion in a state where a surface impedance is loaded.
【0009】[0009]
【作用】図5(a)に示したように導電性遮へい材10
が導体14と接触している場合には、導電性遮へい材1
0と導体14との接触部では、接触抵抗が導体表面の抵
抗よりも大きくなる。これを等価回路で示すと、図5(
b)のようになる。導電性遮へい材10と導体4の間の
接触抵抗Rcが導体14表面の表面抵抗Rsより大きい
ため、導体表面を流れる高周波電流Ieのほとんどは、
抵抗の低い導体表面を流れる。この高周波電流Ieが漏
洩電磁波の原因となる。図4(a)に示すように導電性
遮へい材1の導体4と接触する部分の一部に磁性体2を
埋め込んだ構造では、図4(b)の等価回路に示すよう
に接触部に表面インピーダンス(Rf+jXf:j=√
−1)が装荷された状態と等価となる。磁性体として透
磁率の大きな材料を用いれば、表面インピーダンスが大
きくなり、導体表面を流れる高周波電流Ieのほとんど
は導電性遮へい材側へ導かれ、電磁波の漏洩を抑制する
ことができる。表面インピーダンス(Rf+jXf)は
使用する磁性体の特性でほぼ決まるため、漏洩電流への
接触抵抗の影響は小さい。本発明による遮へい体は従来
の導電性遮へい材と比較して漏洩電流の抑制効果が大き
いため、比較的誘起電流の生じやすい低インピーダンス
波源の遮へい効果に対し大幅な改善が図られる。[Operation] As shown in FIG. 5(a), the conductive shielding material 10
is in contact with the conductor 14, the conductive shielding material 1
At the contact portion between 0 and the conductor 14, the contact resistance is greater than the resistance on the surface of the conductor. This is shown in an equivalent circuit in Figure 5 (
b) Since the contact resistance Rc between the conductive shielding material 10 and the conductor 4 is larger than the surface resistance Rs of the conductor 14 surface, most of the high frequency current Ie flowing through the conductor surface is
Flows on the surface of a conductor with low resistance. This high frequency current Ie causes leakage electromagnetic waves. In the structure in which the magnetic material 2 is embedded in a part of the part of the conductive shielding material 1 that contacts the conductor 4 as shown in FIG. 4(a), the contact part has a surface as shown in the equivalent circuit of FIG. Impedance (Rf+jXf:j=√
-1) is equivalent to the loaded state. If a material with high magnetic permeability is used as the magnetic body, the surface impedance will increase, and most of the high frequency current Ie flowing on the conductor surface will be guided to the conductive shielding material side, making it possible to suppress leakage of electromagnetic waves. Since the surface impedance (Rf+jXf) is almost determined by the characteristics of the magnetic material used, the influence of contact resistance on leakage current is small. Since the shielding body according to the present invention has a greater effect of suppressing leakage current than conventional conductive shielding materials, it can significantly improve the shielding effect of low-impedance wave sources that are relatively likely to generate induced currents.
【0010】0010
【実施例】以下、本発明の実施例を図面を参照して説明
する。Embodiments Hereinafter, embodiments of the present invention will be described with reference to the drawings.
【0011】(実施例1)図1は、本発明の実施例1を
示す斜視図である。(Embodiment 1) FIG. 1 is a perspective view showing Embodiment 1 of the present invention.
【0012】図において、本実施例の電磁遮へい体1は
、断面が角形の弾力性を有する導電性遮へい材3を有し
、導電性遮へい材3の導体との接触端面3aに一列の長
溝3bを設け、長溝3b内に棒状磁性体2を埋め込み一
体化した構造としたものである。棒状磁性体2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。導電性遮へい材3は、導電性ゴムやポリウレタンフ
ォーム材を銀蒸着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。磁性体2は一磁性体当りの断面積を小
さくし数多く配置した方が遮へい効果が大きい。In the figure, the electromagnetic shielding body 1 of this embodiment has an elastic conductive shielding material 3 having a rectangular cross section, and a row of long grooves 3b are formed in the contact end surface 3a of the conductive shielding material 3 with the conductor. It has a structure in which the rod-shaped magnetic body 2 is embedded and integrated into the long groove 3b. The rod-shaped magnetic body 2 is made of a sintered ferrite material, a polymer material mixed with ferrite powder, and a magnetic alloy such as a magnetic amorphous alloy or permalloy. A sintered ferrite material with small deterioration is suitable. The conductive shielding material 3 is made of a conductive gasket material having a structure in which conductive rubber or polyurethane foam material is coated with silver-deposited cloth, or an elastic conductive material such as a conductive finger. The shielding effect is greater when a large number of magnetic bodies 2 are arranged with a smaller cross-sectional area per magnetic body.
【0013】図2は、本実施例による遮へい体1を2つ
の導体4で構成される隙間部に適用した状態を示した断
面図である。FIG. 2 is a sectional view showing a state in which the shield 1 according to this embodiment is applied to a gap formed between two conductors 4. As shown in FIG.
【0014】本実施例では遮へい体1の導体4への取り
付け部5に磁性体2が設けられていないため、取り付け
に際してはネジ止めを頻繁に行うなどして電磁遮へい体
1と導体部4の接触を確実にし、この部分からの高周波
電流の漏洩を抑制する必要がある。導電性遮へい材3は
断面形状が円形やL字形等、他の形状のものでもよい。
その際には導体と接触する部分に溝を設けて磁性体を埋
め込んだ構造とする。In this embodiment, since the magnetic material 2 is not provided at the attachment part 5 of the shielding body 1 to the conductor 4, the electromagnetic shielding body 1 and the conductor part 4 are connected by frequently tightening screws during attachment. It is necessary to ensure contact and suppress leakage of high frequency current from this part. The conductive shielding material 3 may have a circular cross-sectional shape, an L-shape, or other shapes. In this case, a structure is used in which a groove is provided in the part that contacts the conductor and a magnetic material is embedded.
【0015】(実施例2)図3は、本発明の実施例2を
示す斜視図である。(Embodiment 2) FIG. 3 is a perspective view showing Embodiment 2 of the present invention.
【0016】本実施例は導電性遮へい材6の断面におけ
る対向した端面6a,6bに長溝6cを設け、長溝6c
内に棒状磁性体2を埋め込み一体化構造としたものであ
る。本実施例に係る遮へい体7は、導体への取り付け部
にも棒状磁性体2が埋め込まれた構造であり、取り付け
部の表面抵抗が大きくなるため、遮へい体7の取り付け
方法を大幅に簡素化できる。実施例1と同様に導電性遮
へい材6は断面形状が円形やL字形等、他の形状のもの
でもよい。In this embodiment, long grooves 6c are provided in opposing end surfaces 6a and 6b in the cross section of the conductive shielding material 6, and the long grooves 6c are
A rod-shaped magnetic body 2 is embedded inside to form an integrated structure. The shielding body 7 according to this embodiment has a structure in which the rod-shaped magnetic material 2 is also embedded in the part where it is attached to the conductor, and the surface resistance of the attachment part becomes large, so the method of attaching the shielding body 7 is greatly simplified. can. As in the first embodiment, the conductive shielding material 6 may have a circular cross-sectional shape, an L-shape, or other shapes.
【0017】[0017]
【発明の効果】以上説明したように本発明による電磁遮
へい体は、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遮へい材
に対し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。[Effects of the Invention] As explained above, the electromagnetic shield according to the present invention has a small effect of contact, so when applied to gaps or joints of metal casings, there is no need for a mechanism to strengthen contact. , it has the effect of being able to take efficient shielding measures. Further, since the shielding body according to the present invention has a greater effect of suppressing leakage current than conventional conductive shielding materials, a significant improvement can be achieved in shielding a low impedance wave source that is likely to generate an induced current.
【図1】本発明の実施例1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】本発明による電磁遮へい体を導体隙間に適用し
た状態を示す斜視図である。FIG. 2 is a perspective view showing a state in which the electromagnetic shield according to the present invention is applied to a conductor gap.
【図3】本発明の実施例2を示す斜視図である。FIG. 3 is a perspective view showing a second embodiment of the present invention.
【図4】本発明の電磁遮へい体の効果を説明するための
図である。FIG. 4 is a diagram for explaining the effect of the electromagnetic shield of the present invention.
【図5】従来の電磁遮へい体の効果を説明するための図
である。FIG. 5 is a diagram for explaining the effect of a conventional electromagnetic shield.
【図6】従来技術による電磁遮へい体を示す図である。FIG. 6 is a diagram showing an electromagnetic shield according to the prior art.
【図7】従来技術による電磁遮へい体を示す図である。FIG. 7 is a diagram showing an electromagnetic shield according to the prior art.
1 電磁遮へい体
2 棒状磁性体
3 弾力性を有する導電性遮へい材
4 導体
5 導電性遮へい材と導体との接触部6 弾力性を
有する導電性遮へい材
7 電磁遮へい体
10 導電性遮へい材
11 シールドフィンガー
12 導電性ガスケット
14 導体1 Electromagnetic shielding body 2 Rod-shaped magnetic body 3 Elastic conductive shielding material 4 Conductor 5 Contact portion between conductive shielding material and conductor 6 Elastic conductive shielding material 7 Electromagnetic shielding body 10 Conductive shielding material 11 Shield Finger 12 Conductive gasket 14 Conductor
Claims (1)
有する電磁遮へい体であって、導電性遮へい材は、弾力
性を有し、導体同士間に形成される隙間内に設置される
ものであり、棒状の磁性体は、導体と接触する導電性遮
へい材の接触部に一体に設けられ、該接触部を表面イン
ピーダンスが装荷された状態とするものであることを特
徴とする電磁遮へい体。[Claim 1] An electromagnetic shielding body comprising a conductive shielding material and a rod-shaped magnetic body, the conductive shielding material having elasticity and being installed in a gap formed between conductors. An electromagnetic shield characterized in that the rod-shaped magnetic body is integrally provided at a contact portion of a conductive shielding material that contacts a conductor, and the contact portion is loaded with surface impedance. body.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP3111054A JPH04317399A (en) | 1991-04-16 | 1991-04-16 | Electromagnetic shield |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP3111054A JPH04317399A (en) | 1991-04-16 | 1991-04-16 | Electromagnetic shield |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH04317399A true JPH04317399A (en) | 1992-11-09 |
Family
ID=14551243
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP3111054A Pending JPH04317399A (en) | 1991-04-16 | 1991-04-16 | Electromagnetic shield |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH04317399A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2012243914A (en) * | 2011-05-18 | 2012-12-10 | Foam Kasei:Kk | Electromagnetic wave shield gasket, and electromagnetic wave shield structure |
Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS61284089A (en) * | 1985-06-07 | 1986-12-15 | 内藤 喜之 | Electromagnetic wave leakage preventor for microwave heater |
JPS6461098A (en) * | 1987-09-01 | 1989-03-08 | Nec Corp | Gasket for electromagnetic shielding |
JPH0410499A (en) * | 1989-11-29 | 1992-01-14 | Nec Corp | Electromagnetic shield and case for electromagnetic shielding |
-
1991
- 1991-04-16 JP JP3111054A patent/JPH04317399A/en active Pending
Patent Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS61284089A (en) * | 1985-06-07 | 1986-12-15 | 内藤 喜之 | Electromagnetic wave leakage preventor for microwave heater |
JPS6461098A (en) * | 1987-09-01 | 1989-03-08 | Nec Corp | Gasket for electromagnetic shielding |
JPH0410499A (en) * | 1989-11-29 | 1992-01-14 | Nec Corp | Electromagnetic shield and case for electromagnetic shielding |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2012243914A (en) * | 2011-05-18 | 2012-12-10 | Foam Kasei:Kk | Electromagnetic wave shield gasket, and electromagnetic wave shield structure |
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