JPH0258799B2 - - Google Patents
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- Publication number
- JPH0258799B2 JPH0258799B2 JP11023288A JP11023288A JPH0258799B2 JP H0258799 B2 JPH0258799 B2 JP H0258799B2 JP 11023288 A JP11023288 A JP 11023288A JP 11023288 A JP11023288 A JP 11023288A JP H0258799 B2 JPH0258799 B2 JP H0258799B2
- Authority
- JP
- Japan
- Prior art keywords
- radio wave
- radio
- extension
- wave absorber
- section
- 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
Links
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- Details Of Measuring And Other Instruments (AREA)
- 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、試験体から放射される電波の測定
に使用される電波無響室に関するものである。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a radio anechoic chamber used for measuring radio waves emitted from a test object.
一般に、電波の測定を普通の部屋で行うと、壁
や床からの反射電波の影響の為に誤差が大きい。
Generally, when radio waves are measured in a normal room, there is a large error due to the influence of reflected radio waves from walls and floors.
このため、此の種の実験には部屋の全壁面を電
波吸収体で構成された所謂電波無響室が使用され
ている。 For this reason, this type of experiment uses a so-called radio anechoic chamber in which the entire wall of the room is made of radio wave absorbers.
しかしながら、従来の電波無響室は、完全な箱
状に構成されているので、試験体から発生する電
波が電波吸収体の壁面に対して垂直でなく斜めに
当たる部分ができる。
However, since conventional radio anechoic chambers are configured in a complete box shape, there are portions where the radio waves generated from the test specimen impinge obliquely rather than perpendicularly to the wall surface of the radio wave absorber.
電波吸収体は、電波が垂直に当たると電波吸収
性が極めて高いが、斜めに当たると吸収性が著し
く低下する。従つて、単に、壁面に電波吸収体を
張りつけただけの電波無響室では、電波を完全に
吸収することは不可能で、余計な反射波が発生し
測定に悪影響を与える。 Radio wave absorbers have extremely high radio wave absorption properties when radio waves strike vertically, but their absorption properties drop significantly when radio waves strike diagonally. Therefore, in a radio anechoic chamber in which a radio wave absorber is simply attached to the wall surface, it is impossible to completely absorb radio waves, and unnecessary reflected waves are generated, which adversely affects measurements.
また電波無響室の壁面全面に電波吸収体を配設
するのは、電波吸収体が高価であるため工事費が
高くなつていた。 Furthermore, installing radio wave absorbers on the entire wall surface of a radio anechoic chamber requires high construction costs because radio wave absorbers are expensive.
この発明は、前記従来の問題点を解決するため
に提案されたもので、電波測定に際し、試験体か
ら発生する不要電波を完全に吸収することができ
るとともに施工費が安価となる電波無響室を提供
することを目的とする。 This invention was proposed in order to solve the above-mentioned conventional problems, and is a radio anechoic chamber that can completely absorb unnecessary radio waves generated from a test object when measuring radio waves and is inexpensive to construct. The purpose is to provide
この発明は屋根断面が楕円形である半球状の無
響室を使用するものである。
This invention uses a hemispherical anechoic chamber with an elliptical roof cross section.
屋根断面は床上の二焦点からの距離の和が一定
な軌跡を描く楕円形である半球体である。この二
焦点を結ぶ直線の延長線上の一側部に前記半球体
から突出する拡張部を設ける。拡張部に近い方の
焦点上に電波試験体を載せ、他方の焦点下に電波
吸収体を埋設する。また拡張部内には測定用アン
テナを設置し、拡張部の端部内壁には電波吸収体
を配設するものである。 The cross section of the roof is an elliptical hemisphere whose sum of distances from the two focal points on the floor follows a constant trajectory. An extension part protruding from the hemisphere is provided on one side of the extension line of the straight line connecting the two focal points. Place the radio wave test object on the focal point closest to the extension, and bury the radio wave absorber under the other focal point. Furthermore, a measurement antenna is installed within the extended portion, and a radio wave absorber is provided on the inner wall of the end portion of the expanded portion.
電波試験体から発せられた電波は楕円形断面の
内壁に反響して、他方の焦点下の電波吸収体に吸
収される。
The radio waves emitted from the radio wave test object are reflected on the inner wall of the elliptical cross section and are absorbed by the other radio wave absorber under the focal point.
拡張部内に浸入した電波はアンテナによつて測
定され、不要な電波は背面の電波吸収体に吸収さ
れる。 Radio waves that have entered the extension are measured by the antenna, and unnecessary radio waves are absorbed by the radio wave absorber on the back.
以下、図に示す一実施例に基づきこの発明を詳
細に説明する。
Hereinafter, the present invention will be explained in detail based on an embodiment shown in the drawings.
図において1は電波無響室の屋根部であつて、
床2上の二焦点F,F′からの距離の和が一定であ
る楕円状の断面を成す半球体である。床2上には
銅メツキ鋼板が敷設されており、この完全反射面
によつて、電波が焦点に向つて正確に収束され
る。屋根部1は、第5図に示すように、フアイバ
ー補強プラスチツク(FRP)によつて形成した
円弧状外周面を有するセグメント3,3によつて
半球体に形成されており、この外周は銅箔4によ
つて葺かれている。セグメント3,3には強化プ
ラスチツクネジ止め5によつて連結されており、
その外周の銅箔4,4はハンダ6によつて接続さ
れている。 In the figure, 1 is the roof of the anechoic chamber,
It is a hemisphere with an elliptical cross section in which the sum of the distances from the bifocal points F and F' on the floor 2 is constant. A copper-plated steel plate is laid on the floor 2, and this completely reflective surface allows radio waves to be accurately converged toward a focal point. As shown in FIG. 5, the roof part 1 is formed into a hemispherical shape by segments 3, 3 having an arcuate outer circumferential surface formed of fiber-reinforced plastic (FRP), and this outer circumference is made of copper foil. It is covered with 4. The segments 3, 3 are connected by reinforced plastic screws 5,
The copper foils 4, 4 on the outer periphery are connected by solder 6.
二焦点F,F′を結ぶ直線の延長線上の一側部に
は屋根部1から側方に張出る拡張部7が形成され
ている。拡張部7の屋根部1′は、拡張部7に近
い焦点Fを中心として放射状に拡がつている。 An extended portion 7 extending laterally from the roof portion 1 is formed on one side of the extension of the straight line connecting the bifocals F and F'. The roof portion 1' of the extension 7 extends radially around a focal point F close to the extension 7.
この拡張部7の端部側内壁にはFを中心とした
球面状に電波吸収体8が配設されている。電波吸
収体8は四角すい状であつて、この電波吸収体8
が複数個突設されている。電波吸収体8としては
カーボン含浸発泡ウレタン等の材質が採用でき
る。また拡張部7内には測定用アンテナ9が設置
されている。二焦点F,F′のうち拡張部7に近い
方の焦点F上には電波発生用の試験体10が載置
されている。 A radio wave absorber 8 is disposed in a spherical shape centered at F on the inner wall of the end portion of the extended portion 7 . The radio wave absorber 8 has a square pyramid shape.
There are multiple protruding pieces. As the radio wave absorber 8, a material such as carbon-impregnated urethane foam can be used. Furthermore, a measurement antenna 9 is installed within the extension section 7. A test specimen 10 for generating radio waves is placed on the focal point F, which is closer to the extension part 7, of the two focal points F and F'.
他方の焦点F′下には電波をスムーズに吸収する
ためにカーボン含浸量が下部にいくに従つて漸増
する円盤状の電波吸収体11が重ねられて複数枚
埋設されている。(“電波浸透桝”)。 Under the other focal point F', a plurality of disc-shaped radio wave absorbers 11, in which the amount of carbon impregnated gradually increases toward the bottom, are stacked and buried in order to smoothly absorb radio waves. (“Radio wave penetration box”).
次に以上のような電波無響室における電波の測
定作業につき説明する。 Next, the radio wave measurement work in the radio anechoic chamber as described above will be explained.
試験体10から発せられた電波は屋根部2内周
面に当たり、楕円の性質から他方の焦点F′に向つ
て反響する。焦点F′下には電波吸収体11が埋設
されており、これによつて電波は吸収されてそれ
以上反響しない。 The radio waves emitted from the test object 10 hit the inner circumferential surface of the roof section 2, and due to the elliptical nature, they reverberate toward the other focal point F'. A radio wave absorber 11 is buried below the focal point F', which absorbs the radio waves and prevents them from reverberating any further.
拡張部7内に浸入した電波は測定アンテナ9に
当つて測定される。測定アンテナ9に当たらない
不要な電波は、背面の電波吸収体8に吸収されて
反響しない。 The radio waves that have entered the extended portion 7 hit the measurement antenna 9 and are measured. Unnecessary radio waves that do not hit the measurement antenna 9 are absorbed by the radio wave absorber 8 on the back and do not echo.
この発明は以上のような構成を有し、以下のよ
うな効果を得ることができる。
The present invention has the above configuration and can obtain the following effects.
(イ) 試験体から出た電波は断面楕円形を成す半球
状の屋根部内面に当つて電波吸収体に向つて反
響するため、屋根全面に電波吸収体を配設する
必要なく、工事費を安価にすることができる。(b) Since the radio waves emitted from the test specimen hit the inner surface of the hemispherical roof with an elliptical cross section and reverberate toward the radio wave absorber, there is no need to install a radio wave absorber over the entire roof, reducing construction costs. It can be made cheap.
(ロ) 拡張部へ浸入した電波は反響せずに測定アン
テナに当たり、正確な測定が可能となる。(b) The radio waves that have entered the extension section hit the measurement antenna without echoing, making accurate measurements possible.
第1図は電波無響室の平面図、第2図、第3図
はそれぞれ第1図の―線、―線断面図、
第4図は電波吸収体の斜視図、第5図は屋根部一
部の構成を示す斜視図である。
1……屋根部、2……床、3……セグメント、
7……拡張部、8……電波吸収体、9……測定用
アンテナ、10……試験体、11……電波吸収体
(“電波浸透桝”)。
Figure 1 is a plan view of the radio anechoic chamber, Figures 2 and 3 are cross-sectional views taken along lines - and - in Figure 1, respectively.
FIG. 4 is a perspective view of the radio wave absorber, and FIG. 5 is a perspective view showing the structure of a part of the roof. 1... Roof, 2... Floor, 3... Segment,
7... Extension portion, 8... Radio wave absorber, 9... Measurement antenna, 10... Test object, 11... Radio wave absorber ("radio wave penetration chamber").
Claims (1)
定な軌跡を描く楕円形を成す半球体であつて、こ
の二焦点を結ぶ直線の延長線上の一側部に前記半
球体から突出する拡張部を設け、前記二焦点のう
ち拡張部に近い方の焦点上に電波試験体を載せ、
他方の焦点下に電波吸収体を埋設するとともに、
拡張部内には測定用アンテナを設置し、拡張部の
端部内壁には電波吸収体を配設したことを特徴と
する電波無響室。1 A hemisphere in which the cross section of the roof forms an ellipse in which the sum of the distances from two focal points on the floor traces a constant trajectory, and an extension protruding from said hemisphere on one side on an extension of a straight line connecting these two focal points. a section, and place a radio wave test object on the focal point closer to the expansion section of the two focal points,
In addition to burying a radio wave absorber under the other focal point,
A radio anechoic chamber characterized in that a measurement antenna is installed inside the extension part, and a radio wave absorber is arranged on the inner wall at the end of the extension part.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP11023288A JPH01280399A (en) | 1988-05-06 | 1988-05-06 | Wave anechoic room |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP11023288A JPH01280399A (en) | 1988-05-06 | 1988-05-06 | Wave anechoic room |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH01280399A JPH01280399A (en) | 1989-11-10 |
| JPH0258799B2 true JPH0258799B2 (en) | 1990-12-10 |
Family
ID=14530444
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP11023288A Granted JPH01280399A (en) | 1988-05-06 | 1988-05-06 | Wave anechoic room |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH01280399A (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2005061949A (en) * | 2003-08-11 | 2005-03-10 | Device Co Ltd | Electromagnetic wave measurement dark box |
| CN101802625B (en) | 2007-09-28 | 2012-08-08 | 安立股份有限公司 | Transmission power measurement method and transmission power measurement device |
-
1988
- 1988-05-06 JP JP11023288A patent/JPH01280399A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPH01280399A (en) | 1989-11-10 |
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