JPH03138999A - Radio wave dark room using reflecting plate - Google Patents
Radio wave dark room using reflecting plateInfo
- Publication number
- JPH03138999A JPH03138999A JP27822689A JP27822689A JPH03138999A JP H03138999 A JPH03138999 A JP H03138999A JP 27822689 A JP27822689 A JP 27822689A JP 27822689 A JP27822689 A JP 27822689A JP H03138999 A JPH03138999 A JP H03138999A
- Authority
- JP
- Japan
- Prior art keywords
- radio wave
- antenna
- wave
- reflected
- radio
- 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
Links
- 239000006096 absorbing agent Substances 0.000 claims abstract description 18
- 230000002093 peripheral effect Effects 0.000 claims abstract description 13
- 230000000903 blocking effect Effects 0.000 claims description 21
- 238000010276 construction Methods 0.000 abstract description 6
- 230000005540 biological transmission Effects 0.000 description 6
- 239000000463 material Substances 0.000 description 6
- 230000000694 effects Effects 0.000 description 5
- XEEYBQQBJWHFJM-UHFFFAOYSA-N Iron Chemical compound [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 description 4
- 238000005259 measurement Methods 0.000 description 4
- 230000001902 propagating effect Effects 0.000 description 4
- 230000005672 electromagnetic field Effects 0.000 description 3
- 238000009434 installation Methods 0.000 description 3
- RYGMFSIKBFXOCR-UHFFFAOYSA-N Copper Chemical compound [Cu] RYGMFSIKBFXOCR-UHFFFAOYSA-N 0.000 description 2
- 229910052782 aluminium Inorganic materials 0.000 description 2
- XAGFODPZIPBFFR-UHFFFAOYSA-N aluminium Chemical compound [Al] XAGFODPZIPBFFR-UHFFFAOYSA-N 0.000 description 2
- 229910052802 copper Inorganic materials 0.000 description 2
- 239000010949 copper Substances 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- 229910052742 iron Inorganic materials 0.000 description 2
- 229910052751 metal Inorganic materials 0.000 description 2
- 239000002184 metal Substances 0.000 description 2
- 230000010287 polarization Effects 0.000 description 2
- OKTJSMMVPCPJKN-UHFFFAOYSA-N Carbon Chemical compound [C] OKTJSMMVPCPJKN-UHFFFAOYSA-N 0.000 description 1
- 239000004698 Polyethylene Substances 0.000 description 1
- 238000010521 absorption reaction Methods 0.000 description 1
- 230000002411 adverse Effects 0.000 description 1
- 238000004378 air conditioning Methods 0.000 description 1
- 229910052799 carbon Inorganic materials 0.000 description 1
- 239000000470 constituent Substances 0.000 description 1
- 239000012212 insulator Substances 0.000 description 1
- 230000001788 irregular Effects 0.000 description 1
- -1 polyethylene Polymers 0.000 description 1
- 229920000573 polyethylene Polymers 0.000 description 1
- 230000002441 reversible effect Effects 0.000 description 1
Landscapes
- Shielding Devices Or Components To Electric Or Magnetic Fields (AREA)
- Testing Electric Properties And Detecting Electric Faults (AREA)
Abstract
Description
【発明の詳細な説明】
産業上の利用分野
本発明は、各種電子機器の電磁場適合性(ELECTR
OMAGNETICCOMPATIBILITY)、即
ち、各種電子機器が電磁場環境のもとで、十分予定され
た効率で動作し得る能力の測定、又は各種電子機器の内
部から発生する電磁雑音による電磁障害(ELECTR
OMAGNETICINTERFERENCE+の測定
を行って、電磁環境対策の資料を得るため等に用いられ
る電波暗室(電波無反射室)に関するものである。DETAILED DESCRIPTION OF THE INVENTION Field of Industrial Application The present invention relates to electromagnetic field compatibility (ELECTR) of various electronic devices.
OMAGNETIC COMPATIBILITY), that is, the ability of various electronic devices to operate with well-defined efficiency in an electromagnetic field environment, or measurement of electromagnetic interference (ELECTR) due to electromagnetic noise generated from within various electronic devices.
This relates to a radio anechoic chamber (radio wave non-reflection chamber) used for measuring OMAGNETIC INTERFERENCE+ and obtaining data on electromagnetic environment countermeasures.
従来の技術
従来の電波暗室は、周壁の内面全域及び天井壁面の全域
に、角錐又は鋸歯状錐(変形角錐)の形状を有し、例え
ば発泡ポリエチレンのシート中に炭素を含ませ、炭素の
含有率の異なるシートを複数枚重ねて形成された電波吸
収体を隙間なく設けて構成されている。2. Description of the Related Art Conventional anechoic chambers have a pyramid or serrated pyramid (deformed pyramid) shape over the entire inner surface of the peripheral wall and the entire ceiling wall. For example, carbon is contained in a sheet of foamed polyethylene. The radio wave absorber is formed by stacking a plurality of sheets with different ratios and is arranged without gaps.
発明が解決しようとする課題
電波暗室内において、上記のような電磁場適合性又は電
磁障害等の測定を行う場合に使用される電波の現行周波
数は、はぼ30MHzからloooMHz(波長で、は
ぼ10メートルから0.3メートル)の範囲である。Problems to be Solved by the Invention The current frequencies of radio waves used when measuring electromagnetic field compatibility or electromagnetic interference as described above in an anechoic chamber are approximately 30 MHz to looo MHz (wavelength: approximately 10 MHz). meters to 0.3 meters).
したがって、電波暗室の周壁の内面全域及び天井壁面に
設けられた角錐又は鋸歯状錐(変形角錐)の形状を有す
る電波吸収体の高さは、電波の最大波長の騒から%の高
さ(はぼ5メートルから2.5メートル)が必要で、個
々の電波吸収体が大形となるから、電波暗室の容積が大
となり、電波暗室を建設するために要する敷地面積も亦
大となる欠点がある。Therefore, the height of the radio wave absorber having the shape of a pyramid or a sawtooth pyramid (deformed pyramid) provided on the entire inner surface of the peripheral wall and the ceiling wall of the anechoic chamber is determined by the height of the maximum wavelength of the radio wave (%). (approximately 5 meters to 2.5 meters), and each radio wave absorber is large, so the volume of the anechoic chamber becomes large and the site area required to construct the anechoic chamber also increases. be.
又、電波を完全に吸収する電波吸収体を実現することは
経済的に困難で、通常用いられている電波吸収体は電波
の一部を反射し1周波数によって反射効果が異なるため
、広帯域に亙って良好な周波数特性を得ることが困難で
ある。In addition, it is economically difficult to realize a radio wave absorber that completely absorbs radio waves, and the radio wave absorbers that are normally used reflect a portion of the radio waves and the reflection effect differs depending on the frequency, so it is difficult to realize a radio wave absorber that completely absorbs radio waves. Therefore, it is difficult to obtain good frequency characteristics.
更に、電波暗室内に供試機器以外の装置又は人間が存在
すると、これらの存在が測定結果に及ぼす影響を無視す
ることが出来ないため、供試機器以外の装置の格納用及
び人間の待機用の部屋を電波暗室と別に設ける必要があ
り、この点からも敷地面積が大となって全体の建設費が
高くなる欠点がある。Furthermore, if equipment other than the equipment under test or people are present in the anechoic chamber, the influence of their presence on the measurement results cannot be ignored. It is necessary to provide a separate room from the anechoic chamber, which also has the disadvantage of increasing the site area and increasing the overall construction cost.
課題を解決するための手段1
本発明電波暗室は、上部を開放した周壁の内側全域に反
射面を斜め上向きにして設けられた電波反射板と、アン
テナと供試機器の載置台との間に設けられ、前記アンテ
ナからの直接波のみを通過せしめる空隙を有する反射波
遮断用スクリーンとを備えて成るものである。Means for Solving the Problems 1 The anechoic chamber of the present invention has a radio wave reflecting plate provided with a reflecting surface facing diagonally upward over the entire inner side of a peripheral wall with an open top, and a mounting table for an antenna and a device under test. and a reflected wave blocking screen having a gap that allows only direct waves from the antenna to pass through.
作用
アンテナから放射された電波の一部は、反射波遮断用ス
クリーンの空隙部分を通って直接供試機器に到達すると
共に、一部は電波反射板で反射され、この反射波の一部
及び床面からの反射波は、反射波遮断用スクリーンによ
って阻止され、電波反射板からの反射波の一部は上方に
向い、電波暗室の上部開放部から天空に放射される。A part of the radio waves radiated from the working antenna directly reaches the equipment under test through the gap in the screen for blocking reflected waves, and a part is reflected by the radio wave reflector. The reflected waves from the surface are blocked by the reflected wave blocking screen, and some of the reflected waves from the radio wave reflector are directed upward and radiated into the sky from the open upper part of the radio anechoic chamber.
天空は電波の理想的な吸収体であるから上方に向った反
射波が再び電波暗室内に戻ることなく。Since the sky is an ideal absorber of radio waves, the upward reflected waves do not return to the anechoic chamber.
アンテナから供試機器に到達する伝搬電波成分は直接波
のみとなる。The propagating radio wave component that reaches the equipment under test from the antenna is only the direct wave.
課題を解決するための手段2
本発明電波暗室は、周壁の内側全域に反射面を斜め上向
きにして設けられた電波反射板と、アンテナと供試機器
の載置台との間に設けられ+ n’記アンテナからの直
接波のみを通過せしめる空隙を有する反射波遮断用スク
リーンと、天井壁面に設けられた電波吸収体とを備えて
成るものである。Means for Solving the Problems 2 The anechoic chamber of the present invention is provided between a radio wave reflecting plate provided with a reflecting surface facing diagonally upward throughout the inner side of a peripheral wall, and a mounting table for an antenna and a device under test. This device comprises a reflected wave blocking screen having a gap that allows only direct waves from the antenna to pass through, and a radio wave absorber provided on the ceiling wall surface.
作用
アンテナから放射された電波の一部は、反射波遮断用ス
クリーンの空隙部分を通って直接供試機器に到達すると
共に、一部は周壁の内側に設けられた電波反射板で反射
され、この反射波の一部は反射波遮断用スクリーンによ
って阻止され、電波反射板からの反射波の一部は上方に
向い、電波暗室の天井壁面に設けられた電波吸収体に吸
収され、アンテナから供試機器に到達する伝搬電波成分
は直接波のみとなる。A part of the radio waves radiated from the working antenna directly reaches the equipment under test through the gap in the screen for blocking reflected waves, and a part is reflected by the radio wave reflecting plate installed inside the surrounding wall. Some of the reflected waves are blocked by the reflected wave blocking screen, and some of the reflected waves from the radio wave reflector are directed upwards and absorbed by the radio wave absorber installed on the ceiling wall of the anechoic chamber, and are transmitted from the antenna to the sample. The propagating radio wave components that reach the equipment are only direct waves.
実施例
第1図は、本発明の一実施例を示す平面図、第2図は、
第1図のA−A断面図、第3図は、第1図のB−B断面
図で、各図において、1は電波暗室の周壁、2は電波反
射板、3はアンテナで。Embodiment FIG. 1 is a plan view showing an embodiment of the present invention, and FIG. 2 is a plan view showing an embodiment of the present invention.
FIG. 1 is a cross-sectional view taken along line AA in FIG. 1, and FIG. 3 is a cross-sectional view taken along line B-B in FIG.
図には棒状体を以て示しであるが、例えばバイコニカル
アンテナ又はパラボラアンテナ等任意のアンテナを用い
ることが出来る。4は供試機器、5は供試機器4の載置
台で1例えば絶縁体によって形成されたターンテーブル
より成る。6は反射波遮断用スクリーンで、第3図に示
すように、中央部にほぼU字形の空隙7を設けである。Although a rod-shaped body is shown in the figure, any antenna such as a biconical antenna or a parabolic antenna can be used. Reference numeral 4 denotes a device under test; 5, a mounting table for the device under test 4; and 1, for example, a turntable made of an insulator. Reference numeral 6 denotes a screen for blocking reflected waves, and as shown in FIG. 3, a substantially U-shaped gap 7 is provided in the center.
電波反射板2は、周壁lの内側全域に、反射面を斜め上
向きにして設けられるが、反射面の床面に対する角度が
小なるほど、又、反射面の上縁の高さが高いほど電気的
効果を大ならしめることが出来る。The radio wave reflecting plate 2 is installed over the entire inner side of the peripheral wall l with the reflecting surface facing diagonally upward, but the smaller the angle of the reflecting surface with respect to the floor surface, and the higher the height of the upper edge of the reflecting surface, the more electrical the It can increase the effect.
然しながら、経済性を考慮すると1反射面の床面に対す
る角度をほぼ70°から25゛の間に選ぶことが望まし
く、又1反射面の上縁の高さはアンテナ3の上端より適
宜高くなるように形成する。However, considering economic efficiency, it is desirable to select the angle of the first reflecting surface to the floor between approximately 70° and 25°, and the height of the upper edge of the first reflecting surface to be appropriately higher than the upper end of the antenna 3. to form.
電波反射へ2の材質は、電波を透過することなく、反射
面を平滑に形成し得るものであればどんな材質でもよい
が、例えばアルミニューム板、鉄板、銅板等の金属板又
は板状金網等を用いて形成するか、市販の建築用板材等
の表面に導電性シートを貼付して形成してもよい。The material for radio wave reflection 2 may be any material as long as it does not transmit radio waves and can form a smooth reflective surface, such as a metal plate such as an aluminum plate, iron plate, or copper plate, or a plate-shaped wire mesh. The conductive sheet may be formed by attaching a conductive sheet to the surface of a commercially available construction board or the like.
反射波遮断用スクリーン6は、アンテナ3と供試機器4
の間に設けられ、空隙7を介してアンテナ3(又は供試
機器4)から供試機器4(又はアンテナ3)を見通すこ
とが出来るように配設されている。The reflected wave blocking screen 6 is used to protect the antenna 3 and the equipment under test 4.
The device under test 4 (or the antenna 3) can be seen through the antenna 3 (or the device under test 4) through the air gap 7.
反射波遮断用スクリーン6の材質は、電波が透過しない
ものであれば何でもよく、電波反射板2と同様に、例え
ばアルミニューム板、鉄板、銅板等の金属板又は板状金
網等を用いて形成するか、市販の建築用板材等の表面に
導電性シートを貼付して形成してもよい。The reflected wave blocking screen 6 may be made of any material as long as it does not allow radio waves to pass through it, and similarly to the radio wave reflecting plate 2, it may be formed using, for example, a metal plate such as an aluminum plate, iron plate, or copper plate, or a plate-shaped wire mesh. Alternatively, a conductive sheet may be attached to the surface of a commercially available construction board or the like.
電波反射板2と反射波遮断用スクリーン6の設置関係に
ついて説明すると、アンテナ3から供試機器4に到達す
る直接波と反射波との路程差(直接波の径路と反射波の
径路との差)が%波長以下となるようなVHF帯の電波
を試験に用いる場合には1反射波遮断用スクリーン6を
省いても支障はないが、直接波と反射波との路程差が鑓
波長より長く、電波反射板2の反射係数が大なる場合に
は1反射波遮断用スクリーン6を設けることが必要で、
アンテナ3から供試機器4を見た場合、又は、供試機器
4からアンテナ3を見た場合に、すべての電波反射板2
に写る相手の像が明瞭に認められないように空隙7の大
きさを選定する。To explain the installation relationship between the radio wave reflector 2 and the reflected wave blocking screen 6, the path difference between the direct wave and the reflected wave reaching the device under test 4 from the antenna 3 (the difference between the path of the direct wave and the path of the reflected wave) ) is less than % of the wavelength, there is no problem in omitting the reflected wave blocking screen 6, but the path difference between the direct wave and the reflected wave is longer than the half wavelength. If the reflection coefficient of the radio wave reflecting plate 2 is large, it is necessary to provide a screen 6 for blocking reflected waves.
When looking at the device under test 4 from the antenna 3, or when looking at the antenna 3 from the device under test 4, all the radio wave reflectors 2
The size of the gap 7 is selected so that the image of the other party cannot be clearly recognized.
尚、図には周壁lの上部を開放状態に保った場合を例示
したが、電波の透過を妨げることな(、雨雪を防ぎ得る
材質より成る屋根を設けることが望ましい。Although the figure shows an example in which the upper part of the peripheral wall l is kept open, it is desirable to provide a roof made of a material that does not impede transmission of radio waves (and can prevent rain and snow).
次に、本発明電波暗室の作動について説明する。Next, the operation of the anechoic chamber of the present invention will be explained.
反射波遮断用スクリーン6を省いた場合には、アンテナ
3から放射されて供試機器4に到達する伝搬電波成分は
、直接波、床面からの反射波及び電波反射板2からの反
射波となるが1本発明電波暗室においてはアンテナ3と
供試機器4との間に、アンテナ3からの直接波のみを通
過せしめる空隙7を有する反射波遮断用スクリーン6を
設けであるので、電波反射板2からの反射波の一部及び
床面からの反射波は、反射波遮断用スクリーン6によっ
て阻止され、電波反射板2からの反射波の一部は上方に
向い、電波暗室の上部開放部から天空に放射される。When the screen 6 for blocking reflected waves is omitted, the propagating radio wave component radiated from the antenna 3 and reaching the device under test 4 is a direct wave, a reflected wave from the floor surface, and a reflected wave from the radio wave reflecting plate 2. However, in the anechoic chamber of the present invention, a reflected wave blocking screen 6 having a gap 7 that allows only direct waves from the antenna 3 to pass is provided between the antenna 3 and the device under test 4, so that a radio wave reflecting plate is used. A part of the reflected wave from the radio wave reflecting plate 2 and a reflected wave from the floor surface are blocked by the reflected wave blocking screen 6, and a part of the reflected wave from the radio wave reflecting plate 2 is directed upward and is transmitted from the upper open part of the anechoic chamber. radiated into the sky.
天空は電波の理想的な吸収体であるから上方に向った電
波が再び電波暗室に戻ることはない。Since the sky is an ideal absorber of radio waves, radio waves traveling upward will never return to the anechoic chamber.
したがって、アンテナ3から供試機器4に到達する伝搬
電波成分は直接波のみとなる。Therefore, the propagating radio wave component that reaches the device under test 4 from the antenna 3 is only a direct wave.
電波の伝搬は可逆的であるから、供試機器4に生じた雑
音電波がアンテナ3に受信される場合にも全く同様に直
接波のみが受信されることとなる。Since the propagation of radio waves is reversible, even when the noise radio waves generated in the device under test 4 are received by the antenna 3, only direct waves are received in exactly the same way.
第4図は1本発明の他の実施例を示す断面図(第5図の
B−B断面図)、第5図は、第4図のA−A断面図、第
6図は、第5図のC−C断面図で、各図において、lは
周壁、2は電波反射板、3はアンテナ、4は供試機器、
5は供試機器4の載置台で、これらは第1図乃至第3図
に示したものと同様の構成である。4 is a sectional view (BB sectional view in FIG. 5) showing another embodiment of the present invention, FIG. 5 is a sectional view taken along AA in FIG. 4, and FIG. In each figure, l is the peripheral wall, 2 is the radio wave reflector, 3 is the antenna, 4 is the equipment under test,
Reference numeral 5 denotes a mounting table for the equipment under test 4, which has the same configuration as that shown in FIGS. 1 to 3.
6は反射波遮断用スクリーンで5本実施例においては、
前実施例のようにほぼU字形の空隙7を設ける代りにほ
ぼ円形の空隙8を穿った点が前実施例における反射波遮
断用スクリーンと異なる他は、反射波遮断用スクリーン
6の材質、電波反射板2との設置関係等は前実施例と全
く同様である。6 is a screen for blocking reflected waves; 5 In this embodiment,
The difference from the reflected wave blocking screen in the previous embodiment is that a substantially circular gap 8 is provided instead of the substantially U-shaped gap 7 as in the previous embodiment, and the material of the reflected wave blocking screen 6 and the radio wave The installation relationship with the reflecting plate 2, etc. are completely the same as in the previous embodiment.
9は電波吸収体で、従来と同様構成の吸収体より成り、
天井壁面の全域に設けである。9 is a radio wave absorber, which consists of an absorber with the same structure as the conventional one,
It is installed over the entire ceiling and wall surface.
この実施例においては、上方に向った電波が電波吸収体
9に吸収される点において前実施例と異なるが、その他
の電波伝搬状態は前実施例と同様で、供試機器4にはア
ンテナ3からの直接波のみが到達することとなる。This embodiment differs from the previous embodiment in that the upward radio waves are absorbed by the radio wave absorber 9, but the other radio wave propagation conditions are the same as in the previous embodiment, and the device under test 4 has an antenna 3. Only direct waves from the
尚、図には示していないが、必要に応じて天井壁の上部
に屋根を設ける。Although not shown in the figure, a roof may be provided above the ceiling wall if necessary.
発明の効果
本発明電波暗室においては、アンテナ3と供試機器4間
における直接波以外の反射波は主に上方に向い、第1図
乃至第3図に示した実施例においては、上方に向った反
射波は天空に放射されて再び電波暗室に戻ることなく、
第4図乃至第6図に示した実施例においては5上方に向
った反射波は電波吸収体9に吸取されるから、何れの実
施例においても供試機器4には直接波のみが到達するこ
ととなり、電波の伝搬安定度が良好であると共に、反復
反射による定在波が立ち難く、又、アンテナ3のインピ
ーダンスに悪影響を与えることがないから、測定誤差を
生ずるおそれが少ない。Effects of the Invention In the anechoic chamber of the present invention, reflected waves other than direct waves between the antenna 3 and the device under test 4 mainly direct upward, and in the embodiments shown in FIGS. 1 to 3, they direct upward. The reflected waves are radiated into the sky and do not return to the anechoic chamber again.
In the embodiments shown in FIGS. 4 to 6, the reflected waves 5 directed upward are absorbed by the radio wave absorber 9, so that only direct waves reach the device under test 4 in any of the embodiments. Therefore, the propagation stability of radio waves is good, standing waves due to repeated reflections are difficult to stand up, and the impedance of the antenna 3 is not adversely affected, so there is little possibility of measurement errors occurring.
従来の電波吸収体は、大きさ、形状及び吸収率等が電波
の波長に関係して変化するが、本発明において使用する
電波反射板は広帯域性が良好で。Conventional radio wave absorbers vary in size, shape, absorption rate, etc. depending on the wavelength of radio waves, but the radio wave reflector used in the present invention has good broadband properties.
又、構造が単純で、加工上の良否が電気的特性に影響す
るおそれは殆どない。In addition, the structure is simple, and there is almost no possibility that the quality of processing will affect the electrical characteristics.
本発明電波暗室における周壁lと、その内側に設けられ
た電波反射板2との間の空間は、電気的に隔離されるの
で、試験機材の置場、空調設備の設置個所又は試験準備
室等として有効に活用出来るから、従来のように別室を
設ける必要がない。Since the space between the peripheral wall l and the radio wave reflecting plate 2 provided inside the anechoic chamber of the present invention is electrically isolated, it can be used as a storage area for test equipment, an installation location for air conditioning equipment, a test preparation room, etc. Since it can be used effectively, there is no need to set up a separate room like in the past.
本発明電波暗室は、構造が簡単で容積が小さく、構成材
料が廉価であり、敷地面積が少なくて済むので、建設費
及び工期の大幅縮減が可能である。The anechoic chamber of the present invention has a simple structure, a small volume, inexpensive constituent materials, and a small site area, making it possible to significantly reduce construction costs and construction period.
第4図乃至第6図に示した実施例は電気的に完全密閉形
であるから、外来雑音電波の多い1例えば大都市におけ
るビルの中間階に設置することも出来る。Since the embodiments shown in FIGS. 4 to 6 are electrically completely sealed, they can be installed on the middle floor of a building in a large city, for example, where there are many external noise radio waves.
第7図及び第8図は、本発明電波暗室の不要反射波の抑
止効果を説明するための曲線図で、両図において、横軸
は伝送周波数f (MHzlで一重部り30MHz 、
縦軸は伝送損失L (dB)で−目盛り1OdB、実線
は水平偏波の実測値、破線は垂直偏波の実測値、第8図
の点線は自由空間相当計算値で、第7図は、建築物の間
に存在する空き地に、幅5メートル、高さ2.5メート
ルの反射板を2枚lOメートルの間隔を隔てて各垂直に
設け、その間に送信用バイコニカルアンテナ及び受信用
バイコニカルアンテナを5メートルの間隔を隔てて設け
、30MHzから330MHzの周波数範囲における伝
送特性の実測値を示したもので、図から明らかなように
振幅が20dBを超^る定在波及び不規則波が存在すス
第8図は、第7図の場合と同一の場所において、前記と
同一条件で設けたバイコニカルアンテナの回りを、上縁
の高さ1.77メートルの反射板を地面に対して角度4
5°で配置して取囲み、前記と同一周波数帯における伝
送損失の実測値の一例である。FIGS. 7 and 8 are curve diagrams for explaining the suppressing effect of unnecessary reflected waves in the anechoic chamber of the present invention. In both figures, the horizontal axis represents the transmission frequency f (30 MHz in single part in MHz,
The vertical axis is the transmission loss L (dB) with a -scale of 1 OdB, the solid line is the measured value of horizontal polarization, the broken line is the measured value of vertical polarization, and the dotted line in Figure 8 is the calculated value equivalent to free space. Two reflectors, each 5 meters wide and 2.5 meters high, were installed vertically at an interval of 10 meters in an open space between buildings, and a transmitting biconical antenna and a receiving biconical antenna were installed between them. The figure shows actual measurements of transmission characteristics in the frequency range from 30MHz to 330MHz with antennas placed 5 meters apart.As is clear from the figure, there are standing waves and irregular waves with amplitudes exceeding 20dB. Figure 8 shows a reflector with a height of 1.77 meters on the upper edge of the biconical antenna installed at the same location as in Figure 7 and under the same conditions as above, with the upper edge of the reflector plate 1.77 meters above the ground. angle 4
This is an example of an actual measured value of transmission loss in the same frequency band as above, arranged and surrounded by 5 degrees.
図から明らかなように、大なる定在波はほとんど抑圧さ
れ、伝送損失は、直接波のみによる自由空間値に数dB
の差で近付くことが示されている。As is clear from the figure, large standing waves are almost suppressed, and the transmission loss is several dB lower than the free space value due to direct waves only.
It has been shown that the difference is close.
第1図乃至第3図は1本発明の一実施例を示す断面図、
第4図乃至第6図は、他の実施例を示す断面図、第7図
及び第8図は、本発明の電気的効果を説明するための曲
線図で、l二周壁、2:M。
波反射板、3:アンテナ、4:供試機器、5:載置台、
6:反射波遮断用スクリーン、7及び8コ空隙、9:電
波吸収体である。1 to 3 are cross-sectional views showing one embodiment of the present invention,
4 to 6 are cross-sectional views showing other embodiments, and FIGS. 7 and 8 are curve diagrams for explaining the electrical effects of the present invention. Wave reflector, 3: antenna, 4: equipment under test, 5: mounting table,
6: Screen for blocking reflected waves, 7 and 8 voids, 9: Radio wave absorber.
Claims (2)
め上向きにして設けられた電波反射板(2)と、 アンテナ(3)と供試機器(4)の載置台(5)との間
に設けられ、前記アンテナ(3)からの直接波のみを通
過せしめる空隙(7)を有する反射波遮断用スクリーン
(6)とを備えたことを特徴とする電波暗室。1. Between the radio wave reflecting plate (2), which is installed with the reflective surface facing diagonally upward, over the entire inner side of the peripheral wall (1) with its top open, and the mounting table (5) for the antenna (3) and the equipment under test (4). 1. A radio anechoic chamber comprising: a reflected wave blocking screen (6) having a gap (7) that allows only direct waves from the antenna (3) to pass through.
設けられた電波反射板(2)と、 アンテナ(3)と供試機器(4)の載置台(5)との間
に設けられ、前記アンテナ(3)からの直接波のみを通
過せしめる空隙(8)を有する反射波遮断用スクリーン
(6)と、 天井壁面に設けられた電波吸収体(9)とを備えたこと
を特徴とする電波暗室。2. A radio wave reflecting plate (2) is provided throughout the inner side of the peripheral wall (1) with the reflecting surface facing diagonally upward, and a radio wave reflecting plate (2) is provided between the antenna (3) and the mounting table (5) for the equipment under test (4), It is characterized by comprising a reflected wave blocking screen (6) having a gap (8) that allows only direct waves from the antenna (3) to pass through, and a radio wave absorber (9) provided on the ceiling wall surface. Anechoic chamber.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP27822689A JPH03138999A (en) | 1989-10-24 | 1989-10-24 | Radio wave dark room using reflecting plate |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP27822689A JPH03138999A (en) | 1989-10-24 | 1989-10-24 | Radio wave dark room using reflecting plate |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH03138999A true JPH03138999A (en) | 1991-06-13 |
Family
ID=17594376
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP27822689A Pending JPH03138999A (en) | 1989-10-24 | 1989-10-24 | Radio wave dark room using reflecting plate |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH03138999A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN108366518A (en) * | 2018-01-30 | 2018-08-03 | 深圳市共进电子股份有限公司 | A kind of metallic shield case |
-
1989
- 1989-10-24 JP JP27822689A patent/JPH03138999A/en active Pending
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN108366518A (en) * | 2018-01-30 | 2018-08-03 | 深圳市共进电子股份有限公司 | A kind of metallic shield case |
| CN108366518B (en) * | 2018-01-30 | 2020-10-27 | 深圳市共进电子股份有限公司 | Metal shielding box |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| KR970007981B1 (en) | RF anechoic chamber | |
| Green | The general theory of antenna scattering | |
| JP2510880B2 (en) | Multilayer type electromagnetic wave absorber and anechoic chamber consisting of the electromagnetic wave absorber | |
| CN106597129B (en) | Microwave darkroom | |
| US4034378A (en) | Antenna with echo cancelling elements | |
| JPH03138999A (en) | Radio wave dark room using reflecting plate | |
| KR102064103B1 (en) | Electro-Magnetic Anechoic Chamber For Testing Electro-Magnetic Interference | |
| CA1062364A (en) | Antenna with echo cancelling elements | |
| JP3280861B2 (en) | Electromagnetic wave reflection box for electromagnetic wave environment test and electromagnetic wave environment test method using the same | |
| JPH10126091A (en) | Window glass with electromagnetic shielding performance | |
| US2292342A (en) | Reflecting system for antennas | |
| EP1195848B1 (en) | Microwave absorber wall | |
| JP2679643B2 (en) | Antenna device | |
| JPH0785517B2 (en) | Anechoic chamber | |
| JPH10242748A (en) | Multipath protection fence | |
| Arowojolu et al. | Time dispersion measurements in urban microcellular environments | |
| JPH0517506B2 (en) | ||
| JP3628548B2 (en) | Signal relay device | |
| JPH1174680A (en) | Shield box | |
| JP3475362B2 (en) | EMC test site for both fully reflective and non-reflective types | |
| JP2979898B2 (en) | Anechoic chamber | |
| JPH04276700A (en) | Radio wave anechoic chamber | |
| JPH06310892A (en) | Radio wave anechoic enclosure | |
| JP2722313B2 (en) | Anechoic box | |
| JP3116928B2 (en) | EMI measuring method and device |