JPS594000A - High voltage testing shield room - Google Patents

High voltage testing shield room

Info

Publication number
JPS594000A
JPS594000A JP11426082A JP11426082A JPS594000A JP S594000 A JPS594000 A JP S594000A JP 11426082 A JP11426082 A JP 11426082A JP 11426082 A JP11426082 A JP 11426082A JP S594000 A JPS594000 A JP S594000A
Authority
JP
Japan
Prior art keywords
high voltage
voltage testing
electromagnetic waves
external electromagnetic
shield room
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
JP11426082A
Other languages
Japanese (ja)
Inventor
博多 哲郎
秀樹 大林
渡邊 次男
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric 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 Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP11426082A priority Critical patent/JPS594000A/en
Publication of JPS594000A publication Critical patent/JPS594000A/en
Pending legal-status Critical Current

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  • Shielding Devices Or Components To Electric Or Magnetic Fields (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】 この発明は、高電圧試験用シールドルームに関するもの
であり、もう少し詳しくいうと、高電圧用電気機器の耐
電圧試験に供する高電圧試験用シールドルームに関する
ものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a shielded room for high-voltage testing, and more specifically, to a shielded room for high-voltage testing that is used for withstanding voltage testing of high-voltage electrical equipment.

高電圧用電気機器は耐電圧試験によって信頼性を検証す
るが、この際、故障個所から発生する微弱な部分放電を
検出することにより、故障個所の有無を判定するいわゆ
る部分放電試験を行うことが多い。このような試験の際
、たとえばラジオ放送波などの空間中の外来電磁波は、
この微弱な放電検出のためには不要な電気的雑音(ノイ
ズ)となるからできるだけこれを小さく抑える必要があ
る。したがって、このような高電圧試験に供するシール
ドルームの天井、側壁、床等に前記の外来電磁波をシー
ルドする構造がとられているのが普通であり、天井、側
壁、床等を金属板またはメツシュ等で製作し、こゎらを
相互に機械的に接続してできるだけ電気的に切れ目のな
い構造体に形成する努力がはられれている。
The reliability of high-voltage electrical equipment is verified through a withstand voltage test. At this time, it is often necessary to perform a so-called partial discharge test, which determines whether there is a faulty part by detecting the weak partial discharge that occurs from the faulty part. many. During such tests, external electromagnetic waves in space, such as radio broadcast waves, are
This weak discharge detection results in unnecessary electrical noise, which must be kept as small as possible. Therefore, the ceiling, side walls, floor, etc. of a shield room used for such high voltage tests are usually constructed to shield the external electromagnetic waves, and the ceiling, side walls, floor, etc. are covered with metal plates or mesh. Efforts are being made to mechanically connect them to form a structure that is as electrically seamless as possible.

一般に、放送波等の外来電磁波は、シールドルームの周
囲のあらゆる方向から到来するが、シールドルームの所
要シールド性能を決定づける最大強度をもつものは、そ
の到来方向を電界強度計によって容易に知ることができ
る。
In general, external electromagnetic waves such as broadcast waves arrive from all directions around a shielded room, but the direction of arrival of the one with the maximum intensity that determines the required shielding performance of the shielded room can be easily determined using a field strength meter. can.

この発明は、シールドルームが建設される地点において
、最大強度をもつ外来電磁波の到来方向を測定により知
った上で、こねに対するシールド効果を最大に発揮した
高電圧試験用シールドルームを得ることを目的とするも
のである。
The purpose of this invention is to obtain a shielded room for high-voltage testing that maximizes the shielding effect against kneading by measuring the arrival direction of external electromagnetic waves with the maximum intensity at the point where the shielded room is constructed. That is.

以下、1この発明の実施例を図によって説明する。Hereinafter, one embodiment of the present invention will be described with reference to the drawings.

第1図fa) + (b) 、fc)はこの種のシール
ドルームを模式的に示したもので、図において、最大強
度の外来磁波の到来方向へは、特別の場合を除き、一定
である。シールドルームlは屋根コ、側壁3.床ダでな
り、いずれも複数の金属板またはその折板で、七わらの
端部をラップさせて形成される。またこれらの部材間接
続部は前述のように、シールド効果をあげるために、一
定のピッチで、溶接等により継ぎ合わせることが多い。
Figure 1 fa) + (b), fc) schematically shows this type of shield room. . The shield room l has a roof, side walls 3. It is made of a plurality of metal plates or folded plates thereof, and the ends of the seven straws are wrapped. Further, as described above, in order to increase the shielding effect, the connecting portions between these members are often joined together at a constant pitch by welding or the like.

Bは地下水面を示す。B indicates the groundwater table.

この発明は、以上のようなシールドルームを形成する各
部材間の隙間から侵入する最大強度の外板材の葺き方を
示すもので、Aは最大強度をケ夙来電磁波、Aaは説明
のための仮想的な外来電磁波を示す。屋根−を構成する
屋根材−2a、コb。
This invention shows how to roof the outer panel material with the maximum strength that penetrates through the gaps between the members forming the shield room, where A indicates the maximum strength and Aa is for explanation. Showing virtual external electromagnetic waves. Roofing materials 2a and 2b constituting the roof.

2cは、コaから2Cに向って葺かれ、ラップ部はこの
順に上に重ねられており、ラップ部の隙間7.2の外部
開口部/2aは外来電磁波の到来方向Aとほぼ逆方向に
開口している。このように屋根コを形成することによっ
て外来電磁波Aは金属面で反射されても、隙間からシー
ルドルームlの内部に侵入することが極小に抑えられ、
シールドルーム/のシールド効果は著しく向上される。
2c is roofed from core a to 2C, the lap parts are stacked on top in this order, and the external opening /2a of the gap 7.2 in the lap part is in a direction almost opposite to the arrival direction A of external electromagnetic waves. It's open. By forming the roof in this way, even if the external electromagnetic waves A are reflected by the metal surface, the intrusion into the interior of the shield room L through the gaps is minimized,
The shielding effect of the shield room/is significantly improved.

もし、上記と逆に葺いた場合は、最大強度の外来電磁波
の到来方向はAaとして仮想的に示すものとなり、部材
ラップ部の隙間を通してシールドルームl内圧侵入しや
すくなることは図から明らかである。
If the roof is installed in the opposite way to the above, the direction of arrival of the external electromagnetic wave with the maximum intensity will be hypothetically shown as Aa, and it is clear from the figure that the internal pressure of the shield room l will easily enter through the gap between the lap parts of the parts. .

このことは実験的にも確かめられた。すナワチ、第3図
(a>に示すように、鉄板Fをラップさせて鉄板Fの直
角方向から電磁波EOを当てたときの透過電界強度E/
の分布を測定した結果6士、同図(b)に示すように電
磁波がラップ部の隙間を左前方力)ら右後方へ通り抜け
ていることを示している。
This was also confirmed experimentally. Sunawachi, as shown in Figure 3 (a), when iron plate F is wrapped and electromagnetic wave EO is applied from the direction perpendicular to iron plate F, the transmitted electric field strength E/
As shown in FIG. 6(b), the results of measuring the distribution of the electromagnetic waves show that the electromagnetic waves pass through the gap between the lap parts from the left front force to the right rear.

側壁3.床Vについても、上記と全く同様の考え方で構
成すればよい。すなわち、第2図(b) 、 (c)に
そねぞね示すように、壁材3a、3b、3cのラップ部
の隙間/3の外部開口部/3a、床材ea。
Side wall 3. The floor V may also be configured in exactly the same way as above. That is, as shown in FIGS. 2(b) and 2(c), the external opening /3a of the lap part of the wall materials 3a, 3b, and 3c is the gap /3, and the floor material ea.

Ilb、Fcのラップ部の隙間/ダの外部開口部/4’
aを、いずれも外来電磁波の到来方向Aに対しほぼ逆向
きになるように側壁3.床ダな形成する。ただ臥床材の
場合は、外来電磁波しま地下水面B等からの反射により
、地下から上方向に至1]来するので、実際に当っては
部材の端部を14’ & + <’ b tWcの順に
ラップさせることが他の部材の場合と異なる。
Gap between lap parts of Ilb and Fc/external opening of da/4'
a to the side wall 3.a so that both sides are substantially opposite to the arrival direction A of the external electromagnetic waves. Form the floor. However, in the case of sleeping floor materials, external electromagnetic waves are reflected from the underground water table B, etc., and come from underground to above, so in reality, the end of the material is It is different from the case of other members that they are wrapped in order.

第す図および第S図にそれぞれこの発明の他の実施4例
を示す。図において6は溶接金網、7&ま金属板に破線
を入れて引伸したいわゆるエキスノくンドメタルである
。これらは床材として用いられている。規模の大きいシ
ールドルームの床は、基礎工事との関係によりシールド
部材の上下でコンクリートを一体とする必要があり、金
属板ではなく、第ダ図、S図のようなメツシュを用いる
ことが多い。メツシュの場合は、外来電磁波の到来方向
がこわらの図においてAで示すようにメツシュのピッチ
が最小の方向からの場合に最もシールド効果が高い。実
験によれば、Aの方向の場合の方がA aの場合よりも
数dBから10dB程度もシールド効果が高い。したが
って、シールドルーム建設地点の最大強度の外来電磁波
の到来方向を測定し、これがいずれもAの方向から到来
するような向きに床材メツシュを敷くことにより、最大
のシールド効果を発揮することができることになる。こ
のため建屋に対して部材を斜め向きに敷く場合も生じる
FIGS. 1 and 2 show four other embodiments of the present invention, respectively. In the figure, 6 is a welded wire mesh, 7 & is a so-called exno-kunded metal made by enlarging a metal plate with broken lines. These are used as flooring materials. For the floor of a large-scale shield room, it is necessary to integrate concrete above and below the shield member due to foundation work, and meshes as shown in Figures D and S are often used instead of metal plates. In the case of a mesh, the shielding effect is highest when the direction in which the external electromagnetic waves arrive is from the direction where the pitch of the mesh is minimum, as shown by A in the figure. According to experiments, the shielding effect in the direction A is several dB to about 10 dB higher than in the case Aa. Therefore, the maximum shielding effect can be achieved by measuring the arrival direction of the highest intensity external electromagnetic waves at the shield room construction point and laying the flooring mesh in such a direction that they all arrive from direction A. become. For this reason, there are cases where members are laid diagonally to the building.

ところで上記説明では、この発明を高電圧電気機器の試
験に利用するシールドルームの場合について述べたが、
その他の用途のシールドルームに利用できることはいう
までもない。
By the way, in the above explanation, the case of a shielded room where the present invention is used for testing high voltage electrical equipment was described.
Needless to say, it can be used as a shield room for other purposes.

この発明は、以上説明したとおり、高電圧試験用シール
ドルームの建設地点における最大強度の外来電磁波の到
来方向を知った後に、こねに対するシールド効果が最大
となるように部材を配置するという簡単な構造により、
通常の建築材を利用して、経済的でしかも高いシールド
効果を具現することができる。
As explained above, this invention has a simple structure in which members are arranged so that the shielding effect against kneading is maximized after knowing the direction of arrival of the maximum intensity external electromagnetic waves at the construction point of the high voltage test shield room. According to
It is possible to realize an economical and high shielding effect by using ordinary construction materials.

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

第1図はこの発明の一実施例の模式的説明図で、五 同図(a)は平面図、(b)は平面図、(c)は側面図
、第−図体1 、 (b) 、 ((りは同じくそれぞ
れ部分断面図、第3図(a)″、(b)はそれぞれ透過
電界強度の説明図および特性線図、第ダ図、第3図はこ
の発明のそれぞれ他の実施例の平面図および斜視図であ
る。 /・・シールドルーム、コ・・屋根1.2a、Jb。 J、c−−屋根材、3・・側壁、3a 、3b 、、?
C・・壁材、ダ・・床、ダa、ダb、ダC・・床材、l
λ、/3./’I−−隙間、/λa、/3a。 /IIa・・外部開口部、6・・溶接金網、り・・エキ
スバンドメタル。 なお、各図中、同一符号は同一または相当部分を示す。 代理人  葛  野  信  − 427
FIG. 1 is a schematic explanatory diagram of an embodiment of the present invention, where (a) is a plan view, (b) is a plan view, (c) is a side view, and FIG. ((2) are also partial sectional views, FIGS. 3(a) and 3(b) are explanatory diagrams and characteristic diagrams of transmitted electric field strength, respectively, and FIGS. They are a plan view and a perspective view of /...shield room, co...roof 1.2a, Jb. J, c--roofing material, 3...side wall, 3a, 3b,...?
C...wall material, da...floor, da a, da b, da C...floor material, l
λ, /3. /'I--gap, /λa, /3a. /IIa...External opening, 6...Welded wire mesh, Ri...Extracted metal. In each figure, the same reference numerals indicate the same or corresponding parts. Agent Shin Kuzuno - 427

Claims (1)

【特許請求の範囲】 (1)端部を互いにラップさせこのラップ部に形成され
る隙間の外部開口部を最大強度の外来電磁波の到来方向
に対してほぼ逆向きとした複数の金属板でなる屋根およ
び側壁を備えてなることを特徴とする高電圧試験用シー
ルドルーム。 (コ)金属板が折板でなる特許請求の範囲第1項記載の
高電圧試験用シールドルーム。 (3)端部を互いにラップさせこのラップ部に形成され
る隙間の外部開口部を最大強度の外来電磁波の到来方向
に対してほぼ逆向きとした複数の金属板でなる床を備え
た特許請求の範囲第1項記載の高電圧試験用シールドル
ーム。 (り)外来電磁波の到来方向に直角な方向の網目ピッチ
が最小となるように配置した金属メツシュを有する床を
備えた特許請求の範囲第7項記載の高電圧試験用シール
ドルーム。
[Claims] (1) Consisting of a plurality of metal plates whose ends are lapped together and the external opening of the gap formed in the lapped portion is oriented almost opposite to the direction in which the external electromagnetic waves of maximum intensity arrive. A shielded room for high voltage testing characterized by having a roof and side walls. (g) A shielded room for high voltage testing according to claim 1, wherein the metal plate is a folded plate. (3) A patent claim comprising a floor made of a plurality of metal plates whose ends are lapped together and the external opening of the gap formed in the lapped portion is oriented substantially opposite to the arrival direction of the maximum intensity of external electromagnetic waves. A shielded room for high voltage testing as described in item 1. (i) A shielded room for high voltage testing according to claim 7, comprising a floor having a metal mesh arranged so that the mesh pitch in the direction perpendicular to the arrival direction of external electromagnetic waves is minimized.
JP11426082A 1982-06-29 1982-06-29 High voltage testing shield room Pending JPS594000A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP11426082A JPS594000A (en) 1982-06-29 1982-06-29 High voltage testing shield room

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP11426082A JPS594000A (en) 1982-06-29 1982-06-29 High voltage testing shield room

Publications (1)

Publication Number Publication Date
JPS594000A true JPS594000A (en) 1984-01-10

Family

ID=14633331

Family Applications (1)

Application Number Title Priority Date Filing Date
JP11426082A Pending JPS594000A (en) 1982-06-29 1982-06-29 High voltage testing shield room

Country Status (1)

Country Link
JP (1) JPS594000A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS62229998A (en) * 1986-03-31 1987-10-08 清水建設株式会社 Electromagnetic shielding structure of assembly board
JPH03128999U (en) * 1990-04-04 1991-12-25

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS4712887U (en) * 1971-03-11 1972-10-16
JPS5637615B2 (en) * 1975-03-26 1981-09-01

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS4712887U (en) * 1971-03-11 1972-10-16
JPS5637615B2 (en) * 1975-03-26 1981-09-01

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS62229998A (en) * 1986-03-31 1987-10-08 清水建設株式会社 Electromagnetic shielding structure of assembly board
JPH0362320B2 (en) * 1986-03-31 1991-09-25 Shimizu Construction Co Ltd
JPH03128999U (en) * 1990-04-04 1991-12-25

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