JPH02102463A - Antenna impedance measuring instrument - Google Patents

Antenna impedance measuring instrument

Info

Publication number
JPH02102463A
JPH02102463A JP25441788A JP25441788A JPH02102463A JP H02102463 A JPH02102463 A JP H02102463A JP 25441788 A JP25441788 A JP 25441788A JP 25441788 A JP25441788 A JP 25441788A JP H02102463 A JPH02102463 A JP H02102463A
Authority
JP
Japan
Prior art keywords
signal
frequency
filter
oscillator
intermediate frequency
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
Application number
JP25441788A
Other languages
Japanese (ja)
Inventor
Hirochika Onozawa
裕親 小野沢
Masataka Fujii
藤井 将貴
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.)
MEGURO ELECTRON CORP
Japan Broadcasting Corp
Original Assignee
MEGURO ELECTRON CORP
Nippon Hoso Kyokai NHK
Japan Broadcasting Corp
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 MEGURO ELECTRON CORP, Nippon Hoso Kyokai NHK, Japan Broadcasting Corp filed Critical MEGURO ELECTRON CORP
Priority to JP25441788A priority Critical patent/JPH02102463A/en
Publication of JPH02102463A publication Critical patent/JPH02102463A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To reduce the influence of radio interference and to take an accurate measurement by providing an intermediate frequency narrow band-pass filter, a detector, and a low-frequency band-pass filter. CONSTITUTION:The output signal of la preselector 15 is mixed by a mixer 16 with the local oscillation signal from a local oscillator 12 and converted to an intermediate frequency. This intermediate frequency signal is passed through the intermediate frequency band-pass filter 8 which has a narrow band width of + or - several tens Hz. Then the received signal passed through the filter 8 is amplified by an amplifier 17, detected by the detector 9, and then sent to the low-frequency band-pass filter 10 to extract a modulated wave, which is multiplied by a multiplier 11 up to the audio frequency of human beings. Then necessary signals such as higher harmonic components generated by the multiplication are removed by the band-pass filter 14 and only a modulated wave which is free from radio interference can be heard through a receiver 18. At the same time, the signal is indicated on a meter 23.

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は空中線、特に中波放送所の空中線のインピーダ
ンスを、ブリッジ回路を使用して測定する空中線インピ
ーダンス測定装置に関するものである。
DETAILED DESCRIPTION OF THE INVENTION (Field of Industrial Application) The present invention relates to an antenna impedance measuring device that measures the impedance of an antenna, particularly an antenna at a medium wave broadcasting station, using a bridge circuit.

(従来の技術) ブリッジを使用する空中線インピーダンス測定装置は従
来からある。この測定装置は第2図のようにブリッジ回
路Aの測定端子を空中線Bに接続し、受信周波数の信号
を受話器Cを用いて耳で聴きながら、その音が最も小さ
くなる点(出力信号零点)を求めてブリッジの平衡をと
るようにしたものである。
(Prior Art) An antenna impedance measuring device using a bridge has been conventionally available. This measuring device connects the measurement terminal of bridge circuit A to antenna B as shown in Figure 2, and listens to the received frequency signal using receiver C, at the point where the sound is the lowest (output signal zero point). The bridge is balanced by finding the following.

従来の空中線インピーダンス測定装置では、ブリッジの
平衡時に希望台がな(なり、一方において中波用の空中
線はきわめて感度が高く他局からの電波が混信し易いた
め、ブリッジの平衡時には混信波だけとなり、正確な測
定が困難になるという問題があった。
With conventional antenna impedance measurement equipment, there is no desired beam when the bridge is balanced.On the other hand, because medium-wave antennas are extremely sensitive and easily interfere with radio waves from other stations, when the bridge is balanced, there is only interference waves. However, there was a problem in that accurate measurement was difficult.

しかも測定者の耳には受話器を通して常に不要な混信台
が入るため、測定者は騒音に悩まされるという問題もあ
った。
Moreover, unnecessary interference is always heard through the receiver in the ears of the person taking the measurements, so there is also the problem that the person taking the measurements is bothered by the noise.

このような問題を解決するため、従来は受信部りの中間
周波段に狭帯域フィルタEが使用されていた。しかし従
来はブリッジ回路Aの信号源となる変調発振回路Fから
発振される変調周波数が8008 、程度であるため、
狭帯域フィルタEの帯域幅をその変調波に合わせて±8
008 、とじである、しかし空中線Bから混入してく
る混信信号には800 H□近傍の成分が多いので、せ
っかく狭帯域フィルタEを用いても、変調波だけでなく
混信信号も同フィルタEを通過してしまい、混信信号除
去効果が少なかった。
In order to solve this problem, a narrowband filter E has conventionally been used in the intermediate frequency stage of the receiving section. However, in the past, the modulation frequency oscillated from the modulation oscillation circuit F, which is the signal source of the bridge circuit A, was approximately 8008m.
Adjust the bandwidth of narrowband filter E to match the modulation wave by ±8
008, but since there are many components in the vicinity of 800 H□ in the interference signal coming in from antenna B, even if narrow band filter E is used, not only the modulated wave but also the interference signal will be filtered through filter E. The interference signal removal effect was low.

そこで従来は帯域幅が±5011□程度の狭帯域フィル
タEが使用されているが、このような狭帯域フィルタE
を使用すると、受信部りの同調がとりにくいので殆ど活
用されていなかった。
Therefore, conventionally, a narrowband filter E with a bandwidth of about ±5011□ has been used;
When using this method, it was difficult to synchronize the receiving section, so it was rarely used.

また、帯域幅が±50Hz程度の狭帯域フィルタでは、
800Hzの変調信号で変調されている受信信号の側波
帯が切りとられてしまうので、実際は800HZの変調
信号による変調を切り、受信部りのビート発振器Gを使
って中間周波数(455K)1.)よりも800 H,
高い(または低い)信号を発振させ、その信号と中間周
波数との差を求めて800H,のビート信号を得るよう
にしていた。
In addition, in a narrowband filter with a bandwidth of about ±50Hz,
Since the sideband of the received signal modulated by the 800Hz modulation signal is cut off, the modulation by the 800Hz modulation signal is actually cut off and the beat oscillator G in the reception section is used to generate the intermediate frequency (455K) 1. ) than 800 H,
A high (or low) signal was oscillated and the difference between the signal and the intermediate frequency was found to obtain a beat signal of 800H.

(発明が解決しようとする問題点) しかし、ビート信号は希望波とだけでなく、混信信号と
も発生し、耳で識別するのが困難であるという問題があ
った。
(Problems to be Solved by the Invention) However, there is a problem in that the beat signal occurs not only as a desired wave but also as an interference signal, making it difficult to distinguish it by ear.

(発明の目的) 本発明の目的は従来の空中線インピーダンス測定装置の
諸問題を解決し、従来の測定装置に比して混信の影響が
格段に少なく、正確な測定が可能で、また測定者が騒音
に悩まされることがなく、しかもビート方式の問題点も
解決した空中線インピーダンス測定装置を提供すること
にある。
(Objective of the Invention) The purpose of the present invention is to solve various problems of the conventional antenna impedance measuring device, to be able to perform accurate measurements with much less influence of interference than the conventional measuring device, and to make it possible for the measuring person to To provide an antenna impedance measuring device which does not suffer from noise and also solves the problems of the beat method.

(問題点を解決するための手段) 本発明の空中線インピーダンス測定装置は前記目的を達
成するため次のような構成にしである。
(Means for Solving the Problems) In order to achieve the above object, the antenna impedance measuring device of the present invention has the following configuration.

請求項第1の発明は第1図のように、空中線1に接続さ
れるブリッジ回路2と、ブリッジ回路2の信号源となる
信号発生部3と、ブリッジ回路2からの信号を受信する
受信部4とを備えた空中線インピーダンス測定装置にお
いて、前記信号発生部3にはブリッジ回路2に与えるR
F倍信号発振するRF発振器5と、同RF信号を変調す
る数十Hzの変調信号が発生される変調波発振器6とが
少なくとも備えられ、受信部4にはブリッジ回路2から
与えられる被変調波信号を中間周波に変換する周波数変
換部7と、帯域幅が士数十Hzの中間周波狭帯域フィル
タ8と、同フィルタ8を通過した中間周波信号を検波す
る検波器9と、検波信号のうち前記変調波を通す低周波
帯域フィルタ10と、同フィルタ10を通過した信号を
人間の可聴周波数まで逓倍する逓倍器11とが少なくと
も備えられ、前記信号発生部3または受信部4のどちら
かに、前記周波数変換部7の局部発振器12の発振周波
数が前記RF発振器5の周波数変化に連動して変化する
ようにした自動周波数制御部13を備えた局部発振器1
2を少なくとも備えられたことを特徴とする空中線イン
ピーダンス測定装置である。
A first aspect of the invention, as shown in FIG. 1, includes a bridge circuit 2 connected to an antenna 1, a signal generating section 3 serving as a signal source of the bridge circuit 2, and a receiving section receiving signals from the bridge circuit 2. In the antenna impedance measuring device equipped with 4, the signal generating section 3 has an R
The receiving section 4 is equipped with at least an RF oscillator 5 that oscillates an F-fold signal and a modulated wave oscillator 6 that generates a modulated signal of several tens of Hz that modulates the RF signal. A frequency converter 7 that converts a signal into an intermediate frequency, an intermediate frequency narrowband filter 8 with a bandwidth of several tens of Hz, a detector 9 that detects the intermediate frequency signal that has passed through the filter 8, and a detector 9 that detects the intermediate frequency signal that has passed through the filter 8. At least a low frequency band filter 10 that passes the modulated wave and a multiplier 11 that multiplies the signal passed through the filter 10 to a human audible frequency are provided, and either the signal generating section 3 or the receiving section 4 includes: A local oscillator 1 comprising an automatic frequency control section 13 in which the oscillation frequency of the local oscillator 12 of the frequency conversion section 7 changes in conjunction with a change in the frequency of the RF oscillator 5.
2. An antenna impedance measuring device characterized by comprising at least the following.

請求項第2の発明は請求項第1の空中線インピーダンス
測定装置において、受信部4に、逓倍器11による逓倍
に伴って発生する高調波成分等の不要信号を除去する帯
域フィルタ14が備えられたことを特徴とするものであ
る。
A second aspect of the invention is the antenna impedance measuring device according to the first aspect, wherein the receiving section 4 is provided with a bandpass filter 14 for removing unnecessary signals such as harmonic components generated due to multiplication by the multiplier 11. It is characterized by this.

請求項第3の発明は請求項第1の空中線インピーダンス
測定装置において、前記帯域フィルタ14の出力側に、
その出力を表示するメータ23が設けられたことを特徴
とするものである。
A third aspect of the present invention is the antenna impedance measuring device according to the first aspect, in which on the output side of the bandpass filter 14,
It is characterized by being provided with a meter 23 that displays the output.

(作用) 本発明の空中線インピーダンス測定装置により第1図の
空中線Iのインピーダンスを測定するには、従来からの
空中線インピーダンス測定装置によりインピーダンス測
定する場合と同様に、ブリッジ回路2の測定端子に空中
線lを接続して行なう。
(Function) To measure the impedance of the antenna I shown in FIG. 1 with the antenna impedance measuring device of the present invention, the antenna I Connect the .

この場合、第1図のRF発振器5から発振されたRF倍
信号、変調波発振器6から発振される変調波(例えば4
0H,)により変調されてブリッジ回路2に送られ、同
ブリッジ回路2からプリセレクタ15に送られ、このプ
リセレクタ15において空中Illを通して混信して(
る他局がらの信号の一部が除去される。
In this case, the RF multiplied signal oscillated from the RF oscillator 5 in FIG.
0H,) and is sent to the bridge circuit 2, and from the bridge circuit 2 to the preselector 15, where it is interfered with through the air Ill.
Some of the signals from other stations are removed.

プリセレクタ15からの出力信号は周波数変換用ミキサ
ー16において、局部発振器12からの局発信号と混合
されて中間周波数に周波数変換される。ここで変換され
た中間周波信号は、帯域幅が士数十Hz(例えば±50
8Z)と狭い中間周波狭帯域フィルタ8を通る。この場
合、前記変調波が数十H,(例えば401(りと低いた
め、この変調波が切りとられることはない。
The output signal from the preselector 15 is mixed with the local oscillator signal from the local oscillator 12 in a frequency conversion mixer 16 and frequency-converted to an intermediate frequency. The intermediate frequency signal converted here has a bandwidth of several tens of Hz (for example, ±50
8Z) and a narrow intermediate frequency narrow band filter 8. In this case, since the modulated wave is as low as several tens of H (for example, 401), this modulated wave is not cut off.

中間周波狭帯域フィルタ8を通った受信信号は増幅器1
7で増幅され、検波器9で検波され後、低周波帯域フィ
ルタ(40H,)10に送られて前記変調波がとりださ
れ、次に逓倍器11において人間の可聴周波数まで逓倍
される。逓倍に伴って発生する高調波成分などの不要信
号は帯域フィルタ14により除去され、受話器18によ
り混信のない変調波だけが聴きとられる。同時にその信
号がメータ23にも指示される。
The received signal that has passed through the intermediate frequency narrow band filter 8 is sent to the amplifier 1.
After being amplified in step 7 and detected in detector 9, the modulated wave is sent to a low frequency band filter (40H,) 10 to extract the modulated wave, and then multiplied by a multiplier 11 to a human audible frequency. Unnecessary signals such as harmonic components generated due to multiplication are removed by bandpass filter 14, and only modulated waves without interference are heard by receiver 18. At the same time, the signal is also transmitted to the meter 23.

また1本発明では局部発振器12から発振される局発信
号がRF発振器5の周波数を変化させるとそれに連動し
て変化する。さらに、同調用ミキサー20及び位相比較
器21並びに水晶発振器22によって構成されたPLL
 (位相同期ループ)により、常時、測定周波数よりも
中間周波数(455KH,)分だけ高い周波数をもつ信
号が作りだされる。このためRF発振器5で測定周波数
を設定すれば、受信部4側では自動的に同調がとれ、且
つ使用中に同調ずれが起きない。
Furthermore, in the present invention, when the frequency of the RF oscillator 5 is changed, the local oscillator signal oscillated from the local oscillator 12 changes in conjunction with the change in frequency. Furthermore, a PLL configured by a tuning mixer 20, a phase comparator 21, and a crystal oscillator 22
(Phase locked loop) always generates a signal with a frequency higher than the measurement frequency by the intermediate frequency (455KH,). Therefore, if the measurement frequency is set with the RF oscillator 5, the receiving section 4 side can automatically be tuned, and no out-of-tuning occurs during use.

(実施例) 第1図は本発明の空中線インピーダンス測定装置の一実
施例である。
(Embodiment) FIG. 1 shows an embodiment of the antenna impedance measuring device of the present invention.

第1図の1は放送局の被測定空中線、2はブリッジ回路
である。ブリッジ回路2は従来の空中線インピーダンス
測定で使用されているものと同じものである。
In FIG. 1, 1 is an antenna to be measured at a broadcasting station, and 2 is a bridge circuit. The bridge circuit 2 is the same as that used in conventional antenna impedance measurements.

第1図の3は信号発生部であり、これにはRF発振器5
と変調波発振器6とが備えられている。
3 in FIG. 1 is a signal generator, which includes an RF oscillator 5.
and a modulated wave oscillator 6.

RF発振器5は500KH,〜1650KH,までを発
振できるようにしである。変調波発振器6は40 Hz
の低周波変調波を発振できるようにしである。この40
Hzは空中線を通して混信する混信波の可聴成分が極め
て少ない周波数域(大部分の可聴成分は100H!以上
にある)である。
The RF oscillator 5 is capable of oscillating up to 500KH to 1650KH. Modulated wave oscillator 6 is 40 Hz
This makes it possible to oscillate low-frequency modulated waves. This 40
Hz is a frequency range in which there are very few audible components of interference waves transmitted through the antenna (most of the audible components are at 100 H! or higher).

第1図の4は受信部であり、ここにはプリセレクタ15
と、周波数変換用ミキサー16と、中間周波狭帯域フィ
ルタ8と、検波器9と、低周波帯域フィルタ10と、逓
倍器11と、帯域フィルタ14と、同調用ミキサー20
と、位相比較器21と、水晶発振器22と、局部発振器
12とが備えられ、しかも局部発振器12及びプリセレ
クタ15は信号発生部3のRF発振器5と連動するよう
にしである。(局部発振器12と、位相同期ループ13
は信号発生部側に置いても差し支えない) 前記プリセレクタ15は空中線1を通して混信している
他局からの信号を除去し、RF発振器5から発振される
RF倍信号通過させるためのバンドパスフィルタである
4 in FIG. 1 is a receiving section, and a preselector 15 is shown here.
, a frequency conversion mixer 16, an intermediate frequency narrow band filter 8, a detector 9, a low frequency band filter 10, a multiplier 11, a band filter 14, and a tuning mixer 20.
, a phase comparator 21 , a crystal oscillator 22 , and a local oscillator 12 , and the local oscillator 12 and preselector 15 are arranged to operate in conjunction with the RF oscillator 5 of the signal generating section 3 . (Local oscillator 12 and phase-locked loop 13
The preselector 15 is a bandpass filter for removing signals from other stations interfering with each other through the antenna 1 and passing the RF multiplied signal oscillated from the RF oscillator 5. It is.

第1図の7は周波数変換部であり、これはプリセレクタ
15を通して受信される受信信号を中間周波に変換する
ためのものであり、周波数変換用ミキサー16と局部発
振器12とにより構成されている。
Reference numeral 7 in FIG. 1 is a frequency conversion section, which converts the received signal received through the preselector 15 into an intermediate frequency, and is composed of a frequency conversion mixer 16 and a local oscillator 12. .

前記中間周波狭帯域フィルタ8は中心周波数455KH
、、帯域幅±50Hzの狭帯域水晶フィルタである。
The intermediate frequency narrow band filter 8 has a center frequency of 455KH.
, is a narrowband crystal filter with a bandwidth of ±50Hz.

前記増幅器17及び検波器9は汎用のものである。The amplifier 17 and detector 9 are general-purpose ones.

前記低周波帯域フィルタ10は変調波発振器6から発振
される40Hzの変調波をとりだすものであり、中心周
波数がその変調波に合わせて4ooz、帯域幅±2 H
z程度に設定されている。
The low frequency band filter 10 extracts a 40 Hz modulated wave oscillated from the modulated wave oscillator 6, and has a center frequency of 4 oz and a bandwidth of ±2 H in accordance with the modulated wave.
It is set to about z.

前記逓倍器11は検波された信号を人間の可聴周波数、
例えば960H,(40H,X24)まで逓倍出来るよ
うにしである。
The multiplier 11 converts the detected signal into a human audible frequency,
For example, it is possible to multiply up to 960H, (40H, X24).

前記帯域フィルタ14は逓倍器11により逓倍すること
により発生した高調波などの不要信号を除去するもので
あり、中心周波数960H,、帯域幅±50Hzとしで
ある。
The bandpass filter 14 removes unnecessary signals such as harmonics generated by multiplication by the multiplier 11, and has a center frequency of 960H and a bandwidth of ±50Hz.

同調用ミキサー20は汎用のものであり、水晶発振器2
2は455KH,の基準信号を発振するものであり、局
部発振器12はRF発振器5より発振されるRF信号の
周波数よりも中間周波数(455Kl(z)分だけ高い
周波数の局発信号を発振するものである。
The tuning mixer 20 is a general-purpose one, and the crystal oscillator 2
2 oscillates a reference signal of 455 KH, and the local oscillator 12 oscillates a local oscillator signal with a frequency higher than the frequency of the RF signal oscillated by the RF oscillator 5 by an intermediate frequency (455 Kl(z)). It is.

位相比較器21は局部発振器12から発振される局発信
号と、RF発振器5から発振されるRF信号との差を、
水晶発振器22から発振される基準信号(455KHz
)と比較し、P、LLにより局部発振器12の発振周波
数がRF発振器5の周波数に対し、正確に455KHz
高くなるように自動的に調節する信号を局部発振器12
に与える− (発明の効果) 本発明の空中線インピーダンス測定装置は次のような効
果がある。
The phase comparator 21 calculates the difference between the local oscillator signal oscillated from the local oscillator 12 and the RF signal oscillated from the RF oscillator 5.
The reference signal (455KHz) oscillated from the crystal oscillator 22
), the oscillation frequency of the local oscillator 12 is exactly 455 KHz compared to the frequency of the RF oscillator 5 due to P and LL.
The local oscillator 12 automatically adjusts the signal to
(Effects of the Invention) The antenna impedance measuring device of the present invention has the following effects.

(1)変調波周波数が40Hz程度の低周波であり、混
信波がもつ可聴成分の極めて少ない周波数域であるため
、混信成分との分離が容易になり、精度の高い測定が可
能になる。ちなみに、従来の測定装置では混信波が測定
波よりl0KH,離れていても測定しにくかったが、本
発明の測定装置では、実験の結果、両波が重なり合って
も測定可能であることが確認できた。
(1) The modulation wave frequency is a low frequency of about 40 Hz, which is a frequency range in which the audible component of the interference wave is extremely small, so it is easy to separate it from the interference component, and highly accurate measurement is possible. By the way, with the conventional measurement device, it was difficult to measure even if the interference wave was 10KH away from the measurement wave, but with the measurement device of the present invention, it was confirmed through experiments that it is possible to measure even when both waves overlap. Ta.

(2)変調周波数が中間周波狭帯域フィルタ8を通過出
来る周波数に設定されているので、従来の様に、受信部
においてビート信号を作り出す必要がなく、ビートを使
用する場合の問題点が全て解消される。
(2) Since the modulation frequency is set to a frequency that can pass through the intermediate frequency narrowband filter 8, there is no need to create a beat signal in the receiver as in the conventional case, and all problems when using beats are solved. be done.

(3)局部発振器12から発振される局発信号がRF発
振器5の周波数変化と連動して変化するため、RF発振
器5で測定周波数を設定すれば、受信部4fllでは自
動的に同調がとれ、且つ使用中に同調ずれが起きない、
このため非常に取り扱い易くなる。
(3) Since the local signal oscillated from the local oscillator 12 changes in conjunction with the frequency change of the RF oscillator 5, if the measurement frequency is set with the RF oscillator 5, the receiving section 4fl will automatically be tuned; And no synchronization occurs during use.
This makes it extremely easy to handle.

(4)検波器9の後に変調波だけが通る低周波帯域フィ
ルタ10を設けたので、混信成分の大半が除去される。
(4) Since the low frequency band filter 10 through which only the modulated wave passes is provided after the detector 9, most of the interference components are removed.

(5)逓倍器llを設けたので、40Hzと低い周波数
の変調波でも聴くことが可能となる。
(5) Since the multiplier 11 is provided, it is possible to listen to modulated waves as low as 40 Hz.

(6)逓倍器11の後に帯域フィルタ14を設けたので
、逓倍によって発生した高調波と、混信成分の残りが除
去される。
(6) Since the bandpass filter 14 is provided after the multiplier 11, harmonics generated by multiplication and the remaining interference components are removed.

(7)ブリッジの平衡検出にメータを併用したので、耳
だけでなくメータの指示でブリッジの平衡点を求めるこ
ともできる。この場合、混信が充分にとり切れないと、
メータの計がふらつくが、この場合は針の振れがある程
度落ちついて、一定値以下になったときの、ブリッジ回
路のダイヤル位置の2点の中点をとって平衡点とみなす
測定も可能となる。
(7) Since a meter is also used to detect the balance of the bridge, the balance point of the bridge can be determined not only by the ear but also by the meter. In this case, if the interference cannot be sufficiently removed,
The meter reading may fluctuate, but in this case, when the needle vibration has stabilized to some extent and is below a certain value, it is possible to measure by taking the midpoint between the two dial positions of the bridge circuit and treating it as the equilibrium point. .

(8)以上の対策が相乗することにより、測定周波数が
混信波に近接しても、混信騒音をほとんど感じることな
く測定でき、測定者が騒音に悩まされることもない。
(8) By combining the above measures, even if the measurement frequency is close to an interference wave, the measurement can be performed with almost no interference noise, and the person taking the measurement will not be bothered by the noise.

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

第1図は本発明の空中線インピーダンス測定装置の一例
を示す説明図、第2図は従来の空中線インピーダンス測
定装置の説明図である。 1は空中線 2はブリッジ回路 3は信号発生部 4は受信部 5はRF発振器 6は変調波発振器 7は周波数変換部 8は中間周波狭帯域フィルタ 9は検波器 10は低周波帯域フィルタ 11は逓倍器 12は局部発振器 13は位相同期ループ 14は帯域フィルタ 23はメータ
FIG. 1 is an explanatory diagram showing an example of the antenna impedance measuring device of the present invention, and FIG. 2 is an explanatory diagram of a conventional antenna impedance measuring device. 1 is an antenna 2 is a bridge circuit 3 is a signal generator 4 is a receiver 5 is an RF oscillator 6 is a modulated wave oscillator 7 is a frequency converter 8 is an intermediate frequency narrow band filter 9 is a detector 10 is a low frequency band filter 11 is a multiplier The device 12 is a local oscillator 13, the phase-locked loop 14 is a bandpass filter 23, and a meter

Claims (3)

【特許請求の範囲】[Claims] (1)空中線1に接続されるブリッジ回路2と、ブリッ
ジ回路2の信号源となる信号発生部3と、ブリッジ回路
2からの信号を受信する受信部4とを備えた空中線イン
ピーダンス測定装置において、前記信号発生部3にはブ
リッジ回路2に与えるRF信号を発振するRF発振器5
と、同RF信号を変調する数十Hzの変調信号が発生さ
れる変調波発振器6とが少なくとも備えられ、受信部4
にはブリッジ回路2から与えられる被変調波信号を中間
周波に変換する周波数変換部7と、帯域幅が数十Hzの
中間周波狭帯域フィルタ8と、同フィルタ8を通過した
中間周波信号を検波する検波器9と、検波信号のうち前
記変調波を通す数十Hzの低周波帯域フィルタ10と、
同フィルタ10を通過した信号を人間の可聴周波数まで
逓倍する逓倍器11とが少なくとも備えられ、前記信号
発生部3または受信部4のどちらかに前記周波数変換部
7の局部発振器12の発振周波数が前記RF発振器5の
周波数変化に連動して変化するようにした自動周波数制
御部13とが少なくとも備えられたことを特徴とする空
中線インピーダンス測定装置。
(1) In an antenna impedance measuring device comprising a bridge circuit 2 connected to an antenna 1, a signal generating section 3 serving as a signal source of the bridge circuit 2, and a receiving section 4 receiving a signal from the bridge circuit 2, The signal generating section 3 includes an RF oscillator 5 that oscillates an RF signal to be applied to the bridge circuit 2.
and a modulated wave oscillator 6 that generates a modulation signal of several tens of Hz for modulating the RF signal, and the receiving section 4
includes a frequency converter 7 that converts the modulated wave signal given from the bridge circuit 2 into an intermediate frequency, an intermediate frequency narrowband filter 8 with a bandwidth of several tens of Hz, and a frequency converter 7 that detects the intermediate frequency signal that has passed through the filter 8. a low frequency band filter 10 of several tens of Hz that passes the modulated wave of the detected signal;
At least a multiplier 11 for multiplying the signal passed through the filter 10 to a human audible frequency is provided, and either the signal generating section 3 or the receiving section 4 receives the oscillation frequency of the local oscillator 12 of the frequency converting section 7. An antenna impedance measuring device comprising at least an automatic frequency control section 13 that changes in conjunction with changes in the frequency of the RF oscillator 5.
(2)前記受信部4に逓倍器11による逓倍に伴って発
生する高調波成分等の不要信号を除去する帯域フィルタ
14が備えられたことを特徴とする請求項第1の空中線
インピーダンス測定装置。
(2) The antenna impedance measuring device according to claim 1, wherein the receiving section 4 is equipped with a bandpass filter 14 for removing unnecessary signals such as harmonic components generated due to multiplication by the multiplier 11.
(3)前記受信部4の前記帯域フィルタ14の出力側に
、その出力が表示されるメータ23が設けられたことを
特徴とする請求項第1の空中線インピーダンス測定装置
(3) An antenna impedance measuring device according to claim 1, characterized in that a meter 23 for displaying the output is provided on the output side of the bandpass filter 14 of the receiving section 4.
JP25441788A 1988-10-08 1988-10-08 Antenna impedance measuring instrument Pending JPH02102463A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP25441788A JPH02102463A (en) 1988-10-08 1988-10-08 Antenna impedance measuring instrument

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP25441788A JPH02102463A (en) 1988-10-08 1988-10-08 Antenna impedance measuring instrument

Publications (1)

Publication Number Publication Date
JPH02102463A true JPH02102463A (en) 1990-04-16

Family

ID=17264688

Family Applications (1)

Application Number Title Priority Date Filing Date
JP25441788A Pending JPH02102463A (en) 1988-10-08 1988-10-08 Antenna impedance measuring instrument

Country Status (1)

Country Link
JP (1) JPH02102463A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE19749872B4 (en) * 1996-11-11 2006-03-16 Mori Seiki Hitech Co., Ltd., Yamatokoriyama Vertical lathe and machining system with two machine areas

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE19749872B4 (en) * 1996-11-11 2006-03-16 Mori Seiki Hitech Co., Ltd., Yamatokoriyama Vertical lathe and machining system with two machine areas

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