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JP4485285B2 - Moving speed measuring method and moving speed measuring method - Google Patents
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JP4485285B2 - Moving speed measuring method and moving speed measuring method - Google Patents

Moving speed measuring method and moving speed measuring method Download PDF

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JP4485285B2
JP4485285B2 JP2004235108A JP2004235108A JP4485285B2 JP 4485285 B2 JP4485285 B2 JP 4485285B2 JP 2004235108 A JP2004235108 A JP 2004235108A JP 2004235108 A JP2004235108 A JP 2004235108A JP 4485285 B2 JP4485285 B2 JP 4485285B2
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frequency shift
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JP2006053054A (en
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豪藏 鹿毛
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東京レーダー株式会社
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この発明は,移動通信の分野において,移動局と固定局の間,又は,移動局間の相対移動速度を,電波を用いて測定するためのものである。   The present invention is for measuring the relative movement speed between a mobile station and a fixed station or between mobile stations using radio waves in the field of mobile communications.

相手局と自局の間の相対移動速度の測定には,(1)相手局から送信された電波を受信して,そのときのフェージングの変動回数(受信信号が平均受信レベルと交差する回数)を測定する方法(例えば,特許文献1参照),(2)受信信号から相手局と自局のキャリア周波数の差を測定しておき,そのキャリア周波数の差の「広がり幅」をもとに移動速度を求める方法(例えば,同じ特許文献1参照)とが考えられている。
特開平11−98071号公報
To measure the relative movement speed between the partner station and the own station, (1) Receive radio waves transmitted from the partner station, and the number of fading fluctuations at that time (number of times the received signal crosses the average reception level) (2) Measure the carrier frequency difference between the partner station and the local station from the received signal, and move based on the "spread width" of the carrier frequency difference. A method for obtaining the speed (for example, refer to the same Patent Document 1) is considered.
JP-A-11-98071

上記(1)のフェージングの変動回数を測定する方法は,伝搬環境によってフェージングの起こり方が異なり,例えば,マルチパスが多い大都市で車の往来の激しい所とマルチパスが少ない郊外地で車があまり来ない所では,明らかに変動回数に差があり,そのために,フェージングの変動回数をもとにした相対移動速度の測定には,大きな測定誤差を伴うものであった。   The method of measuring the number of fading fluctuations in (1) above differs in the way fading occurs depending on the propagation environment. For example, in a large city with many multipaths, a car can be used in a suburban area where there is a lot of traffic and where there are few multipaths. Where there is not much frequency, there is clearly a difference in the number of fluctuations. Therefore, the measurement of relative movement speed based on the number of fluctuations in fading involves a large measurement error.

他方(2)の受信信号から相手局と自局のキャリア周波数の差を測定する方法は,どの程度ドップラー効果で周波数がシフトしたかを測定するために,高安定なクリスタルが必要であり,それでも実現性に課題があった。例えば,1〜2GHz程度のキャリアを有する携帯電話システムでは,時速60km/hで端末が移動する場合,最大ドップラー周波数として,
d =キャリア周波数×無線局の相対速度/電波伝搬速度
=(1〜2)×109 ×60/(60×60×300000)
=56〜111Hz
程度になる。
On the other hand, the method of measuring the difference between the carrier frequency of the partner station and the own station from the received signal in (2) requires a highly stable crystal to measure how much the frequency has shifted due to the Doppler effect. There was a problem in feasibility. For example, in a mobile phone system having a carrier of about 1 to 2 GHz, when the terminal moves at a speed of 60 km / h, the maximum Doppler frequency is
f d = carrier frequency × radio station relative speed / radio wave propagation speed = (1-2) × 10 9 × 60 / (60 × 60 × 300000)
= 56-111Hz
It will be about.

しかしながら,0.1×10-6程度の高安定度のクリスタルでも,1〜2GHz×0.1×10-6=100〜200Hz程度の周波数誤差を伴うため,クリスタルの周波数がシフトしたのかドップラー効果でシフトしたのかの区別がつかず,ドップラー周波数の測定が困難であった。 However, 0.1 at high stability crystal of about × 10 -6, since with frequency error of approximately 1~2GHz × 0.1 × 10 -6 = 100~200Hz , the or Doppler effect frequency of the crystal is shifted It was difficult to measure the Doppler frequency.

そこで,この方法では,絶えず変動する受信周波数の広がり幅から,ドップラー効果による周波数シフトを求める方法が考えられるが,この場合にも,電波伝搬環境によってドップラー効果の起こり方が異なるため,測定誤差が大きくなって,やはり移動速度を精度よく求めることは困難であった。特に,この方法は,電波が一方向だけから到来するような場合には,一方向に周波数がシフトしたままで,広がり幅の測定ができないため,ドップラー効果による周波数の測定が不可能であった。   Therefore, in this method, a method of obtaining the frequency shift due to the Doppler effect from the continuously changing frequency of the received frequency can be considered. However, in this case as well, the measurement error is different because the Doppler effect occurs depending on the radio wave propagation environment. As it became larger, it was difficult to accurately determine the moving speed. In particular, this method cannot measure the frequency by the Doppler effect because the spread width cannot be measured while the frequency is shifted in one direction when the radio wave comes from only one direction. .

また,上記(1)及び(2)の方法は,ともにフェージングの影響を取り除いて,十分な測定精度を得るまでに,非常に長い時間を必要とするものであった。   Further, the methods (1) and (2) both require a very long time before the influence of fading is removed and sufficient measurement accuracy is obtained.

本発明は,従来の移動速度測定方法の問題点を解決して,クリスタルの安定度に影響されずにドップラー効果による周波数シフトの値を正確に求めることができる相対移動速度の測定方法及び測定方式の提供を目的とするものである。   The present invention solves the problems of the conventional moving speed measuring method, and measures and measures the relative moving speed capable of accurately obtaining the value of the frequency shift due to the Doppler effect without being affected by the stability of the crystal. It is intended to provide.

本発明は,上記課題を解決し,限られた周波数帯域において,しかも単調な波形(例えば,正弦波)で,移動局と固定局の間,あるいは移動局間の相対的な移動速度の測定を可能にするものである。このため,本発明は,周波数の異なる2つの波を送信し,相手局において2つの波を受信すると,それぞれ周波数シフトして折り返し,折り返してきた2つの波と相手局へ送信した2つの波を用いて,相手局で周波数シフト時に付加された周波数の不確定成分の影響を受けないように相殺した新たな2つの波を生成し,このとき,新たな2つの波の周波数差はドップラー効果による影響分だけとなるようにして,それらの周波数差を測定することを最も主要な特徴とする。   The present invention solves the above problems, and measures the relative movement speed between a mobile station and a fixed station or between mobile stations in a limited frequency band and with a monotonous waveform (for example, a sine wave). It is what makes it possible. Therefore, according to the present invention, when two waves having different frequencies are transmitted and the two waves are received at the other station, the two waves returned by the frequency shift are returned, and the two waves transmitted to the other station are returned. To generate two new waves that cancel each other so that they are not affected by the frequency uncertainty component added at the time of frequency shift at the other station. At this time, the frequency difference between the two new waves is due to the Doppler effect. The most important feature is to measure the frequency difference between the affected parts.

図1は,本発明の概要を説明するための図である。本発明においては,無線局1の第1の発振手段101から周波数f1 の第1の波を発振して,第2の発振手段102から周波数f2 (f2 ≠f1 )の第2の波を発振して,送信手段103からそれぞれの波を無線局2に送信する。 FIG. 1 is a diagram for explaining the outline of the present invention. In the present invention, the first oscillating means 101 of the radio station 1 oscillates a first wave of frequency f 1, the second oscillating means 102 frequency f 2 second of (f 2 ≠ f 1) Waves are oscillated and each wave is transmitted from the transmission means 103 to the radio station 2.

無線局2の受信手段201は,第1の波及び第2の波を受信する。そして,周波数シフト手段202は,それぞれの波の周波数を所定の周波数シフト用の波によりシフトする。この周波数シフト手段202による周波数の処理により,第1の波から周波数f3 の第3の波が生成され,第2の波から周波数f4 (f4 ≠f3 )の第4の波が生成される。送信手段203は,生成された第3の波及び第4の波を無線局1に送信する。 The receiving means 201 of the radio station 2 receives the first wave and the second wave. Then, the frequency shift means 202 shifts the frequency of each wave by a predetermined frequency shift wave. By the frequency processing by the frequency shift means 202, a third wave having the frequency f 3 is generated from the first wave, and a fourth wave having the frequency f 4 (f 4 ≠ f 3 ) is generated from the second wave. Is done. The transmission unit 203 transmits the generated third wave and fourth wave to the radio station 1.

周波数シフト手段202によって周波数f1 ,f2 の波をシフトするのは,送信手段203によって無線局2から無線局1へ送信する波が,無線局2の受信手段201によって受信され,無線局1からの波と混同してしまわないようにするためである。 The frequency shift means 202 shifts the waves having the frequencies f 1 and f 2 because the wave transmitted from the radio station 2 to the radio station 1 by the transmission means 203 is received by the reception means 201 of the radio station 2 and the radio station 1 This is so as not to be confused with the wave from.

無線局1の受信手段104が第3の波及び第4の波を受信すると,周波数シフト手段105は,第1の波と第2の波と第3の波と第4の波の,相異なる2組の2つの波を用いて,それぞれ周波数をシフトすることにより,周波数差が第1の無線局と第2の無線局間の相対移動速度に起因するドップラー効果で決められる第5の波と第6の波を生成する。この第5の波と第6の波の生成方法としては,次のいずれを用いてもよい。   When the receiving means 104 of the wireless station 1 receives the third wave and the fourth wave, the frequency shifting means 105 is different between the first wave, the second wave, the third wave, and the fourth wave. By shifting the frequency using two sets of two waves, a fifth wave whose frequency difference is determined by the Doppler effect due to the relative moving speed between the first radio station and the second radio station; A sixth wave is generated. Any of the following may be used as a method of generating the fifth wave and the sixth wave.

(1)第1の波と第2の波を入力して周波数をシフトする周波数シフト手段により第5の波を生成し,第3の波と第4の波を入力して周波数をシフトする他の周波数シフト手段により第6の波を生成する。   (1) The fifth wave is generated by the frequency shift means for shifting the frequency by inputting the first wave and the second wave, and the frequency is shifted by inputting the third wave and the fourth wave. The sixth wave is generated by the frequency shift means.

(2)第1の波と第3の波を入力して周波数をシフトする周波数シフト手段により第5の波を生成し,第2の波と第4の波を入力して周波数をシフトする他の周波数シフト手段により第6の波を生成する。   (2) The fifth wave is generated by the frequency shift means for shifting the frequency by inputting the first wave and the third wave, and the frequency is shifted by inputting the second wave and the fourth wave. The sixth wave is generated by the frequency shift means.

(3)第1の波と第4の波を入力して周波数をシフトする周波数シフト手段により第5の波を生成し,第2の波と第3の波を入力して周波数をシフトする他の周波数シフト手段により第6の波を生成する。   (3) The fifth wave is generated by the frequency shift means for shifting the frequency by inputting the first wave and the fourth wave, and the frequency is shifted by inputting the second wave and the third wave. The sixth wave is generated by the frequency shift means.

上記(1)〜(3)のいずれの方法を用いても,無線局2で周波数シフト手段202によって周波数シフト時に付加された周波数の不確定成分の影響を受けないように相殺した新たな2つの波を生成できる。しかも,このとき,第5の波と第6の波の周波数差はドップラー効果による影響分だけとなるようにして,それらの周波数差を測定することが可能である。   Even if any one of the above methods (1) to (3) is used, two new offsets are made so as not to be affected by the frequency indeterminate component added at the time of frequency shift by the frequency shift means 202 in the radio station 2. Can generate waves. In addition, at this time, it is possible to measure the frequency difference between the fifth wave and the sixth wave so that the frequency difference is only an influence due to the Doppler effect.

測定手段106は,生成された第5の波と第6の波の周波数差に基づいて,無線局1と無線局2の間の相対移動速度を求める。   The measuring means 106 obtains the relative moving speed between the radio station 1 and the radio station 2 based on the generated frequency difference between the fifth wave and the sixth wave.

本発明は,自局と相手局のキャリア周波数の安定度に関係なく,ドップラー効果によって周波数がシフトした分を直接求める方法であるから,一方向からのみ連続して到来するような波であっても,短時間で正確な測定が可能になる。特に,1〜2GHz程度以上の,キャリア周波数が高く,ドップラー効果によってシフトした周波数の値とキャリア周波数そのものの安定度が不十分なためにシフトした周波数の値とが同程度であっても,本発明はなんら問題なく,ドップラー効果の影響によって周波数のシフトした分を測定することが可能である。   Since the present invention is a method for directly obtaining the frequency shift due to the Doppler effect regardless of the stability of the carrier frequency of the local station and the counterpart station, it is a wave that arrives continuously only from one direction. However, accurate measurement is possible in a short time. In particular, even if the carrier frequency is about 1 to 2 GHz or higher and the frequency value shifted by the Doppler effect and the frequency value shifted because the stability of the carrier frequency itself is insufficient, The invention can measure the frequency shift due to the influence of the Doppler effect without any problem.

本発明は,単調な周期性信号のドップラー効果を測定する方法を用いているため,周波数帯域を広げることなく,電波で直接,移動局と固定局,あるいは移動局間の相対移動速度の測定が可能であるという効果がある。   Since the present invention uses a method for measuring the Doppler effect of a monotonic periodic signal, it is possible to directly measure the relative moving speed between a mobile station and a fixed station or a mobile station by radio waves without widening the frequency band. There is an effect that it is possible.

〔第1の実施の形態〕
本発明の第1の実施の形態は,第1の無線局と第2の無線局の間の相対移動速度を測定する方式であって,第1の無線局と第2の無線局は,それぞれ以下に述べる手段を備える。
[First Embodiment]
The first embodiment of the present invention is a method for measuring the relative movement speed between a first radio station and a second radio station, and the first radio station and the second radio station are respectively Means described below are provided.

第1の無線局は,
第1の波を発振する第1の発振手段と,
第2の波を発振する第2の発振手段と,
第1の波を電波として送信する第1の送信手段と,
第2の波を電波として送信する第2の送信手段とを備え,
第1の波と第2の波を第2の無線局へ送信する。
The first radio station
First oscillating means for oscillating a first wave;
A second oscillating means for oscillating a second wave;
First transmission means for transmitting the first wave as a radio wave;
Second transmitting means for transmitting the second wave as a radio wave,
The first wave and the second wave are transmitted to the second radio station.

第2の無線局は,
送信された第1の波を受信する第1の受信手段と,
送信された第2の波を受信する第2の受信手段と,
周波数シフト用の波を発振する第3の発振手段と,
第1の受信手段で受信した第1の波と周波数シフト用の波を入力して,周波数をシフトして第3の波を出力する第1の周波数シフト手段と,
第2の受信手段で受信した第2の波と周波数シフト用の波を入力して,周波数をシフトして第4の波を出力する第2の周波数シフト手段と,
第3の波を送信する第3の送信手段と,
第4の波を送信する第4の送信手段とを備え,
第3の波と第4の波を第1の無線局へ送信する。
The second radio station
First receiving means for receiving the transmitted first wave;
Second receiving means for receiving the transmitted second wave;
A third oscillation means for oscillating a frequency shift wave;
A first frequency shift means for inputting a first wave received by the first receiving means and a wave for frequency shift, shifting the frequency and outputting a third wave;
A second frequency shift means for inputting a second wave and a frequency shift wave received by the second reception means, shifting the frequency and outputting a fourth wave;
A third transmission means for transmitting a third wave;
A fourth transmission means for transmitting the fourth wave,
The third wave and the fourth wave are transmitted to the first radio station.

さらに,第1の無線局は,
第3の波を受信する第3の受信手段と,
第4の波を受信する第4の受信手段と,
第1の発振手段から得られた第1の波,第2の発振手段から得られた第2の波,第3の受信手段から得られた第3の波,及び第4の受信手段から得られた第4の波を入力して,それぞれの周波数をシフトするマルチ周波数シフト手段と,
マルチ周波数シフト手段の処理結果に従って,第1の無線局と第2の無線局の間の相対的移動によって生じるドップラー効果による周波数シフトを測定するドップラー周波数シフト測定手段と,
測定したドップラー周波数シフトを相対移動速度に変換する変換手段を備え,
第1の無線局と第2の無線局の相対移動速度を測定する。
Furthermore, the first radio station
Third receiving means for receiving a third wave;
A fourth receiving means for receiving a fourth wave;
Obtained from the first wave obtained from the first oscillating means, the second wave obtained from the second oscillating means, the third wave obtained from the third receiving means, and the fourth receiving means. Multi-frequency shift means for inputting the received fourth wave and shifting the respective frequencies;
Doppler frequency shift measuring means for measuring a frequency shift due to the Doppler effect caused by relative movement between the first radio station and the second radio station according to the processing result of the multi-frequency shift means;
A conversion means for converting the measured Doppler frequency shift into a relative movement speed;
The relative moving speed between the first radio station and the second radio station is measured.

〔第2の実施の形態〕
本発明の第2の実施の形態は,上記第1の実施の形態において,
第1の無線局における前記マルチ周波数シフト手段は,
第3の受信手段で受信した第3の波と第4の受信手段で受信した第4の波を入力して,周波数をシフトする第3の周波数シフト手段と,
第1の発振手段から得られた第1の波と第2の発振手段から得られた第2の波を入力して,周波数をシフトする第4の周波数シフト手段とを備え,
前記ドップラー周波数シフト測定手段は,
第3の周波数シフト手段出力と第4の周波数シフト手段出力を入力してドップラー周波数シフトを取り出すための周波数シフト抽出手段を備える。
[Second Embodiment]
The second embodiment of the present invention is the same as the first embodiment described above.
The multi-frequency shift means in the first radio station is:
Third frequency shifting means for inputting the third wave received by the third receiving means and the fourth wave received by the fourth receiving means and shifting the frequency;
A fourth frequency shift means for inputting the first wave obtained from the first oscillation means and the second wave obtained from the second oscillation means and shifting the frequency;
The Doppler frequency shift measuring means is:
Frequency shift extraction means for taking out the Doppler frequency shift by inputting the output of the third frequency shift means and the output of the fourth frequency shift means is provided.

〔第3の実施の形態〕
また,本発明の第3の実施の形態は,上記第1の実施の形態において,
第1の無線局における前記マルチ周波数シフト手段は,
第3の受信手段で受信した第3の波と第1の発振手段から得られた第1の波を入力して,周波数をシフトする第5の周波数シフト手段と,
第4の受信手段で受信した第4の波と第2の発振手段から得られた第2の波を入力して,周波数をシフトする第6の周波数シフト手段とを備え,
前記ドップラー周波数シフト測定手段は,
第5の周波数シフト手段出力と第6の周波数シフト手段出力を入力してドップラー周波数シフトを取り出すための周波数シフト抽出手段を備える。
[Third Embodiment]
The third embodiment of the present invention is the same as the first embodiment described above.
The multi-frequency shift means in the first radio station is:
A fifth frequency shift means for shifting the frequency by inputting the third wave received by the third receiving means and the first wave obtained from the first oscillation means;
A fourth frequency shift means for inputting the fourth wave received by the fourth reception means and the second wave obtained from the second oscillation means and shifting the frequency;
The Doppler frequency shift measuring means is:
Frequency shift extracting means for taking out the Doppler frequency shift by inputting the outputs of the fifth frequency shift means and the sixth frequency shift means is provided.

〔第4の実施の形態〕
また,本発明の第4の実施の形態は,上記第1の実施の形態において,
第1の無線局における前記マルチ周波数シフト手段は,
第3の受信手段で受信した第3の波と第2の発振手段から得られた第2の波を入力して,周波数をシフトする第7の周波数シフト手段と,
第4の受信手段で受信した第4の波と第1の発振手段から得られた第1の波を入力して,周波数をシフトする第8の周波数シフト手段とを備え,
前記ドップラー周波数シフト測定手段は,
第7の周波数シフト手段出力と第8の周波数シフト手段出力を入力してドップラー周波数シフトを取り出すための周波数シフト抽出手段を備える。
[Fourth Embodiment]
The fourth embodiment of the present invention is the same as the first embodiment described above.
The multi-frequency shift means in the first radio station is:
A seventh frequency shift means for inputting the third wave received by the third receiving means and the second wave obtained from the second oscillating means and shifting the frequency;
An eighth frequency shift means for inputting the fourth wave received by the fourth reception means and the first wave obtained from the first oscillation means and shifting the frequency;
The Doppler frequency shift measuring means is:
Frequency shift extracting means for taking out the Doppler frequency shift by inputting the outputs of the seventh frequency shift means and the eighth frequency shift means is provided.

〔第5の実施の形態〕
また,本発明の第5の実施の形態は,上記第1〜第4の実施の形態において,
第1の無線局の第1の送信手段と第2の送信手段とを共通に使用する第1の共通送信手段を設け,第1の波と第2の波を合成して,第1の共通送信手段によって送信する。
[Fifth Embodiment]
The fifth embodiment of the present invention is the same as the first to fourth embodiments described above.
A first common transmission unit that uses the first transmission unit and the second transmission unit of the first wireless station in common is provided, and the first common wave and the second wave are combined to form a first common Transmit by transmission means.

〔第6の実施の形態〕
また,本発明の第6の実施の形態は,上記第1〜第5の実施の形態において,
第2の無線局の第1の受信手段と第2の受信手段とを共通に使用する第1の共通受信手段を設け,第1の無線局から送信された第1の波と第2の波を第1の共通受信手段によって受信し,その出力を,分離して使用する。
[Sixth Embodiment]
The sixth embodiment of the present invention is the same as the first to fifth embodiments described above.
First common receiving means for commonly using the first receiving means and the second receiving means of the second wireless station is provided, and the first wave and the second wave transmitted from the first wireless station are provided. Are received by the first common receiving means, and their outputs are used separately.

〔第7の実施の形態〕
また,本発明の第7の実施の形態は,上記第1〜第6の実施の形態において,
第2の無線局の第3の送信手段と第4の送信手段とを共通に使用する第2の共通送信手段を設け,第3の波と第4の波を合成して,第2の共通送信手段によって送信する。
[Seventh Embodiment]
The seventh embodiment of the present invention is the same as the first to sixth embodiments described above.
A second common transmission unit that uses the third transmission unit and the fourth transmission unit of the second radio station in common is provided, and the third wave and the fourth wave are combined to form a second common Transmit by transmission means.

〔第8の実施の形態〕
また,本発明の第8の実施の形態は,上記第1〜第7の実施の形態において,
第1の無線局の第3の受信手段と第4の受信手段とを共通に使用する第2の共通受信手段を設け,第3の波と第4の波を第2の共通受信手段によって受信し,その出力を,分離して使用する。
[Eighth Embodiment]
The eighth embodiment of the present invention is the same as the first to seventh embodiments described above.
A second common receiving means for commonly using the third receiving means and the fourth receiving means of the first radio station is provided, and the third wave and the fourth wave are received by the second common receiving means. The output is used separately.

以下,図面を参照しながら,お互いに移動している無線局1と無線局2について,電波のドップラー効果を測定することにより,無線局1と無線局2の相対移動速度を測定する本発明の実施例について説明する。   Hereinafter, the relative movement speed of the radio station 1 and the radio station 2 is measured by measuring the Doppler effect of the radio wave for the radio station 1 and the radio station 2 moving with each other with reference to the drawings. Examples will be described.

図2は,本発明の実施例1を示す図である。無線局1と無線局2は相対移動速度Vdで移動しているものとする。無線局1においては,周波数f1 の波を発振する発振器3と周波数f2 の波を発振する発振器4がある。それぞれの発振器出力は,発振器3の出力が,増幅器5とアンテナ6からなる第1の送信機より送信されて,発振器4の出力が,増幅器7とアンテナ8からなる第2の送信機より送信される。ここで,
・アンテナ6から送信される電波の周波数はf1
・アンテナ8から送信される電波の周波数はf2
である。
FIG. 2 is a diagram showing Example 1 of the present invention. It is assumed that the radio station 1 and the radio station 2 are moving at the relative movement speed Vd. The radio station 1 includes an oscillator 3 that oscillates a wave having a frequency f 1 and an oscillator 4 that oscillates a wave having a frequency f 2 . The output of the oscillator 3 is transmitted from the first transmitter including the amplifier 5 and the antenna 6, and the output of the oscillator 4 is transmitted from the second transmitter including the amplifier 7 and the antenna 8. The here,
The frequency of the radio wave transmitted from the antenna 6 is f 1
The frequency of the radio wave transmitted from the antenna 8 is f 2
It is.

無線局2において,アンテナ6から送信された波は,アンテナ9,受信増幅器10,帯域通過フィルタ11からなる第1の受信機により受信され,他方,アンテナ8から送信された波は,アンテナ12,受信増幅器13,帯域通過フィルタ14からなる第2の受信機により受信される。このとき,それぞれのアンテナで受信する波はドップラー効果の影響を受けてシフトしており,
・アンテナ9で受信した電波の周波数はf1 +fd1
・アンテナ12で受信した電波の周波数はf2 +fd2
である。
In the radio station 2, the wave transmitted from the antenna 6 is received by the first receiver including the antenna 9, the receiving amplifier 10, and the band pass filter 11, while the wave transmitted from the antenna 8 is the antenna 12, The signal is received by the second receiver comprising the receiving amplifier 13 and the band pass filter 14. At this time, the wave received by each antenna is shifted under the influence of the Doppler effect,
・ The frequency of the radio wave received by the antenna 9 is f 1 + f d1 ,
The frequency of the radio wave received by the antenna 12 is f 2 + f d2 ,
It is.

ここで,fd1,fd2はドップラー効果によってシフトした周波数の値であり,電波の伝搬速度を光速cとすると,
d1=Vd×f1 /c …(1)
d2=Vd×f2 /c …(2)
である。
Here, f d1 and f d2 are the values of the frequency shifted by the Doppler effect, and the propagation speed of the radio wave is the speed of light c.
f d1 = Vd × f 1 / c (1)
f d2 = Vd × f 2 / c (2)
It is.

本発明の実施例では,発振器15で周波数シフト用の波(周波数Δf)を発振させておき,それぞれ受信した波を周波数シフト手段16及び19によって周波数をシフトする。ここでは,説明を簡単にするために,始めに,f1 >f2 >Δf>0 の場合について述べる。 In the embodiment of the present invention, a frequency shift wave (frequency Δf) is oscillated by the oscillator 15, and the frequency of the received waves is shifted by the frequency shift means 16 and 19. Here, in order to simplify the description, a case where f 1 > f 2 >Δf> 0 is described first.

周波数シフト手段16は,ミキサー17と低域通過フィルタ18から構成され,帯域通過フィルタ11の出力の周波数について,減算する方向(MIX−DOWN:以下同様)にシフトする。すなわち,周波数シフト手段16の出力の周波数は,
3 =f1 +fd1−Δf …(3)
である。
The frequency shift means 16 includes a mixer 17 and a low-pass filter 18 and shifts the output frequency of the band-pass filter 11 in a subtracting direction (MIX-DOWN: the same applies hereinafter). That is, the frequency of the output of the frequency shift means 16 is
f 3 = f 1 + f d1 −Δf (3)
It is.

周波数シフト手段19はミキサー20と低域通過フィルタ21から構成され,帯域通過フィルタ14の出力の周波数について,減算する方向にシフトする。すなわち,周波数シフト手段19の出力の周波数は,
4 =f2 +fd2−Δf …(4)
である。
The frequency shift means 19 comprises a mixer 20 and a low-pass filter 21 and shifts the frequency of the output of the band-pass filter 14 in the subtracting direction. That is, the frequency of the output of the frequency shift means 19 is
f 4 = f 2 + f d2 −Δf (4)
It is.

周波数シフト手段16の出力は増幅器22,アンテナ23からなる第3の送信機によって送信され,他方,周波数シフト手段19の出力は増幅器24,アンテナ25からなる第4の送信機によって送信される。   The output of the frequency shift means 16 is transmitted by a third transmitter comprising an amplifier 22 and an antenna 23, while the output of the frequency shift means 19 is transmitted by a fourth transmitter comprising an amplifier 24 and an antenna 25.

ここで,
・アンテナ23から送信される電波の周波数はf3 =f1 +fd1−Δf …(5)
・アンテナ25から送信される電波の周波数はf4 =f2 +fd2−Δf …(6)
である。
here,
The frequency of the radio wave transmitted from the antenna 23 is f 3 = f 1 + f d1 −Δf (5)
The frequency of the radio wave transmitted from the antenna 25 is f 4 = f 2 + f d2 −Δf (6)
It is.

無線局1においては,アンテナ23から送信された波は,アンテナ26,受信増幅器27,帯域通過フィルタ28からなる第3の受信機により受信され,他方,アンテナ25から送信された波は,アンテナ29,受信増幅器30,帯域通過フィルタ31からなる第4の受信機により受信される。   In the radio station 1, the wave transmitted from the antenna 23 is received by a third receiver including the antenna 26, the receiving amplifier 27, and the band pass filter 28, while the wave transmitted from the antenna 25 is transmitted to the antenna 29. , Reception amplifier 30 and band-pass filter 31.

このとき,それぞれのアンテナで受信する波はドップラー効果の影響を受けてシフトしており,
・アンテナ26で受信した電波の周波数はf3 +fd3
・アンテナ29で受信した電波の周波数はf4 +fd4
である。
At this time, the wave received by each antenna is shifted under the influence of the Doppler effect,
The frequency of the radio wave received by the antenna 26 is f 3 + f d3 ,
・ The frequency of the radio wave received by the antenna 29 is f 4 + f d4 ,
It is.

ここで,fd3,fd4はドップラー効果によってシフトした周波数の値であり,
d3=Vd×f3 /c=(f1 +fd1−Δf)Vd/c …(7)
d4=Vd×f4 /c=(f2 +fd2−Δf)Vd/c …(8)
である。
Here, f d3 and f d4 are values of the frequency shifted by the Doppler effect,
f d3 = Vd × f 3 / c = (f 1 + f d1 −Δf) Vd / c (7)
f d4 = Vd × f 4 / c = (f 2 + f d2 −Δf) Vd / c (8)
It is.

無線局1では,発振器3で発振した周波数f1 の波と発振器4で発振した周波数f2 の波と帯域通過フィルタ28の出力の周波数f3 +fd3の波と帯域通過フィルタ31の出力の周波数f4 +fd4の波をマルチ周波数シフト手段32へ入力し,その結果を使って,無線局1と無線局2の相対移動速度を求める。 In the radio station 1, the wave of the frequency f 1 oscillated by the oscillator 3, the wave of the frequency f 2 oscillated by the oscillator 4, the wave of the frequency f 3 + f d3 of the output of the band pass filter 28, and the frequency of the output of the band pass filter 31. The wave of f 4 + f d4 is input to the multi-frequency shift means 32, and the relative movement speed between the radio station 1 and the radio station 2 is obtained using the result.

図2に示す実施例1の場合,マルチ周波数シフト手段32は,2つの周波数シフト手段33及び34からなる。周波数シフト手段33は,ミキサー35と低域通過フィルタ36からなり,帯域通過フィルタ28の出力の周波数と帯域通過フィルタ31の出力の周波数について,減算する方向にシフトする。   In the case of the first embodiment shown in FIG. 2, the multi-frequency shift means 32 includes two frequency shift means 33 and 34. The frequency shift means 33 includes a mixer 35 and a low-pass filter 36, and shifts the output frequency of the band-pass filter 28 and the output frequency of the band-pass filter 31 in the subtracting direction.

その結果,周波数シフト手段33の出力の周波数は,
5 =(f3 +fd3)−(f4 +fd4
=(f1 −f2 )+(f1 −f2 )(2+Vd/c)Vd/c …(9)
となる。
As a result, the frequency of the output of the frequency shift means 33 is
f 5 = (f 3 + f d3 ) − (f 4 + f d4 )
= (F 1 −f 2 ) + (f 1 −f 2 ) (2 + Vd / c) Vd / c (9)
It becomes.

周波数シフト手段34は,ミキサー37と低域通過フィルタ38からなり,周波数f1 の波と周波数f2 の波の差の周波数の波,
6 =f1 −f2 …(10)
を得る。
The frequency shift means 34 comprises a mixer 37 and a low-pass filter 38, and has a frequency wave that is the difference between the frequency f 1 wave and the frequency f 2 wave,
f 6 = f 1 −f 2 (10)
Get.

無線局間の相対移動速度の測定手段として,周波数シフト手段39及び速度表示手段42が使われる。まず,式(9)と式(10)とを比べると,周波数f5 と周波数f6 の差をとるとドップラー効果による影響分だけが残ることが分かる。そこで,実施例1では,この影響分を取り出すために,周波数シフト手段33の出力と周波数シフト手段34の出力を周波数シフト手段39へ入力している。 Frequency shift means 39 and speed display means 42 are used as means for measuring the relative movement speed between radio stations. First, comparing Equation (9) with Equation (10), it can be seen that if the difference between the frequency f 5 and the frequency f 6 is taken, only the influence due to the Doppler effect remains. Therefore, in the first embodiment, the output of the frequency shift means 33 and the output of the frequency shift means 34 are input to the frequency shift means 39 in order to extract this influence.

周波数シフト手段39は,ミキサー40と低域通過フィルタ41からなり,周波数f5 の波と周波数f6 の波の差の周波数の波,
7 =f5 −f6
=(f1 −f2 )(2+Vd/c)Vd/c …(11)
を得る。ここでは,ドップラー周波数シフト抽出手段として,周波数シフト手段39によって,f5 とf6 の差の周波数を求めたが,例えば,周波数カウンターを使って,それぞれf5 の周波数とf6 の周波数を求めて,演算手段によって,これらの差の周波数を求めても良い。他の実施例でも同様である。
The frequency shift means 39 is composed of a mixer 40 and a low-pass filter 41, and has a frequency wave that is the difference between the frequency f 5 wave and the frequency f 6 wave,
f 7 = f 5 −f 6
= (F 1 −f 2 ) (2 + Vd / c) Vd / c (11)
Get. Here, as the Doppler frequency shift extraction means, the frequency difference between f 5 and f 6 is obtained by the frequency shift means 39. For example, the frequency of f 5 and the frequency of f 6 are obtained by using a frequency counter, for example. Thus, the frequency of these differences may be obtained by a calculation means. The same applies to other embodiments.

速度表示手段42によって,周波数シフト手段39の出力の周波数を求めて,f7 ×c/{2(f1 −f2 )}なる演算を行い,表示することにより,次の測定結果を得る。
・相対移動速度の測定結果=Vd{1+Vd/(2c)}≒Vd …(12)
図2の本発明の実施例1では,周波数シフト手段16,19,33,34の周波数に関してシフトする極性は,いずれも減算する方向(MIX−DOWN)にシフトしたが,それぞれの周波数シフト手段でシフトする極性について,それ以外に複数の組み合わせが可能である。
The speed display means 42 obtains the frequency of the output of the frequency shift means 39, calculates f 7 × c / {2 (f 1 −f 2 )}, and displays it to obtain the next measurement result.
Measurement result of relative movement speed = Vd {1 + Vd / (2c)} ≈Vd (12)
In the first embodiment of the present invention shown in FIG. 2, the polarity of the frequency shift means 16, 19, 33, and 34 is shifted in the direction of subtraction (MIX-DOWN). Several other combinations of shifting polarity are possible.

1 >f2 >Δf>0の場合について,周波数シフト手段39の出力の周波数とそれぞれの周波数シフト手段の極性の関係例を表1に示す。「加算」は周波数の絶対値が大きくなる方向(MIX−UP)にシフトする意味であり,減算は周波数の絶対値が減少する方向(MIX−DOWN)にシフトする意味である。 Table 1 shows an example of the relationship between the frequency of the output of the frequency shift means 39 and the polarity of each frequency shift means for the case of f 1 > f 2 >Δf> 0. “Addition” means shifting in a direction in which the absolute value of the frequency increases (MIX-UP), and subtraction means shifting in a direction in which the absolute value of the frequency decreases (MIX-DOWN).

Figure 0004485285
Figure 0004485285

1 >Δf>f2 >0の場合について,周波数シフト手段39の出力の周波数とそれぞれの周波数シフト手段の極性の関係例を表2に示す。 Table 2 shows an example of the relationship between the frequency of the output of the frequency shift means 39 and the polarity of each frequency shift means in the case of f 1 >Δf> f 2 > 0.

Figure 0004485285
Figure 0004485285

Δf>f1 >f2 >0の場合について,周波数シフト手段39の出力の周波数とそれぞれの周波数シフト手段の極性の関係例を表3に示す。 Table 3 shows an example of the relationship between the output frequency of the frequency shift means 39 and the polarity of each frequency shift means when Δf> f 1 > f 2 > 0.

Figure 0004485285
Figure 0004485285

表1〜3を見ると,f7 の周波数は,(f1 +f2 )(2+Vd/c)Vd/cになる場合と,(f1 −f2 )(2+Vd/c)Vd/cになる場合とがある。相対移動速度を求めるには,前者の場合,f7 にc/{2(f1 +f2 )}をかけ,後者の場合,f7 にc/{2(f1 −f2 )}をかける。いずれも,Vd/cを十分小さい値と見て無視すれば,その演算結果は実用上Vdと等しくなることが分かる。 From Tables 1 to 3, the frequency of f 7 is (f 1 + f 2 ) (2 + Vd / c) Vd / c and (f 1 −f 2 ) (2 + Vd / c) Vd / c. There are cases. To determine the relative moving velocity, in the former case, multiplied by c / {2 (f 1 + f 2)} to f 7, in the latter case, applying a c / {2 (f 1 -f 2)} to f 7 . In any case, if Vd / c is regarded as a sufficiently small value and ignored, the calculation result is practically equal to Vd.

図3は,この発明の実施例2を示す図である。図2と図3の差異は,図2のマルチ周波数シフト手段32において,第1の波と第2の波(送信波どうし)をミキシングして得た波と,第3の波と第4の波(受信波どうし)をミキシングして得た波を比べてドップラー効果の影響を求めたが,図3ではマルチ周波数シフト手段43において,第1の波と第3の波(送信波と受信波)をミキシングして得た波と,第2の波と第4の波(もう一方の送信波と受信波)をミキシングして得た波を比べてドップラー効果の影響を測定する。   FIG. 3 is a diagram showing Embodiment 2 of the present invention. The difference between FIG. 2 and FIG. 3 is that, in the multi-frequency shift means 32 of FIG. 2, the wave obtained by mixing the first wave and the second wave (transmission waves), the third wave and the fourth wave The influence of the Doppler effect was obtained by comparing the waves obtained by mixing the waves (between the received waves). In FIG. 3, the first and third waves (transmitted wave and received wave) are obtained in the multi-frequency shift means 43. ) And a wave obtained by mixing the second wave and the fourth wave (the other transmission wave and reception wave) are measured to measure the influence of the Doppler effect.

図3の無線局1においても,図2の場合と同様に,アンテナ6及びアンテナ8から送信される波の周波数は,それぞれf1 及びf2 である。 Also in the radio station 1 of FIG. 3, the frequencies of the waves transmitted from the antenna 6 and the antenna 8 are f 1 and f 2 , respectively, as in the case of FIG.

図3の無線局2においては,それぞれの波がドップラー効果の影響を受けて受信され,図2の場合と同様に,
・アンテナ9で受信した電波の周波数はf1 +fd1
・アンテナ12で受信した電波の周波数はf2 +fd2
である。fd1とfd2は,それぞれ,式(1)及び式(2)で与えられる。
In the radio station 2 of FIG. 3, each wave is received under the influence of the Doppler effect, and as in the case of FIG.
・ The frequency of the radio wave received by the antenna 9 is f 1 + f d1 ,
The frequency of the radio wave received by the antenna 12 is f 2 + f d2 ,
It is. f d1 and f d2 are given by Equation (1) and Equation (2), respectively.

この場合も,説明を簡単にするために,始めは,f1 >f2 >Δf>0の場合について述べる。図3に示す本発明の実施例2においても,無線局2は図2の実施例1の場合と全く同様に,2つの周波数f1 +fd1とf2 +fd2とは,Δfだけ減算する方向にシフトして,
・アンテナ23から送信される電波の周波数はf3 =f1 +fd1−Δf …(13)
・アンテナ25から送信される電波の周波数はf4 =f2 +fd2−Δf …(14)
である。
Also in this case, in order to simplify the description, a case where f 1 > f 2 >Δf> 0 will be described first. Also in the second embodiment of the present invention shown in FIG. 3, the radio station 2 uses the same frequency as in the first embodiment of FIG. 2 to subtract the two frequencies f 1 + f d1 and f 2 + f d2 by Δf. Shift to
The frequency of the radio wave transmitted from the antenna 23 is f 3 = f 1 + f d1 −Δf (13)
The frequency of the radio wave transmitted from the antenna 25 is f 4 = f 2 + f d2 −Δf (14)
It is.

このとき,無線局1のそれぞれのアンテナ26及び29で受信する波はドップラー効果の影響を受けてシフトしており,
・アンテナ26で受信した電波の周波数はf3 +fd3
・アンテナ29で受信した電波の周波数はf4 +fd4
である。
At this time, the waves received by the respective antennas 26 and 29 of the radio station 1 are shifted under the influence of the Doppler effect,
The frequency of the radio wave received by the antenna 26 is f 3 + f d3 ,
・ The frequency of the radio wave received by the antenna 29 is f 4 + f d4 ,
It is.

ここで,fd3,fd4はドップラー効果によってシフトした周波数の値であり,
d3=Vd×f3 /c=(f1 +fd1−Δf)Vd/c …(15)
d4=Vd×f4 /c=(f2 +fd2−Δf)Vd/c …(16)
である。
Here, f d3 and f d4 are values of the frequency shifted by the Doppler effect,
f d3 = Vd × f 3 / c = (f 1 + f d1 −Δf) Vd / c (15)
f d4 = Vd × f 4 / c = (f 2 + f d2 −Δf) Vd / c (16)
It is.

無線局1では,発振器3で発振した周波数f1 の波と発振器4で発振した周波数f2 の波と帯域通過フィルタ28の出力の周波数f3 +fd3の波と帯域通過フィルタ31の出力の周波数f4 +fd4の波をマルチ周波数シフト手段43へ入力し,その結果を使って,無線局1と無線局2の相対移動速度を求める。 In the radio station 1, the wave of the frequency f 1 oscillated by the oscillator 3, the wave of the frequency f 2 oscillated by the oscillator 4, the wave of the frequency f 3 + f d3 of the output of the band pass filter 28, and the frequency of the output of the band pass filter 31. The wave of f 4 + f d4 is input to the multi-frequency shift means 43, and the relative movement speed between the radio station 1 and the radio station 2 is obtained using the result.

図3に示す実施例2の場合,マルチ周波数シフト手段43は,2つの周波数シフト手段44及び45からなる。周波数シフト手段44は,ミキサー46と低域通過フィルタ47からなり,帯域通過フィルタ28の出力の周波数と発振器3の出力の周波数f1 について,減算する方向にシフトする。その結果,周波数シフト手段44の出力の周波数は,
8 =f1 −(f3 +fd3) …(17)
となる。
In the case of the second embodiment shown in FIG. 3, the multi-frequency shift means 43 includes two frequency shift means 44 and 45. The frequency shift means 44 comprises a mixer 46 and a low-pass filter 47, and shifts the frequency of the output of the band-pass filter 28 and the frequency f 1 of the output of the oscillator 3 in the subtracting direction. As a result, the frequency of the output of the frequency shift means 44 is
f 8 = f 1 − (f 3 + f d3 ) (17)
It becomes.

周波数シフト手段45は,ミキサー48と低域通過フィルタ49からなり,帯域通過フィルタ31の出力の周波数と発振器4の出力の周波数f2 について,減算する方向にシフトする。その結果,周波数シフト手段45の出力の周波数は,
9 =f2 −(f4 +fd4) …(18)
となる。
The frequency shift means 45 comprises a mixer 48 and a low-pass filter 49, and shifts the frequency of the output of the band-pass filter 31 and the frequency f 2 of the output of the oscillator 4 in the subtracting direction. As a result, the frequency of the output of the frequency shift means 45 is
f 9 = f 2 − (f 4 + f d4 ) (18)
It becomes.

実施例2では,無線局間の相対移動速度の測定手段として,周波数シフト手段39及び速度表示手段42が使われる。周波数シフト手段39では,周波数シフト手段44の出力と周波数シフト手段45の出力を入力して,f8 とf9 の差を求めて,ドップラー効果の影響分を取り出している。 In the second embodiment, frequency shift means 39 and speed display means 42 are used as means for measuring the relative movement speed between radio stations. The frequency shift means 39 inputs the output of the frequency shift means 44 and the output of the frequency shift means 45, obtains the difference between f 8 and f 9 and extracts the influence of the Doppler effect.

10=f9 −f8
=(f1 −f2 )(2+Vd/c)Vd/c …(19)
を得る。
f 10 = f 9 −f 8
= (F 1 −f 2 ) (2 + Vd / c) Vd / c (19)
Get.

以下,実施例1の場合と同様に,速度表示手段42によって,周波数シフト手段39の出力の周波数を求めて,f10×c/{2(f1 −f2 )}なる演算を行い,表示することにより,次の測定結果を得る。
・相対移動速度の測定結果=Vd{1+Vd/(2c)}≒Vd …(20)
図3の本発明の実施例2では,周波数シフト手段16,19,44,45の周波数に関してシフトする極性は,いずれも減算する方向(MIX−DOWN)にシフトしたが,それぞれの周波数シフト手段でシフトする極性について,それ以外に複数の組み合わせが可能である。
Thereafter, as in the case of the first embodiment, the speed display means 42 obtains the frequency of the output of the frequency shift means 39, calculates f 10 × c / {2 (f 1 −f 2 )}, and displays it. By doing so, the following measurement results are obtained.
Measurement result of relative movement speed = Vd {1 + Vd / (2c)} ≈Vd (20)
In the second embodiment of the present invention shown in FIG. 3, the polarities shifted with respect to the frequencies of the frequency shift means 16, 19, 44, 45 are all shifted in the subtracting direction (MIX-DOWN). Several other combinations of shifting polarity are possible.

1 >f2 >Δf>0の場合について,周波数シフト手段39の出力の周波数とそれぞれの周波数シフト手段の極性の関係例を表4に示す。「加算」は周波数の絶対値が大きくなる方向(MIX−UP)にシフトする意味であり,減算は周波数の絶対値が減少する方向(MIX−DOWN)にシフトする意味である。 Table 4 shows an example of the relationship between the output frequency of the frequency shift means 39 and the polarity of each frequency shift means in the case of f 1 > f 2 >Δf> 0. “Addition” means shifting in a direction in which the absolute value of the frequency increases (MIX-UP), and subtraction means shifting in a direction in which the absolute value of the frequency decreases (MIX-DOWN).

Figure 0004485285
Figure 0004485285

1 >Δf>f2 >0の場合について,周波数シフト手段39の出力の周波数とそれぞれの周波数シフト手段の極性の関係例を表5に示す。 Table 5 shows an example of the relationship between the output frequency of the frequency shift means 39 and the polarity of each frequency shift means for the case of f 1 >Δf> f 2 > 0.

Figure 0004485285
Figure 0004485285

Δf>f1 >f2 >0の場合について,周波数シフト手段39の出力の周波数とそれぞれの周波数シフト手段の極性の関係例を表6に示す。 Table 6 shows an example of the relationship between the output frequency of the frequency shift means 39 and the polarity of each frequency shift means when Δf> f 1 > f 2 > 0.

Figure 0004485285
Figure 0004485285

表4〜6を見ると,実施例1と同様に,f10の周波数は,(f1 +f2 )(2+Vd/c)Vd/cになる場合と,(f1 −f2 )(2+Vd/c)Vd/cになる場合とがある。相対移動速度を求めるには,前者の場合,f10にc/{2(f1 +f2 )}をかけ,後者の場合,f10にc/{2(f1 −f2 )}をかける。いずれも,Vd/cを十分小さい値と見て無視すれば,その演算結果は実用上Vdと等しくなることが分かる。 As can be seen from Tables 4 to 6, as in Example 1, the frequency of f 10 is (f 1 + f 2 ) (2 + Vd / c) Vd / c, and (f 1 −f 2 ) (2 + Vd / c) Vd / c. To determine the relative moving velocity, in the former case, multiplied by c / {2 (f 1 + f 2)} to f 10, in the latter case, applying a c / {2 (f 1 -f 2)} to f 10 . In any case, if Vd / c is regarded as a sufficiently small value and ignored, the calculation result is practically equal to Vd.

図4は,この発明の実施例3を示す図である。図3の場合と同様に,無線局2の帯域通過フィルタ11と14の出力の周波数は,f1 +fd1とf2 +fd2(fd1とfd2は,それぞれ式(1)及び式(2)で与えられる。)であるが,周波数シフト手段50及び53において,2つの周波数f1 +fd1及びf2 +fd2はΔfだけ加算する方向にシフトされる。 FIG. 4 is a diagram showing Embodiment 3 of the present invention. Similarly to the case of FIG. 3, the frequencies of the outputs of the bandpass filters 11 and 14 of the radio station 2 are f 1 + f d1 and f 2 + f d2 (f d1 and f d2 are the expressions (1) and (2), respectively. In the frequency shift means 50 and 53, the two frequencies f 1 + f d1 and f 2 + f d2 are shifted in the direction of adding Δf.

周波数シフト手段50はミキサー51と高域通過フィルタ52から構成され,帯域通過フィルタ11の出力の周波数とΔfを加算する方向にシフトする。周波数シフト手段53はミキサー54と高域通過フィルタ55から構成され,帯域通過フィルタ14の出力の周波数とΔfについて,加算する方向にシフトする。その結果,
・アンテナ23から送信される電波の周波数はf3 =f1 +fd1+Δf …(21)
・アンテナ25から送信される電波の周波数はf4 =f2 +fd2+Δf …(22)
である。
The frequency shift means 50 is composed of a mixer 51 and a high-pass filter 52, and shifts in the direction of adding Δf to the output frequency of the band-pass filter 11. The frequency shift means 53 includes a mixer 54 and a high-pass filter 55, and shifts the output frequency of the band-pass filter 14 and Δf in the adding direction. as a result,
The frequency of the radio wave transmitted from the antenna 23 is f 3 = f 1 + f d1 + Δf (21)
The frequency of the radio wave transmitted from the antenna 25 is f 4 = f 2 + f d2 + Δf (22)
It is.

このとき,無線局1のそれぞれのアンテナ26及び29で受信する波はドップラー効果の影響を受けてシフトしており,
・アンテナ26で受信した電波の周波数はf3 +fd3
・アンテナ29で受信した電波の周波数はf4 +fd4
である。
At this time, the waves received by the respective antennas 26 and 29 of the radio station 1 are shifted under the influence of the Doppler effect,
The frequency of the radio wave received by the antenna 26 is f 3 + f d3 ,
・ The frequency of the radio wave received by the antenna 29 is f 4 + f d4 ,
It is.

ここで,fd3,fd4はドップラー効果によってシフトした周波数の値であり,
d3=Vd×f3 /c=(f1 +fd1+Δf)Vd/c …(23)
d4=Vd×f4 /c=(f2 +fd2+Δf)Vd/c …(24)
である。
Here, f d3 and f d4 are values of the frequency shifted by the Doppler effect,
f d3 = Vd × f 3 / c = (f 1 + f d1 + Δf) Vd / c (23)
f d4 = Vd × f 4 / c = (f 2 + f d2 + Δf) Vd / c (24)
It is.

無線局1では,発振器3で発振した周波数f1 の波と発振器4で発振した周波数f2 の波と帯域通過フィルタ28の出力の周波数f3 +fd3の波と帯域通過フィルタ31の出力の周波数f4 +fd4の波をマルチ周波数シフト手段56へ入力し,その結果を使って,無線局1と無線局2の相対移動速度を求める。 In the radio station 1, the wave of the frequency f 1 oscillated by the oscillator 3, the wave of the frequency f 2 oscillated by the oscillator 4, the wave of the frequency f 3 + f d3 of the output of the band pass filter 28, and the frequency of the output of the band pass filter 31. The wave of f 4 + f d4 is input to the multi-frequency shift means 56, and the relative movement speed between the radio station 1 and the radio station 2 is obtained using the result.

図4に示す実施例3の場合,マルチ周波数シフト手段56は,2つの周波数シフト手段57及び58からなる。周波数シフト手段57は,ミキサー59と高域通過フィルタ60からなり,帯域通過フィルタ28の出力の周波数と発振器4の出力の周波数f2 について,加算する方向にシフトする。その結果,周波数シフト手段57の出力の周波数は,
11=f2 +(f3 +fd3) …(25)
となる。
In the third embodiment shown in FIG. 4, the multi-frequency shift means 56 includes two frequency shift means 57 and 58. Frequency shifting means 57, a mixer 59 made of a high-pass filter 60, the frequency f 2 of the output frequency and the oscillator 4 of the output of the band pass filter 28 is shifted in the direction of addition. As a result, the frequency of the output of the frequency shift means 57 is
f 11 = f 2 + (f 3 + f d3 ) (25)
It becomes.

周波数シフト手段58は,ミキサー61と高域通過フィルタ62からなり,帯域通過フィルタ31の出力の周波数と発振器3の出力の周波数f1 について,加算する方向にシフトする。その結果,周波数シフト手段58の出力の周波数は,
12=f1 +(f4 +fd4) …(26)
となる。
The frequency shift means 58 includes a mixer 61 and a high-pass filter 62, and shifts the output frequency of the band-pass filter 31 and the frequency f 1 of the output of the oscillator 3 in the adding direction. As a result, the frequency of the output of the frequency shift means 58 is
f 12 = f 1 + (f 4 + f d4 ) (26)
It becomes.

実施例3でも,無線局間の相対移動速度の測定手段として,周波数シフト手段39及び速度表示手段42が使われる。周波数シフト手段39では,周波数シフト手段57の出力と周波数シフト手段58の出力を入力して,f11とf12の差を求めて,ドップラー効果の影響分を取り出している。周波数f11の波と周波数f12の波の差の周波数の波は,
13=f11−f12
=(f1 −f2 )(2+Vd/c)Vd/c …(27)
を得る。
Also in the third embodiment, frequency shift means 39 and speed display means 42 are used as means for measuring the relative movement speed between radio stations. The frequency shifting means 39 inputs the outputs of the frequency shifting means 58 of the frequency shifting means 57, and determines the difference between f 11 and f 12, is taken out the influence component of the Doppler effect. The wave of the frequency difference between the wave of frequency f 11 and the wave of frequency f 12 is
f 13 = f 11 −f 12
= (F 1 −f 2 ) (2 + Vd / c) Vd / c (27)
Get.

以下,実施例2の場合と同様に,速度表示手段42によって,周波数シフト手段39の出力の周波数を求めて,f13×c/{2(f1 −f2 )}なる演算を行い,表示することにより,次の測定結果を得る。
・相対移動速度の測定結果=Vd{1+Vd/(2c)}≒Vd …(20)
図4の本発明の実施例3では,周波数シフト手段50,53,57,58の周波数に関してシフトする極性は,いずれも加算する方向(MIX−UP)にシフトしたが,それぞれの周波数シフト手段でシフトする極性について,それ以外に複数の組み合わせが可能である。
Thereafter, as in the case of the second embodiment, the speed display means 42 obtains the frequency of the output of the frequency shift means 39, calculates f 13 × c / {2 (f 1 −f 2 )}, and displays it. By doing so, the following measurement results are obtained.
Measurement result of relative movement speed = Vd {1 + Vd / (2c)} ≈Vd (20)
In the third embodiment of the present invention shown in FIG. 4, the polarities of the frequency shift means 50, 53, 57, and 58 are shifted in the adding direction (MIX-UP). Several other combinations of shifting polarity are possible.

1 >f2 >Δf>0の場合について,周波数シフト手段39の出力の周波数とそれぞれの周波数シフト手段の極性の関係例を表7に示す。「加算」は周波数の絶対値が大きくなる方向(MIX−UP)にシフトする意味であり,減算は周波数の絶対値が減少する方向(MIX−DOWN)にシフトする意味である。 Table 7 shows an example of the relationship between the output frequency of the frequency shift means 39 and the polarity of each frequency shift means in the case of f 1 > f 2 >Δf> 0. “Addition” means shifting in a direction in which the absolute value of the frequency increases (MIX-UP), and subtraction means shifting in a direction in which the absolute value of the frequency decreases (MIX-DOWN).

Figure 0004485285
Figure 0004485285

1 >Δf>f2 >0の場合について,周波数シフト手段39の出力の周波数とそれぞれの周波数シフト手段の極性の関係例を表8に示す。 Table 8 shows an example of the relationship between the output frequency of the frequency shift means 39 and the polarity of each frequency shift means when f 1 >Δf> f 2 > 0.

Figure 0004485285
Figure 0004485285

Δf>f1 >f2 >0の場合について,周波数シフト手段39の出力の周波数とそれぞれの周波数シフト手段の極性の関係例を表9に示す。 Table 9 shows an example of the relationship between the frequency of the output of the frequency shift means 39 and the polarity of each frequency shift means when Δf> f 1 > f 2 > 0.

Figure 0004485285
Figure 0004485285

表7〜9を見ると,実施例1,実施例2と同様に,f13の周波数は,(f1 +f2 )(2+Vd/c)Vd/cになる場合と,(f1 −f2 )(2+Vd/c)Vd/cになる場合とがある。相対移動速度を求めるには,前者の場合,f13にc/{2(f1 +f2 )}をかけ,後者の場合,f13にc/{2(f1 −f2 )}をかける。いずれも,Vd/cを十分小さい値と見て無視すれば,その演算結果は実用上Vdと等しくなることが分かる。 As can be seen from Tables 7 to 9, the frequency of f 13 is (f 1 + f 2 ) (2 + Vd / c) Vd / c, and (f 1 −f 2 ), as in Examples 1 and 2. ) (2 + Vd / c) Vd / c. To determine the relative moving velocity, in the former case, multiplied by c / {2 (f 1 + f 2)} to f 13, in the latter case, applying a c / {2 (f 1 -f 2)} to f 13 . In any case, if Vd / c is regarded as a sufficiently small value and ignored, the calculation result is practically equal to Vd.

図5は,本発明の実施例4である。この実施例では,図2の第1の送信機と第2の送信機に相当する増幅器5,アンテナ6と増幅器7,アンテナ8を,図5の加算器63,及び増幅器64とアンテナ65からなる第1の共通送信手段で構成して,図2の第1の受信機と第2の受信機に相当するアンテナ9,受信増幅器10,帯域通過フィルタ11とアンテナ12,受信増幅器13,帯域通過フィルタ14を,アンテナ66,受信増幅器67,帯域通過フィルタ11,14からなる第1の共通受信手段で構成している。   FIG. 5 shows a fourth embodiment of the present invention. In this embodiment, the amplifier 5, the antenna 6, the amplifier 7 and the antenna 8 corresponding to the first transmitter and the second transmitter in FIG. 2 are composed of the adder 63, the amplifier 64 and the antenna 65 in FIG. The antenna 9, the reception amplifier 10, the bandpass filter 11 and the antenna 12, the reception amplifier 13, the bandpass filter corresponding to the first receiver and the second receiver of FIG. 14 is constituted by a first common receiving means comprising an antenna 66, a receiving amplifier 67, and bandpass filters 11 and 14.

さらに,図2の第3の送信機と第4の送信機に相当する増幅器22,アンテナ23と増幅器24,アンテナ25を,図5の加算器68,及び増幅器69とアンテナ70からなる第2の共通送信手段で構成しており,図2の第3の受信機と第4の受信機に相当するアンテナ26,受信増幅器27,帯域通過フィルタ28とアンテナ29,受信増幅器30,帯域通過フィルタ31を,図5のアンテナ71,受信増幅器72,帯域通過フィルタ28,31からなる第2の共通受信手段で構成している。   Further, an amplifier 22, an antenna 23, an amplifier 24, and an antenna 25 corresponding to the third transmitter and the fourth transmitter in FIG. 2 are added to the second adder 68, the amplifier 69, and the antenna 70 in FIG. The antenna 26, the reception amplifier 27, the band-pass filter 28 and the antenna 29, the reception amplifier 30, and the band-pass filter 31 corresponding to the third receiver and the fourth receiver in FIG. , And a second common receiving means comprising the antenna 71, the receiving amplifier 72, and the band-pass filters 28 and 31 shown in FIG.

本発明の実施例1〜実施例3では,周波数f1 とf2 が非常に離れている場合にそれぞれ,周波数毎に専用の増幅器を用いた例であるが,お互いの周波数f1 とf2 が近いときには,増幅器を共通に使用可能であり,経済的である。また,増幅器を共通化した場合,増幅器による遅延時間のバラツキが,別々に構成される場合に比べて,軽減されるメリットがある。 In Examples 1 to 3 of the present invention, respectively when the frequency f 1 and f 2 are very far, although an example using a dedicated amplifier for each frequency, the frequency of each other f 1 and f 2 Is close, the amplifier can be used in common and it is economical. In addition, when amplifiers are shared, there is an advantage that variations in delay time due to amplifiers are reduced compared to a case where they are configured separately.

本発明の概要を説明する図である。It is a figure explaining the outline | summary of this invention. 本発明の実施例1を示す図である。It is a figure which shows Example 1 of this invention. 本発明の実施例2を示す図である。It is a figure which shows Example 2 of this invention. 本発明の実施例3を示す図である。It is a figure which shows Example 3 of this invention. 本発明の実施例4を示す図である。It is a figure which shows Example 4 of this invention.

符号の説明Explanation of symbols

1,2 無線局
3,4,15 発振器
5,7,22,24,64,69 増幅器
6,8,9,12,23,25,26,29,65,66,70,71 アンテナ
10,13,27,30,67,72 受信増幅器
11,14,28,31 帯域通過フィルタ
16,19,33,34,39,44,45,50,53,57,58,105,
202 周波数シフト手段
17,20,35,37,40,46,48,51,54,59,61 ミキサー
18,21,36,38,41,47,49 低域通過フィルタ
52,55,60,62 高域通過フィルタ
32,43,56 マルチ周波数シフト手段
42 速度表示手段
63,68 加算器
101 第1の発振手段
102 第2の発振手段
103,203 送信手段
104,201 受信手段
106 測定手段
1, 2, radio station 3, 4, 15 oscillator 5, 7, 22, 24, 64, 69 amplifier 6, 8, 9, 12, 23, 25, 26, 29, 65, 66, 70, 71 antenna 10, 13 27, 30, 67, 72 Receiving amplifier 11, 14, 28, 31 Band pass filter 16, 19, 33, 34, 39, 44, 45, 50, 53, 57, 58, 105,
202 Frequency shift means 17, 20, 35, 37, 40, 46, 48, 51, 54, 59, 61 Mixer 18, 21, 36, 38, 41, 47, 49 Low-pass filter 52, 55, 60, 62 High-pass filter 32, 43, 56 Multi-frequency shift means 42 Speed display means 63, 68 Adder 101 First oscillating means 102 Second oscillating means 103, 203 Transmitting means 104, 201 Receiving means 106 Measuring means

Claims (2)

第1の無線局と第2の無線局間の相対移動速度を測定する方法であって,
前記第1の無線局から周波数の異なる第1の波および第2の波を電波として送信し,
前記第2の無線局では,前記第1の無線局から送信された第1の波および第2の波を受信し,前記受信した第1の波と所定の周波数シフト用の波とをミキシングすることにより周波数をシフトして第3の波を生成し,前記受信した第2の波と前記所定の周波数シフト用の波とをミキシングすることにより周波数をシフトして第4の波を生成し,その第3の波および第4の波を電波として送信し,
前記第1の無線局では,前記第2の無線局から送信された第3の波および第4の波を受信し,
(a)前記送信した第1の波と前記送信した第2の波とをミキシングすることにより周波数をシフトして第5の波を生成し,前記受信した第3の波と前記受信した第4の波とをミキシングすることにより周波数をシフトして第6の波を生成するか,または,
(b)前記送信した第1の波と前記受信した第3の波とをミキシングすることにより周波数をシフトして第5の波を生成し,前記送信した第2の波と前記受信した第4の波とをミキシングすることにより周波数をシフトして第6の波を生成するか,または,
(c)前記送信した第1の波と前記受信した第4の波とをミキシングすることにより周波数をシフトして第5の波を生成し,前記送信した第2の波と前記受信した第3の波とをミキシングすることにより周波数をシフトして第6の波を生成し,
前記第5の波と前記第6の波の周波数差に基づいて,前記第1の無線局と第2の無線局間の相対速度を測定する
ことを特徴とする移動速度測定方法。
A method for measuring a relative movement speed between a first radio station and a second radio station, comprising:
Transmitting a first wave and a second wave having different frequencies from the first radio station as radio waves;
The second radio station receives the first wave and the second wave transmitted from the first radio station , and mixes the received first wave with a predetermined frequency shift wave. Thereby shifting the frequency to generate a third wave, mixing the received second wave and the predetermined frequency shifting wave to shift the frequency to generate a fourth wave, Send the third and fourth waves as radio waves,
The first radio station receives the third wave and the fourth wave transmitted from the second radio station,
(A) A frequency is shifted by mixing the transmitted first wave and the transmitted second wave to generate a fifth wave, and the received third wave and the received fourth wave To generate a sixth wave with a frequency shift by mixing with
(B) A frequency is shifted by mixing the transmitted first wave and the received third wave to generate a fifth wave, and the transmitted second wave and the received fourth wave To generate a sixth wave with a frequency shift by mixing with
(C) A frequency is shifted by mixing the transmitted first wave and the received fourth wave to generate a fifth wave, and the transmitted second wave and the received third wave To generate a sixth wave by shifting the frequency by mixing
The fifth on the basis of the frequency difference of the wave and the sixth wave of the moving speed measuring method characterized by measuring the relative velocity between the first radio station and the second radio station.
第1の無線局と第2の無線局間の相対移動速度を測定する方式であって,
前記第1の無線局は,
周波数の異なる第1の波および第2の波を電波として送信する送信手段と,
前記第2の無線局から送信された第3の波および第4の波を受信する受信手段と,
(a)前記送信した第1の波と前記送信した第2の波とをミキシングすることにより周波数をシフトして第5の波を生成し,前記受信した第3の波と前記受信した第4の波とをミキシングすることにより周波数をシフトして第6の波を生成するか,または,(b)前記送信した第1の波と前記受信した第3の波とをミキシングすることにより周波数をシフトして第5の波を生成し,前記送信した第2の波と前記受信した第4の波とをミキシングすることにより周波数をシフトして第6の波を生成するか,または,(c)前記送信した第1の波と前記受信した第4の波とをミキシングすることにより周波数をシフトして第5の波を生成し,前記送信した第2の波と前記受信した第3の波とをミキシングすることにより周波数をシフトして第6の波を生成する周波数シフト手段と,
前記第5の波と前記第6の波の周波数差に基づいて,前記第1の無線局と第2の無線局間の電波の相対移動速度を測定する測定手段とを備え,
前記第2の無線局は,
前記第1の無線局から送信された第1の波および第2の波を受信する受信手段と,
前記受信した第1の波と所定の周波数シフト用の波とをミキシングすることにより周波数をシフトして第3の波を生成し,前記受信した第2の波と前記所定の周波数シフト用の波とをミキシングすることにより周波数をシフトして第4の波を生成する周波数シフト手段と,
前記第3の波および前記第4の波を電波として送信する送信手段とを備える
ことを特徴とする移動速度測定方式。
A method for measuring a relative moving speed between a first radio station and a second radio station,
The first radio station is:
Transmitting means for transmitting the first wave and the second wave having different frequencies as radio waves;
Receiving means for receiving a third wave and a fourth wave transmitted from the second radio station;
(A) A frequency is shifted by mixing the transmitted first wave and the transmitted second wave to generate a fifth wave, and the received third wave and the received fourth wave The frequency is shifted by mixing the first wave and the sixth wave to generate the sixth wave, or (b) the frequency is mixed by mixing the transmitted first wave and the received third wave. Shift to generate a fifth wave and mix the transmitted second wave and the received fourth wave to shift the frequency to generate a sixth wave, or (c ) A frequency is shifted by mixing the transmitted first wave and the received fourth wave to generate a fifth wave, and the transmitted second wave and the received third wave The frequency is shifted by mixing the And the frequency shift means for generating,
The fifth on the basis of the frequency difference of the wave and the sixth wave of, and a measuring means for measuring the radio wave of the relative movement speed between the first radio station and the second radio station,
The second radio station is
Receiving means for receiving the first wave and the second wave transmitted from the first radio station;
The received first wave and a predetermined frequency shift wave are mixed to generate a third wave by shifting the frequency, and the received second wave and the predetermined frequency shift wave A frequency shift means for generating a fourth wave by shifting the frequency by mixing
Moving speed measuring method characterized by comprising a transmitting means for transmitting the third wave and the fourth wave of the radio wave.
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