JPH08186394A - Electromagnetic wave screening breathing hole - Google Patents

Electromagnetic wave screening breathing hole

Info

Publication number
JPH08186394A
JPH08186394A JP6337877A JP33787794A JPH08186394A JP H08186394 A JPH08186394 A JP H08186394A JP 6337877 A JP6337877 A JP 6337877A JP 33787794 A JP33787794 A JP 33787794A JP H08186394 A JPH08186394 A JP H08186394A
Authority
JP
Japan
Prior art keywords
electromagnetic wave
shielding
breathing hole
vent hole
ventilation hole
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.)
Granted
Application number
JP6337877A
Other languages
Japanese (ja)
Other versions
JP2788862B2 (en
Inventor
Kenichi Hatakeyama
賢一 畠山
Hitoshi Togawa
斉 戸川
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
Tokin Corp
Original Assignee
NEC Corp
Tokin 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
Family has litigation
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Application filed by NEC Corp, Tokin Corp filed Critical NEC Corp
Priority to JP6337877A priority Critical patent/JP2788862B2/en
Publication of JPH08186394A publication Critical patent/JPH08186394A/en
Application granted granted Critical
Publication of JP2788862B2 publication Critical patent/JP2788862B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Abstract

PURPOSE: To provide an electromagnetic wave screening breathing hole used for an electric dark room and an electromagnetic screening room for screening electromagnetic waves within a wide band from a low frequency to a mm-wave region. CONSTITUTION: In an electromagnetic wave screening breathing hole, a honeycomb screening material is provided in the entrance of the breathing hole and a pyramid or wedge-shaped electric wave absorbing material is fitted to the inner wall of the breathing hole. In the electric wave absorber, the view up to an exit is closed since the section entire region of the breathing hole is hidden by either absorbing body when viewed from the entrance surface of the breathing hole, and the installation position of the electric wave absorber is shifted in the depth direction of the breathing hole to secure the circulation of air. A length L of the breathing hole for fitting the electric wave absorbing body should be 2-3 wavelengths or longer. With this structure, an improved screening property can be achieved within a wide frequency range from a low frequency region to a mm-wave region.

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、電磁波遮蔽通気孔に関
し、特に電磁波遮蔽室、電波暗室等の通気孔の電磁波遮
蔽に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an electromagnetic wave shielding vent hole, and more particularly to electromagnetic wave shielding of a vent hole in an electromagnetic wave shielding room, an anechoic chamber or the like.

【0002】[0002]

【従来の技術】電磁遮蔽室や電波暗室では、床、天井を
含むすべての壁は電磁波を遮蔽するために金属板で囲ま
れているが、金属壁で囲むことができない箇所がある。
その一つが通気孔であり、この部分は空気の流通を確保
すると同時に、電磁波に対してはそれを遮蔽するもので
なければならない。従来、この種の電磁波遮蔽室や電波
暗室の通気孔には、図8に示すようなハニカム遮蔽材を
用いるもの、また、図9に示すように通気孔の内壁に電
波吸収体(ニ)を装着した壁で構成され、通路として直
線的な見通しができないように折り曲げ、電磁波が漏れ
ないようにして、電磁波遮蔽を行うものが知られてい
る。
2. Description of the Related Art In an electromagnetically shielded room or an anechoic chamber, all walls including a floor and a ceiling are surrounded by metal plates for shielding electromagnetic waves, but there are some places that cannot be surrounded by metal walls.
One of them is a vent, and this part must ensure the circulation of air and at the same time shield it from electromagnetic waves. Conventionally, a honeycomb shielding material as shown in FIG. 8 is used for the ventilation holes of this type of electromagnetic shielding room or anechoic chamber, and an electromagnetic wave absorber (d) is provided on the inner wall of the ventilation hole as shown in FIG. It is known that the device is constructed of a mounted wall, and is bent so as not to have a straight line of sight as a passage to prevent electromagnetic waves from leaking and shield electromagnetic waves.

【0003】[0003]

【発明が解決しようとする課題】上記従来技術におい
て、次のような問題点があった。図8に示すハニカムフ
ィルターの遮蔽材は、その拡大図に示すように金属の小
さい導波路が集合したものであり、この導波路が電磁波
伝搬に対して遮断するものである。そしてこのハニカム
遮蔽材の導波路が、電磁波伝搬に対して遮断となる周波
数範囲では電磁波遮蔽が可能である。これについて、導
波路の断面が4角形のものについて考察すると、例え
ば、その断面が横幅a、高さbの4角形(a>b)であ
るとき、自由空間波長λが、2a<λ となる周波数範
囲で導波路は電磁波遮断となる。従って、2a=λとな
る周波数をfoとすると、foより低い周波数範囲では
遮断となる。
The above-mentioned prior art has the following problems. As shown in the enlarged view, the shielding material of the honeycomb filter shown in FIG. 8 is a collection of small metal waveguides, and these waveguides block electromagnetic wave propagation. The electromagnetic wave can be shielded in the frequency range in which the waveguide of the honeycomb shielding material blocks electromagnetic wave propagation. Regarding this, when considering a waveguide having a quadrangular cross section, for example, when the cross section is a quadrangle (a> b) having a width a and a height b, the free space wavelength λ becomes 2a <λ. In the frequency range, the waveguide blocks electromagnetic waves. Therefore, if the frequency at which 2a = λ is fo, the cutoff occurs in the frequency range lower than fo.

【0004】図8に示すハニカムの導波路断面は6角形
であるが、上記導波路の断面が4角形のものの考察の例
からの類推により、ハニカムの導波路断面の径をaとす
れば、2a<<λとなる周波数範囲では遮断導波路とな
ると考えてよい。通常、通気孔の遮蔽材として用いられ
るハニカムでは、a>3mmである。これより小さい径
aでは通気が十分ではなくなるのでこのサイズが用いら
れるている。ここで、径aが3mmのハニカムが遮蔽と
して作用する上限の周波数を見積もってみる。自由空間
波長λは20mm程度必要であるとすると、周波数は1
5GHzであり、これより高い周波数では、ハニカムは
電磁波を遮蔽するものとならないという問題点があっ
た。
The honeycomb cross section of the honeycomb shown in FIG. 8 is hexagonal. By analogy with the example of consideration of the above-mentioned waveguide having a square cross section, if the diameter of the honeycomb waveguide cross section is a. It may be considered that the cut-off waveguide is formed in the frequency range where 2a << λ. Normally, a> 3 mm in a honeycomb used as a ventilation hole shielding material. This size is used because the ventilation is insufficient with a diameter a smaller than this. Here, the upper limit frequency at which the honeycomb having a diameter a of 3 mm acts as a shield will be estimated. If the free space wavelength λ requires about 20 mm, the frequency is 1
The frequency is 5 GHz, and at a frequency higher than this, there is a problem that the honeycomb does not shield electromagnetic waves.

【0005】また、図9に示すように、通気孔内壁に電
波吸収体(ニ)を装着した壁で構成されるもので、通気
孔の空間を直線的な見通しができないように折り曲げ、
実質的な遮蔽として利用しようとするものでは、電波吸
収体の周波数特性によって周波数帯の制限がある。ここ
で用いられる電波吸収体(ニ)は、できる限り周波数帯
域が広い方がよいので、ピラミッド形、或いは楔形の電
波吸収体が用いられるが、どちらの電波吸収体でもその
高さが、およそ波長と同程度になる周波数以上でのみ電
波吸収量が大きい。
As shown in FIG. 9, the inner wall of the ventilation hole is formed of a wall on which a radio wave absorber (d) is mounted, and the space of the ventilation hole is bent so that it cannot be seen straight.
In what is intended to be used as a substantial shield, the frequency band is limited by the frequency characteristics of the radio wave absorber. The electromagnetic wave absorber (d) used here should have a wide frequency band as much as possible, so a pyramid-shaped or wedge-shaped electromagnetic wave absorber is used, but the height of both electromagnetic wave absorbers is about the wavelength. The amount of electromagnetic wave absorption is large only at frequencies above the same level as

【0006】例えば、通気孔断面は一辺300mm程度
の大きさであり、電波吸収体は高さ50mmのピラミッ
ド形を用いるとすると、周波数6GHz(波長が50m
m)以下では吸収量が大きくなく、その結果、十分な遮
蔽が期待できない。このように、吸収体を通気孔の内壁
に装着した場合は、吸収体の性能により低周波数側では
遮蔽ができないと言う問題点があった。最近では、周波
数の高いミリ波領域まで電子機器の周波数が広がり、そ
の結果、電波暗室、電磁波遮蔽室ではこれまでの低い周
波数(1GHz以下)からミリ波領域にまで達する広い
周波数範囲で遮蔽が求められているが、上記従来技術で
は、対応できないという問題があった。
For example, if the cross section of the vent hole is about 300 mm on a side and the radio wave absorber is a pyramid shape with a height of 50 mm, the frequency is 6 GHz (the wavelength is 50 m).
Below m), the amount of absorption is not large, and as a result, sufficient shielding cannot be expected. As described above, when the absorber is attached to the inner wall of the ventilation hole, there is a problem that the absorber cannot be shielded on the low frequency side due to the performance of the absorber. Recently, the frequency of electronic devices has spread to the high-frequency millimeter wave region, and as a result, shielding is required in a wide frequency range from the low frequency (1 GHz or less) that has hitherto been reached to the millimeter wave region in anechoic chambers and electromagnetic shield rooms. However, the above-mentioned conventional technique has a problem that it cannot be dealt with.

【0007】[0007]

【課題を解決するための手段】本発明は、金属板よりな
る通気孔で、前記通気孔の内壁面にピラミッド形電波吸
収体、或いは楔形電波吸収体を装着し、かつ通気孔の入
り口、或いは出口の少なくともどちらか一方の断面をハ
ニカム遮蔽材で覆ったことを特徴とする電磁波遮蔽通気
孔である。また、本発明は、通気孔は、その入り口から
出口までを直線で見通せないように折り曲げた通気孔で
あることを特徴とする上記に記載の電磁波遮蔽通気孔で
ある。
According to the present invention, there is provided a ventilation hole made of a metal plate, wherein a pyramid-shaped electromagnetic wave absorber or a wedge-shaped electromagnetic wave absorber is attached to an inner wall surface of the ventilation hole, and an inlet of the ventilation hole, or The electromagnetic wave shielding vent hole is characterized in that at least one of the cross sections of the outlet is covered with a honeycomb shielding material. Further, the present invention is the electromagnetic wave shielding vent hole described above, wherein the vent hole is a vent hole that is bent so that a straight line cannot be seen from the inlet to the outlet.

【0008】また、本発明は、金属板よりなる通気孔
で、前記通気孔断面より小さい底面のピラミッド形電波
吸収体、或いは楔形電波吸収体を複数個用いて通気孔入
り口面から見たときに断面全領域がいずれかの吸収体に
より隠されて出口まで見通せなく、かつ通気孔の奥行き
方向には電波吸収体の設置位置をずらして空気の流通を
確保し、かつ通気孔の入り口、或いは出口の少なくとも
どちらか一方の断面をハニカム遮蔽材で覆ったことを特
徴とする電磁波遮蔽通気孔である。なお、本発明におい
て、通気孔の入り口、出口とは、通気孔の電波暗室また
は電磁遮蔽室側が入り口であり、通気孔の外部側が出口
である。図1で示せば、通気孔(ロ)の電波暗室または
電磁遮蔽室(イ)に設けられている側が入り口であり、
空気の矢印の側が出口である。
Further, according to the present invention, when a plurality of ventilation holes made of a metal plate are used, the pyramid-shaped radio wave absorber or the wedge-shaped radio wave absorber having a bottom surface smaller than the cross section of the vent hole is used and viewed from the vent hole entrance surface. The entire cross-sectional area is hidden by one of the absorbers so that it cannot be seen through to the outlet, and the air absorber is installed in the depth direction of the ventilation hole to ensure air circulation, and the inlet or outlet of the ventilation hole is also secured. The electromagnetic wave shielding vent hole is characterized in that at least one of the cross sections is covered with a honeycomb shielding material. In addition, in the present invention, the inlet and outlet of the vent hole are the entrance on the side of the anechoic chamber or the electromagnetic shield room of the vent hole, and the exit side is the outside of the vent hole. As shown in FIG. 1, the side of the ventilation hole (b) provided in the anechoic chamber or the electromagnetically shielded room (a) is the entrance,
The side of the air arrow is the exit.

【0009】[0009]

【作用】本発明の作用について説明する。本発明におい
ては、電磁波遮蔽通気孔が、金属板よりなる通気孔であ
って、その内壁面にピラミッド形電波吸収体、或いは楔
形電波吸収体を装着し、かつ通気孔の入り口、あるいは
出口の少なくともどちらか一方の断面はハニカム遮蔽材
で覆う構造にする。この通気孔は、電波吸収体が比較的
小さい場合には、通気孔の入り口から出口までを直線で
見通せないように折り曲げた構造にするものであり、ま
た、通気孔断面より小さい底面のピラミッド形電波吸収
体、或いは楔形電波吸収体を複数個用いて通気孔入り口
面から見たときに断面全領域がいずれかの吸収体により
隠されて出口まで見通せなく、かつ通気孔の奥行き方向
には電波吸収体の設置位置をずらして空気の流通を確保
し、かつ通気孔の入り口、あるいは出口の少なくともど
ちらか一方の断面はハニカム遮蔽材で覆う構造にする。
The function of the present invention will be described. In the present invention, the electromagnetic wave shielding ventilation hole is a ventilation hole made of a metal plate, the inner wall surface of which is fitted with a pyramidal radio wave absorber or a wedge radio wave absorber, and at least an inlet or an outlet of the vent hole. The cross section of either one is covered with a honeycomb shielding material. When the radio wave absorber is relatively small, this vent has a structure that is bent so that the entrance to the exit of the vent cannot be seen in a straight line. When multiple radio wave absorbers or wedge-shaped radio wave absorbers are used, the entire cross-section area is hidden by one of the absorbers when viewed from the entrance surface of the vent hole, and the radio wave is not visible in the depth direction of the vent hole. A structure is adopted in which the installation position of the absorber is shifted to ensure air circulation, and at least one of the inlet and outlet of the ventilation hole is covered with a honeycomb shielding material.

【0010】このような構造にすることにより、低周波
数からミリ波領域にまで達する広い周波数範囲で良好な
遮蔽が得られる。ただし、良好な遮蔽を実現するために
は、ハニカム遮蔽材と電波吸収体の両者の周波数特性を
考慮して組み合わせなければならない。すなわち、本発
明においては、図1に示すような電波暗室、または電磁
遮蔽室(イ)に設けられる通気孔(ロ)で、その通気孔
が低い周波数(1GHz以下)からミリ波領域にまで達
する広い周波数範囲で電磁波を遮蔽するものである。こ
れは、ハニカム遮蔽材は低い周波数領域で電磁波遮蔽に
寄与し、電波吸収体は高い周波数領域で遮蔽に寄与する
もので、電波吸収体とハニカム遮蔽材との両者により広
い帯域で電磁波遮蔽がなされるものである。
With such a structure, good shielding can be obtained in a wide frequency range from low frequencies to the millimeter wave region. However, in order to achieve good shielding, the honeycomb shielding material and the electromagnetic wave absorber must be combined in consideration of the frequency characteristics. That is, in the present invention, the ventilation hole (b) provided in the anechoic chamber or the electromagnetic shielding room (a) as shown in FIG. 1 extends from the low frequency (1 GHz or less) to the millimeter wave region. It shields electromagnetic waves in a wide frequency range. This is because the honeycomb shielding material contributes to electromagnetic wave shielding in the low frequency region, and the electromagnetic wave absorber contributes to shielding in the high frequency region.The electromagnetic wave shielding is performed in a wide band by both the electromagnetic wave absorber and the honeycomb shielding material. It is something.

【0011】[0011]

【実施例】本発明の実施例について図面を用いて説明す
る。 [実施例1]本発明の一実施例を図2、図3に示す。図
2は、本発明の一実施例を示す電磁波遮蔽通気孔の構成
図である。通気孔の入り口にハニカム遮蔽材(ハ)を設
け、通気孔内壁にはピラミッド形、或いは楔形の電波吸
収材(ニ)を装着する。電波吸収体(ニ)は、図2に示
すように通気孔(ロ)入り口面から見たときに、通気孔
の断面全領域がいずれかの吸収体により隠されて出口ま
で見通せないもので、かつ通気孔の奥行き方向には電波
吸収体(ニ)の設置位置をずらして、空気の流通を確保
しているものである。
Embodiments of the present invention will be described with reference to the drawings. [Embodiment 1] An embodiment of the present invention is shown in FIGS. FIG. 2 is a configuration diagram of an electromagnetic wave shielding vent hole showing an embodiment of the present invention. A honeycomb shielding material (c) is provided at the entrance of the vent hole, and a pyramid-shaped or wedge-shaped radio wave absorber (d) is attached to the inner wall of the vent hole. As shown in FIG. 2, the radio wave absorber (d) is such that when viewed from the inlet surface of the vent hole (b), the entire cross-sectional area of the vent hole is hidden by one of the absorbers and the outlet cannot be seen through. In addition, the installation position of the electromagnetic wave absorber (d) is shifted in the depth direction of the ventilation hole to ensure air circulation.

【0012】電波吸収体を装着する通気孔の長さLは、
どの程度の遮蔽を必要とするかによって決まるが、経験
的には2〜3波長以上必要であるとされている。いま、
ハニカム遮蔽材が有効である上限周波数をfsとし、そ
のときの自由空間波長をλsとしたとき、電波吸収体は
ハニカムが有効でなくなる高い周波数領域で遮蔽に寄与
するので通気孔の長さLは、2〜3λs以上必要である
ことになる。ハニカム遮蔽材は、通気孔の入り口、或い
は出口の少なくともどちらか一方の断面を覆うように設
けるものであるが、図3に示す電磁波遮蔽通気孔の構成
図では、ハニカム遮蔽材(ハ)は通気孔の出口側に設け
ているもので、図2と遮蔽の効果は同じである。
The length L of the ventilation hole for mounting the radio wave absorber is
Although it depends on how much shielding is required, it is empirically said that two or more wavelengths are required. Now
When the upper limit frequency at which the honeycomb shielding material is effective is fs and the free space wavelength at that time is λs, the radio wave absorber contributes to shielding in a high frequency region where the honeycomb is not effective, and therefore the length L of the vent hole is , 2-3 λs or more is required. The honeycomb shielding material is provided so as to cover the cross section of at least one of the inlet and the outlet of the ventilation hole. In the configuration of the electromagnetic wave shielding ventilation hole shown in FIG. Since it is provided on the outlet side of the pores, the shielding effect is the same as in FIG.

【0013】[実施例2]本発明の第2の実施例を図4
に示す。図4は、第2の実施例の電磁波遮蔽通気孔の構
成例で、内壁に電波吸収体(ニ)を装着した通気孔
(ロ)を、通気孔の入り口から出口までを直線上に見通
せないように折り曲げ、入り口にハニカム遮蔽材(ハ)
を設けた構造の電磁波遮蔽通気孔である。通気孔の長さ
(L1+L2)は実施例1の場合と同じく、2〜3λs
以上必要である。通気孔(ロ)の内壁に電波吸収体
(ニ)の装着において、電波吸収材であるピラミッド
形、或いは楔形の装着は、通気孔内壁の対向する2面だ
けに設けても、あるいは内壁の4面全てに装着してもよ
い。
[Embodiment 2] A second embodiment of the present invention is shown in FIG.
Shown in FIG. 4 is a configuration example of the electromagnetic wave shielding ventilation hole of the second embodiment, in which the ventilation hole (b) having the electromagnetic wave absorber (d) attached to the inner wall cannot be seen straight from the entrance to the exit of the ventilation hole. So that the honeycomb shielding material at the entrance (c)
It is an electromagnetic wave shielding vent having a structure provided with. The length (L1 + L2) of the ventilation hole is 2 to 3 λs, as in the case of the first embodiment.
The above is necessary. When the radio wave absorber (d) is attached to the inner wall of the ventilation hole (b), the pyramid-shaped or wedge-shaped attachment of the radio wave absorber may be provided only on two opposite surfaces of the ventilation hole inner wall, or the inner wall of It may be attached to all surfaces.

【0014】[実施例3]本発明の第3の実施例を図
5、図6及び図7で説明する。図5、図6は、第3の実
施例の電磁波遮蔽通気孔の構成例であり、図7はハニカ
ム遮蔽材と電波吸収体の組み合わせ方法を説明するため
の図である。図5は、通気孔に電波吸収体(ニ)を設け
ているもので、電波吸収体(ニ)はピラミッド形電波吸
収体、或いは楔形電波吸収体である。この電波吸収体
(ニ)は通気孔内に細い棒、例えばプラスチックの細い
棒で支持されているものである。そして、電波吸収体
(ニ)はピラミッド形のものでは、その頂点が下(入り
口)側に、楔形のものでは、その先端が下(入り口)側
に設けられている。通気孔入り口にハニカム遮蔽材
(ハ)を設けられている。
[Embodiment 3] A third embodiment of the present invention will be described with reference to FIGS. 5, 6 and 7. FIG. 5 and FIG. 6 are configuration examples of the electromagnetic wave shielding vent hole of the third embodiment, and FIG. 7 is a diagram for explaining a method of combining the honeycomb shielding material and the radio wave absorber. In FIG. 5, a radio wave absorber (d) is provided in the ventilation hole, and the radio wave absorber (d) is a pyramid-shaped radio wave absorber or a wedge-shaped radio wave absorber. This radio wave absorber (d) is supported by a thin rod, for example, a plastic thin rod, in the vent hole. The pyramid-shaped radio wave absorber (d) has its apex on the lower (entrance) side, and the wedge-shaped one has its tip on the lower (entrance) side. A honeycomb shielding material (c) is provided at the inlet of the ventilation hole.

【0015】図5において、通気孔(ロ)を導波路と考
え、この導波路を伝搬する電磁波を減衰させるように複
数の電波吸収体(ニ)を導波路内に設け、そして、通気
孔入り口にはハニカム遮蔽材(ハ)を設けたものであ
る。また複数の電波吸収体(ニ)は、通気孔の入り口か
ら出口までを直線上に見通せないように位置をずらして
設ける。この導波路内に設けられる複数の電波吸収体
(ニ)は、通気を確保するための配慮もなされているも
ので、その点からも複数の電波吸収体を、通気孔の入り
口から出口までを直線上に見通せないように位置をずら
して設ける。
In FIG. 5, the ventilation hole (b) is considered to be a waveguide, and a plurality of electromagnetic wave absorbers (d) are provided in the waveguide so as to attenuate the electromagnetic wave propagating in the waveguide, and the ventilation hole entrance. Is provided with a honeycomb shielding material (C). Further, the plurality of radio wave absorbers (d) are provided so that the positions from the entrance to the exit of the ventilation hole cannot be seen in a straight line. The plurality of radio wave absorbers (d) provided in this waveguide are also designed to ensure ventilation, and from that point as well, a plurality of radio wave absorbers should be installed from the inlet to the outlet of the ventilation hole. The position should be staggered so that the line of sight cannot be seen.

【0016】図6は、図5と同様に、通気孔に電波吸収
体(ニ)を細い棒、例えばプラスチックの細い棒で支持
して設ているもので、ハニカム遮蔽材(ハ)を通気孔の
奥側(通気孔出口)に設けたものである。このようにす
ると通気孔入り口は少なくとも高い周波数帯では電波吸
収特性が保てるので、電波暗室の通気孔として適してい
る。電波吸収体を装着する通気孔の長さLは、実施例
1、2と同様の理由で、2〜3λs以上必要である。
Similar to FIG. 5, FIG. 6 shows the ventilation hole in which the electromagnetic wave absorber (d) is supported by a thin rod, for example, a thin plastic rod, and the honeycomb shielding material (c) is provided in the ventilation hole. It is provided on the back side (outlet of the vent). In this way, the entrance of the vent hole can maintain the radio wave absorption property at least in a high frequency band, and is therefore suitable as a vent hole of an anechoic chamber. The length L of the ventilation hole to which the radio wave absorber is attached needs to be 2 to 3 λs or more for the same reason as in the first and second embodiments.

【0017】ハニカム遮蔽材と電波吸収体は、両者によ
り広い帯域で遮蔽が得られるように組み合わせなければ
ならない。図7は組み合わせかたの原理を示したもの
で、左縦軸はハニカム遮蔽材の遮蔽量S、右縦軸は電波
吸収体の遮蔽量Tである。ハニカム遮蔽材は、その導波
路の径がおよそ波長と同程度のサイズになると急激に遮
蔽が悪くなる。いま、十分に低い周波数での遮蔽量の9
0%の遮蔽量をSoとし、そのときの周波数をfsとす
る。また、楔形、ピラミッド形の電波吸収体の遮蔽量は
吸収体の高さhと波長λの比h/λに依存し、この比が
大きいほど遮蔽量が大きくなる。従って、電波吸収体の
遮蔽量は周波数が高いほど大きくなる。
The honeycomb shielding material and the electromagnetic wave absorber must be combined so that shielding can be obtained in a wider band by both. FIG. 7 shows the principle of combination, where the left vertical axis is the shielding amount S of the honeycomb shielding material and the right vertical axis is the shielding amount T of the radio wave absorber. When the diameter of the waveguide of the honeycomb shielding material is about the same as the wavelength, the shielding is rapidly deteriorated. Now, the shielding amount at a sufficiently low frequency is 9
The shielding amount of 0% is So, and the frequency at that time is fs. Further, the shielding amount of the wedge-shaped or pyramidal-shaped radio wave absorber depends on the ratio h / λ of the height h of the absorber and the wavelength λ, and the larger the ratio, the larger the shielding amount. Therefore, the shielding amount of the radio wave absorber increases as the frequency increases.

【0018】いま、Soと同じ値をToとし、そのとき
の周波数をfTとする。広周波数帯域に亘って遮蔽を保
つためには、fs≧fTとなるように組み合わせること
が必要で、もしこの関係が保たれない場合は、fsとf
Tの間は遮蔽が悪くなる。また、電波吸収体はできる限
りその高さが低いほど経済的にも、空間の占有率の点か
らも望ましいので、fTはfsよりも極端に低く設定す
る必要はない。fsとfTの関係は実施例1、2でも同
様に成り立つ。
Now, let us say that the same value as So is To and the frequency at that time is fT. In order to maintain the shielding over a wide frequency band, it is necessary to combine them so that fs ≧ fT. If this relationship cannot be maintained, fs and f
During T, the shielding becomes poor. In addition, since it is desirable that the height of the radio wave absorber is as low as possible economically and in terms of space occupancy, fT does not need to be set extremely lower than fs. The relationship between fs and fT holds similarly in the first and second embodiments.

【0019】[0019]

【発明の効果】本発明の電磁波遮蔽通気孔を用いること
により、通気孔を広帯域で遮蔽することが可能になる。
すなわち、低い周波数(1GHz以下)から周波数の高
いミリ波領域にまで達する広い周波数範囲で遮蔽がする
ことができるという効果を奏するものである。
By using the electromagnetic wave shielding vent hole of the present invention, the vent hole can be shielded in a wide band.
That is, the present invention has an effect that the shielding can be performed in a wide frequency range from a low frequency (1 GHz or less) to a high frequency millimeter wave region.

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

【図1】 電波暗室、電磁遮蔽室に設けられた通気孔を
示す図。
FIG. 1 is a diagram showing ventilation holes provided in an anechoic chamber and an electromagnetically shielded room.

【図2】 本発明の第1の実施例の電磁波遮蔽通気孔の
構成例。
FIG. 2 is a structural example of an electromagnetic wave shielding vent hole according to the first embodiment of the present invention.

【図3】 本発明の第1の実施例の電磁波遮蔽通気孔の
構成例。
FIG. 3 is a configuration example of an electromagnetic wave shielding vent hole according to the first embodiment of the present invention.

【図4】 本発明の第2の実施例の電磁波遮蔽通気孔の
構成例。
FIG. 4 is a structural example of an electromagnetic wave shielding vent hole according to a second embodiment of the present invention.

【図5】 本発明の第3の実施例の電磁波遮蔽通気孔の
構成例。
FIG. 5 is a structural example of an electromagnetic wave shielding vent hole according to a third embodiment of the present invention.

【図6】 本発明の第3の実施例の電磁波遮蔽通気孔の
構成例。
FIG. 6 is a structural example of an electromagnetic wave shielding vent hole according to a third embodiment of the present invention.

【図7】 ハニカム遮蔽材と電波吸収体の組み合わせ方
法を説明するための図。
FIG. 7 is a diagram for explaining a method of combining the honeycomb shielding material and the radio wave absorber.

【図8】 従来例のハニカム遮蔽材の図。FIG. 8 is a diagram of a conventional honeycomb shielding material.

【図9】 従来例の電波吸収体を装着した通気孔の図。FIG. 9 is a view of a ventilation hole in which a radio wave absorber of a conventional example is attached.

【符号の説明】[Explanation of symbols]

イ: 電波暗室、または電磁波遮蔽室。 ロ: 通気孔。 ハ: ハニカム遮蔽材。 ニ: 電波吸収体。 L,L1、L2: 電波吸収体装着部の長さ B: An anechoic chamber or an electromagnetic shield room. B: Vent hole. C: Honeycomb shielding material. D: Radio wave absorber. L, L1, L2: Length of the electromagnetic wave absorber mounting part

Claims (3)

【特許請求の範囲】[Claims] 【請求項1】 金属板よりなる通気孔で、前記通気孔の
内壁面にピラミッド形電波吸収体、或いは楔形電波吸収
体を装着し、かつ通気孔の入り口、或いは出口の少なく
ともどちらか一方の断面をハニカム遮蔽材で覆ったこと
を特徴とする電磁波遮蔽通気孔。
1. A vent hole formed of a metal plate, wherein a pyramidal radio wave absorber or a wedge radio wave absorber is mounted on an inner wall surface of the vent hole, and a cross section of at least one of an entrance and an exit of the vent hole. An electromagnetic wave shielding ventilation hole characterized by covering the above with a honeycomb shielding material.
【請求項2】 通気孔は、その入り口から出口までを直
線で見通せないように折り曲げた通気孔であることを特
徴とする請求項1に記載の電磁波遮蔽通気孔。
2. The electromagnetic wave shielding vent hole according to claim 1, wherein the vent hole is a vent hole that is bent so that a straight line cannot be seen from the entrance to the exit.
【請求項3】 金属板よりなる通気孔で、前記通気孔断
面より小さい底面のピラミッド形電波吸収体、或いは楔
形電波吸収体を複数個用いて通気孔入り口面から見たと
きに断面全領域がいずれかの吸収体により隠されて出口
まで見通せなく、かつ通気孔の奥行き方向には電波吸収
体の設置位置をずらして空気の流通を確保し、かつ通気
孔の入り口、或いは出口の少なくともどちらか一方の断
面をハニカム遮蔽材で覆ったことを特徴とする電磁波遮
蔽通気孔。
3. A ventilation hole made of a metal plate, and when a plurality of pyramid-shaped electromagnetic wave absorbers or wedge-shaped electromagnetic wave absorbers having a bottom surface smaller than the cross section of the ventilation hole are used and the entire cross-sectional area is viewed from the entrance surface of the ventilation hole One of the inlets and / or the outlets of the ventilation holes is hidden by one of the absorbers and cannot be seen through to the outlet, and the air absorber is displaced in the depth direction of the ventilation hole to ensure air circulation. An electromagnetic wave shielding ventilation hole, characterized in that one section is covered with a honeycomb shielding material.
JP6337877A 1994-12-27 1994-12-27 Electromagnetic wave shielding vent Expired - Lifetime JP2788862B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP6337877A JP2788862B2 (en) 1994-12-27 1994-12-27 Electromagnetic wave shielding vent

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP6337877A JP2788862B2 (en) 1994-12-27 1994-12-27 Electromagnetic wave shielding vent

Publications (2)

Publication Number Publication Date
JPH08186394A true JPH08186394A (en) 1996-07-16
JP2788862B2 JP2788862B2 (en) 1998-08-20

Family

ID=18312837

Family Applications (1)

Application Number Title Priority Date Filing Date
JP6337877A Expired - Lifetime JP2788862B2 (en) 1994-12-27 1994-12-27 Electromagnetic wave shielding vent

Country Status (1)

Country Link
JP (1) JP2788862B2 (en)

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR100447887B1 (en) * 1998-08-28 2004-09-08 티디케이가부시기가이샤 Radio Wave Transmitting Material
JP2006344825A (en) * 2005-06-09 2006-12-21 Takenaka Komuten Co Ltd Electromagnetic wave shielding device
CN103383139A (en) * 2012-05-04 2013-11-06 赵阿萌 Air return port system with acoustic absorption wedges of silencer
US8987610B2 (en) 2012-01-06 2015-03-24 Electronics And Telecommunications Research Institute Vent structure for electromagnetic shielding
JP2020122616A (en) * 2019-01-30 2020-08-13 三菱重工業株式会社 duct
JP2022120572A (en) * 2021-02-05 2022-08-18 アンリツ株式会社 Temperature testing device and temperature testing method

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH04202981A (en) * 1990-11-29 1992-07-23 Tomoe Corp Outside air intake for air conditioning in electromagnetic wave shielded structure
JPH0546318U (en) * 1991-11-30 1993-06-22 渡文株式会社 Tatami room

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH04202981A (en) * 1990-11-29 1992-07-23 Tomoe Corp Outside air intake for air conditioning in electromagnetic wave shielded structure
JPH0546318U (en) * 1991-11-30 1993-06-22 渡文株式会社 Tatami room

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR100447887B1 (en) * 1998-08-28 2004-09-08 티디케이가부시기가이샤 Radio Wave Transmitting Material
JP2006344825A (en) * 2005-06-09 2006-12-21 Takenaka Komuten Co Ltd Electromagnetic wave shielding device
US8987610B2 (en) 2012-01-06 2015-03-24 Electronics And Telecommunications Research Institute Vent structure for electromagnetic shielding
CN103383139A (en) * 2012-05-04 2013-11-06 赵阿萌 Air return port system with acoustic absorption wedges of silencer
JP2020122616A (en) * 2019-01-30 2020-08-13 三菱重工業株式会社 duct
JP2022120572A (en) * 2021-02-05 2022-08-18 アンリツ株式会社 Temperature testing device and temperature testing method

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