JPH0681106B2 - Radio wave propagation characteristics measurement method - Google Patents
Radio wave propagation characteristics measurement methodInfo
- Publication number
- JPH0681106B2 JPH0681106B2 JP62108524A JP10852487A JPH0681106B2 JP H0681106 B2 JPH0681106 B2 JP H0681106B2 JP 62108524 A JP62108524 A JP 62108524A JP 10852487 A JP10852487 A JP 10852487A JP H0681106 B2 JPH0681106 B2 JP H0681106B2
- Authority
- JP
- Japan
- Prior art keywords
- signal
- amplitude
- radio wave
- received
- characteristic
- 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 - Fee Related
Links
Landscapes
- Monitoring And Testing Of Transmission In General (AREA)
Description
【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、電波伝搬通路において反射、回折、散乱等に
より発生する多重波の遅延特性および振幅特性を瞬時に
測定する方法に関する。TECHNICAL FIELD The present invention relates to a method for instantaneously measuring delay characteristics and amplitude characteristics of multiple waves generated by reflection, diffraction, scattering, etc. in a radio wave propagation path.
送信機から受信機に伝搬する電波は、すべてが最短距離
で伝搬するのではなく、反射、回折、散乱等により、最
短距離で伝搬した電波に遅れて受信機に到達する成分が
生じる。このような成分を多重波という。送信機から受
信機への電波伝搬通路を評価するためには、このような
多重波の遅延特性およびその振幅特性を測定することが
必要となる。The radio waves propagating from the transmitter to the receiver do not all propagate at the shortest distance, but due to reflection, diffraction, scattering, etc., components that arrive at the receiver after the radio waves propagated at the shortest distance are generated. Such components are called multiple waves. In order to evaluate the radio wave propagation path from the transmitter to the receiver, it is necessary to measure the delay characteristics and the amplitude characteristics of such multiple waves.
電波伝搬特性を測定する方法としては、従来、周波数相
関法、PN信号相関法、テレビ放送波利用法、周波数掃引
法等が用いられている。これらの測定方法について以下
に説明する。Conventionally, a frequency correlation method, a PN signal correlation method, a television broadcast wave utilization method, a frequency sweep method and the like have been used as methods for measuring the radio wave propagation characteristics. These measuring methods will be described below.
(i)周波数相関法 周波数相関法では。周波数差Δfが非常に近接した二つ
の周波数を用いて、受信電界強度の異なる受信点間の周
波数相関関数ρΔf(m)を求める。周波数相関関数ρ
Δf(m)は、 で表される。ここで、 x(n)、y(n):各周波数の電界強度、 N:計算に用いるデータ数、 m:位置のずれ、 <m>:mを越えない整数 である。この関係式を用いて、あらかじめ計算により求
めた伝搬モデルと比較することにより多重波の伝搬路長
差を推定する。(I) Frequency correlation method In the frequency correlation method. The frequency correlation function ρΔf (m) between reception points having different reception electric field strengths is obtained by using two frequencies having very close frequency differences Δf. Frequency correlation function ρ
Δf (m) is It is represented by. Here, x (n), y (n): electric field strength of each frequency, N: number of data used for calculation, m: position shift, <m>: integer not exceeding m. By using this relational expression, the propagation path length difference of the multiple waves is estimated by comparing with the propagation model calculated in advance.
この方法については、電子通信学会技術研究報告AP81-2
3、「市街地伝搬モデルと周波数相関特性」に詳しく説
明されている。For this method, refer to IEICE Technical Report AP81-2.
It is explained in detail in "3. Urban Propagation Model and Frequency Correlation Characteristics".
(ii)PN信号相関法 PN信号の自己相関関数が、時間的に同期して同一波形と
なったときに最大となる性質を利用する。(Ii) PN signal correlation method The property that the autocorrelation function of a PN signal becomes maximum when the same waveform is synchronized in time is used.
送信側では、精度の高い基準時間をもつPN信号を送信す
る。受信側では、遅延時間を可変に設定しながら送信側
と同一波形のPN信号を発生し、送信側から到来した信号
との相関検波を行う。このとき、相関検波の出力が最大
となるような受信側PN信号の遅延時間が多重波伝搬路長
差により遅延時間に等しくなる。したがって、主波の検
波出力値と相対検波出力値との比が相対的な多重波振幅
値となる。The transmitting side transmits a PN signal having a highly accurate reference time. The receiving side generates a PN signal having the same waveform as the transmitting side while variably setting the delay time, and performs correlation detection with the signal coming from the transmitting side. At this time, the delay time of the PN signal on the receiving side that maximizes the output of the correlation detection becomes equal to the delay time due to the difference in the lengths of the multiple wave propagation paths. Therefore, the ratio between the detection output value of the main wave and the relative detection output value becomes the relative multiple wave amplitude value.
この方法によれば、相関検波出力と受信PN信号遅延時間
とから、多重波の伝搬遅延特性と相対振幅特性とを同時
に求めることができる。According to this method, it is possible to simultaneously obtain the propagation delay characteristic and the relative amplitude characteristic of the multiple wave from the correlation detection output and the received PN signal delay time.
この方法については、「コリレーション・バンドウィド
ス・アンド・ディレイ・スプレッド・マルチパス・プロ
パゲーション・スタティスティクス・フォー910MHzアー
バン・モービル・ラジオ・チャネルズ」、IEEEトランザ
クション第COM-23巻第11号1975年第1271〜1280頁("Cor
relationBandwidth and Delay Spread Multipath Propa
gation Statistics for 910 MHz Urban Moble RadioCha
nnels",IEEE Trans.COM-23,No.11,pp1271-1280,1975)
に詳しく説明されている。This method is described in “Correlation Bandwidth and Delay Spread Multipath Propagation Statistics for 910MHz Urban Mobile Radio Channels”, IEEE Transaction No. COM-23, No. 11, 1975. Pages 1271-1280 ("Cor
relationBandwidth and Delay Spread Multipath Propa
gation Statistics for 910 MHz Urban Moble RadioCha
nnels ", IEEE Trans.COM-23, No.11, pp1271-1280,1975)
Are described in detail in.
(iii)搬送波パルス法 送信側では、測定しようとする周波数の搬送波を短い時
間間隔で断続的に送信する。受信側では、受信した多重
波を直接検波してその特性を測定する。(Iii) Carrier wave pulse method On the transmitting side, the carrier wave of the frequency to be measured is intermittently transmitted at short time intervals. On the receiving side, the received multiple waves are directly detected and their characteristics are measured.
(iv)テレビ放送波利用法 この測定方法では、テレビ放送波に含まれる色バースト
信号の位相差と水平同期信号の遅延時間とを測定し、こ
れらの測定値により遅延通路差を求める。(Iv) Television Broadcast Wave Utilization Method In this measurement method, the phase difference of the color burst signal and the delay time of the horizontal synchronizing signal included in the television broadcast wave are measured, and the delay path difference is obtained from these measured values.
基準となる受信信号と被測定受信信号とは、伝搬路長差
に応じて色バースト信号の色副搬送波に位相のずれが生
じる。この位相差を測定することにより伝搬路長差を求
めることができる。しかし、色バースト信号の位相差を
測定するだけでは、色副搬送波(NTSC方式の場合には約
3.58MHz)の波長の整数倍を加えた距離と区別できな
い。そこで、水平同期信号の遅延時間によりおおよその
時間を求めて決定する。A phase difference occurs between the reference received signal and the measured received signal in the color subcarrier of the color burst signal depending on the propagation path length difference. By measuring this phase difference, the propagation path length difference can be obtained. However, it is only necessary to measure the phase difference of the color burst signal,
(3.58MHz) is indistinguishable from an integer multiple of the wavelength. Therefore, the delay time of the horizontal synchronizing signal is used to determine an approximate time.
(v)周波数掃引法 送信側の搬送波周波数を掃引し、受信した各々のレベル
から伝搬路の振幅周波数特性を求める。この周波数特性
から伝搬路長差を求めることができる。(V) Frequency sweep method The carrier frequency on the transmitting side is swept, and the amplitude frequency characteristic of the propagation path is obtained from each received level. The propagation path length difference can be obtained from this frequency characteristic.
しかし、以上の方法にはそれぞれ以下の欠点がある。 However, each of the above methods has the following drawbacks.
(i)周波数相関法 この方法では、無数に存在する多重波の数を有限(2波
程度)のモデルで推定するため、複雑な多重波モデルで
は誤差が大きくなる。また、モデル化等の推定を行うた
めの計算量が多く、瞬時に推定値を求めることはできな
い。さらにこの方法では、振幅特性の推定は困難であ
る。(I) Frequency Correlation Method In this method, the number of multiple waves existing in innumerable is estimated by a finite (about two waves) model, and therefore the error becomes large in a complicated multiple wave model. In addition, the amount of calculation for estimating the model is large, and the estimated value cannot be obtained instantaneously. Furthermore, with this method, it is difficult to estimate the amplitude characteristic.
(ii)PN信号相関法 この方法では、相関検波を行うために、送信側および受
信側の双方に高精度の周波数基準が必要となるため、測
定を行うためには振動や温度等の場所的制約があり、迅
速に測定結果を得ることはできない。(Ii) PN signal correlation method This method requires a highly accurate frequency reference on both the transmitting side and the receiving side to perform correlation detection. There are restrictions and it is not possible to obtain measurement results quickly.
(iii)搬送波パルス法 この方法では、断続された搬送波を測定するため、精度
を高めるためには、パルス幅を非常に狭くする必要があ
る。このような非常にパルス幅の狭い電波を安定に受信
復調することは受信機の特性上困難であり、狭いパルス
幅で受信機を高精度に較正し、到来した電波の振幅特性
を精度よく測定することは容易ではない。(Iii) Carrier wave pulse method In this method, a discontinuous carrier wave is measured. Therefore, in order to improve accuracy, it is necessary to make the pulse width extremely narrow. It is difficult to stably receive and demodulate radio waves with such a very narrow pulse width due to the characteristics of the receiver.Therefore, the receiver is accurately calibrated with a narrow pulse width and the amplitude characteristics of incoming radio waves are measured accurately. It's not easy to do.
(iv)テレビ放送波利用法 この方法では、テレビ放送局からの位相精度の高い色バ
ースト信号を利用しているため、高精度に遅延時間を測
定できるが、測定基準用と測定用との二つの受信系が必
要であり、また、各々の系を相互に較正しなければ精度
がとれないため、装置が大規模となる。(Iv) Television Broadcast Wave Utilization This method uses a color burst signal with high phase accuracy from a television broadcasting station, so the delay time can be measured with high accuracy. Two receiving systems are required, and the accuracy cannot be obtained unless the systems are mutually calibrated, resulting in a large-scale device.
また、多重波を分離できないので、2以上の多重波が存
在する場合には測定できない。In addition, since multiple waves cannot be separated, measurement cannot be performed when two or more multiple waves exist.
さらに、任意の区間で測定しようとすると、送信信号の
色バースト信号の位相をテレビ放送局で使用している程
度に高精度にする必要がある。Furthermore, when attempting to measure in an arbitrary section, it is necessary to make the phase of the color burst signal of the transmission signal as accurate as that used by a television broadcasting station.
(v)周波数掃引法 多重波を直接に測定するわけではないので誤差が大き
く、送信側と受信側とを同期させる必要があるため、瞬
時に測定することは困難である。(V) Frequency sweep method Since multiple waves are not measured directly, the error is large, and it is difficult to measure instantaneously because it is necessary to synchronize the transmitting side and the receiving side.
本発明は、以上の問題点を解決し、多重波の伝搬路長に
よる伝搬遅延時間と、各々の波のレベルとを同時にかつ
瞬時に直接測定することのできる電波伝搬特性の測定方
法を提供することを目的とする。The present invention solves the above problems and provides a method for measuring radio wave propagation characteristics, which allows direct and simultaneous measurement of the propagation delay time due to the propagation path length of multiple waves and the level of each wave. The purpose is to
本発明の測定方法は、反射、散乱または回折により生じ
る複数の伝搬路を含む電波伝搬通路を経由して伝搬する
信号の遅延特性および振幅特性を測定する電波伝搬特性
測定方法において、送信側では、受信側で実質的に一定
の振幅が得られる程度にパルス幅の長い基準信号と、上
記複数の伝搬路の長さにより生じる遅延時間差に比較し
て短いパルス幅の測定信号とを被測定周波数により振幅
変調して送信し、受信側では、各伝搬路を経由して到来
した受信測定信号の振幅を上記基準信号の受信振幅値に
より補正して振幅特性を求め、上記受信測定信号の時間
差から遅延特性を求めることを特徴とする。The measurement method of the present invention is a radio wave propagation characteristic measurement method for measuring delay characteristics and amplitude characteristics of a signal propagating through a radio wave propagation path including a plurality of propagation paths generated by reflection, scattering, or diffraction, and on the transmission side, A reference signal with a pulse width that is long enough to obtain a substantially constant amplitude on the receiving side, and a measurement signal with a short pulse width compared to the delay time difference caused by the lengths of the plurality of propagation paths are set according to the measured frequency. Amplitude-modulated and transmitted, and at the receiving side, the amplitude of the received measurement signal that arrived via each propagation path is corrected by the received amplitude value of the reference signal to obtain the amplitude characteristic, and the delay is delayed from the time difference of the received measurement signal. It is characterized by obtaining characteristics.
本発明の測定方法は、電波伝搬通路で生じる多重波の各
々について、振幅と最短距離を伝搬した波に対する遅延
時間とを同時にかつ瞬時に直接測定できる。送受信を行
う信号に振幅値の基準を含むため、測定精度が高く、測
定結果を得るための計算機等により処理を必要としな
い。したがって、瞬時に多重波の伝搬遅延特性と振幅特
性とを同時に測定できる。The measuring method of the present invention can directly and instantaneously measure the amplitude and the delay time of the wave propagating the shortest distance for each of the multiple waves generated in the radio wave propagation path. Since the signal to be transmitted / received includes the reference of the amplitude value, the measurement accuracy is high and the processing is not required by the computer or the like for obtaining the measurement result. Therefore, it is possible to simultaneously measure the propagation delay characteristic and the amplitude characteristic of multiple waves at the same time.
第1図は本発明方法を実施するための測定装置のブロッ
ク構成図を示す。FIG. 1 shows a block diagram of a measuring apparatus for carrying out the method of the present invention.
送信信号発生部1は送信部2を介して送信用アンテナ3
に接続される。送信用アンテナ3から送信された電波
は、電波伝搬通路7を介して受信用アンテナ4に到達す
る。受信用アンテナ4は受信部5を介して測定部6に接
続される。The transmission signal generation unit 1 transmits the transmission antenna 3 via the transmission unit 2.
Connected to. The radio wave transmitted from the transmitting antenna 3 reaches the receiving antenna 4 via the radio wave propagation path 7. The receiving antenna 4 is connected to the measuring unit 6 via the receiving unit 5.
電波伝搬通路7は、最短の距離で電波を伝搬する主波伝
搬路と、反射、屈折、散乱等により生じた多重波を伝搬
する多重波伝搬路とを含む。The radio wave propagation path 7 includes a main wave propagation path for propagating a radio wave at the shortest distance and a multiwave propagation path for propagating multiple waves generated by reflection, refraction, scattering and the like.
第2図は送信信号発生部1の出力する送信信号を示す。FIG. 2 shows a transmission signal output from the transmission signal generator 1.
送信信号発生部1の出力する送信信号は、時間および振
幅の基準となる基準信号8と、多重波の遅延時間および
振幅を測定するための測定信号9とを含む。この測定信
号9に対して、受信側では、各伝搬路を経由して到来し
た受信測定信号の振幅を上記基準信号の受信振幅値によ
り補正して振幅特性を求め、上記受信測定信号の時間差
から遅延特性を求めることができる。The transmission signal output from the transmission signal generator 1 includes a reference signal 8 serving as a reference for time and amplitude, and a measurement signal 9 for measuring delay time and amplitude of multiple waves. With respect to this measurement signal 9, on the reception side, the amplitude of the reception measurement signal arriving via each propagation path is corrected by the reception amplitude value of the reference signal to obtain the amplitude characteristic, and from the time difference of the reception measurement signal, The delay characteristic can be obtained.
ここで、基準信号8および測定信号9の振幅値をそれぞ
れA、Bとし、時間幅をそれぞれC、Dとする。また、
送信信号の周期時間をEとし、測定信号9から次の基準
信号8までの時間をFとする。基準信号8の時間幅Cの
パルス幅は、電波伝搬通路7において多重波のために波
形歪が発生した場合でも、波形の一部分に基準振幅値を
保持できる値に設定される。時間Fは、測定しようとす
る伝搬遅延時間の最大値より長く設定される。時間幅D
は、多重波搬路による伝搬遅延時間の最小値より短く設
定される。Here, the amplitude values of the reference signal 8 and the measurement signal 9 are A and B, respectively, and the time widths are C and D, respectively. Also,
The cycle time of the transmission signal is E, and the time from the measurement signal 9 to the next reference signal 8 is F. The pulse width of the time width C of the reference signal 8 is set to a value capable of holding the reference amplitude value in a part of the waveform even when waveform distortion occurs due to multiple waves in the radio wave propagation path 7. The time F is set longer than the maximum value of the propagation delay time to be measured. Time width D
Is set to be shorter than the minimum value of the propagation delay time due to the multipath.
第3図は送信部2の出力波形を示す。FIG. 3 shows the output waveform of the transmitter 2.
送信部2は、送信信号を測定対称の周波数で振幅変調す
る。この振幅変調された信号が送信用アンテナ3から送
信され、電波伝搬通路7を経由して受信用アンテナ4に
達し、受信部5により検波される。The transmitter 2 amplitude-modulates the transmission signal at a frequency symmetrical to the measurement. This amplitude-modulated signal is transmitted from the transmitting antenna 3, reaches the receiving antenna 4 via the radio wave propagation path 7, and is detected by the receiving unit 5.
第4図は受信部5が検波した受信信号の波形の一例を示
す。FIG. 4 shows an example of the waveform of the received signal detected by the receiver 5.
この受信信号は、基準信号8に対応する受信基準信号
8′と、測定信号に対応する受信測定信号とを含む。受
信測定信号は、主波伝搬路を経由した主波信号9(0)およ
び多重波伝搬路を経由した多重波信号9(1)、9(2)、
9(3)、…を含む。受信基準信号8′および受信測定信号
の振幅は、それぞれA′、B0′、B1′、B2′、B3′、…
である。多重波信号9(1)、9(2)、9(3)、…は、その伝搬
通路長により、主波信号9(0)が到来してからそれぞれ遅
延時間F1、F2、F3、…の後に到来する。The received signal includes a received reference signal 8'corresponding to the reference signal 8 and a received measurement signal corresponding to the measurement signal. The received measurement signals are the main wave signal 9 (0) passing through the main wave propagation path and the multiple wave signals 9 (1) , 9 (2)
9 (3) , including ... Received reference signal 8 'amplitude and receiving measurement signals, respectively A', B 0 ', B 1', B 2 ', B 3', ...
Is. Due to the propagation path length, the multiple wave signals 9 (1) , 9 (2) , 9 (3) , ... Have delay times F 1 , F 2 , F 3 after the main wave signal 9 (0) arrives. , ... comes after.
ここで、受信基準信号8′に多重波による歪が生じる場
合でも、送信側の基準信号8のパルス幅を適当に選ぶこ
とにより基準振幅値を保持できる。伝搬通路長差は光速
を遅延時間F1、F2、F3、…で除算することにより得られ
る。Here, even when the reception reference signal 8'is distorted by multiple waves, the reference amplitude value can be held by appropriately selecting the pulse width of the reference signal 8 on the transmission side. The propagation path length difference is obtained by dividing the speed of light by the delay times F 1 , F 2 , F 3 , ....
第5図は受信信号の他の波形例を示す。FIG. 5 shows another example of the waveform of the received signal.
この例では、受信基準信号8′の振幅A′と主波信号9
(0)の振幅B0′との比が、送信側の基準信号8の振幅A
と測定信号9の振幅Bとの比と異なる。このときには、 B′=(A′/A)×B として主波の振幅比の絶対測定を行うことができる。In this example, the amplitude A'of the received reference signal 8'and the main wave signal 9 '
The ratio of (0) to the amplitude B 0 ′ is the amplitude A of the reference signal 8 on the transmitting side.
And the amplitude B of the measurement signal 9 are different. At this time, the absolute measurement of the amplitude ratio of the main wave can be performed by B '= (A' / A) × B.
第6図は基準信号の多重波成分を含む受信波形を示す。FIG. 6 shows a received waveform including multiple wave components of the reference signal.
受信波形に基準信号の多重波成分10が含まれる場合に
は、送信側で基準信号8と測定信号9との時間間隔を測
定しようとする多重波の遅延時間の最大値以上に選択す
る。これにより、基準信号の多重波成分10が受信測定信
号の領域で発生しないようにすることができる。When the received waveform includes the multiple wave component 10 of the reference signal, the time interval between the reference signal 8 and the measurement signal 9 is selected to be equal to or greater than the maximum delay time of the multiple wave to be measured on the transmission side. As a result, the multiple wave component 10 of the reference signal can be prevented from occurring in the area of the received measurement signal.
第7図は基準信号の多重波成分を含む他の受信波形を示
す。FIG. 7 shows another received waveform including multiple wave components of the reference signal.
送信信号発生部1は、測定信号9を含まない送信信号
と、基準信号8および測定信号9を含む送信信号とを一
周期毎に交互に発生する。測定部6では、測定信号9を
含まない周期Gにおける基準信号の多重波成分を記憶
し、この値により測定信号9を含む周期Hにおける受信
信号を補正する。The transmission signal generator 1 alternately generates a transmission signal that does not include the measurement signal 9 and a transmission signal that includes the reference signal 8 and the measurement signal 9 for each cycle. The measuring unit 6 stores the multiple wave component of the reference signal in the period G that does not include the measurement signal 9, and corrects the received signal in the period H that includes the measurement signal 9 by this value.
以上の実施例では送信側に専用の装置を用いたが、送信
信号としてテレビジョン信号を利用しても本発明を同様
に実施できる。テレビジョン信号は残留側波帯変調とい
う振幅変調を用いており、基準信号として水平同期信号
を用いる。その場合には、特別に送信機を設ける必要な
しに測定できる。In the above embodiments, a dedicated device was used on the transmission side, but the present invention can be similarly implemented by using a television signal as a transmission signal. The television signal uses amplitude modulation called vestigial sideband modulation, and uses a horizontal synchronizing signal as a reference signal. In that case, the measurement can be performed without the need to provide a special transmitter.
本発明の測定方法と従来例方法との比較を表に示す。The table shows a comparison between the measuring method of the present invention and the conventional method.
〔発明の効果〕 以上説明したように、本発明の電波伝搬特性測定方法
は、電波伝搬通路において反射、回折、散乱等により発
生した多重波の伝搬通路長に起因する遅延時間および振
幅値の二つの特性を瞬時にかつ同時に測定することがで
きる。したがって、短時間の多くの測定が可能となり、
また、自動車等による移動走行中でも上記二つの特性を
測定できる効果がある。 [Effects of the Invention] As described above, the radio wave propagation characteristic measuring method of the present invention is characterized in that the delay time and the amplitude value due to the propagation path length of multiple waves generated by reflection, diffraction, scattering, etc. in the radio wave propagation path Two characteristics can be measured instantaneously and simultaneously. Therefore, many measurements in a short time are possible,
Further, there is an effect that the above two characteristics can be measured even while traveling by a car or the like.
第1図は本発明を実施するための測定装置のブロック構
成図。 第2図は送信信号発生部の出力する送信信号の波形を示
す図。 第3図は送信部の出力波形を示す図。 第4図は受信信号波形の一例を示す図。 第5図は受信信号波形の他の例を示す図。 第6図は基準信号の多重波成分を含む受信波形を示す
図。 第7図は基準信号の多重波成分を含む他の受信波形を示
す図。 1……送信信号発生部、2……送信部、3……送信用ア
ンテナ、4……受信用アンテナ、5……受信部、6……
測定部、7……電波伝搬通路、8……基準信号、8′…
…受信基準信号、9……測定信号、9(0)……主波信号、
9(1)、9(2)、9(3)……多重波信号、10……基準信号の多
重波成分。FIG. 1 is a block configuration diagram of a measuring apparatus for carrying out the present invention. FIG. 2 is a diagram showing a waveform of a transmission signal output from the transmission signal generator. FIG. 3 is a diagram showing an output waveform of the transmitter. FIG. 4 is a diagram showing an example of a received signal waveform. FIG. 5 is a diagram showing another example of the received signal waveform. FIG. 6 is a diagram showing a received waveform including multiple wave components of a reference signal. FIG. 7 is a diagram showing another received waveform including multiple wave components of the reference signal. 1 ... Transmission signal generating section, 2 ... Transmission section, 3 ... Transmission antenna, 4 ... Reception antenna, 5 ... Reception section, 6 ...
Measuring unit, 7 ... Radio wave propagation path, 8 ... Reference signal, 8 '...
… Reception reference signal, 9 …… Measurement signal, 9 (0) …… Main wave signal,
9 (1) , 9 (2) , 9 (3) …… Multiple wave signal, 10 …… Multiple wave component of the reference signal.
Claims (1)
伝搬路を含む電波伝搬通路を経由して伝搬する信号の遅
延特性および振幅特性を測定する電波伝搬特性測定方法
において、 送信側では、受信側で実質的に一定の振幅が得られる程
度にパルス幅の長い基準信号と、上記複数の伝搬路の長
さにより生じる遅延時間差に比較して短いパルス幅の測
定信号とを被測定周波数により振幅変調して送信し、 受信側では、各伝搬路を経由して到来した受信測定信号
の振幅を上記基準信号の受信振幅値により補正して振幅
特性を求め、上記受信測定信号の時間差から遅延特性を
求める ことを特徴とする電波伝搬特性測定方法。1. A radio wave propagation characteristic measuring method for measuring a delay characteristic and an amplitude characteristic of a signal propagating through a radio wave propagation path including a plurality of propagation paths generated by reflection, scattering or diffraction. Amplitude modulation of a reference signal with a long pulse width to obtain a substantially constant amplitude and a measurement signal with a short pulse width compared to the delay time difference caused by the lengths of the above multiple propagation paths with the measured frequency. Then, on the receiving side, the amplitude of the received measurement signal arriving via each propagation path is corrected by the received amplitude value of the reference signal to obtain the amplitude characteristic, and the delay characteristic is calculated from the time difference of the received measurement signal. A method for measuring the characteristics of radio wave propagation, which is characterized by finding.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP62108524A JPH0681106B2 (en) | 1987-05-01 | 1987-05-01 | Radio wave propagation characteristics measurement method |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP62108524A JPH0681106B2 (en) | 1987-05-01 | 1987-05-01 | Radio wave propagation characteristics measurement method |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS63274231A JPS63274231A (en) | 1988-11-11 |
| JPH0681106B2 true JPH0681106B2 (en) | 1994-10-12 |
Family
ID=14486987
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP62108524A Expired - Fee Related JPH0681106B2 (en) | 1987-05-01 | 1987-05-01 | Radio wave propagation characteristics measurement method |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0681106B2 (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US5680142A (en) * | 1995-11-07 | 1997-10-21 | Smith; David Anthony | Communication system and method utilizing an antenna having adaptive characteristics |
-
1987
- 1987-05-01 JP JP62108524A patent/JPH0681106B2/en not_active Expired - Fee Related
Also Published As
| Publication number | Publication date |
|---|---|
| JPS63274231A (en) | 1988-11-11 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| US4443801A (en) | Direction finding and frequency identification method and apparatus | |
| CN103248384B (en) | Antenna test method and antenna test system based on wireless pulse technology | |
| EP2788788A1 (en) | Method of determining distance and speed of fmcw radar terminals | |
| CN104215954B (en) | Networking method for stepping variable-frequency radar communication integration | |
| US2502454A (en) | Method and means for improving signal to noise ratio of selected pulse signals | |
| US3596182A (en) | Multipath delay and correlation bandwidth analyzer | |
| US6049720A (en) | Link delay calculation and compensation system | |
| US2714205A (en) | Radar apparatus for distinguishing between moving and stationary objects | |
| JPS5916229B2 (en) | Data transfer method and device between two stations | |
| JP2000115087A (en) | Delay profile measurement device | |
| RU2146833C1 (en) | Method for synchronization of time scales | |
| CN110376576B (en) | Multi-base cooperative radio detection system and detection method | |
| JPH0681106B2 (en) | Radio wave propagation characteristics measurement method | |
| JP4138059B2 (en) | Spectrum analyzer | |
| JP2555289B2 (en) | Radio wave propagation characteristic measuring device | |
| JP3474942B2 (en) | Positioning system | |
| US4035802A (en) | Method and apparatus for wind measurement | |
| JP2001183447A (en) | Range finding method and device | |
| JP2953507B2 (en) | Transmission line amplitude characteristic measurement device | |
| JPH05264729A (en) | Range finder | |
| JP2523766B2 (en) | Phase difference measurement method | |
| JP4000321B2 (en) | Distance measuring method and distance measuring method | |
| JPS60213877A (en) | Ultrasonic distance measuring apparatus | |
| GB1330970A (en) | Distance measurement systems | |
| JP2581417B2 (en) | Bistatic radar |
Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| LAPS | Cancellation because of no payment of annual fees |