JPS60244100A - Unnecessary radiation preventing method of electronic equipment - Google Patents

Unnecessary radiation preventing method of electronic equipment

Info

Publication number
JPS60244100A
JPS60244100A JP9850384A JP9850384A JPS60244100A JP S60244100 A JPS60244100 A JP S60244100A JP 9850384 A JP9850384 A JP 9850384A JP 9850384 A JP9850384 A JP 9850384A JP S60244100 A JPS60244100 A JP S60244100A
Authority
JP
Japan
Prior art keywords
electronic equipment
unnecessary radiation
ferrite
loss
magnetic material
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
JP9850384A
Other languages
Japanese (ja)
Inventor
石野 健
米須 賢徳
成宮 義和
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.)
TDK Corp
Original Assignee
TDK 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 TDK Corp filed Critical TDK Corp
Priority to JP9850384A priority Critical patent/JPS60244100A/en
Publication of JPS60244100A publication Critical patent/JPS60244100A/en
Pending legal-status Critical Current

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  • Compositions Of Macromolecular Compounds (AREA)
  • Shielding Devices Or Components To Electric Or Magnetic Fields (AREA)
  • Aerials With Secondary Devices (AREA)

Abstract

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 (技術分野) この発明は、外部への放射ノイズを効果的に防止可能な
電子機器の不要輻射防止方法に関する。
DETAILED DESCRIPTION OF THE INVENTION (Technical Field) The present invention relates to a method for preventing unnecessary radiation in electronic equipment that can effectively prevent noise radiated to the outside.

(背景技術) 放射ノイズの問題は今日のエレクトロニクス機器におい
て重要な問題としてと如あげられ、法的規制も厳しく、
その対策が重要な課題となっている。この対策として、
従来、電子機器の外装材料にシールド特性を有する金属
ケース、或いは導電性プラスチックケースを用いる等種
々の工夫がなされてきた。
(Background technology) The problem of radiated noise has been raised as an important issue in today's electronic equipment, and legal regulations are strict.
Countermeasures against this problem have become an important issue. As a countermeasure for this,
Conventionally, various ideas have been made, such as using metal cases with shielding properties or conductive plastic cases as exterior materials for electronic devices.

しかしながら、電子機器を完全に密閉シールド出来ない
高周波電源スィッチ、電子レンジ(通風口、扉の開閉部
その他)、ビデオディスク装置等においてはその空隙部
分よりノイズが外部に放射−される問題があり、このこ
とは完全に解決されていないのが実情である。更に、各
種電子部品(発振器等)から発生する放射ノイズ電波は
、シールドケース内で該シールドケースの寸法及びその
内部の部品構成によシ共振現象を発生せしめ、大きな電
磁エネルギーとなって該シールドケース内の他の回路素
子にも悪影響を及ぼし、動作周波数の不安定化等種々の
問題が生じていた。
However, in high-frequency power switches, microwave ovens (ventilation openings, door openings, etc.), video disc devices, etc., where electronic equipment cannot be completely hermetically shielded, there is a problem that noise is radiated to the outside from the gaps. The reality is that this issue has not been completely resolved. Furthermore, the radiated noise radio waves generated from various electronic components (oscillators, etc.) cause a resonance phenomenon within the shield case due to the dimensions of the shield case and the internal component configuration, and become large electromagnetic energy, causing the shield case to This also adversely affected other circuit elements within the device, causing various problems such as instability of the operating frequency.

(発明の目的) この発明は、上述の如き従来技術の欠点を解決するため
に々されたものであって、金属、導電性プラスチック等
から成る外装ケースにおおわれた電子機器における。こ
れらの外装ケースの空隙から放射されるノイズの防止及
び外装ケース内部で生じる共振現象にもとづく高エネル
ギーを除去することを目的とする。
(Object of the Invention) The present invention has been made to solve the above-mentioned drawbacks of the prior art, and relates to an electronic device covered with an outer case made of metal, conductive plastic, or the like. The purpose is to prevent noise radiated from the voids in these outer cases and to remove high energy caused by resonance phenomena occurring inside the outer case.

(発明の概要) この発明は、フェライトと金属磁性材料とを重量比で3
ニアないし7:3の割合で混合した材料を有機高分子材
料に60重量襲以上分散させてなる複合磁性材料を電子
機器の外装シールドケースの磁界最大位置に取シつける
ととにより電子機器の不要輻射を効果的に防止すること
を特徴としている。
(Summary of the Invention) This invention provides a method for combining ferrite and metal magnetic material in a weight ratio of 3.
A composite magnetic material made by dispersing materials mixed in a ratio of 7:3 to an organic polymer material of 60% by weight or more is installed at the position of maximum magnetic field in the external shielding case of electronic equipment, thereby eliminating the need for electronic equipment. It is characterized by effectively preventing radiation.

この発明で用いられるフェライトとしては1例えばNi
−Zn系フェライト、Mn−Zn系フェライトが挙げら
れ、金属磁性材料としては例えばカーボニル鉄が挙げら
れる。1だ有機高分子材料としては例えばコゝム、プラ
スチック樹脂が使用される。
The ferrite used in this invention is 1, for example, Ni.
Examples include -Zn ferrite and Mn-Zn ferrite, and examples of metal magnetic materials include carbonyl iron. As the organic polymer material, for example, com or plastic resin is used.

なお、ことに例示しだ材料は本発明を限定するものでな
く1本発明の目的を達成するために適当な種々の材料が
使用可能である。
It should be noted that the materials exemplified above do not limit the present invention, and various materials suitable for achieving the object of the present invention can be used.

(発明の構成及び作用) 一般に金属等で周囲をかこった筐体においては。(Structure and operation of the invention) Generally, in cases surrounded by metal etc.

その筐体の縦、横、高さの寸法で決まる共振モードが存
在する。この共振モードは、筐体の縦、横。
There is a resonance mode determined by the length, width, and height of the casing. This resonance mode occurs both vertically and horizontally of the housing.

高さの寸法をそれぞれa 、b 、 cとすると。Let the height dimensions be a, b, and c, respectively.

で示される波長で生ずる(ただしm、n 、qはそれぞ
れ縦(X軸)、横(y軸)、高さく2軸)方向のモード
番号)。
(where m, n, and q are mode numbers in the vertical (X-axis), horizontal (y-axis), and height (two-axis) directions, respectively).

例えば71.4 X 71.4. X 32.3 rM
Iの金属筐体の共振モードの一例を第1図に示す。この
例はTEモードでの励振の場合である。
For example, 71.4 x 71.4. X 32.3 rM
An example of the resonance mode of the metal casing of I is shown in FIG. This example is for excitation in TE mode.

空隙を有するシールドケースにおける不要輻射電磁波は
、不要輻射電磁波(ノイズ)に含まれる周波数成分のす
べてがノイズの各周波数成分の強度に応じて外部に放射
されるわけではない。即ち。
Regarding unnecessary radiated electromagnetic waves in a shield case having a gap, not all of the frequency components included in the unnecessary radiated electromagnetic waves (noise) are radiated to the outside according to the intensity of each frequency component of the noise. That is.

電子機器のシールド外装ケースの寸法及びその内部にあ
る各種電子部品によシ決まる。その電子機器固有の共振
モードが存在し、その共振周波数に相当する周波数のノ
イズが特に強く外部に放射される。
It is determined by the dimensions of the shielded outer case of the electronic device and the various electronic components inside. There is a resonance mode unique to the electronic device, and noise at a frequency corresponding to the resonance frequency is particularly strongly radiated to the outside.

この放射を防止する方法としてはシールド外装ケース内
面のすべてに電波吸収部材を取シつけることが考えられ
ている。たしかにこの方法により外部への放射ノイズが
大幅に減少することが確認されている。しかし、この方
法ではコストが大幅に高くな)実用性に問題がある。更
に、これまで(5) は無線電波(約I GHz ) 、ビデオディスク装置
(約IG±)等のように30MH2〜I GHzまでの
周波数帯が問題にされていだが、最近では12 GHz
帯の放送衛星の実用化にともない12 GH7,帯の放
射ノイズも問題化しており、今後はむしろI GHz〜
18GHzでの放射ノイズが問題化されている。このよ
うなマイクロ波領域で広帯域特性を有する適当々材料が
これまでみあたらなかった。
As a method of preventing this radiation, it has been considered to attach a radio wave absorbing member to the entire inner surface of the shield outer case. It has been confirmed that this method significantly reduces the noise radiated to the outside. However, this method has problems in terms of practicality (as the cost is significantly high). Furthermore, until now (5), the frequency band from 30 MHz to I GHz, such as wireless radio waves (approximately I GHz), video disc devices (approximately I GHz), etc., has been a problem, but recently the frequency band of 12 GHz has been considered.
With the practical application of broadcasting satellites in the 12 GHz band, radiation noise in the 12 GHz band has also become a problem, and in the future it will be more likely that
Radiation noise at 18 GHz has become a problem. Until now, no suitable material having such broadband characteristics in the microwave region has been found.

上記の目的を達成する材料としては、カーボン系の誘電
損失材料と、フェライトに代表される磁気損失材料とが
考えられる。しかしながら、ケースのシールド面では磁
界最大、電界最小のため磁気損失材料の使用に限定され
る。また磁気損失材料を薄型で外装ケースの内部有効ス
ペースを損することなく使用するためにはシールドケー
ス面での取りつけが有効である。
Possible materials for achieving the above purpose include carbon-based dielectric loss materials and magnetic loss materials represented by ferrite. However, since the magnetic field is maximum and the electric field is minimum on the shielding surface of the case, the use of magnetic loss materials is limited. Furthermore, in order to use a thin magnetic loss material without sacrificing the internal effective space of the outer case, it is effective to attach it to the surface of the shield case.

以上のことに鑑み、この発明では磁気損失材料として用
い、該防止部材の取りつけに関しては。
In view of the above, this invention uses the magnetic loss material as a magnetic loss material and attaches the prevention member.

シールド外装ケース内の各電子装置できまる固有の共振
モードに着目し、その共振モードを主体に(6) y軸、y軸、y軸ごとに磁界最大位置を確認し。
Focusing on the unique resonance mode created by each electronic device inside the shielded exterior case, check the maximum magnetic field position for each y-axis, y-axis, and y-axis, mainly using that resonance mode.

これらの磁界最大位置に相当するケース部分に前記防止
部材を取りつけ共振モードを除去することにより外部へ
の放射ノイズを防止するようにした。
The prevention member is attached to the case portion corresponding to the maximum position of these magnetic fields to eliminate the resonance mode, thereby preventing noise radiated to the outside.

磁気損失材料としてはフェライトが代表的な素材である
。その特性の例を第2図及び第3図に示す。第2図はM
n−Znフェライトを80重量%含み樹脂をマトリクス
とした複合磁性材料の特性を示す図であり、第3図はN
i−Znフェライトを85重量%含み樹脂をマ) IJ
クスとした複合磁性材料の特性を示す図である。ここで
μ′、μ″は複素透磁率μ(−μ′+jμ″、ただしj
−レ−]□)の実部及び虚部であり、ε′、ε″は複素
誘電率ε(−ε′+jε″)の実部及び虚部である。こ
れらのうちμ″が磁気損失を示す。第2図及び第3図か
ら明らかなように4 GHzまでは大きな損失を示して
いるが4 GHz以上では急速に損失が減少している。
Ferrite is a typical magnetic loss material. Examples of its characteristics are shown in FIGS. 2 and 3. Figure 2 is M
Fig. 3 is a diagram showing the characteristics of a composite magnetic material containing 80% by weight of n-Zn ferrite and having a resin matrix;
(contains 85% by weight of i-Zn ferrite and contains resin) IJ
FIG. 3 is a diagram showing the characteristics of a smooth composite magnetic material. Here, μ′, μ″ are the complex magnetic permeability μ(−μ′+jμ″, where j
ε′ and ε″ are the real and imaginary parts of the complex dielectric constant ε(−ε′+jε″). Among these, μ'' indicates magnetic loss. As is clear from FIGS. 2 and 3, there is a large loss up to 4 GHz, but the loss rapidly decreases above 4 GHz.

一方、第4図に金属粉末磁性材料であるカーボニル鉄8
0重量%を含み樹脂をマトリクスとする複合材料の特性
を示すが、この場合、損失はそれほど大きく々いがI 
GHz〜10 GHz以上まで安定した損失となってい
る。
On the other hand, Fig. 4 shows carbonyl iron 8, which is a metal powder magnetic material.
0% by weight and has a resin matrix, but in this case, the loss is very large, but I
The loss is stable from GHz to over 10 GHz.

この発明では、上記の両者の特徴を加味し、IGHzか
ら10 GHz以上まで大きな損失を確保するため。
In this invention, both of the above features are taken into account to ensure a large loss from IGHz to 10 GHz or higher.

フェライトと金属磁性材料とを混合させた。両者の混合
割合は主としてノイズのどの周波数が最も大きいかによ
って選択されるが、良好な損失特性を持たせるためには
重量比で3=7ないし7:3程度の混合が有効である。
A mixture of ferrite and metal magnetic material. The mixing ratio of the two is selected mainly depending on which frequency of noise is the largest, but in order to have good loss characteristics, it is effective to mix the two at a weight ratio of about 3=7 to 7:3.

壕だ、上記混合材料と1よ 有機高分子材料との複合比−磁性材料が多いほど有効で
あるが、成型性の問題から95重量%以上の混合は無理
である。従って、磁気損失が有効に生かされる60重量
%以上の複合比が望ましい。
The composite ratio of the above-mentioned mixed material and the organic polymer material (1) is more effective as the amount of magnetic material increases, but it is impossible to mix more than 95% by weight due to moldability problems. Therefore, a composite ratio of 60% by weight or more is desirable so that magnetic loss can be effectively utilized.

第5図にこの発明の一実施例の複合磁性材料(Ni−Z
nフェライト35重量%、カーボニル鉄55重量%を樹
脂10重量%と混合して々る混合材料)の特性を示す。
FIG. 5 shows a composite magnetic material (Ni-Z
The characteristics of a mixed material made by mixing 35% by weight of n-ferrite and 55% by weight of carbonyl iron with 10% by weight of resin are shown.

この図から1〜10 GHz以上まで犬き々損失を示し
ていることが分かる。この実施例の複合磁性材料を第1
図のデータを得るのに使用したものと同じ金属筐体の内
壁の一部(磁界最大位置)に取りつけだ場合の電磁波の
状態を第6図に示す。この図を第1図と比較すると1本
実施例によればモードが太きく減衰し、良好な不要輻射
防止が可能となることが分かる。
It can be seen from this figure that there is a constant loss from 1 to 10 GHz or higher. The composite magnetic material of this example was
Figure 6 shows the state of electromagnetic waves when it is attached to a part of the inner wall (the position of maximum magnetic field) of the same metal casing used to obtain the data in the figure. Comparing this figure with FIG. 1, it can be seen that according to this embodiment, the mode is greatly attenuated, making it possible to effectively prevent unnecessary radiation.

(発明の効果) この発明によれば、電子機器の外装ケースの空隙から放
射されるノイズを効果的に防止すると共にケース内部で
生じる共振現象にもとづく高エネルギーの除去が可能と
なる。しかもケースの磁界最大位置にノイズ放射防止部
材を取りつければ良く、ケース内面全体に該部材を設け
る必要がないので、安価に不要輻射防止を行なうことが
できる。
(Effects of the Invention) According to the present invention, it is possible to effectively prevent noise radiated from a gap in an external case of an electronic device, and to remove high energy based on a resonance phenomenon occurring inside the case. Moreover, since it is only necessary to attach the noise radiation prevention member to the position of the maximum magnetic field of the case, and there is no need to provide the noise radiation prevention member on the entire inner surface of the case, unnecessary radiation can be prevented at low cost.

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

第1図は金属筐体の共振モードの一例を示す図。 第2図はMn −Znフェライトを樹脂に混合してなる
材料の損失特性を示す図、第3図はNi−Znフェライ
トを樹脂に混合してなる材料の損失特性を示す図、第4
図はカーボニル鉄を樹脂に混合して々る材料の損失特性
を示す図、第5図はこの発明の一実施例の複合磁性材料
の特性を示す図、第6図は(9) 第1図で用いた金属筐体の内面の一部(磁界最大位置)
にこの発明の実施例の複合磁性材料を設けた場合の電磁
波の状態を示す図である。 特許出願人 ティーディーケイ株式会社特許出願代理人
 弁理士 山 本 恵 −(10)
FIG. 1 is a diagram showing an example of a resonance mode of a metal casing. Figure 2 shows the loss characteristics of a material made by mixing Mn-Zn ferrite with resin, Figure 3 shows the loss characteristics of a material made by mixing Ni-Zn ferrite with resin, and Figure 4 shows the loss characteristics of a material made by mixing Ni-Zn ferrite with resin.
Figure 5 shows the loss characteristics of a material made by mixing carbonyl iron with resin, Figure 5 shows the characteristics of a composite magnetic material according to an embodiment of the present invention, and Figure 6 shows (9) Figure 1. Part of the inner surface of the metal casing used in (maximum magnetic field position)
FIG. 3 is a diagram showing the state of electromagnetic waves when a composite magnetic material according to an embodiment of the present invention is provided in the device. Patent applicant TDC Co., Ltd. Patent application agent Patent attorney Megumi Yamamoto - (10)

Claims (4)

【特許請求の範囲】[Claims] (1) フェライトと金属磁性材料とを重量比で3ニア
ないし7:3の割合で混合した材料を有機高分子材料に
60重量%以上分散させてなる複合磁性材料を、電子機
器の外装シールドケースの磁界最大位置に取りつけるこ
とにより電子機器の不要輻射を防止することを特徴とす
る電子機器の不要輻射防止方法。
(1) A composite magnetic material made by dispersing 60% by weight or more of a material obtained by mixing ferrite and a metal magnetic material at a weight ratio of 3 to 7 in an organic polymer material is used as an external shield case for electronic equipment. A method for preventing unnecessary radiation from electronic equipment, characterized by preventing unnecessary radiation from the electronic equipment by installing the electronic equipment at a position where the magnetic field is maximum.
(2)前記フェライトがMP’e204 (MはNi、
Co。 Fe 、Mn +Zn 、Cd 、Mg 、 Liなど
の元素の1種もしくは2種以上の組合せ)の化学式を持
つスピネルフェライトであることを特徴とする特許請求
の範囲第1項に記載の不要輻射防止方法。
(2) The ferrite is MP'e204 (M is Ni,
Co. The method for preventing unnecessary radiation according to claim 1, characterized in that the spinel ferrite is a spinel ferrite having a chemical formula of (one or a combination of two or more elements such as Fe, Mn + Zn, Cd, Mg, Li, etc.) .
(3) 前記金属磁性材料がカーボニル鉄であることを
特徴とする特許請求の範囲第1項または第2項に記載の
不要輻射防止方法。
(3) The method for preventing unnecessary radiation according to claim 1 or 2, wherein the metal magnetic material is carbonyl iron.
(4)前記有機高分子材料がゴムまだはプラスチック樹
脂であることを特徴とする特許請求の範囲第1項〜第3
項のうちのいずれか一項に記載の不要輻射防止方法。
(4) Claims 1 to 3, characterized in that the organic polymer material is rubber or plastic resin.
The unnecessary radiation prevention method described in any one of the following paragraphs.
JP9850384A 1984-05-18 1984-05-18 Unnecessary radiation preventing method of electronic equipment Pending JPS60244100A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP9850384A JPS60244100A (en) 1984-05-18 1984-05-18 Unnecessary radiation preventing method of electronic equipment

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP9850384A JPS60244100A (en) 1984-05-18 1984-05-18 Unnecessary radiation preventing method of electronic equipment

Publications (1)

Publication Number Publication Date
JPS60244100A true JPS60244100A (en) 1985-12-03

Family

ID=14221441

Family Applications (1)

Application Number Title Priority Date Filing Date
JP9850384A Pending JPS60244100A (en) 1984-05-18 1984-05-18 Unnecessary radiation preventing method of electronic equipment

Country Status (1)

Country Link
JP (1) JPS60244100A (en)

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