JPH06160450A - Plane scanning instrument for measuring electric field near antenna - Google Patents

Plane scanning instrument for measuring electric field near antenna

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Publication number
JPH06160450A
JPH06160450A JP9365492A JP9365492A JPH06160450A JP H06160450 A JPH06160450 A JP H06160450A JP 9365492 A JP9365492 A JP 9365492A JP 9365492 A JP9365492 A JP 9365492A JP H06160450 A JPH06160450 A JP H06160450A
Authority
JP
Japan
Prior art keywords
antenna
measured
scanner
plane
wave absorber
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
JP9365492A
Other languages
Japanese (ja)
Other versions
JP3115093B2 (en
Inventor
Hiroyuki Arai
宏之 新井
Tomoichi Hamada
倫一 濱田
Yuji Nakahara
祐治 中原
Hitoshi Kita
仁 喜多
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.)
Icom Inc
Original Assignee
Icom Inc
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 Icom Inc filed Critical Icom Inc
Priority to JP04093654A priority Critical patent/JP3115093B2/en
Publication of JPH06160450A publication Critical patent/JPH06160450A/en
Application granted granted Critical
Publication of JP3115093B2 publication Critical patent/JP3115093B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Abstract

PURPOSE:To provide a plane scanning instrument for measuring electric fields near an antenna, which does not require any unechoic chamber nor large installation space and can be manufactured at a low cost. CONSTITUTION:A table 12 is set upward at the center of a space section surrounded by four vertical supports 10, 10, 10, and 10 and the surface of the table 12 is coated with a first wave absorber 14 and, at the same time, an antenna 16 to be measured is fixed on the surface of the table 12. A scanner 18 which scans in a plane is provided on the tops of the supports 10, 10, 10, and 10 and the surface of the mobile section 20 of the scanner 18 on the table 12 side is coated with a second wave absorber 22. Then probe antennas 24 and 26 are projected from the surface of the absorber 22. In addition, the circumference of the space section surrounded by the supports 10, 10, 10, and 10 is surrounded with third wave absorbers 28, 28, 28, and 28. An arithmetic processing means 38 calculates the remote radiating characteristic of the antenna 16 from the positional information of the probe antennas 24 and 26 and received electric field values.

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、アンテナの近傍で電磁
界を測定して遠方放射特性を算出する平面走査型近傍電
界測定装置に関するものである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a plane-scanning type near electric field measuring apparatus for measuring far-field radiation characteristics by measuring an electromagnetic field near an antenna.

【0002】[0002]

【従来の技術】アンテナの測定は、自由空間中に被測定
アンテナと測定用アンテナを十分な距離を隔てて対向さ
せて行なわれる。しかるに、地面や周囲の障害物による
電磁波の反射が存在し、これらが測定に誤差をもたら
す。しかも、必要となるアンテナ間距離は、アンテナが
大きくなる程、また周波数が高くなる程増加し、測定上
の制約が著しい。
2. Description of the Related Art An antenna is measured in a free space with a measured antenna and a measuring antenna facing each other with a sufficient distance. However, there are reflections of electromagnetic waves from the ground and surrounding obstacles, which cause errors in measurement. Moreover, the required inter-antenna distance increases as the antenna becomes larger and the frequency becomes higher, and the restriction on measurement is significant.

【0003】そこで、上述の遠方電界測定による制約を
避けて高精度の測定を行なう方法として、アンテナの近
傍の電磁界を測定し、それらから遠方放射特性を求める
アンテナの近傍電界測定の技術が発展しつつある。これ
らの状況が詳しく、電子通信学会誌1979年10月号
(Vol.62,No.10)第1145乃至第115
3頁に示されている。
Therefore, as a method of performing highly accurate measurement while avoiding the above-mentioned restriction due to the far electric field measurement, a technique for measuring the near electric field of the antenna for measuring the electromagnetic field in the vicinity of the antenna and obtaining the far radiation characteristic therefrom has been developed. I am doing it. These situations are detailed, and the Institute of Electronics and Communication Engineers, October 1979 issue (Vol. 62, No. 10) No. 1145 to No. 115.
It is shown on page 3.

【0004】ここで、簡単に近傍電界測定の一例につい
て説明すれば、例えば、特開昭60−61664号公報
や特開昭62−54175号公報や特開平3−4877
6号および米国特許第3879733号等に示されるご
とく、被測定アンテナから放射される電磁界を、この被
測定アンテナに近接する平面上を走査し得るスキャナの
可動部に設けられたプローブアンテナで測定し、このプ
ローブアンテナの位置情報とその位置で測定された近傍
電界値より、コンピュータ等の演算処理手段により被測
定アンテナの遠方放射特性が算出される。そして、この
測定は電磁波の反射や外部からの雑音電波の影響を排除
すべく、電波暗室内にて行なわれる。
An example of the near electric field measurement will be briefly described below. For example, JP-A-60-61664, JP-A-62-54175, and JP-A-3-4877.
6 and US Pat. No. 3,879,733, the electromagnetic field radiated from the antenna to be measured is measured by a probe antenna provided on a movable part of the scanner capable of scanning on a plane close to the antenna to be measured. Then, the far radiation characteristic of the measured antenna is calculated by the arithmetic processing means such as a computer from the position information of the probe antenna and the near electric field value measured at the position. Then, this measurement is performed in an anechoic chamber in order to eliminate the influence of reflection of electromagnetic waves and noise radio waves from the outside.

【0005】[0005]

【発明が解決しようとする課題】近傍電界測定にあって
は、電波暗室内にて測定を行なうため、遠方電界測定の
ごとき制約が排除できる利点がある。しかるに、被測定
アンテナとプローブアンテナおよびプローブアンテナを
走査させるためのスキャナ等の装置全体を収納できる大
きさの容積を有する電波暗室が必要である。
In the near electric field measurement, since the measurement is performed in the anechoic chamber, there is an advantage that restrictions such as the far electric field measurement can be eliminated. However, an anechoic chamber having a volume large enough to accommodate the device under test, the probe antenna, and a device for scanning the probe antenna, such as a scanner, is required.

【0006】この電波暗室の建設費用は、通常の実験・
研究用の建物と比べて高額である。そこで、アンテナの
開発や評価および測定を行なう上で大きな障害となって
いた。
[0006] The construction cost of this anechoic chamber is
It is more expensive than a research building. Therefore, it has been a major obstacle to the development, evaluation and measurement of the antenna.

【0007】本発明は、かかる従来技術の事情に鑑みて
なされたもので、設置スペースが小さく、しかも安価に
製造し得る平面走査型近傍電界測定装置を提供すること
を目的とする。
The present invention has been made in view of the circumstances of the prior art, and an object of the present invention is to provide a planar scanning type near electric field measuring apparatus which has a small installation space and can be manufactured at low cost.

【0008】[0008]

【課題を解決するための手段】かかる目的を達成するた
めに、本発明の平面走査型近傍電界測定装置は、被測定
アンテナから放射される電磁界を、この被測定アンテナ
に近接する平面上を走査し得るスキャナの可動部に設け
られたプローブアンテナで測定し、このプローブアンテ
ナの位置情報とその位置で測定された近傍電界値より演
算処理手段により前記被測定アンテナの遠方放射特性を
算出する平面走査型近傍電界測定装置において、前記被
測定アンテナを固定するテーブルの表面を覆うように第
1の電波吸収体を設け、前記スキャナの可動部の前記テ
ーブルと対向する面を覆うように第2の電波吸収体を設
け、前記テーブルと前記スキャナが設けられた側を除い
て、前記テーブルと前記スキャナの可動部の周囲を第3
の電波吸収体で囲んで構成されている。
In order to achieve such an object, a plane scanning type near electric field measuring apparatus of the present invention is designed so that an electromagnetic field radiated from an antenna to be measured is placed on a plane close to the antenna to be measured. A plane which is measured by a probe antenna provided on a movable part of a scanner capable of scanning, and a far radiation characteristic of the antenna under measurement is calculated by arithmetic processing means from position information of the probe antenna and a near electric field value measured at the position. In the scanning type near electric field measuring apparatus, a first electromagnetic wave absorber is provided so as to cover a surface of a table on which the antenna to be measured is fixed, and a second electromagnetic wave absorber is provided so as to cover a surface of the movable portion of the scanner facing the table. A radio wave absorber is provided, and a third part is provided around the movable part of the table and the scanner except for the side where the table and the scanner are provided.
It is constructed by enclosing it with a radio wave absorber.

【0009】そして、前記テーブルの表面を上方に向け
て配設し、前記スキャナを垂直に立設された4本の支柱
によって前記テーブルの上方水平面にて走査できるよう
に支持し、前記支柱で囲まれる空間部の周面に前記第3
の電波吸収体を配置して構成しても良い。
Then, the surface of the table is arranged so as to face upward, and the scanner is supported by four vertically standing columns so that the scanner can scan on the horizontal plane above the table, and is surrounded by the columns. The third surface on the peripheral surface of the space
You may arrange | position the radio wave absorber of.

【0010】[0010]

【作 用】被測定アンテナが固定されるテーブルの表面
と、プローブアンテナが突設されるスキャナの可動部の
面を覆うようにそれぞれ第1と第2の電波吸収体を設け
るとともに、テーブルとスキャナが設けられた側を除い
て、周囲を第3の電波吸収体で囲んでいるので、被測定
アンテナおよびプローブアンテナは、電磁波の反射や外
部からの雑音電波の影響を受けることがない。
[Operation] The first and second electromagnetic wave absorbers are provided so as to cover the surface of the table to which the antenna to be measured is fixed and the surface of the movable portion of the scanner on which the probe antenna is projected, respectively, and the table and the scanner are provided. Since the surroundings are surrounded by the third electromagnetic wave absorber except for the side where is provided, the antenna to be measured and the probe antenna are not affected by reflection of electromagnetic waves and noise electromagnetic waves from the outside.

【0011】そして、テーブルの表面を上方に向け、ス
キャナをテーブルの上方水平面にて走査させるならば、
スキャナの可動部の移動に重力の影響を受けることがな
く、スキャナの可動部を高い精度で移動制御でき、それ
だけ測定精度を向上させ得る。しかも、スキャナを支持
する支柱で囲まれる空間部の周面に第3の電波吸収体を
配置するので、第3の電波吸収体の組み付け構造も簡単
である。
If the surface of the table is directed upward and the scanner is scanned in the horizontal plane above the table,
The movement of the movable portion of the scanner is not affected by gravity and the movement of the movable portion of the scanner can be controlled with high accuracy, and the measurement accuracy can be improved accordingly. Moreover, since the third electromagnetic wave absorber is arranged on the peripheral surface of the space surrounded by the columns supporting the scanner, the assembly structure of the third electromagnetic wave absorber is also simple.

【0012】[0012]

【実施例】以下、本発明の一実施例につき図1および図
2を参照して説明する。図1は、本発明の平面走査型近
傍電界測定装置の一実施例の構造を示す縦断面図であ
り、図2は、装置全体の一部切り欠き外観斜視図であ
る。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS An embodiment of the present invention will be described below with reference to FIGS. FIG. 1 is a vertical cross-sectional view showing the structure of one embodiment of the planar scanning type near-field measuring apparatus of the present invention, and FIG. 2 is a partially cutaway external perspective view of the entire apparatus.

【0013】図1および図2において、垂直(Z方向)
に立設された4本の支柱10,10,10,10で囲ま
れる空間部の中央に、表面を上方に向けてテーブル12
が配置される。このテーブル12の表面は第1の電波吸
収体14で覆われるとともに適宜に被測定アンテナ16
が固定できるものとする。しかも、テーブル12は、シ
リンダー等により昇降可動に構成される。また、支柱1
0,10,10,10の上端に、水平面上を走査し得る
(X−Y方向)スキャナ18が配置され、その可動部2
0のテーブル12に対向する面を覆うように第2の電波
吸収体22が配置される。さらに、この可動部20に
は、第2の電波吸収体22から2本のプローブアンテナ
24,26が突設される。この2本のプローブアンテナ
24,26は、直交するように配設される。さらに、支
柱10,10,10,10で囲まれる空間部の周面に
は、第3の電波吸収体28,28,28,28が支柱1
0,10,10,10により支持固定される。そして、
プローブアンテナ24,26に接続される同軸ケーブル
がケーブルガイドレール30により支持される。そして
また、スキャナ18のX−Y方向位置とテーブル12の
Z方向位置および2本のプローブアンテナ24,26を
切り換える同軸リレー32の切り換えが制御コンピュー
タ34により制御され、被測定アンテナ16から放射さ
せる電磁界の制御および所定位置に制御されたプローブ
アンテナ24,26で受信された近傍電界値が測定装置
36で測定処理される。そしてさらに、制御コンピュー
タ34にスキャナ18の位置情報と測定装置36で測定
されたデータが蓄積され、制御コンピュータ34でスキ
ャナ18の位置情報とプローブアンテナ24,26によ
る近傍電界値から遠方放射特性が算出される。この制御
コンピュータ34と測定装置36とで演算処理手段38
が構成される。
In FIGS. 1 and 2, vertical (Z direction)
The table 12 with its surface facing upward is placed in the center of the space surrounded by the four columns 10, 10, 10, 10.
Are placed. The surface of the table 12 is covered with the first electromagnetic wave absorber 14, and the antenna 16 to be measured is appropriately placed.
Can be fixed. Moreover, the table 12 is configured to be movable up and down by a cylinder or the like. In addition, prop 1
A scanner 18 capable of scanning on a horizontal plane (X-Y direction) is arranged at the upper ends of 0, 10, 10, 10 and its movable part 2
The second electromagnetic wave absorber 22 is arranged so as to cover the surface of the table 0 facing the table 12. Further, the movable portion 20 is provided with two probe antennas 24 and 26 protruding from the second radio wave absorber 22. The two probe antennas 24 and 26 are arranged so as to be orthogonal to each other. Further, the third electromagnetic wave absorbers 28, 28, 28, 28 are provided on the circumferential surface of the space surrounded by the columns 10, 10, 10, 10.
It is supported and fixed by 0, 10, 10, 10. And
A coaxial cable connected to the probe antennas 24 and 26 is supported by the cable guide rail 30. Further, the control computer 34 controls the switching of the position of the scanner 18 in the XY direction, the position of the table 12 in the Z direction, and the switching of the coaxial relay 32 for switching the two probe antennas 24 and 26. The electric field values received by the probe antennas 24 and 26 controlled at the field and at the predetermined positions are measured by the measuring device 36. Further, the position information of the scanner 18 and the data measured by the measuring device 36 are further accumulated in the control computer 34, and the far radiation characteristic is calculated by the control computer 34 from the position information of the scanner 18 and the near electric field values by the probe antennas 24 and 26. To be done. The control computer 34 and the measuring device 36 combine the arithmetic processing means 38.
Is configured.

【0014】かかる構成において、被測定アンテナ16
から放射された電磁界が側方周囲の第3の電波吸収体2
8,28,28,28に至ると、適宜に吸収されて反射
されることがない。また、後側への放射は、テーブル1
2上の第1の電波吸収体14で吸収されて反射されるこ
とがない。そして、スキャナ18の可動部20に至る放
射は、プローブアンテナ24,26で受信されたもの以
外は、第2の電波吸収体22で吸収されて反射されるこ
とがない。しかも、外部からの雑音電波等も第1と第2
および第3の電波吸収体14,22,28,28,2
8,28で遮断される。この結果、従来の電波暗室にお
ける近傍電界測定と同様に、反射電波や外部からの雑音
電波の影響を受けずに近傍電界測定ができる。
In such a configuration, the antenna under test 16
Electromagnetic field radiated from the third electromagnetic wave absorber 2 around the side
When it reaches 8, 28, 28, 28, it is not properly absorbed and reflected. In addition, the radiation to the rear side is the table 1
It is not absorbed and reflected by the first radio wave absorber 14 above. The radiation reaching the movable portion 20 of the scanner 18 is not absorbed and reflected by the second radio wave absorber 22, except for the radiation received by the probe antennas 24 and 26. In addition, noise radio waves from the outside are also the first and the second.
And the third electromagnetic wave absorbers 14, 22, 28, 28, 2
It is cut off at 8, 28. As a result, similar to the conventional electric field measurement in the anechoic chamber, the electric field measurement can be performed without being affected by the reflected electric wave and the noise electric wave from the outside.

【0015】そして、本発明の構成では、装置を部分的
に電波吸収体で囲むにすぎず、従来の電波暗室に比べて
その設置スペースが小さく、しかも安価に製造できる。
In the structure of the present invention, the device is only partially surrounded by the electromagnetic wave absorber, and the installation space is smaller than that of the conventional anechoic chamber, and the manufacturing cost is low.

【0016】なお、上記実施例では、被測定アンテナ1
6から電磁界を放射させ、プローブアンテナ24,26
で受信して近傍電界値を測定するものを説明したが、こ
れとは逆に、プローブアンテナ24,26の一方から電
磁界を放射させ、これを被測定アンテナ16で受信し、
その近傍電界値より遠方放射特性を算出するものであっ
ても良い。さらに、実施例では、スキャナは水平面上
(X−Y方向)を走査し得るように配設したが、これに
限られず、図2におけるZ−X方向またはZ−Y方向に
走査するように配設しても良い。
In the above embodiment, the antenna under test 1
6 to radiate an electromagnetic field, and probe antennas 24, 26
Although the one in which the electric field value in the vicinity is measured by receiving in, the electromagnetic field is radiated from one of the probe antennas 24 and 26, and the antenna 16 to be measured receives the electromagnetic field.
The far radiation characteristic may be calculated from the value of the near electric field. Further, in the embodiment, the scanner is arranged so that it can scan on the horizontal plane (X-Y direction), but the present invention is not limited to this, and the scanner is arranged so as to scan in the Z-X direction or the Z-Y direction. You can set it up.

【0017】[0017]

【発明の効果】以上説明したところから明らかなよう
に、本発明の平面走査型近傍電界測定装置は以下のごと
き格別な効果を奏する。
As is apparent from the above description, the plane scanning type near field measuring apparatus of the present invention has the following special effects.

【0018】まず、請求項1および2記載の平面走査型
近傍電界測定装置は、被測定アンテナとプローブアンテ
ナの周囲が電波吸収体で囲まれ、プローブアンテナまた
は被測定アンテナから放射されて電波吸収体に至る電磁
波は吸収されて反射することがない。このため、従来の
電波暗室と同様の測定精度が得られる簡易電波暗室が構
成される。しかも、構造が簡単であり、安価に製造で
き、しかも設置スペースが小さくて良い。
First, in the plane scanning type near-field measuring apparatus according to the first and second aspects, the antenna to be measured and the probe antenna are surrounded by a radio wave absorber, and the radio wave absorber is radiated from the probe antenna or the antenna to be measured. The electromagnetic waves that reach the are not absorbed and reflected. Therefore, a simple anechoic chamber that provides the same measurement accuracy as the conventional anechoic chamber is configured. Moreover, the structure is simple, the manufacturing cost is low, and the installation space is small.

【0019】そして、請求項3記載の平面走査型近傍電
界測定装置にあっては、スキャナの可動部の走査が重力
に影響されることがないので、プローブアンテナの位置
を精度良く制御することができ、それだけ遠方放射特性
を精度良く算出することができる。また、第3の電波吸
収体の支持を支柱を用いて簡単な構造で行なうことがで
きる。
Further, in the plane scanning type near field measuring apparatus according to the third aspect, since the scanning of the movable portion of the scanner is not influenced by the gravity, the position of the probe antenna can be controlled accurately. Therefore, the far radiation characteristic can be calculated with high accuracy. In addition, the third radio wave absorber can be supported by using a pillar with a simple structure.

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

【図1】本発明の平面走査型近傍電界測定装置の一実施
例の構造を示す縦断面図である。
FIG. 1 is a vertical cross-sectional view showing the structure of an embodiment of a planar scanning type near-field measuring device of the present invention.

【図2】本発明の平面走査型近傍電界測定装置の装置全
体の一部切り欠き外観斜視図である。
FIG. 2 is a partially cutaway external perspective view of the entire apparatus of the planar scanning type near electric field measuring apparatus of the present invention.

【符号の説明】 10 支柱 12 テーブル 14 第1の電波吸収体 16 被測定アンテナ 18 スキャナ 20 可動部 22 第2の電波吸収体 24,26 プローブアンテナ 28 第3の電波吸収体 38 演算処理手段[Explanation of Codes] 10 Supports 12 Table 14 First Electromagnetic Wave Absorber 16 Antenna to be Measured 18 Scanner 20 Movable Part 22 Second Electromagnetic Wave Absorber 24, 26 Probe Antenna 28 Third Electromagnetic Wave Absorber 38 Calculation Processing Means

───────────────────────────────────────────────────── フロントページの続き (72)発明者 濱田 倫一 大阪府大阪市平野区加美鞍作1丁目6番19 号 アイコム株式会社内 (72)発明者 中原 祐治 大阪府大阪市平野区加美鞍作1丁目6番19 号 アイコム株式会社内 (72)発明者 喜多 仁 大阪府大阪市平野区加美鞍作1丁目6番19 号 アイコム株式会社内 ─────────────────────────────────────────────────── ─── Continued Front Page (72) Inventor Rinichi Hamada 1-6-19 Kami Kuramasaku, Hirano-ku, Osaka City, Osaka Prefecture Icom Co., Ltd. 6-19 No. Icom Co., Ltd. (72) Inventor Hitoshi Kita 1-6-19 Kami Kuramasaku Hirano-ku, Osaka City Osaka Prefecture Icom Co., Ltd.

Claims (3)

【特許請求の範囲】[Claims] 【請求項1】 被測定アンテナから放射される電磁界
を、この被測定アンテナに近接する平面上を走査し得る
スキャナの可動部に設けられたプローブアンテナで測定
し、このプローブアンテナの位置情報とその位置で測定
された近傍電界値より演算処理手段により前記被測定ア
ンテナの遠方放射特性を算出する平面走査型近傍電界測
定装置において、前記被測定アンテナを固定するテーブ
ルの表面を覆うように第1の電波吸収体を設け、前記ス
キャナの可動部の前記テーブルと対向する面を覆うよう
に第2の電波吸収体を設け、前記テーブルと前記スキャ
ナが設けられた側を除いて、前記テーブルと前記スキャ
ナの可動部の周囲を第3の電波吸収体で囲んで構成した
ことを特徴とする平面走査型近傍電界測定装置。
1. An electromagnetic field radiated from an antenna to be measured is measured by a probe antenna provided in a movable part of a scanner capable of scanning on a plane close to the antenna to be measured, and position information of the probe antenna is obtained. In a plane scanning type near field measuring device for calculating a far radiation characteristic of the antenna to be measured by an arithmetic processing means from a near electric field value measured at the position, a first surface covering a surface of a table fixing the antenna to be measured. A radio wave absorber is provided, and a second radio wave absorber is provided so as to cover a surface of the movable portion of the scanner facing the table, and the table and the scanner are provided except for the side where the table and the scanner are provided. A plane-scanning type near-field electric field measuring device characterized in that the movable part of the scanner is surrounded by a third radio wave absorber.
【請求項2】 請求項1記載の平面走査型近傍電界測定
装置において、前記プローブアンテナより電磁界を放射
し、この電磁界を前記被測定アンテナで受信し、前記プ
ローブアンテナの位置情報と前記被測定アンテナで受信
された近傍電界値より前記演算処理手段で遠方放射特性
を算出することを特徴とした平面走査型近傍電界測定装
置。
2. The plane scanning type near electric field measuring device according to claim 1, wherein an electromagnetic field is radiated from the probe antenna, and the electromagnetic field is received by the antenna to be measured, and the position information of the probe antenna and the object to be measured are received. A plane-scanning type near-field measuring apparatus, characterized in that the calculation processing means calculates the far-field radiation characteristic from the near-field value received by the measuring antenna.
【請求項3】 請求項1または2記載の平面走査型近傍
電界測定装置において、前記テーブルの表面を上方に向
けて配設し、前記スキャナを垂直に立設された4本の支
柱によって前記テーブルの上方水平面にて走査できるよ
うに支持し、前記支柱で囲まれる空間部の周面に前記第
3の電波吸収体を配置して構成したことを特徴とする平
面走査型近傍電界測定装置。
3. The flat-scanning type near-field measuring apparatus according to claim 1, wherein the table is arranged with the surface of the table facing upward, and the scanner is constituted by four columns vertically erected. 2. A plane scanning type near electric field measuring device, characterized in that the third radio wave absorber is arranged so as to be supported so as to be able to scan on the upper horizontal plane, and the third radio wave absorber is arranged on the peripheral surface of the space surrounded by the columns.
JP04093654A 1992-03-19 1992-03-19 Planar scanning near-field measuring device Expired - Lifetime JP3115093B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP04093654A JP3115093B2 (en) 1992-03-19 1992-03-19 Planar scanning near-field measuring device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP04093654A JP3115093B2 (en) 1992-03-19 1992-03-19 Planar scanning near-field measuring device

Publications (2)

Publication Number Publication Date
JPH06160450A true JPH06160450A (en) 1994-06-07
JP3115093B2 JP3115093B2 (en) 2000-12-04

Family

ID=14088374

Family Applications (1)

Application Number Title Priority Date Filing Date
JP04093654A Expired - Lifetime JP3115093B2 (en) 1992-03-19 1992-03-19 Planar scanning near-field measuring device

Country Status (1)

Country Link
JP (1) JP3115093B2 (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2006007004A3 (en) * 2004-06-18 2006-06-01 Centurion Wireless Tech Inc Method and apparatus to control an antenna efficiency test device
US7109932B2 (en) * 2004-06-18 2006-09-19 Centurion Wireless Technologies, Inc. Antenna efficiency test device
WO2020037838A1 (en) * 2018-08-23 2020-02-27 清华大学 Terahertz leaky wave antenna measurement system

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2006007004A3 (en) * 2004-06-18 2006-06-01 Centurion Wireless Tech Inc Method and apparatus to control an antenna efficiency test device
US7109931B2 (en) * 2004-06-18 2006-09-19 Centurion Wireless Technologies, Inc. Method and apparatus to control an antenna efficiency test device
US7109932B2 (en) * 2004-06-18 2006-09-19 Centurion Wireless Technologies, Inc. Antenna efficiency test device
WO2006007003A3 (en) * 2004-06-18 2007-01-11 Centurion Wireless Tech Inc Antenna efficiency test device
WO2020037838A1 (en) * 2018-08-23 2020-02-27 清华大学 Terahertz leaky wave antenna measurement system
US11437729B2 (en) 2018-08-23 2022-09-06 Tsinghua University Terahertz leaky-wave antenna measuring system

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