JPH0322718B2 - - Google Patents
Info
- Publication number
- JPH0322718B2 JPH0322718B2 JP60262067A JP26206785A JPH0322718B2 JP H0322718 B2 JPH0322718 B2 JP H0322718B2 JP 60262067 A JP60262067 A JP 60262067A JP 26206785 A JP26206785 A JP 26206785A JP H0322718 B2 JPH0322718 B2 JP H0322718B2
- Authority
- JP
- Japan
- Prior art keywords
- air supply
- anechoic chamber
- exhaust
- electromagnetic waves
- port
- 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.)
- Expired - Lifetime
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Landscapes
- Shielding Devices Or Components To Electric Or Magnetic Fields (AREA)
Description
【発明の詳細な説明】
〔産業上の利用分野〕
この発明は、電磁波の計測を行なう電波暗室の
構造に関するものである。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to the structure of an anechoic chamber for measuring electromagnetic waves.
一般に、微弱な電磁波の計測は、障害電波ある
いは有害な反射波の影響を排除した電波暗室で行
なわれる。従来、この種の電波暗室の構造とし
て、第3図に示した電波暗室構造Aが知られてい
る。電波暗室構造Aについて説明すると、図にお
いて符号1は、コンクリート建造物1a内に設け
られた電波暗室である。電波暗室1は薄厚の鉄板
からなる、天盤部2と、床部3と、給気口4およ
び排気口5を有する側壁部6a,6bとから構成
され、その内部に測定室7が形成されたものであ
る。前記天盤部2と側壁部6a,6b内側には、
電磁波吸収材8が張設されている。また、前記給
気口4には給気フアン9と金網10が取付られ、
前記排気口5には排気フアン11と金網12が取
付られている。一方、測定室1の底部3の下方に
はケーブルピツト13aが設けられ、同測定室1
の天盤部2には照明装置13bが備えられてい
る。前記電波暗室構造Aは、電波暗室1を構成す
る鉄板および金網10,12によつて外部からの
電磁波を遮断し、電磁波吸収材8によつて内部で
発生した電磁波を吸収し、給気口4に備えた給気
フアン9と排気口5に備えた排気フアン11によ
つてその内部の換気を行なうものである。
Generally, weak electromagnetic waves are measured in an anechoic chamber that eliminates the effects of interfering radio waves or harmful reflected waves. Conventionally, as a structure of this type of anechoic chamber, an anechoic chamber structure A shown in FIG. 3 is known. To explain the anechoic chamber structure A, reference numeral 1 in the figure is an anechoic chamber provided within a concrete building 1a. The anechoic chamber 1 is composed of a top panel 2 made of a thin iron plate, a floor section 3, and side walls 6a and 6b having an air supply port 4 and an exhaust port 5, and a measurement chamber 7 is formed therein. It is something that Inside the top plate portion 2 and side wall portions 6a and 6b,
An electromagnetic wave absorbing material 8 is stretched. Further, an air supply fan 9 and a wire mesh 10 are attached to the air supply port 4,
An exhaust fan 11 and a wire mesh 12 are attached to the exhaust port 5. On the other hand, a cable pit 13a is provided below the bottom 3 of the measurement chamber 1.
The top panel 2 is equipped with a lighting device 13b. The anechoic chamber structure A blocks electromagnetic waves from the outside by the iron plates and wire meshes 10 and 12 that constitute the anechoic chamber 1, absorbs electromagnetic waves generated inside by the electromagnetic wave absorbing material 8, and The interior is ventilated by an air supply fan 9 provided at the exhaust port 5 and an exhaust fan 11 provided at the exhaust port 5.
ところで、上記の電波暗室構造Aにおいては、
給気口4および排気口5から浸入する外界の電磁
波を金網10,12によつて遮断していたため、
金網10,12の網目から電磁波が浸入し、給気
口4および排気口5部分のシールド性能が低下す
るという問題があつた。また、上記の電波暗室構
造Aにおいては、給気口4および排気口5に電磁
波吸収材8が張設されていないため、内部で発生
した電磁波が給気口4および排気口5部分で反射
し、これによつて測定室で行なう電磁波の計測に
支障を来すという問題があつた。更に、前記給気
口4および排気口5に電磁波吸収および電磁波遮
蔽の処理を施すには、コストの上からも問題があ
つた。この発明は、上記の事情に鑑みてなされた
もので上記の欠点を解消し得る電波暗室構造を如
何に実現するかを問題としている。
By the way, in the above anechoic chamber structure A,
Because the electromagnetic waves from the outside world that entered from the air supply port 4 and the exhaust port 5 were blocked by the wire meshes 10 and 12,
There was a problem in that electromagnetic waves penetrated through the meshes of the wire meshes 10 and 12, and the shielding performance of the air supply port 4 and exhaust port 5 portions deteriorated. In addition, in the above-mentioned anechoic chamber structure A, since the electromagnetic wave absorbing material 8 is not stretched over the air supply port 4 and the exhaust port 5, the electromagnetic waves generated inside are reflected at the air supply port 4 and the exhaust port 5. This caused a problem in that it interfered with electromagnetic wave measurements performed in the measurement room. Furthermore, there is a problem in terms of cost in applying electromagnetic wave absorption and electromagnetic wave shielding treatments to the air supply port 4 and the exhaust port 5. This invention was made in view of the above circumstances, and the problem is how to realize an anechoic chamber structure that can eliminate the above drawbacks.
本発明の実施例を第1図、第2図を参照して説
明する。第1図、第2図は電波暗室構造Bを示す
図であつて、これらの図において符号14はコン
クリート建造物14a内に設けられた電波暗室で
ある。電波暗室14は薄厚の鉄板(電磁波遮蔽
体)からなる、側壁部15a,15b,15c,
15dと、天盤部16と、床部17とから構成さ
れ、その内部に測定室18が形成されたものであ
る。前記側壁部15a,15b,15c,15d
および天盤部16の内側には、電磁波吸収材19
が張設されている。
Embodiments of the present invention will be described with reference to FIGS. 1 and 2. 1 and 2 are diagrams showing an anechoic chamber structure B, and in these figures, reference numeral 14 is an anechoic chamber provided within a concrete building 14a. The anechoic chamber 14 has side walls 15a, 15b, 15c, and 15c made of thin iron plates (electromagnetic shielding bodies).
15d, a top plate part 16, and a floor part 17, and a measurement chamber 18 is formed inside thereof. Said side wall portions 15a, 15b, 15c, 15d
And inside the top plate part 16, an electromagnetic wave absorbing material 19 is provided.
is installed.
また、前記電波暗室14の床部17は、地面m
の近傍に配設され、平行な床面20aと床面20
bとから構成されたものであり、これら床面20
aと床面20bの間は、空間部23になつてい
る。前記床面20aには、給気口24および排気
口25が形成され、これら給気口24および排気
口25には、空気流通孔26,26……を有する
鉄盤27,28が各々取付けられている。 Further, the floor portion 17 of the anechoic chamber 14 is located at the ground m.
A parallel floor surface 20a and a floor surface 20
b, and these floor surfaces 20
A space 23 is formed between a and the floor surface 20b. An air supply port 24 and an exhaust port 25 are formed in the floor surface 20a, and iron plates 27 and 28 having air circulation holes 26, 26, . . . are respectively attached to these air supply ports 24 and exhaust port 25. ing.
前記給気口24および排気口25下方の空間部
23には、給気ピツト31および排気ピツト32
が各々設けられている。給気ピツト31および排
気ピツト32は、給気パイプ33および排気パイ
プ34に各々接続されている。この場合、これら
給気パイプ33および排気パイプ34は共に、下
方の床面20bよりもさらに下方に、すなわち地
盤内に配設されている。これら給気ピツト31お
よび排気ピツト32の内部には、測定室18内の
給排気を行なう図示しない給気フアンおよび排気
フアンが各々備えられている。また、前記床部1
7の空間部23には、ケーブルピツト35が設け
られている。一方、床部17の床面20a上に
は、測定部18内の照明を行なうスタンド型の照
明装置36,36が床から取付られている。 In the space 23 below the air supply port 24 and the exhaust port 25, an air supply pit 31 and an exhaust pit 32 are provided.
are provided for each. The air supply pit 31 and the exhaust pit 32 are connected to an air supply pipe 33 and an exhaust pipe 34, respectively. In this case, both the air supply pipe 33 and the exhaust pipe 34 are arranged further below the lower floor surface 20b, that is, in the ground. Inside the air supply pit 31 and the exhaust pit 32, an air supply fan and an exhaust fan (not shown) for supplying and exhausting the inside of the measurement chamber 18 are provided, respectively. Further, the floor portion 1
A cable pit 35 is provided in the space 23 of 7. On the other hand, on the floor surface 20a of the floor section 17, stand-type lighting devices 36, 36 for illuminating the inside of the measuring section 18 are mounted from the floor.
上記の電波暗室構造Aは、測定室18を構成す
る鉄板によつて外部からの電磁波を遮断し、電磁
波吸収材19によつて内部で発生した電磁波を吸
収し、給気ピツト31に備えた給気フアンと排気
ピツト32に備えた排気フアンによつてその内部
の換気を行なうものである。 In the above-mentioned anechoic chamber structure A, the iron plate constituting the measurement chamber 18 blocks electromagnetic waves from the outside, the electromagnetic wave absorbing material 19 absorbs the electromagnetic waves generated inside, and the The interior is ventilated by an air fan and an exhaust fan provided in the exhaust pit 32.
上記の構成からなる電波暗室構造Bを使用する
際には、まず必要に応じて照明装置36,36に
より内部を照明した上で、給気フアンと排気フア
ンを動作させる。これら給気フアンと排気フアン
の動作により外部の空気は、給気パイプ33、給
気口24を通じて測定室18に取入られ、一方測
定室18内の空気は、排気口25、排気パイプ3
4を通じて外部に放出される。 When using the anechoic chamber structure B having the above configuration, the interior is first illuminated by lighting devices 36, 36 as required, and then the air supply fan and exhaust fan are operated. Through the operation of these air supply fans and exhaust fans, external air is taken into the measurement chamber 18 through the air supply pipe 33 and the air supply port 24, while air inside the measurement chamber 18 is taken into the measurement chamber 18 through the air supply pipe 33 and the air supply port 24.
It is released to the outside through 4.
以上の動作によつて換気が行なわれ、電磁波の
計測を行ない得る状態となる。一方、上記の構成
からなる電波暗室構造Bでは、外部からの電磁波
を鉄板が遮断し、また電磁波の計測等により発生
した測定室18内の電磁波を電磁波吸収材19が
吸収する。 Through the above operations, ventilation is performed and a state is reached in which electromagnetic waves can be measured. On the other hand, in the anechoic chamber structure B having the above configuration, the iron plate blocks electromagnetic waves from outside, and the electromagnetic wave absorbing material 19 absorbs electromagnetic waves within the measurement chamber 18 generated by electromagnetic wave measurement or the like.
上記の電波暗室構造Bにおいては、従来の電波
暗室構造Aと同様に給気口24と排気口25が設
けられているが、従来の電波暗室構造Bと異な
り、これら給気口24と排気口25が地面mに近
い床部17に設けられているため、地面mが外界
からの電磁波を遮断して、これら給気口24およ
び排気口25からの電磁波の浸入を防止すること
ができる。また、上記の電波暗室構造Bにおいて
は、従来の電波暗室構造Aのように給気口と排気
口を側壁部に設ける必要がないため、外界からの
電磁波の影響を受け易くかつ内部で発生した電磁
波の反射の起こり易い側壁部15a〜15dおよ
ひ天盤部16に一切の欠損部を与えることがな
く、よつてそれら側壁部15a〜15d、天盤部
16のすべてを鉄板と電磁波吸収材19によつて
遮蔽することができる。しかして、上記の電波暗
室構造Bでは、従来の電波暗室構造Aと比較し
て、シールド性能が向上すると共に、測定室18
内で発生した電磁波の吸収性能が向上し、その結
果電波暗室構造B内で微弱な電磁波の計測を支障
なく行なうことができる。また、床部17は、前
記空間部23を介して、鉄板より成る床面20
a,20bにより二重に構成したものであるか
ら、床部17に給気口24、排気口25等の開口
部を形成したにも拘わらず、床部17からの漏洩
電磁波を確実に遮蔽することができる。なぜな
ら、前記給気口24、排気口25等の開口部は上
方の(つまり測定室内側の)床面20aに形成さ
れており、該床面20aの下方にはさらに床面2
0bが地面mとの境界に配されるため、該下方の
床面20bにより地面m側からの電磁波はほぼ遮
断されるからである。さらにその際、上記の如
く、給気ピツト31、排気ピツト32、あるいは
ケーブルピツト35等は上下の床面20a,20
bの間の前記空間部23に構成したので、下方の
床面20bに欠損部が形成されるのを極力阻止し
て、より完全に近いシールド効果が得られるもの
となつている。更に、上記の電波暗室構造Bで
は、給気口24および排気口25を床部17に設
けたので、施工、管理コストが安価なもので済
む。 In the above anechoic chamber structure B, an air supply port 24 and an exhaust port 25 are provided like the conventional anechoic chamber structure A, but unlike the conventional anechoic chamber structure B, these air supply ports 24 and exhaust port 25 is provided on the floor 17 near the ground m, the ground m blocks electromagnetic waves from the outside world, and can prevent electromagnetic waves from entering from the air supply port 24 and the exhaust port 25. In addition, in the above-mentioned anechoic chamber structure B, unlike the conventional anechoic chamber structure A, there is no need to provide an air supply port and an exhaust port on the side wall, so it is susceptible to the influence of electromagnetic waves from the outside world and is susceptible to electromagnetic waves generated inside. There are no defects in the side walls 15a to 15d and the top plate 16, where electromagnetic waves are likely to be reflected.Therefore, all of the side walls 15a to 15d and the top plate 16 are made of iron plates and electromagnetic wave absorbing material. 19. Therefore, in the above-mentioned anechoic chamber structure B, the shielding performance is improved compared to the conventional anechoic chamber structure A, and the measurement chamber 18
The absorption performance of electromagnetic waves generated within the chamber is improved, and as a result, weak electromagnetic waves can be measured within the anechoic chamber structure B without any hindrance. Further, the floor portion 17 is connected to a floor surface 20 made of an iron plate through the space portion 23.
Since it has a double structure with a and 20b, leakage electromagnetic waves from the floor 17 can be reliably shielded even though openings such as the air supply port 24 and the exhaust port 25 are formed in the floor 17. be able to. This is because the openings such as the air supply port 24 and the exhaust port 25 are formed on the upper floor surface 20a (that is, on the inside of the measurement chamber), and there is a further floor surface 2 below the floor surface 20a.
0b is arranged at the boundary with the ground m, so that electromagnetic waves from the ground m side are substantially blocked by the lower floor surface 20b. Furthermore, in that case, as mentioned above, the air supply pit 31, exhaust pit 32, cable pit 35, etc.
Since it is arranged in the space 23 between the holes 20a and 20b, the formation of a defective portion on the lower floor surface 20b is prevented as much as possible, and a more perfect shielding effect can be obtained. Furthermore, in the above-mentioned anechoic chamber structure B, since the air supply port 24 and the exhaust port 25 are provided in the floor portion 17, construction and management costs can be kept low.
この発明の電波暗室によれば、床部を、空間部
を介して電磁波遮蔽体により二重に形成すると共
に、給気口および排気口等の開口部を上方の床面
に形成し、かつ前記給気口および排気口のための
給気ピツトおよび排気ピツトを前記空間部の内部
に構成したので、これら給気口および排気口から
の電磁波の浸入をほほ完全に防止することがで
き、また、外界の電磁波の影響を受け易くかつ内
部で発生した電磁波の反射の起こり易い側壁部と
天盤部に一切の欠損部を与えることがなく、よつ
てそれら側壁部および天盤部のすべてを鉄板と電
磁波吸収材で遮蔽することができ、従つて、側壁
部に給気口と排気口が設けられた従来の電波暗室
と比較した場合、シールド性能、電磁波吸収性能
共に向上し、その結果、内部で微弱な電磁波の計
測を支障なく行なうことができるという利点があ
る。更に、給気口および排気口を床部に設けたの
で、施工、管理コストが安価なもので済むという
利点がある。
According to the anechoic chamber of the present invention, the floor portion is formed in double form with an electromagnetic wave shielding member through the space portion, and openings such as an air supply port and an exhaust port are formed in the upper floor surface, and Since the air supply pit and the exhaust pit for the air supply port and the exhaust port are configured inside the space, it is possible to almost completely prevent electromagnetic waves from entering from the air supply port and the exhaust port, and There is no damage to the side walls and top panel, which are easily affected by external electromagnetic waves and where internally generated electromagnetic waves are likely to be reflected. It can be shielded with electromagnetic wave absorbing material, and therefore, when compared to a conventional anechoic chamber with air supply and exhaust ports on the side wall, both shielding performance and electromagnetic wave absorption performance are improved, and as a result, the internal It has the advantage that weak electromagnetic waves can be measured without any problems. Furthermore, since the air supply and exhaust ports are provided on the floor, there is an advantage that construction and management costs are low.
第1図は本発明の実施例として示した電波暗室
構造の縦断正面図、第2図はそのa−a視線平面
図、第3図は従来の電波暗室構造を示す縦断正面
図である。
B……電波暗室構造、17……床部、20a…
…床面、20b……床面、23……空間部、24
……給気口、25……排気口、給気ピツト……3
1、排気ピツト……32、36……照明設備。
FIG. 1 is a longitudinal sectional front view of a radio anechoic chamber structure shown as an embodiment of the present invention, FIG. 2 is a plan view taken along line a-a, and FIG. 3 is a longitudinal sectional front view showing a conventional radio anechoic chamber structure. B...Anechoic chamber structure, 17...Floor, 20a...
...Floor surface, 20b...Floor surface, 23...Space part, 24
...Air supply port, 25 ...Exhaust port, air supply pit...3
1. Exhaust pit...32, 36...Lighting equipment.
Claims (1)
波暗室の構造であつて、床部を、空間部を介して
電磁波遮蔽体により二重に形成すると共に、給気
口および排気口等の開口部を上方の床面に形成
し、かつ前記給気口および排気口のための給気ピ
ツトおよび排気ピツトを前記空間部の内部に構成
したことを特徴とする電波暗室の構造。 2 照明設備を床上に取付けたことを特徴とする
特許請求の範囲第1項記載の電波暗室の構造。[Scope of Claims] 1. A structure of an anechoic chamber surrounded by an electromagnetic wave shielding body, in which the floor portion is formed double with the electromagnetic wave shielding body through a space, and an air supply port and an exhaust port are formed. 1. A structure of an anechoic chamber, characterized in that an opening such as a mouth is formed in an upper floor surface, and an air supply pit and an exhaust pit for the air supply port and the exhaust port are formed inside the space. 2. The structure of the anechoic chamber according to claim 1, characterized in that the lighting equipment is installed on the floor.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP26206785A JPS62122199A (en) | 1985-11-21 | 1985-11-21 | Wave absorbing chamer structure |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP26206785A JPS62122199A (en) | 1985-11-21 | 1985-11-21 | Wave absorbing chamer structure |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS62122199A JPS62122199A (en) | 1987-06-03 |
| JPH0322718B2 true JPH0322718B2 (en) | 1991-03-27 |
Family
ID=17370567
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP26206785A Granted JPS62122199A (en) | 1985-11-21 | 1985-11-21 | Wave absorbing chamer structure |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS62122199A (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH01154697U (en) * | 1988-04-18 | 1989-10-24 | ||
| CN108468449B (en) * | 2018-04-23 | 2019-09-24 | 北京环境特性研究所 | A kind of overturning cover board for microwave dark room melt pit |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5638500U (en) * | 1979-08-31 | 1981-04-11 |
-
1985
- 1985-11-21 JP JP26206785A patent/JPS62122199A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS62122199A (en) | 1987-06-03 |
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