JPS5912623Y2 - Power supply device with reference polarization generation mechanism - Google Patents

Power supply device with reference polarization generation mechanism

Info

Publication number
JPS5912623Y2
JPS5912623Y2 JP8434679U JP8434679U JPS5912623Y2 JP S5912623 Y2 JPS5912623 Y2 JP S5912623Y2 JP 8434679 U JP8434679 U JP 8434679U JP 8434679 U JP8434679 U JP 8434679U JP S5912623 Y2 JPS5912623 Y2 JP S5912623Y2
Authority
JP
Japan
Prior art keywords
polarization
signal
reference polarization
terminal
power supply
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
Application number
JP8434679U
Other languages
Japanese (ja)
Other versions
JPS563459U (en
Inventor
敏雄 佐藤
文男 巻田
信一 別段
義彦 吉川
Original Assignee
ケイディディ株式会社
三菱電機株式会社
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 ケイディディ株式会社, 三菱電機株式会社 filed Critical ケイディディ株式会社
Priority to JP8434679U priority Critical patent/JPS5912623Y2/en
Publication of JPS563459U publication Critical patent/JPS563459U/ja
Application granted granted Critical
Publication of JPS5912623Y2 publication Critical patent/JPS5912623Y2/en
Expired legal-status Critical Current

Links

Description

【考案の詳細な説明】 この考案はアンテナ装置の偏波特性を高精度に測定する
場合に必要となる基準となる偏波を発生する機構を備え
た給電装置に関するものである。
[Detailed Description of the Invention] This invention relates to a power feeding device equipped with a mechanism for generating polarized waves as a reference necessary for measuring polarization characteristics of an antenna device with high accuracy.

アンテナ装置の偏波特性、(チルト角(偏波の長軸の傾
き角)と楕円偏波率)を測定する場合、基準となる偏波
を何かの方法で被測定アンテナ装置に供給する必要があ
る。
When measuring the polarization characteristics of an antenna device (tilt angle (inclination angle of the long axis of polarization) and elliptical polarization coefficient), the reference polarization must be supplied to the antenna device under test by some method. There is a need.

従来この基準となる偏波を供給する手段として第1図に
示すように、被測定アンテナ装置とは離れた場所に設置
された基準偏波発生装置から既知の基準偏波を送信し、
これを被測定アンテナ装置で受信する方法が広く用いら
れてきた。
Conventionally, as a means for supplying this reference polarized wave, as shown in FIG.
A method of receiving this signal with an antenna device under test has been widely used.

かかる手段を用いたアンテナ装置の偏波特性の測定系に
ついて説明する。
A measurement system for polarization characteristics of an antenna device using such means will be explained.

第1図において1はいわゆるコリメーション装置であり
、無線周波信号発振器2、偏波変換器3およびアテナ4
などで構或されている。
In FIG. 1, 1 is a so-called collimation device, including a radio frequency signal oscillator 2, a polarization converter 3, and an athena 4.
It is structured as follows.

5は被測定アンテナ装置であり、アンテナ6、給電装置
7、送信機又は受信機等の無線機を接続する為の端子8
,9を有する。
5 is an antenna device to be measured, which includes an antenna 6, a power supply device 7, and a terminal 8 for connecting a radio device such as a transmitter or a receiver.
, 9.

10は偏波特性測定装置であり、端子8と9に出力する
無線周波信号(以下単に信号と呼ぶ)の振幅比と位相差
を検出し、偏波特性を測定するものである。
Reference numeral 10 denotes a polarization characteristic measuring device, which detects the amplitude ratio and phase difference of radio frequency signals (hereinafter simply referred to as signals) outputted to terminals 8 and 9, and measures the polarization characteristics.

次にこの測定系の動作について説明する。Next, the operation of this measurement system will be explained.

コリメーション装置1から送られてくる信号を被測定ア
ンテナ装置5で受信すると、端子8と9にはコリメーシ
ョン装置1と被測定アンテナ装置5の偏波特性の合或特
性によって定まる振幅比と位相差を有する信号が現われ
る。
When the antenna device under test 5 receives a signal sent from the collimation device 1, terminals 8 and 9 receive an amplitude ratio and a phase difference determined by the combination or characteristics of the polarization characteristics of the collimation device 1 and the antenna device under test 5. A signal with .

従って、この振幅比と位相差を偏波特性測定装置10で
検出することによりコリメーション装置1と被測定アン
テナ装置5の合或偏波特性が測定できる。
Therefore, by detecting this amplitude ratio and phase difference with the polarization characteristic measuring device 10, the combined polarization characteristics of the collimation device 1 and the antenna device under test 5 can be measured.

この測定法は端子8と9に得られる二つの信号の間の位
相差φ及び振幅比mとJ,θとが次式で示されることを
利用している。
This measurement method utilizes the fact that the phase difference φ and amplitude ratio m, J, and θ between the two signals obtained at terminals 8 and 9 are expressed by the following equations.

?こで、jは被測定アンテナ装置5の楕円偏波率に対応
した誤差θは、信号の偏波面の水平方向を基準とした傾
き角度である。
? Here, j corresponds to the elliptical polarization factor of the antenna device under test 5, and error θ is the inclination angle of the polarization plane of the signal with respect to the horizontal direction.

測定は次のように行う。Measurement is performed as follows.

被測定アンテナ装置5が円偏波アンテナ装置の場合はま
ず水平面から既知の角度θだけ傾いた直線偏波信号をコ
リメーション装置1から送出し、これを被測定アンテナ
装置5で受信し、端子8,9に得られる二つの信号の振
幅比m′と位相差φ′を求めて、式(1) . (2)
のm,φと比較する。
If the antenna device 5 to be measured is a circularly polarized antenna device, first, a linearly polarized signal tilted by a known angle θ from the horizontal plane is sent out from the collimation device 1, received by the antenna device 5 to be measured, and then sent to the terminals 8, Determine the amplitude ratio m' and phase difference φ' of the two signals obtained in step 9, and use equation (1). (2)
Compare with m and φ.

これがずれている場合はm′とφ′を調整して測定系を
標準状態に収正する。
If this is deviated, m' and φ' are adjusted to correct the measurement system to the standard state.

一″′ ′以上の校正後コ
リメーション装置1からの信号を完全な円偏波信号に変
えて送出し、この信号によって得られる端子8,9の信
号の振幅比をM(dB)位相差をφ度を測定する。
After a calibration of more than 1''', the signal from the collimation device 1 is changed into a completely circularly polarized signal and sent out. measure degree.

被測定アンテナの楕円偏波率ep,チルト角τは次式で
求められる。
The elliptical polarization coefficient ep and tilt angle τ of the antenna to be measured are determined by the following equations.

ep= 17.87 X 1G (dB)
−−−(3)l τ =−(Φ+90) (度) ・・・(4)2 従来の偏波特性測定法では以上のような較正法を用いる
ため、コリメーション設備としてその偏波特性を変化で
きる機能が変化できる機能が必要であった。
ep= 17.87 x 1G (dB)
---(3) l τ =-(Φ+90) (degrees) ... (4) 2 Since the above calibration method is used in the conventional polarization characteristic measurement method, the polarization characteristics of the collimation equipment are We needed a function that could change the function.

また被測定アンテナの開口径が大きなものである場合に
は、コリメーションと被測定アンテナとの距離を十分大
きくする必要がある。
Furthermore, if the antenna to be measured has a large aperture diameter, it is necessary to make the distance between the collimation and the antenna to be measured sufficiently large.

こ?ため近年の衛星通信用地球局アンテナの偏波特性測
定のためには、コリメーションの立地場所の確保が困難
な場合が多く、衛星をコリメーション装置1の代りに用
いるケースが多くなる。
child? Therefore, in order to measure the polarization characteristics of earth station antennas for satellite communications in recent years, it is often difficult to secure a location for collimation, and a satellite is often used instead of the collimation device 1.

このとき衛星では上記のような偏波特性を変化すること
は不可能であり、偏波特性の較正法が課題であった。
At this time, it was impossible to change the polarization characteristics of the satellite as described above, and the problem was how to calibrate the polarization characteristics.

この考案は上記のような従来のものの欠点を除去するた
めになされたもので、被測定アンテナの給電装置に基準
偏波検出端子を設置し、これより基準偏波信号を給電す
るようにし、コリメータ装置の偏波特性を変化すること
なく偏波特性を高精度に測定する場合に必要とされる所
定の基準偏波を供給し得る手段を提供することを目的と
している。
This idea was made in order to eliminate the drawbacks of the conventional ones as described above. A reference polarization detection terminal is installed on the feeding device of the antenna under test, and the reference polarization signal is fed from this, and the collimator It is an object of the present invention to provide a means for supplying a predetermined reference polarized wave required for measuring polarization characteristics with high accuracy without changing the polarization characteristics of the device.

以下、この考案の一実施例を図について説明する。An embodiment of this invention will be described below with reference to the drawings.

第2図において、11は偏波変換器、12は基準偏波を
検出し得る端子15を有する基準偏波結合器、13は偏
分波器である。
In FIG. 2, 11 is a polarization converter, 12 is a reference polarization coupler having a terminal 15 capable of detecting the reference polarization, and 13 is a polarization splitter.

上記基準偏波結合器12は偏波変換器11と偏波分器1
3間の電波の伝送軸を回転で゛きるようにしたもので゛
、かつその回転角度を正確に読取れる機構を有する。
The reference polarization coupler 12 includes a polarization converter 11 and a polarization splitter 1.
The radio wave transmission axis between the two can be rotated, and it has a mechanism that allows the angle of rotation to be read accurately.

14は発振器である。14 is an oscillator.

端子15に印加される信号は、基準偏波結合器12内に
直線偏波で励振されるようになっている。
The signal applied to the terminal 15 is adapted to be excited into the reference polarization coupler 12 with linear polarization.

この直線偏波で励振これを信号は偏分波器13に第4図
のようにφ傾いたEなる電界で入力し、互に直交する関
係にある偏分波器13の端子8及9には、端子8:EX
、端子9:Ey、なる電界で分渡される。
This linearly polarized wave is excited and the signal is input to the polarization splitter 13 with an electric field E tilted by φ as shown in Fig. is terminal 8: EX
, terminal 9: Ey.

ここで、ExとEyとの振幅比はEy / Ex
= tan l (s)となる。
Here, the amplitude ratio of Ex and Ey is Ey/Ex
= tan l (s).

なお、ExとEyは同相であり、φは基準偏波結合器1
2における電波の伝送軸の回転角である。
Note that Ex and Ey are in phase, and φ is the reference polarization coupler 1.
This is the rotation angle of the radio wave transmission axis in 2.

従って基準偏波結合器12における回転角を読みとるこ
とにより、同相で振幅比が(1)式で定まる既知の基準
信号を端子8,9に得ることができる。
Therefore, by reading the rotation angle in the reference polarization coupler 12, a known reference signal that is in phase and whose amplitude ratio is determined by equation (1) can be obtained at the terminals 8 and 9.

すなわち、従来コリメーション装置からの送信波を用い
て実施していた端子8と9の位相と振幅の関係の較正を
、被測定アンテナ装置自身で実施できることになる。
In other words, the calibration of the relationship between the phase and amplitude of the terminals 8 and 9, which was conventionally carried out using transmitted waves from a collimation device, can be carried out by the antenna device under test itself.

この場合、特定の楕円偏波率の較正値のみが必要な場合
は上記回転機構は不要である。
In this case, if only a calibration value of a specific elliptical polarization factor is required, the above rotation mechanism is not necessary.

以上の校正を行ったのちは従来と同様、コリメーション
装置からの信号を用いて偏波特性を測定を行う。
After performing the above calibration, the polarization characteristics are measured using the signal from the collimation device as in the conventional case.

第3図は、第2図での較正法をさらに正確に実施できる
ようにしたこの考案の別の実施例である。
FIG. 3 is another embodiment of the invention which allows the calibration method of FIG. 2 to be carried out more accurately.

図において、16は可変減衰器、17は可変位相器、1
8は無線周波増幅器、19は基準偏波結合器であり第2
図の基準偏波結合器12と同様の機構と機能のものでも
よいが、本手段では第4図のφが45゜の固定の偏波で
励振できる構造が最も正確に較正できるので、以下の説
明では一二45゜になるように基準偏波結合器19を設
置すると、端子15への入力波は端子8と9には同相で
がっ同振幅の信号として分波される。
In the figure, 16 is a variable attenuator, 17 is a variable phase shifter, 1
8 is a radio frequency amplifier; 19 is a reference polarization coupler;
Although it may be of the same mechanism and function as the reference polarization coupler 12 shown in the figure, in this method, the structure that can be excited with a fixed polarized wave with φ of 45° as shown in Fig. 4 can be most accurately calibrated, so the following method is used. In the description, when the reference polarization coupler 19 is installed so that the polarization angle is 1245 degrees, the input wave to the terminal 15 is split into terminals 8 and 9 as signals having the same phase and the same amplitude.

端子8の信号は増幅器18で増幅後、偏波特性測定装置
10に印加する。
The signal at the terminal 8 is amplified by the amplifier 18 and then applied to the polarization characteristic measuring device 10 .

端子9の信号は無線周波数増幅器18で増幅後、可変減
衰器16と可変位相器17を経由して偏波特性測定装置
1oに印加する。
The signal at the terminal 9 is amplified by a radio frequency amplifier 18 and then applied to the polarization characteristic measuring device 1o via a variable attenuator 16 and a variable phase shifter 17.

可変減衰器16の減衰量をα(dB)、可変位相器17
の位相量をθ(度)とすると較正用の基準偏波は チルト角〔度〕=466+ # (nなる関係
式で算出できるので、αとθより求められた偏波特性の
値が、基準偏波結合器19から印加される基準偏波信号
の偏波特性の値と一致するようαとθを補正すること、
によって校正を行う。
The attenuation amount of the variable attenuator 16 is α (dB), and the variable phase shifter 17
If the phase amount of is θ (degrees), then the reference polarization for calibration is tilt angle [degrees] = 466 + # (Since it can be calculated using the relational expression n, the value of the polarization characteristic determined from α and θ is correcting α and θ so that they match the values of the polarization characteristics of the reference polarization signal applied from the reference polarization coupler 19;
Calibration is performed by

基準偏波検出端子15を有する基準偏波結合器12およ
び19の一構戊例を第5図に示す。
An example of the structure of the reference polarization couplers 12 and 19 having the reference polarization detection terminal 15 is shown in FIG.

同図は?向性結合器形のモード結合器であリ、20は円
形導波管、21は結合孔、22は方形導波管である。
What about the same figure? The mode coupler is a directional coupler type, and 20 is a circular waveguide, 21 is a coupling hole, and 22 is a rectangular waveguide.

端子15から入力された信号波は基準偏波結合器19を
経て偏分波器13の側に円形導波管の基本モードである
TH1モードの直接偏波の励振を行う。
The signal wave inputted from the terminal 15 passes through the reference polarization coupler 19 and excites direct polarization in the TH1 mode, which is the fundamental mode of the circular waveguide, to the polarization splitter 13 side.

なお、第3図において、減衰量αと位相量θを変化させ
る手段は可変減衰器16と可変移相器17にこだわらず
、偏波特性測定装置10内に設けられた減衰器及び移相
器によっても変化できる。
In FIG. 3, the means for changing the attenuation amount α and the phase amount θ is not limited to the variable attenuator 16 and the variable phase shifter 17, but may be an attenuator and a phase shifter provided in the polarization characteristic measuring device 10. It can also change depending on the device.

なお、上記実施例では端子15に較正用信号を入力する
場合について説明したが、偏波特性測定装置10の所に
発振器を、発振器14の所に偏波特性測定装置を配置す
る構或でも偏波基準信号を得ることができる。
In the above embodiment, the case where the calibration signal is input to the terminal 15 has been described, but it is also possible to arrange the oscillator at the polarization characteristic measuring device 10 and the polarization characteristic measuring device at the oscillator 14. However, it is possible to obtain a polarization reference signal.

この場合、発振器出力を2分割後、端子8に入力する信
号波にのみ変調を与え、偏波特性測定装置にはこれを復
調する機能を備えることが必要である。
In this case, it is necessary to modulate only the signal wave input to the terminal 8 after dividing the oscillator output into two, and to provide the polarization characteristic measuring device with a function to demodulate this.

また、基準偏波結合器12あるいは19として、円偏波
で励振する構戒でも算出式を変更するのみで実現できる
が、基準偏波結合器の構造が複雑になり、かつ理想的な
円偏波の作戒が困難なことに起因して較正値として誤差
が本方式に比べて大きくなるなどの欠点があり実用的で
はない。
In addition, as the reference polarization coupler 12 or 19, it is possible to realize a configuration in which circularly polarized waves are excited by simply changing the calculation formula, but the structure of the reference polarization coupler becomes complicated and the ideal circular polarization is not achieved. This method has drawbacks such as the fact that the error in the calibration value is larger than that of the present method due to the difficulty in controlling the waves, making it impractical.

以上のように、この考案によればアンテナ給電装置に基
準偏波発生機能を持つように構威したので、アンテナ装
置の偏波特性を測定する場合、コリメー夕側の偏波面を
変更することなく高精度の偏波特性の測定ができる効果
がある。
As described above, according to this invention, the antenna feeding device is configured to have a reference polarization generation function, so when measuring the polarization characteristics of the antenna device, it is necessary to change the polarization plane on the collimator side. This has the effect of making it possible to measure polarization characteristics with high precision.

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

第1図は従来の基準偏波作戒手段を含む測定装置のブロ
ック図、第2図はこの考案の一実施例による基準偏波発
生機構付給電装置のブロック図、第3図はこの考案の他
の実施例による基準偏波発生機構付給電装置のブロック
図、第4図は偏分波器の動作を示す説明図、第5図はこ
の考案による装置に用いる基準偏波結合器の一構戊例を
示す斜視図である。 図において、12.19・・・・・・基準偏波結合器、
13・・・・・・偏分波器、8,9・・・・・・送受信
機への接続端子、15・・・・・・基準偏波検出端子で
ある。 なお、図中、同一符号は同一、又は相当部分を示す。
Fig. 1 is a block diagram of a measuring device including a conventional reference polarization control means, Fig. 2 is a block diagram of a power supply device with a reference polarization generating mechanism according to an embodiment of this invention, and Fig. 3 is a block diagram of a power supply device with a reference polarization generating mechanism according to an embodiment of this invention. A block diagram of a power supply device with a reference polarization generating mechanism according to another embodiment, FIG. 4 is an explanatory diagram showing the operation of a polarization splitter, and FIG. 5 is a structure of a reference polarization coupler used in the device according to this invention. It is a perspective view showing an example. In the figure, 12.19...Reference polarization coupler,
13... Polarization splitter, 8, 9... Connection terminal to transmitter/receiver, 15... Reference polarization detection terminal. In addition, in the figures, the same reference numerals indicate the same or equivalent parts.

Claims (3)

【実用新案登録請求の範囲】[Scope of utility model registration request] (1)入力端子と、この入力端子を経て給電される通過
信号に対し、所定の偏波変換を行う偏波変換器と、前記
偏波変換器からの通過信号を偏分波する偏分波器及び偏
分波器出力信号を外部へ導く一対の出力端子と、主回路
が前記偏波変換器と前記偏分波器の間又は前記人力端子
と偏波変換器の間に配設され、この主回路に所定の伝送
角を有する直線偏波の基準偏波信号を給電できる基準偏
波信号端子を有する基準偏波結合器、とを備え、通過信
号に対して所定の偏波変換と偏分波を行うと共に前記一
対の出力端子に前記基準偏波信号によってこれに対応し
て得られる校正信号を発生させ得るようにしたことを特
徴とする基準偏波発生機構付給電装置。
(1) An input terminal, a polarization converter that performs a predetermined polarization conversion on a passing signal fed through the input terminal, and a polarization converter that polarizes and separates the passing signal from the polarization converter. a pair of output terminals that guide the polarization splitter output signal to the outside, and a main circuit arranged between the polarization converter and the polarization splitter or between the manual terminal and the polarization converter, A reference polarization coupler having a reference polarization signal terminal capable of feeding a reference polarization signal of linear polarization having a predetermined transmission angle to this main circuit, A power supply device with a reference polarization generating mechanism, characterized in that it is capable of performing demultiplexing and generating a calibration signal corresponding to the reference polarization signal at the pair of output terminals.
(2)基準偏波信号の伝送軸を可変にできる機構を基準
偏波結合器に備え、基準偏波信号の伝送軸を変化させる
ことにより等価的に基準偏波信号端子へ給電される基準
偏波信号の偏波特性を変化させるようにしたことを特徴
とする前記実用新案登録請求の範囲第1項の記載の基準
偏波発生機構付給電装置。
(2) The reference polarization coupler is equipped with a mechanism that can vary the transmission axis of the reference polarization signal, and by changing the transmission axis of the reference polarization signal, the reference polarization signal is equivalently supplied to the reference polarization signal terminal. A power supply device with a reference polarized wave generating mechanism according to claim 1 of the above-mentioned utility model registration, characterized in that the polarization characteristic of a wave signal is changed.
(3)偏分波器と一対の出力端子の間に配設される2本
の伝送線の一方又は双方に可変減衰器と可変位相器を備
え、2本の伝送線の減衰特性及び位相特性を変更して相
互に特性に差をもたせることにより、等価的に基準偏波
信号端子へ給電される基準偏波信号の偏波特性を変化さ
せるようにしたことを特徴とする前記実用新案登録請求
の範囲第1項記載の基準偏波発生機構付給電装置。
(3) A variable attenuator and a variable phase shifter are provided on one or both of the two transmission lines arranged between the polarization splitter and the pair of output terminals, and the attenuation characteristics and phase characteristics of the two transmission lines are provided. The above-mentioned utility model registration is characterized in that the polarization characteristics of the reference polarization signal that is equivalently fed to the reference polarization signal terminal are changed by changing the characteristics to have a difference in characteristics. A power supply device with a reference polarization generation mechanism according to claim 1.
JP8434679U 1979-06-20 1979-06-20 Power supply device with reference polarization generation mechanism Expired JPS5912623Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP8434679U JPS5912623Y2 (en) 1979-06-20 1979-06-20 Power supply device with reference polarization generation mechanism

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP8434679U JPS5912623Y2 (en) 1979-06-20 1979-06-20 Power supply device with reference polarization generation mechanism

Publications (2)

Publication Number Publication Date
JPS563459U JPS563459U (en) 1981-01-13
JPS5912623Y2 true JPS5912623Y2 (en) 1984-04-16

Family

ID=29317547

Family Applications (1)

Application Number Title Priority Date Filing Date
JP8434679U Expired JPS5912623Y2 (en) 1979-06-20 1979-06-20 Power supply device with reference polarization generation mechanism

Country Status (1)

Country Link
JP (1) JPS5912623Y2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5850236A (en) * 1981-09-19 1983-03-24 正進化粧ベニヤ株式会社 Decorative panel

Also Published As

Publication number Publication date
JPS563459U (en) 1981-01-13

Similar Documents

Publication Publication Date Title
CN108037374B (en) Array antenna near field calibration method
CN110346655B (en) Device and method for measuring polarization parameters of antenna
US20040056799A1 (en) Phased array calibration using sparse arbitrarily spaced rotating electric vectors and a scalar measurement system
JPS5912623Y2 (en) Power supply device with reference polarization generation mechanism
EP0261828A1 (en) Microwave network analyser
US7098646B2 (en) Radio frequency power generation and power measurement
US3890571A (en) Radio frequency polarimeter
US4195299A (en) Loran-C system monitor circuit
US7002357B2 (en) Method and apparatus for phase calculation from attenuation values using a Hilbert transform for FDR measurements
JPS61172408A (en) Antenna adjusting method
SU1282022A1 (en) Device for measuring parameters of anisotropic materials
US3566286A (en) System for determining the gain compression of an r.f. amplifier
RU2242769C1 (en) Device for measuring ellipticity of electromagnetic wave
RU2090963C1 (en) Method of adaptive conversion of polarization of radio signals
SU1645912A1 (en) Interferometer with high frequency paths non-identity correction
US3357017A (en) System for obtaining difference curves of stacked beam antennas
CN117706466A (en) Interferometer phase real-time correction method
JPS6340884A (en) Microwave range finder
Savini An improved automatic tracking system for linear and circular polarization
SU1506393A1 (en) Apparatus for measuring amplitude-phase distribution in aerial aperture
Mallat et al. Antenna phase pattern measurements at millimeter wave frequencies using the differential phase method with only one power meter
JPS592863B2 (en) Antenna pattern measurement device
SU1149187A1 (en) Device for measuring dielectric film thickness and permittivity
JPH019016Y2 (en)
JPH023951B2 (en)