JPH06331733A - Method and equipment for measuring distance - Google Patents
Method and equipment for measuring distanceInfo
- Publication number
- JPH06331733A JPH06331733A JP5144290A JP14429093A JPH06331733A JP H06331733 A JPH06331733 A JP H06331733A JP 5144290 A JP5144290 A JP 5144290A JP 14429093 A JP14429093 A JP 14429093A JP H06331733 A JPH06331733 A JP H06331733A
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- wave
- amount
- distance value
- measured
- distance
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- 238000000034 method Methods 0.000 title claims abstract description 48
- 238000005259 measurement Methods 0.000 claims abstract description 80
- 230000005540 biological transmission Effects 0.000 claims abstract description 54
- 238000006073 displacement reaction Methods 0.000 claims description 54
- 238000004364 calculation method Methods 0.000 claims description 50
- 238000012937 correction Methods 0.000 claims description 4
- 238000004904 shortening Methods 0.000 abstract 2
- 230000003252 repetitive effect Effects 0.000 abstract 1
- 238000001514 detection method Methods 0.000 description 16
- 238000010586 diagram Methods 0.000 description 13
- 238000005070 sampling Methods 0.000 description 8
- 238000006243 chemical reaction Methods 0.000 description 7
- 238000001914 filtration Methods 0.000 description 7
- 230000010355 oscillation Effects 0.000 description 7
- 230000000630 rising effect Effects 0.000 description 6
- 230000000694 effects Effects 0.000 description 4
- 238000012545 processing Methods 0.000 description 4
- 239000011159 matrix material Substances 0.000 description 3
- 230000002159 abnormal effect Effects 0.000 description 2
- 238000009499 grossing Methods 0.000 description 2
- 241000251468 Actinopterygii Species 0.000 description 1
- 238000004891 communication Methods 0.000 description 1
- 238000007796 conventional method Methods 0.000 description 1
- 230000007423 decrease Effects 0.000 description 1
- 230000003111 delayed effect Effects 0.000 description 1
- 239000006185 dispersion Substances 0.000 description 1
- 230000010365 information processing Effects 0.000 description 1
- 230000001788 irregular Effects 0.000 description 1
- 238000000691 measurement method Methods 0.000 description 1
- 230000010363 phase shift Effects 0.000 description 1
- 230000001105 regulatory effect Effects 0.000 description 1
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Abstract
Description
【0001】[0001]
【産業上の利用分野】この発明は反射探知による距離測
定とドップラー効果による変移量測定との組み合わせに
よる追尾型の距離計測方法ならびにこの方法を用いる距
離計測装置に関するものである。なお、この発明の数値
または演算記号において、記号の前に*を付したものは
当該記号がベクトルを表示することを表し、当該記号を
「 」で挟んだものは推定値を表し、上つき記号T は転
置を表すものである。また、記号のiは、1,2,3…
…Nを代表する記号であって、得られた回の次数を表す
ものであり、例えば、何回目の測定値であるかなどを表
すものである。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a tracking type distance measuring method using a combination of distance measurement by reflection detection and displacement measurement by the Doppler effect, and a distance measuring device using this method. In addition, in the numerical values or operation symbols of the present invention, a symbol preceded by * indicates that the symbol represents a vector, a symbol enclosed by “” indicates an estimated value, and a superscript symbol. T represents transposition. The symbol i is 1, 2, 3, ...
... is a symbol representing N and represents the order of the obtained times, for example, how many times the measured value is.
【0002】[0002]
【従来の技術】反射探知による距離測定としては、周期
的に繰り返す送信波の反射波を得るとともに、送信波の
各周期の規定点から反射波の各周期の規定点までの経過
時間、例えば、送信パルス波から受信パルス波までの経
過時間にもとづいて探知地点から物標までの距離を計測
するようにしたパルス反射型距離計測装置が周知であ
り、こうしたパルス反射型距離計測装置としては、レー
ザや電磁波を用いるレーダと、超音波を用いる魚群探知
機や距離測定装置などがある。2. Description of the Related Art As a distance measurement by reflection detection, a reflected wave of a transmission wave that repeats periodically is obtained, and an elapsed time from a specified point of each cycle of the transmitted wave to a specified point of each cycle of the reflected wave, for example, A pulse reflection type distance measuring device that measures the distance from the detection point to the target based on the elapsed time from the transmitted pulse wave to the received pulse wave is well known, and such a pulse reflection type distance measuring device is a laser. And radar using electromagnetic waves, and fish finder and distance measuring device using ultrasonic waves.
【0003】ドップラー効果による変移量測定として
は、一定周波数送信波に対する反射波の周波数変化量に
もとづいて物標の移動速度・移動量を計測するようにし
た電磁波または超音波による速度計測装置・変移量計測
装置などがある。こうした速度計測装置・変移量計測装
置には、送信波として連続波を用いるものと搬送波をパ
ルス変調したパルス波を用いるものとがある。As a displacement amount measurement by the Doppler effect, a velocity measuring device / displacement using electromagnetic waves or ultrasonic waves, which measures the moving velocity / moving amount of a target based on the frequency varying amount of a reflected wave with respect to a constant frequency transmission wave There is a quantity measuring device. Such speed measuring devices and displacement amount measuring devices include those that use a continuous wave as a transmission wave and those that use a pulse wave obtained by pulse-modulating a carrier wave.
【0004】レーダを用いた目標追尾、つまり、トラッ
カにおいて、位置平滑定数αと速度平滑定数βとを係合
して追尾精度を向上するα−βトラッカと、こうしたト
ラッカにおいて、カルマンフィルタによる最適推定理論
を適用した演算により追尾する追尾フィルタ構成のもの
とがあり、さらに、目標の速度変化量γをも考慮したα
−β−γトラッカを検討されていることが、昭和54年
3月オーム社発行「電子通信ハンドブック」の第28編
第1部門5(レーダ情報処理)に開示されている。In a target tracking using a radar, that is, in a tracker, an α-β tracker for improving tracking accuracy by engaging a position smoothing constant α and a velocity smoothing constant β, and an optimal estimation theory by a Kalman filter in such a tracker. There is a tracking filter configuration that performs tracking by an operation that applies .alpha., And α that also considers the target speed change amount γ
The fact that-[beta]-[gamma] trackers have been studied is disclosed in "Electronic Communication Handbook", March 28, 1979, Vol. 28, No. 1, Section 5 (Radar Information Processing).
【0005】周波数変化量または位相変化量を検出する
ための周波数弁別回路として直角位相の信号を掛算する
直角位相形周波数弁別回路が、上記文献の第10編第2
部門3(角度変調)に開示されている。As a frequency discriminating circuit for detecting a frequency change amount or a phase change amount, a quadrature type frequency discriminating circuit for multiplying a quadrature phase signal is described in the second volume of the tenth edition of the above-mentioned document.
It is disclosed in department 3 (angle modulation).
【0006】カルマンフィルタにおいて、リカッチ形の
方程式により一定値に収束する方法を用いて計測を行う
ことが、上記文献の第5編第1部門2(ろ波と予測)に
開示されている。In the Kalman filter, the measurement using the method of converging to a constant value by the Riccati type equation is disclosed in the 5th volume, 1st section 2 (filtering and prediction) of the above-mentioned document.
【0007】パルス反射型距離計測では、図10のよう
に、送信パルス波Aの規定点aから受信パルス波Bの規
定点bまでの時間taを測定し、この時間taとパルス
波の伝搬速度cとの積から計測距離値Rを得ている。こ
の計測では、送信から反射波の受信までの時間経過を主
体にして計測しているため、計測値が間欠的にしか得ら
れないことになる。In the pulse reflection type distance measurement, as shown in FIG. 10, the time ta from the specified point a of the transmitted pulse wave A to the specified point b of the received pulse wave B is measured, and this time ta and the propagation speed of the pulse wave are measured. The measured distance value R is obtained from the product with c. In this measurement, the time lapse from the transmission to the reception of the reflected wave is mainly measured, so the measured value can be obtained only intermittently.
【0008】また、パルス波が探知点と物標の間を往復
する間の伝搬経路、物標の反射面、雑音などの影響を受
けて受信パルス波Bの波形は、図11のように、送信パ
ルス波Aの波形に対して不規則に変形してしまうため、
規定点bの位置も不規則に変化するなどの理由で、計測
距離値Rは必然的に不規則な誤差を含むことになり、毎
回の計測距離値R(i)をプロットしてみると、図12
のように、一定しない誤差値を含んでいるため、分散し
たものになってしまう。Further, as shown in FIG. 11, the waveform of the received pulse wave B is affected by the propagation path of the pulse wave traveling back and forth between the detection point and the target, the reflecting surface of the target, noise, etc. Since the waveform of the transmission pulse wave A is irregularly deformed,
The measured distance value R inevitably includes an irregular error because the position of the defined point b also changes irregularly. When the measured distance value R (i) is plotted every time, 12
As described above, since the error values are not constant, they are dispersed.
【0009】ドップラー変移量計測では、図13のよう
に、周波数foの連続波による送信波Cが、物標の移動
速度Sによって生ずるドップラー効果により、周波数f
sに偏移して受信波Dになるので、周波数fsと周波数
foとを比較して検出した周波数または位相の変化量△
fまたは△pを測定して得られる移動速度Sと時間tb
とから移動距離値、つまり、計測変移量rを求めてい
る。この計測では、周波数変化を主体にして計測してい
るため、計測値が連続的に得られる上に、比較的高い測
定精度が得られ、初回の測定点での距離値R(0)が分
かっていれば、これに都度の計測変移量r(i)を積算
して得られる積算距離値をプロットしてみると、図12
のように、誤差値の少ない線状になって得られるという
利点がある。In the Doppler shift amount measurement, as shown in FIG. 13, a transmission wave C of a continuous wave having a frequency fo is generated by the Doppler effect generated by the moving speed S of the target, so that the frequency f
Since the received wave D shifts to s, the amount of change in frequency or phase detected by comparing the frequency fs with the frequency fo is Δ
Moving speed S and time tb obtained by measuring f or Δp
The moving distance value, that is, the measured displacement amount r is calculated from In this measurement, since the frequency change is mainly measured, the measurement value is continuously obtained, and relatively high measurement accuracy is obtained, and the distance value R (0) at the first measurement point is known. If so, the accumulated distance value obtained by accumulating the measured displacement amount r (i) at each time is plotted, and FIG.
As described above, there is an advantage that it can be obtained in a linear form with a small error value.
【0010】[0010]
【発明が解決しようとする課題】上記のような積算距離
のプロットの途中において、送信波を目的物体以外の物
体の通過などにより計測変移量r(i)が撹乱され、ま
たは、遮断されてしまうと、その撹乱または遮断による
移動量によって積算距離値に多量の誤差値を生じたり、
実質的に計測が不能になるという不都合が生ずる。In the course of plotting the integrated distance as described above, the measured displacement r (i) is disturbed or interrupted by the passage of the transmitted wave by an object other than the target object. And a large amount of error value in the integrated distance value due to the movement amount due to the disturbance or interruption,
This causes the inconvenience that measurement becomes substantially impossible.
【0011】したがって、パルス反射型距離計測とドッ
プラー変移量計測とを係合するとともに最適推定理論を
適用して計測距離値を演算する方法が極めて有効であ
る。Therefore, a method of engaging the pulse reflection type distance measurement and the Doppler shift amount measurement and applying the optimum estimation theory to calculate the measured distance value is extremely effective.
【0012】しかしながら、従来の最適推定理論を適用
する方法では、最適推定のための演算における収束にお
いて、あまりにも長い時間が掛かり過ぎて、こうした追
尾型の距離計測においては、移動体の速度変化が速い場
合や移動データを綿密に得たい場合には、積算距離値の
算出が間に合わず、目的を達し得ないという不都合が生
ずる。However, in the conventional method of applying the optimum estimation theory, it takes too long time for the convergence in the calculation for the optimum estimation, and in such tracking type distance measurement, the velocity change of the moving body is changed. If the speed is high or if the movement data is to be obtained in detail, the calculation of the integrated distance value cannot be completed in time, and the purpose cannot be achieved.
【0013】このため、こうした不都合のない距離計測
方法ならびに距離計測装置の提供が望まれているという
課題がある。Therefore, there is a problem that it is desired to provide a distance measuring method and a distance measuring device which do not have such inconvenience.
【0014】[0014]
【課題を解決するための手段】この発明は、上記のよう
なパルス反射型距離計測とドップラー変移量計測とを係
合するとともに最適推定理論を適用して、計測距離値を
収束するようにした距離計測方法において、逐次型最小
二乗法による収束演算を行うことにより、演算時間の短
縮を可能にして上記の課題を解決し得るようにしたもの
である。According to the present invention, the pulse reflection type distance measurement and the Doppler shift amount measurement as described above are engaged with each other, and the optimum estimation theory is applied to converge the measurement distance value. In the distance measuring method, the convergence time is calculated by the recursive least squares method so that the calculation time can be shortened and the above problems can be solved.
【0015】[0015]
【作用】最適推定理論の演算方法、カルマンフィルタに
おける方程式では非常に長い多重の演算式を解かねばな
らないが、逐次型最小二乗法による収束演算の場合の演
算式の展開は、はるかに短く単行程の演算で行えるた
め、演算時間を極度に短縮し得るようになり、移動体の
速度変化が速い場合や移動データを綿密に得たい場合の
追尾に対しても、オンライン式の構成で行わせることが
できる。Although the calculation method of the optimal estimation theory and the equation in the Kalman filter must solve a very long multiple calculation expression, the expansion of the calculation expression in the case of the convergence calculation by the recursive least squares method is much shorter and the single stroke The calculation time can be extremely shortened because it can be performed by the calculation of, and the online configuration can also be used for tracking when the speed change of the moving body is fast or when it is necessary to obtain detailed movement data. You can
【0016】[0016]
〔第1実施例〕以下、図1〜図4により第1実施例を説
明する。図1〜図4において図10〜図13における符
号と同一符号で示す部分は図10〜図13で説明した同
一符号の部分と同一機能をもつ部分である。[First Embodiment] A first embodiment will be described below with reference to FIGS. In FIGS. 1 to 4, portions indicated by the same reference numerals as those in FIGS. 10 to 13 have the same functions as the portions having the same reference numerals described in FIGS. 10 to 13.
【0017】図1において、距離計測部1は、図10・
図11のように、電波の送信パルス波Aを送信して目的
とする物標Eから反射して来る受信パルス波Bを受信し
て、両パルス波の規定点aから規定点bまでの間の時間
taを測定し、毎回の計測距離値R(i)に対応する時
間量ta(i)を得る部分である。そして、送信パルス
Aは、周期的に繰り返し送信しているので、時間量ta
(i)は、要約すると、送信パルスAの規定点a、つま
り、送信波の各周期の規定点から、受信パルスBの規定
点b、つまり、反射波の各周期における送信波の規定点
に対応する規定点までの時間量を得ていることになる。In FIG. 1, the distance measuring unit 1 is shown in FIG.
As shown in FIG. 11, a transmission pulse wave A of a radio wave is transmitted, a reception pulse wave B reflected from a target E is received, and a predetermined point a to a predetermined point b of both pulse waves is received. Is a part of measuring the time ta of and obtaining the amount of time ta (i) corresponding to the measured distance value R (i) every time. Since the transmission pulse A is repeatedly transmitted periodically, the time amount ta
In summary, (i) is from the defined point a of the transmission pulse A, that is, the defined point of each cycle of the transmitted wave, to the defined point b of the received pulse B, that is, the defined point of the transmitted wave in each cycle of the reflected wave. You have gained the amount of time to the corresponding regulatory point.
【0018】変移計測部2は、図13のように、周波数
foの送信波Cを送信し、物標Eから反射して来る受信
波パルスDを受信して、物標Eの移動速度S(計測地点
に対して遠ざかる場合を+Sとし、近付く場合を−Sと
する)によって偏移した受信波Dの周波数fsの波形の
同一周期点、例えば、波形のゼロクロス点の間の時間量
tcを測定することにより、その逆数から周波数fsを
測定し、毎回の計測変移量r(i)に対応する周波数変
化量fs(i)(周波数変化量が微小変化である場合に
は位相変化量を測定するが、この実施例では、こうした
場合における位相変化量を含めて周波数変化量という)
を得る部分である。As shown in FIG. 13, the displacement measuring section 2 transmits a transmission wave C having a frequency fo, receives a reception wave pulse D reflected from the target E, and moves at a moving speed S ( (+ S when moving away from the measurement point and -S when approaching the measurement point) measures the same period point of the waveform of the frequency fs of the received wave D, which is deviated by, for example, the time amount tc between the zero cross points of the waveform. By doing so, the frequency fs is measured from the reciprocal thereof, and the frequency change amount fs (i) corresponding to the measurement change amount r (i) every time (when the frequency change amount is a minute change, the phase change amount is measured). However, in this embodiment, the amount of phase change in such a case is called the amount of frequency change.)
Is the part to get.
【0019】そして、距離計測部1と変移計測部2と
は、各計測をアナログ的に処理するアナログ処理部分を
構成している。The distance measuring unit 1 and the displacement measuring unit 2 form an analog processing unit that processes each measurement in an analog manner.
【0020】修正距離値演算部3は、距離計測部1と変
移計測部2とで得られた各アナログ計測値をA/D変換
して所要のディジタル処理を行う部分であり、第1に
は、距離値計測手段をもっており、この手段は、距離計
測部1で得られる毎回の時間量ta(i)と、電波の伝
搬速度cとの積によって、毎回の計測距離値R(i)を
得るための計測を行うものである。The corrected distance value calculation unit 3 is a unit for A / D converting the analog measurement values obtained by the distance measurement unit 1 and the displacement measurement unit 2 to perform the required digital processing. , And has a distance value measuring means, and this means obtains a measured distance value R (i) for each time by the product of the time amount ta (i) for each time obtained by the distance measuring unit 1 and the propagation velocity c of the radio wave. The measurement is performed for.
【0021】第2には、変移量計測手段をもっており、
この手段は、変移量計測部2によって得られる毎回の周
波数変化量fs(i)は、電波の伝搬速度cにもとづい
て、ドップラー効果による周波数偏移が、次の算定式Secondly, it has a displacement amount measuring means,
According to this means, the frequency shift amount fs (i) obtained each time by the shift amount measuring unit 2 is based on the propagation speed c of the radio wave, and the frequency shift due to the Doppler effect is
【数1】 によって関係付けられることから、次の算定式[Equation 1] Since it is related by
【数2】 によって移動速度Sを求める演算を行うとともに、周波
数fsをサンプルして上記の演算を行い、次のサンプル
を行うまでの間の時間tbとの積によって、毎回の計測
変移量r(i)を得るものである。[Equation 2] The calculation of the moving speed S is performed, the frequency fs is sampled, the above calculation is performed, and a product of the frequency fs and the time tb until the next sampling is performed to obtain the measured displacement amount r (i) every time. It is a thing.
【0022】第3には、最適推定演算手段をもってお
り、この手段は、所定時点に距離計測手段によって得ら
れる初期計測距離値R(0)と、この所定時点以後に、
距離計測手段によって得られる毎回の計測距離値R
(i)と、変移量計測手段によって得られる毎回の計測
変移量r(i)とにもとづいて、カルマンフィルタによ
る最適推定の演算処理を行うが、演算処理の過程をリカ
ッチ形の分散方程式に代えて、逐次型最小二乗法により
収束を行う演算を用いるようにしたものである。Thirdly, it has an optimum estimation calculation means, which means an initial measured distance value R (0) obtained by the distance measuring means at a predetermined time point and, after this predetermined time point,
Measured distance value R obtained by the distance measuring means every time
On the basis of (i) and the measured displacement amount r (i) obtained by the displacement amount measuring means each time, the calculation process of the optimal estimation by the Kalman filter is performed, but the process of the calculation process is replaced by the Riccati type dispersion equation. , An operation for performing convergence by the recursive least squares method is used.
【0023】つまり、係数をα、α≠1、誤差値をε
(i)とする方程式That is, the coefficient is α, α ≠ 1, and the error value is ε.
Equation (i)
【数3】 を適用するとともに、誤差値ε(i)の二乗和が最小に
なるR(0)の推定値「R(0,1)」を求める演算式[Equation 3] And an equation for calculating the estimated value “R (0,1)” of R (0) that minimizes the sum of squares of the error value ε (i)
【数4】 を設定して演算した推定値「R(i)」を修正距離値R
cとして、つまり、[Equation 4] The estimated value “R (i)” calculated by setting
As c, that is,
【数5】 として修正距離値Rcを求める手段を設けたものであ
る。[Equation 5] A means for obtaining the corrected distance value Rc is provided.
【0024】上記の各手段を行うための処理は、修正距
離値演算部3に設けた演算処理器(この発明においてC
PUという)によって行い、所要の定数値・係数値など
はCPU内に予め記憶してある。The processing for performing each of the above means is performed by an arithmetic processor (C in the present invention) provided in the corrected distance value arithmetic unit 3.
(PU) and required constant values, coefficient values, etc. are stored in advance in the CPU.
【0025】表示部4は、修正距離値演算部3によって
得られる修正距離値R(N)と計測時間の経過とを数値
表示により表示し、または、これらの各値をアナログ値
に変換したものを画面上にプロットして表示する部分で
ある。The display unit 4 displays the corrected distance value R (N) obtained by the corrected distance value calculation unit 3 and the elapsed measurement time on a numerical display, or converts each of these values into an analog value. Is a part for plotting and displaying on the screen.
【0026】表示部4をアナログ値のプロットで表示す
る場合の図形によって、計測値の収束経過を示すと、図
2のように、初期計測距離値R(0)における誤差値ε
R (0)が、毎回の計測変移量r(i)の積算値によっ
て徐々に減少し、毎回の修正距離値R(i)が、真の毎
回の距離値RT (i)に収束して、距離測定精度が向上
することになるものである。FIG. 2 shows an error value ε at the initial measured distance value R (0) when the convergence of measured values is shown by a figure when the display unit 4 is displayed by plotting analog values.
R (0) gradually decreases according to the integrated value of the measurement displacement amount r (i) each time, and the corrected distance value R (i) converges to the true distance value R T (i) each time. The distance measurement accuracy is improved.
【0027】上記の所定時点を、計測開始の時点、計測
変移量r(i)と計測距離値R(i)との各計測値を得
るための送信波が目的とする物標以外の反射物体によっ
て妨げられて異常な計測値を発生し、または、計測値が
得られなくなった異常時後に、予測し得る計測値に近い
計測値が得られるように復活した時点などに設定するた
めの検出を各計測値の演算処理によって行う機能を修正
距離値演算部3に設けることによって、図3のように、
上記の復活した時点を計測開始として、同様に、距離測
定精度を向上することができる。The above predetermined time point is the measurement start time point, and the reflected wave other than the target object is the transmission wave for obtaining the respective measured values of the measured displacement amount r (i) and the measured distance value R (i). Detection to set an abnormal measurement value that is interrupted by the measurement, or when the measurement value is no longer available and that the measurement value is close to a predictable measurement value when the measurement value is restored. As shown in FIG. 3, by providing the corrected distance value calculation unit 3 with the function of performing calculation processing of each measured value,
Similarly, the distance measurement accuracy can be improved by starting the measurement at the point of time when the measurement is restored.
【0028】図3の場合、上記の異常時をデータ欠損時
として扱い、この間における修正距離値R(N)と、計
測変移量r(i)を累積した積算値を、データ欠損前の
値に保持して、変化が無かったものとみなしているが、
このデータ欠損部分のデータをゼロにリセットして計測
しても、データ復活後の経過は、実質的には同一結果に
なる。また、データ欠損時以前の移動データどおりの値
と推定して延長軌跡にしてもよい場合もあるが、この間
に反対方向に移動すると、かえって誤差が大きくなるの
で、この間に、計測距離値R(i)が間欠的にでも得ら
れる場合には、図4のように、この間の計測距離値R
(i)の数回分の平均をスライドさせながら得た平均値
を修正距離値R(N)の代わりに置き換えて表示した方
が、無難な結果が得られることは言うまでもない。In the case of FIG. 3, the above abnormal time is treated as a data loss, and the integrated value obtained by accumulating the corrected distance value R (N) and the measured displacement amount r (i) during this period is set as the value before the data loss. I keep it and consider it to have not changed,
Even if the data in the data-missing portion is reset to zero and measured, the progress after the data restoration is substantially the same. In some cases, it may be possible to make an extension trajectory by estimating the value as the movement data before the data loss, but if the movement is made in the opposite direction during this time, the error becomes rather large. When i) is obtained even intermittently, the measured distance value R during this period is as shown in FIG.
It goes without saying that a safe result can be obtained by replacing the corrected distance value R (N) with the average value obtained by sliding the average of several times in (i) and displaying it.
【0029】〔計測原理〕上記の演算式により現在時点
の修正距離値Rcが求め得る理由、つまり、計測方法の
原理を以下に説明する。図12において、ある計測点に
おいて、真の距離値RT (i)に対する真の初期計測距
離値RT (0)と真の変移量rT (i)の関係は次式で
表すことができる。[Measurement Principle] The reason why the corrected distance value Rc at the present time can be obtained by the above arithmetic expression, that is, the principle of the measurement method will be described below. In FIG. 12, at a certain measurement point, the relationship between the true initial measured distance value R T (0) and the true displacement amount r T (i) with respect to the true distance value R T (i) can be expressed by the following equation. .
【数6】 [Equation 6]
【0030】また、毎回の計測距離値R(i)の誤差値
をεR (i)、毎回の計測変移量r(i)の誤差値をε
r (i)とすると、上記のように、ドップラー変移量計
測の場合の誤差値、つまり、εr (i)は、パルス反射
型距離計測の場合の誤差値、つまり、εR (i)に比べ
て、はるかに小さいので、次のように関係づけることが
できる。The error value of each measured distance value R (i) is ε R (i), and the error value of each measured displacement amount r (i) is ε.
Assuming r (i), as described above, the error value in the case of Doppler displacement measurement, that is, ε r (i), becomes the error value in the case of pulse reflection type distance measurement, that is, ε R (i). By comparison, it is much smaller, so we can relate it as follows:
【数7】 [Equation 7]
【0031】初期計測距離値R(0)の誤差値をεR
(0)とし、また、毎回の計測誤差値をε(i)とする
と、The error value of the initial measured distance value R (0) is set to ε R
(0) and the measurement error value for each time is ε (i),
【数8】 [Equation 8]
【0032】したがって、計測変移量r(i)と計測距
離値R(i)との各計測値から誤差値ε(i)の二乗和
が最小となるように、R(0)の推定値「R(0,
i)」を求めたときの計測距離値R(i)の推定値「R
(i)」が、修正距離値Rcになるようにすればよいわ
けであるから、次式のように設定することができる。Therefore, the estimated value R (0) of R (0) is minimized so that the sum of squares of the error value ε (i) is minimized from the measured values of the measured displacement amount r (i) and the measured distance value R (i). R (0,
i) ", the estimated value" R of the measured distance value R (i) "
Since (i) ”should be set to the corrected distance value Rc, it can be set as in the following equation.
【数9】 [Equation 9]
【0033】この式(13)のr(i)には係数を設け
ていないが、推定計算の演算過程の都合上、係数αを設
けて推定するものとし、現在時点までに、N個の計測距
離値R(i)と計測変移量r(i)とが得られたとする
と、式(10)から次式が得られる。Although no coefficient is provided for r (i) in the equation (13), the coefficient α is provided for the sake of convenience in the calculation process of the estimation calculation, and N measurements are made up to the present time. Assuming that the distance value R (i) and the measured displacement amount r (i) are obtained, the following equation is obtained from the equation (10).
【数10】 [Equation 10]
【0034】ここで、上記の式(14)を行列表現にす
るために、ベクトルを示す記号*と行列Zを設定する
と、Here, in order to make the above expression (14) into a matrix expression, if the symbol * indicating the vector and the matrix Z are set,
【数11】 [Equation 11]
【0035】となり、これらの式から上記の式(14)
は次式のように簡潔に表すことができる。From these equations, the above equation (14) is obtained.
Can be expressed simply as
【数12】 [Equation 12]
【0036】ここで、推定したい量はαとR(0)とを
含むベクトル*θであるから、ここで、推定誤差の分散
行列をP(i)、最小二乗法を用いて収束させるための
荷重をρとおくと、最小二乗推定値「*θ(N)」は次
式のように表すことができることになる。Here, since the quantity to be estimated is the vector * θ including α and R (0), here, the variance matrix of the estimation error is set to P (i) by using the least square method. When the weight is set to ρ, the least squares estimated value “* θ (N)” can be expressed as the following equation.
【数13】 [Equation 13]
【0037】また、荷重ρは、1に十分近い値なので、
初期値として、Since the load ρ is a value close to 1 sufficiently,
As an initial value,
【数14】 [Equation 14]
【0038】とおき、さらに、式の展開に寄与させるた
めの介在記号として、C,P11,P12,P21,P22,
q,s,t,u,vを設定すると、求める係数推定値
「α(N)」と距離値の推定値「R(0,N)」とは、
次式で表すことができることになる。Furthermore, C, P 11 , P 12 , P 21 , P 22 , and P 22 , as an intervening symbol for contributing to the expansion of the equation.
When q, s, t, u, and v are set, the coefficient estimated value “α (N)” and the estimated distance value “R (0, N)” are
It can be expressed by the following equation.
【数15】 [Equation 15]
【0039】そして、これらの式において、Then, in these equations,
【数16】 であり、また、式(26)によって「R(0,N)」を
算定した値を、上記の式(13)の推定値「R(0,
i)」に代入すれば、求める修正距離値Rcを得ること
ができる。[Equation 16] Further, the value obtained by calculating “R (0, N)” by the equation (26) is used as the estimated value “R (0, N)” of the equation (13).
i) ”, the corrected distance value Rc to be obtained can be obtained.
【0040】つまり、式(25)の「α(N)」は「α
(i)」として、式(26)の「R(0,N)」は「R
(0,i)」として、また、式(25)・式(26)の
r(N)はr(i)として書き表せられるので、式(1
3)を解くことができるわけである。That is, "α (N)" in the equation (25) is "α
(I) ”,“ R (0, N) ”in the equation (26) is“ R
(0, i) ”, and r (N) in equations (25) and (26) can be written as r (i), so that equation (1
3) can be solved.
【0041】上記の第1実施例による構成を要約する
と、第1の構成として、周期的に繰り返す送信波、例え
ば、送信パルス波Aの反射波、例えば、発信パルス波B
を得るとともに、送信波の各周期の規定点aから反射波
の規定点aに対応する規定点bまでの時間量の測定値に
もとづいて得られる計測距離値を、送信波の周波数fo
に対する反射波の周波数変化量または位相変化量の測定
値にもとづいて得られる計測変移量で修正することによ
り修正距離値を得る距離測定方法において、前記修正を
行うための最適推定の演算を、逐次型最小二乗法による
収束を用いて演算するようにした距離計測方法を提供す
るものである。To summarize the configuration according to the first embodiment described above, as the first configuration, a periodically repeated transmission wave, for example, a reflected wave of the transmission pulse wave A, for example, the transmission pulse wave B is used.
And the measured distance value obtained based on the measured value of the amount of time from the specified point a of each cycle of the transmitted wave to the specified point b corresponding to the specified point a of the reflected wave is the frequency fo of the transmitted wave.
In the distance measuring method for obtaining the corrected distance value by correcting the measured displacement amount obtained based on the measured value of the frequency change amount or the phase change amount of the reflected wave, the optimum estimation calculation for performing the correction is sequentially performed. The present invention provides a distance measuring method adapted to perform a calculation by using convergence by a type least square method.
【0042】また、第2の構成として、上記の第1の構
成による距離計測方法において、所定時点に得られた初
期計測距離値をR(0)、上記の所定時点以後に得られ
る毎回の計測変移量をr(i)、毎回の計測距離値をR
(i)、また、修正距離値をRc、誤差の二乗和が最小
となる計測距離値の推定値を「R(0,i)」として、
演算式 Rc=「R(i)」=「R(0,i)」+r(i) により修正距離値を得る演算を行うようにした距離計測
方法を提供するものである。As a second structure, in the distance measuring method according to the first structure, the initial measured distance value obtained at a predetermined time point is R (0), and each time measurement is made after the predetermined time point. The displacement amount is r (i), and the measured distance value for each measurement is R
(I) In addition, the corrected distance value is Rc, and the estimated value of the measured distance value that minimizes the sum of squared errors is “R (0, i)”,
The present invention provides a distance measuring method for performing a calculation to obtain a corrected distance value by a calculation formula Rc = “R (i)” = “R (0, i)” + r (i).
【0043】また、第3の構成として、上記の第1の構
成または第2の構成などによる距離計測方法を用いる装
置おいて、上記の計測距離値を得るための時間量を測定
する距離計測部、例えば、距離計測部1と、上記の計測
変移量を得るための周波数変化量または位相変化量を測
定する変移計測部、例えば、変移計測部2と、上記の時
間量と、上記の周波数変化量または位相変化量とにもと
づいて上記の計測距離値と上記の変化量とを計測すると
ともに、上記の演算式にもとづく演算を行なって上記の
修正距離値を得る修正距離値演算部、例えば、修正距離
値演算部3とを設けた距離計測装置を提供するものであ
る。As a third structure, in a device using the distance measuring method according to the first structure or the second structure, the distance measuring unit for measuring the amount of time for obtaining the measured distance value. For example, the distance measuring unit 1 and a displacement measuring unit that measures the amount of frequency change or the amount of phase change for obtaining the amount of measurement displacement, for example, the displacement measuring unit 2, the amount of time, and the frequency change described above. A correction distance value calculator for obtaining the above-mentioned correction distance value by measuring the above-mentioned measured distance value and the above-mentioned change amount based on the amount or the phase change amount, and performing the calculation based on the above-mentioned arithmetic expression, for example, The present invention provides a distance measuring device provided with a corrected distance value calculation unit 3.
【0044】〔第2実施例〕次に、図5〜図9により、
第2実施例を説明する。図5〜図9において図1〜図4
における符号と同一符号で示す部分は図1〜図4で説明
した同一符号の部分と同一機能をもつ部分であり、ま
た、図5の構成における各部の信号を図6〜図8に示し
てある。[Second Embodiment] Next, referring to FIGS.
A second embodiment will be described. 1 to 4 in FIGS.
The parts denoted by the same reference numerals as in FIG. 4 have the same functions as the parts denoted by the same reference numerals explained in FIGS. 1 to 4, and the signals of the respective parts in the configuration of FIG. 5 are shown in FIGS. .
【0045】図5において、発振回路11は、送信すべ
き周波数よりも高い周波数の連続波を発振して得られる
信号を微分またはハードリミットして矩形波または狭い
パルス波にした発振信号11aを発生し、第1分周回路
12と90°/2相回路22とに与える。In FIG. 5, an oscillating circuit 11 generates an oscillating signal 11a which is a rectangular wave or a narrow pulse wave by differentiating or hard limiting a signal obtained by oscillating a continuous wave having a frequency higher than the frequency to be transmitted. Then, it is applied to the first frequency dividing circuit 12 and the 90 ° / 2-phase circuit 22.
【0046】第1分周回路12は、発振信号11aを分
周して、図13で説明したような送信波Cの周波数f0
の信号に相当する周期t0をもつ矩形波の第1分周信号
12aを作り、第2分周回路13と変調回路14と90
°/2相回路22とに与える。The first frequency dividing circuit 12 divides the frequency of the oscillation signal 11a to obtain the frequency f0 of the transmission wave C as described with reference to FIG.
The first frequency-divided signal 12a having a rectangular wave having a period t0 corresponding to the signal of
And the two-phase circuit 22.
【0047】第2分周回路13は、第1分周信号12a
を、さらに分周して、図10で説明したような送信パル
ス波Aに相当するような図6のパルス幅t1もつパルス
p1を所定の周期でを繰り返し送信するための周期Tと
パルス幅t1に相当する周期とを作るとともに、パルス
幅t1を周期T毎に選択して送信パルス波信号13aを
作り、変調回路14と比較回路26とに与える。The second frequency dividing circuit 13 has a first frequency dividing signal 12a.
Is further divided into a cycle T and a pulse width t1 for repeatedly transmitting a pulse p1 having a pulse width t1 in FIG. 6 corresponding to the transmission pulse wave A as described in FIG. 10 at a predetermined cycle. And a pulse width t1 is selected for each cycle T to generate a transmission pulse wave signal 13a, which is applied to the modulation circuit 14 and the comparison circuit 26.
【0048】変調回路14は、第1分周信号12aを送
信パルス波信号13aによって変調するが、この場合、
中間の変調率、例えば、50%程度の変調率で変調して
変調波信号14aを作り、送信回路15に与える。The modulation circuit 14 modulates the first divided signal 12a with the transmission pulse wave signal 13a. In this case,
The modulated wave signal 14a is generated by modulating at an intermediate modulation rate, for example, a modulation rate of about 50%, and is provided to the transmission circuit 15.
【0049】送信回路15は、変調波信号14aを電力
増幅して送波器16に与えることにより、図10・図1
3で説明した送信パルス波Aと送信波Cとを複合した信
号を送信波A1として物標Eに向けて送波する。また、
必要に応じて、周期t0に相当する周波数の共振回路を
介在させてもよい。The transmitting circuit 15 power-amplifies the modulated wave signal 14a and supplies the amplified wave signal 14a to the wave transmitter 16 so that the signal shown in FIGS.
A signal obtained by combining the transmission pulse wave A and the transmission wave C described in 3 is transmitted as the transmission wave A1 toward the target E. Also,
If necessary, a resonance circuit having a frequency corresponding to the cycle t0 may be interposed.
【0050】物標Eからの反射波B1を受波器17で受
波して得られた受波信号を増幅回路18で所要の振幅値
に増幅して、図10・図13で説明した受信パルス波B
と受信波Dとを複合した受信信号18aを作り、この受
信信号18aを振幅制限回路20と検波回路25とに与
える。The received signal obtained by receiving the reflected wave B1 from the target E by the wave receiver 17 is amplified by the amplifier circuit 18 to a desired amplitude value, and the reception described with reference to FIGS. Pulse wave B
A reception signal 18a is generated by combining the received signal D and the received wave D, and the reception signal 18a is given to the amplitude limiting circuit 20 and the detection circuit 25.
【0051】検波回路25は、反射波B1と同様の波形
をもつ受信信号18aを振幅検波して、図10で説明し
た受信パルス波Bに相当する波形もつ受信パルス波信号
25aを作り、必要に応じて波形成形を行った後、比較
回路26与える。The detection circuit 25 amplitude-detects the reception signal 18a having a waveform similar to that of the reflected wave B1 to produce the reception pulse wave signal 25a having a waveform corresponding to the reception pulse wave B described in FIG. The waveform is shaped accordingly and then provided to the comparison circuit 26.
【0052】比較回路26は、図10で説明した規定点
aから規定点bまでの間に相当する時間taを検出する
もので、送信パルス波信号13aと受信パルス波信号2
5aとの規定点、例えば、送信パルス波信号13aは送
信パルスp1の立ち上がり点を、また、受信パルス波信
号25aは受信パルスp2の立ち上がりの中間振幅点、
もしくは、受信パルスp2を立ち上がり部分を微分した
波形の所定振幅点を検出して得られる各信号によって、
この各信号の期間をゲートするゲート信号を比較検出信
号26aとしてゲート回路19に与える。The comparison circuit 26 detects the time ta corresponding to the period from the defined point a to the defined point b described with reference to FIG. 10, and it includes the transmission pulse wave signal 13a and the reception pulse wave signal 2
5a, for example, the transmission pulse wave signal 13a is the rising point of the transmission pulse p1, the reception pulse wave signal 25a is the intermediate amplitude point of the rising of the reception pulse p2,
Alternatively, by each signal obtained by detecting a predetermined amplitude point of the waveform obtained by differentiating the rising portion of the reception pulse p2,
A gate signal that gates the period of each signal is given to the gate circuit 19 as the comparison detection signal 26a.
【0053】ゲート回路27は、図示しないクロックパ
ルス、例えば、発振回路11の発振信号11aを比較検
出信号26aでゲートしたパルス、つまり、図10で説
明した時間ta、つまり、物標Eまでの距離値に対応し
た時間量に相当するパルス量、または、比較検出信号の
期間を積分して得られる電圧量を時間量信号27aとし
てA/D変換回路31に与える。The gate circuit 27 uses a clock pulse (not shown), for example, a pulse obtained by gating the oscillation signal 11a of the oscillation circuit 11 with the comparison detection signal 26a, that is, the time ta described in FIG. 10, that is, the distance to the target E. The pulse amount corresponding to the time amount corresponding to the value or the voltage amount obtained by integrating the period of the comparison detection signal is given to the A / D conversion circuit 31 as the time amount signal 27a.
【0054】A/D変換回路31は、複数のA/D変換
回路をもつ回路群であり、時間量信号26aをディジタ
ル値の信号に変換してCPU32に与える。振幅制限回
路20は、受信信号18aの振幅を一定にする振幅制限
を行った信号を濾波回路21に与える。濾波回路21
は、帯域通過型濾波回路であって、受信信号18a中の
搬送波、つまり、第1分周信号12aの周期t0に相当
する周波数成分が位相偏移または周波数偏移を受けた正
弦波状の信号、つまり、図13の受信波Dの周波数fs
を濾波して抽出することにより得られた受信位相信号2
1aをサンプルホールド回路23とサンプルホールド回
路24とに与える。The A / D conversion circuit 31 is a circuit group having a plurality of A / D conversion circuits, and converts the time amount signal 26a into a digital value signal and gives it to the CPU 32. The amplitude limiting circuit 20 gives a signal whose amplitude has been limited so that the amplitude of the received signal 18a is constant, to the filtering circuit 21. Filtering circuit 21
Is a band-pass type filtering circuit, and is a carrier wave in the received signal 18a, that is, a sinusoidal signal in which the frequency component corresponding to the period t0 of the first divided signal 12a is phase-shifted or frequency-shifted, That is, the frequency fs of the received wave D in FIG.
Received phase signal 2 obtained by filtering and extracting
1a is supplied to the sample hold circuit 23 and the sample hold circuit 24.
【0055】受信位相信号21aは、物標Eが移動によ
って位相偏移を受けるので、遠方側に移動した場合に
は、その移動速度に従って、例えば、図8の位相φ1の
信号または位相φ2の信号のように位相が遅れた信号と
なり、移動速度がさらに速い場合には、位相偏移を累積
した周波数偏移になって現れることになる。Since the target E is phase-shifted by the movement of the target E, the reception phase signal 21a is, for example, a signal of the phase φ1 or a signal of the phase φ2 shown in FIG. When the signal has a delayed phase as described above and the moving speed is higher, it appears as a frequency shift in which the phase shift is accumulated.
【0056】90°/2相回路22は、第1分周信号1
2aから90°の位相差をもつ2相の周波数信号を得る
もので、第1分周信号12aの周期t0を1/4だけず
らせた位相の時点をサンプルするためサンプル時点信号
22a、つまり、90°移相した信号と第1分周信号1
2aそのものの位相の時点をサンプルするためのサンプ
ル時点信号22bとの2相信号を得る回路であり、サン
プル時点信号22aをサンプルホールド回路23に、ま
た、サンプル時点信号22bをサンプルホールド回路2
4に与える。The 90 ° / 2-phase circuit 22 uses the first divided signal 1
A two-phase frequency signal having a phase difference of 90 ° from 2a is obtained. The sampling time point signal 22a, that is, 90 degrees, is used to sample the time point of a phase obtained by shifting the period t0 of the first divided signal 12a by ¼ ° Phase-shifted signal and first divided signal 1
2a is a circuit for obtaining a two-phase signal with a sample time point signal 22b for sampling the time point of the phase of itself, and the sample time point signal 22a is sent to the sample hold circuit 23, and the sample time point signal 22b is sent to the sample hold circuit 2
Give to 4.
【0057】また、90°/2相回路22は、例えば、
ワンショットマルチバイブレータとカウンタとの組み合
わせとし、ワンショットマルチバイブレータで第1分周
信号の立上始縁に対応する幅の狭いパルスを作ってサン
プル時点信号22aを得るとともに、第1分周信号12
aの分周比を4にしておき、第1分周信号の立上始縁か
ら第1分周信号12aの1パルス後に幅の狭いパルスを
作ってサンプル時点信号22bを得るようにすることが
でき。また、上記の分周比を4の整数倍にしておき、第
1分周信号の立上始縁から上記の分周比の逆数の1/4
に相当する数だけ発信信号11aのパルスを計数した時
点で幅の狭いパルスを作るようにしてサンプル時点信号
22bを得ることもできる。The 90 ° / 2-phase circuit 22 is, for example,
A combination of a one-shot multivibrator and a counter is used, and a pulse having a narrow width corresponding to the rising edge of the first divided signal is generated by the one-shot multivibrator to obtain the sample time point signal 22a, and the first divided signal 12
It is possible to set the frequency division ratio of a to 4 and generate a narrow pulse after one pulse of the first frequency division signal 12a from the rising edge of the first frequency division signal to obtain the sampling time point signal 22b. I can. The frequency division ratio is set to an integral multiple of 4, and 1/4 of the reciprocal of the frequency division ratio is calculated from the rising edge of the first frequency division signal.
It is also possible to obtain the sampling time point signal 22b by making a pulse having a narrow width at the time point when the pulses of the transmission signal 11a are counted by the number corresponding to.
【0058】サンプルホールド回路23・24は、受信
位相信号21aを各サンプリングして得られたレベル値
の信号を保持するとともに新たなサンプル毎にサンプル
したレベル値を更新して保持するようにした市販のサン
プルホールド素子であり、それぞれ、サンプルホールド
して得られるサンプルホールド信号23aとサンプルホ
ールド信号24aとをA/D変換回路31に与える。The sample-and-hold circuits 23 and 24 hold the signal of the level value obtained by sampling the reception phase signal 21a and update and hold the sampled level value for each new sample. The sample-hold signal 23a and the sample-hold signal 24a obtained by sample-holding are applied to the A / D conversion circuit 31.
【0059】図8において、受信位相信号21aの実線
で示す信号は、検出基準位相、つまり、検出位相0°の
場合を示し、破線で示す信号は、位相φ1と位相φ2だ
け偏移した信号を示しており、サンプル時点信号22a
とサンプル時点信号22bとの位相は、検出基準位相を
基準にしてみると、それぞれ、sin成分のレベルを得
る位相点とcos成分のレベルを得る位相点とに相当し
ていることになる。そして、90°/2相回路22とサ
ンプルホールド回路23・24で構成した部分は、90
独立/2相によるsin成分の信号とcos成分の信号
とを、それぞれ、受信位相信号21aに掛算した信号と
して、サンプルホールド信号23aとサンプルホールド
信号24aとを得ているものである。In FIG. 8, the signal shown by the solid line of the reception phase signal 21a shows the case of the detection reference phase, that is, the detection phase of 0 °, and the signal shown by the broken line is the signal shifted by only phase φ1 and phase φ2. Shown, the sample time point signal 22a
When the detection reference phase is used as a reference, the phases of the sampling time point signal 22b and the sampling time point signal 22b correspond to a phase point for obtaining the sin component level and a phase point for obtaining the cos component level, respectively. The 90 ° / 2-phase circuit 22 and the sample hold circuits 23 and 24 are
A sample hold signal 23a and a sample hold signal 24a are obtained as signals obtained by multiplying the signal of the sin component and the signal of the cos component by the independent / 2 phases by the reception phase signal 21a.
【0060】したがって、図9のように、検出基準位相
を真上0におき、位相角度を右回りに取った極座標で見
ると、サンプルホールド信号23aとサンプルホールド
信号24aとは、その各レベルの極性を図9のように置
いたことになり、位相φ1と位相φ2との角度値を極座
標値で検出していることになるものである。Therefore, as shown in FIG. 9, when the detection reference phase is set right above 0 and the polar angle is taken in the clockwise direction, the sample hold signal 23a and the sample hold signal 24a have the respective levels. The polarities are arranged as shown in FIG. 9, and the angle value between the phase φ1 and the phase φ2 is detected by the polar coordinate value.
【0061】A/D変換回路31では、サンプルホール
ド信号23a・24aとの各レベル値をディジタル値に
変換してCPU32に与える。In the A / D conversion circuit 31, each level value of the sample and hold signals 23a and 24a is converted into a digital value and given to the CPU 32.
【0062】CPU32は、A/D変換回路31からの
物標Eまでの距離値と、物標Eの変移量とに対応するデ
ィジタル値、つまり、ゲート計数信号27aにもとづく
ディジタル値と、サンプルホールド信号23a・24a
にもとづくディジタル値とをメモリに取り込んで記憶
し、これらディジタル値と、CPU32に予め記憶して
おいた所要の係数値とにもとづいて、計測距離値R
(i)と計測変移量r(i)とを計測し、これら計測値
にもとづいて、上記の第1実施例で説明したところの逐
次型最小二乗法による収束演算を適用した最適推定を演
算して、目的とする修正距離値R(N)を得る処理を行
い、得られた毎回の修正距離値R(N)を記憶保持す
る。The CPU 32 has a digital value corresponding to a distance value from the A / D conversion circuit 31 to the target E and a displacement amount of the target E, that is, a digital value based on the gate count signal 27a, and a sample hold. Signals 23a and 24a
Based on these digital values and the required coefficient values stored in advance in the CPU 32, the measured distance value R is stored.
(I) and the measured displacement amount r (i) are measured, and based on these measured values, the optimum estimation is applied by applying the convergence calculation by the recursive least squares method described in the first embodiment. Then, a process for obtaining a target corrected distance value R (N) is performed, and the obtained corrected distance value R (N) is stored and held.
【0063】CPU32に記憶した毎回の修正距離値R
(N)を読み出して得られるデータをプリンタ41で数
字印字し、または、読み出したデータをD/A変換して
得られるアナログ値のデータにもとづいて表示器43に
図2〜図4のような図形を表示するものである。Corrected distance value R stored in the CPU 32 every time
2 to 4 are displayed on the display 43 based on the analog value data obtained by D / A converting the data obtained by reading the data obtained by reading (N) with the printer 41. It is for displaying a figure.
【0064】上記の第2実施例を要約すると、第4の構
成として、上記の第1実施例で説明した第1の構成また
は第2の構成による距離計測方法において、図6の変調
波信号14aのように、1つの連続波、例えば、第1分
周信号12aのような波形の振幅を所要の周期、例え
ば、周期T1で部分的にパルス状に振幅変調した送信
波、例えば、パルスp1で変調した送信波を用い、上記
のパルス状の部分を上記の計測距離値を得るための送信
波とし、上記の連続波を上記の計測変移量を得るための
送信波として用いるようにした距離計測方法を提供する
ものである。To summarize the second embodiment described above, as the fourth configuration, in the distance measuring method according to the first configuration or the second configuration described in the first embodiment, the modulated wave signal 14a shown in FIG. 6 is used. As described above, with one continuous wave, for example, a transmission wave, for example, a pulse p1 in which the amplitude of a waveform such as the first frequency-divided signal 12a is partly pulse-modulated at a required period, for example, a period T1. Distance measurement using a modulated transmission wave, using the above-mentioned pulse-shaped portion as the transmission wave for obtaining the above measurement distance value, and using the above continuous wave as the transmission wave for obtaining the above measurement displacement amount It provides a method.
【0065】また、第5の構成として、上記の第4の構
成による距離計測方法において、上記の振幅変調を中間
の変調率、例えば、50%変調で変調した送信波を用い
るようにした距離計測方法を提供するものである。As a fifth configuration, in the distance measuring method according to the fourth configuration, the distance measurement is performed by using a transmission wave which is obtained by modulating the amplitude modulation with an intermediate modulation rate, for example, 50% modulation. It provides a method.
【0066】また、第6の構成として、上記の第1の構
成、第2の構成、第4の構成、第5の構成による距離計
測方法を用いる距離計測装置であって、上記の送信波を
送信するための送信回路、例えば、発振回路11・第1
分周回路12・第2分周回路13・変調回路14・送信
回路15などで構成した回路と、上記の送信波による反
射波を受信する受信回路、増幅回路18・振幅制限回路
20・検波回路25などで構成した回路と、上記の送信
波の周波数をもつ正弦波信号と余弦波信号とを得る基準
波回路、例えば、90°/2相回路22などで構成した
回路と、上記の受信回路により得られる反射波の周波数
信号を、上記の正弦波信号と余弦波信号とにもとづいて
検出することにより、例えば、サンプルホールド回路2
3・サンプルホールド回路24などで構成した回路によ
って、上記の計測変移量を得る変移量計測手段と、上記
の受信回路により得られる反射波のパルス信号と送信波
のパルス信号との間の時間量にもとづいて、例えば、比
較回路26・ゲート回路27などで構成した回路によ
り、上記の計測距離値を得る距離値計測手段と、上記の
計測変移量と計測距離値とにもとづいて、上記の演算式
による演算を、例えば、CPU32によって行うことに
より修正距離値を得る最適推定演算手段とを設けた距離
計測装置を提供するものである。A sixth structure is a distance measuring device using the distance measuring method according to the first structure, the second structure, the fourth structure, and the fifth structure described above, wherein Transmitting circuit for transmitting, for example, oscillating circuit 11 / first
A circuit composed of the frequency dividing circuit 12, the second frequency dividing circuit 13, the modulating circuit 14, the transmitting circuit 15 and the like, a receiving circuit for receiving the reflected wave of the transmitting wave, an amplifying circuit 18, an amplitude limiting circuit 20, and a detecting circuit. 25, a reference wave circuit that obtains a sine wave signal and a cosine wave signal having the frequency of the transmission wave, for example, a circuit that is configured by a 90 ° / 2-phase circuit 22 and the like, and the above reception circuit By detecting the frequency signal of the reflected wave obtained by the above method based on the sine wave signal and the cosine wave signal, for example, the sample hold circuit 2
3. The amount of time between the displacement amount measuring means for obtaining the above-mentioned measured displacement amount and the pulse signal of the reflected wave and the pulse signal of the transmitted wave, which are obtained by the receiving circuit, by the circuit configured by the sample hold circuit 24 and the like. On the basis of the above, for example, by the circuit configured by the comparison circuit 26 and the gate circuit 27, the distance value measuring means for obtaining the above measured distance value, and the above calculation based on the above measured displacement amount and measured distance value. The present invention provides a distance measuring device provided with an optimum estimation calculation means for obtaining a corrected distance value by performing a calculation by an expression by the CPU 32, for example.
【0067】また、第7の構成として、上記の第6の構
成による距離計測装置において、上記の変移量計測手段
と、距離値計測手段と、最適推定演算手段とを1つのC
PU、例えば、CPU32により演算する演算手段を設
けた距離計測装置を提供するものである。As a seventh configuration, in the distance measuring device according to the sixth configuration, the displacement amount measuring means, the distance value measuring means, and the optimum estimation calculating means are combined into one C.
The present invention provides a distance measuring device provided with a calculation unit that is calculated by a PU, for example, a CPU 32.
【0068】〔変形実施〕この発明は次のように変形し
て実施することができる。 (1)変移量の計測に用いる反射波が得られないことを
検出した出力により、距離計測用のパルス波を送信し、
または、距離計測用のパルス変調を行うように構成す
る。[Modified Implementation] The present invention can be modified and implemented as follows. (1) A pulse wave for distance measurement is transmitted by the output that detects that the reflected wave used for measuring the displacement amount cannot be obtained,
Alternatively, it is configured to perform pulse modulation for distance measurement.
【0069】(2)表示器43を、ディジタル値による
距離値表示器とアナログ値による距離値表示器とを設け
て構成し、アナログ値による距離値表示器を設ける。(2) The display unit 43 is constructed by providing a distance value display by digital value and a distance value display by analog value, and the distance value display by analog value is provided.
【0070】(3)上記(2)のアナログ表示器を、サ
ンプルホールド信号23a・24aのアナログ信号、ま
たは、D/A変換器42から得られるこれらの信号に対
応する各アナログ信号を、図9のように、ブラウン管の
X・Y偏向電極に所要の極性で与えることにより、位相
φ1・位相φ2などに対応する位相点像を表示して、周
辺に設けた単位距離目盛によって、距離値の小さい変化
状況を細かくアナログ的に読み取り得るようにする。ま
た、表示するアナログ値の信号を鋸歯状波にした波形に
することにより、位相線像にして見易く表示する。さら
に、ブラウン管に代え、2相式メータを用いて表示す
る。(3) The analog display of (2) above is converted into analog signals of the sample and hold signals 23a and 24a, or analog signals corresponding to these signals obtained from the D / A converter 42, as shown in FIG. As described above, by giving the X and Y deflection electrodes of the cathode ray tube with the required polarities, the phase point image corresponding to the phase φ1, the phase φ2, etc. is displayed, and the distance value is small by the unit distance scale provided in the periphery. Make it possible to read the change situation in a fine analog manner. Further, the displayed analog value signal is formed into a sawtooth wave so that a phase line image is displayed for easy viewing. Further, instead of the cathode ray tube, a two-phase meter is used for the display.
【0071】(4)90°/2相回路22とサンプルホ
ールド回路23・24とによって掛算出力を得る部分
を、90°/2相回路の出力を正弦波状の波形によるs
in成分信号とcos成分信号に変更し、サンプルホー
ルド回路23・24と掛算回路に変更するとともに、掛
算回路の出力を積分回路または濾波回路もしくはこれら
組み合わせに与えることによって、サンプルホールド信
号23a・24aと同様の掛算出力を得るように構成す
る。(4) The 90 ° / 2-phase circuit 22 and the sample-hold circuits 23 and 24 are used to obtain the multiplication calculation force, and the output of the 90 ° / 2-phase circuit is represented by a sine wave waveform.
By changing the in-component signal and the cos-component signal to the sample-hold circuits 23 and 24 and the multiplying circuit, and applying the output of the multiplying circuit to the integrating circuit, the filtering circuit, or a combination thereof, It is configured to obtain a similar multiplication calculation force.
【0072】(5)α−β−γトラッカのように距離と
方向との追尾を行う構成において、距離の追尾を行う部
分に、上記の各実施例および各変形実施の距離計測方法
または距離計測装置を用いて構成する。(5) In a configuration such as an α-β-γ tracker for tracking a distance and a direction, the distance measuring method or the distance measuring in each of the above-mentioned embodiments and each modified embodiment is performed in the portion for tracking the distance. Configured using the device.
【0073】(6)第1実施例または第2実施例の計測
変移量r(i)を得るアナログ計測部分を、受信周波数
fsを送信周波数f0と比較して得られる周波数の変化
量△fまたは位相の変化量△pを検出して、△fまたは
△pから対応する変移量を得るように構成する。(6) A variation amount Δf of the frequency obtained by comparing the reception frequency fs with the transmission frequency f0 in the analog measurement portion for obtaining the measurement displacement amount r (i) of the first or second embodiment. The phase change amount Δp is detected, and the corresponding shift amount is obtained from Δf or Δp.
【0074】(7)第2実施例における送信波A1のパ
ルスp1による変調を全振幅変調、つまり、100%変
調にするとともに、パルスp1のパルス幅t1を、サン
プルホールド信号23a・24aが目的を十分に目的を
果し得る程度の時間長になるように変更して構成する。
また、この構成の場合において、図7の送信波A1にお
ける短いt1の箇所が無振幅になるようにして形成し、
図7の受信パルス波信号25aを波形が逆転した波形に
して時間taを検出し、または、受信信号18aを逆検
波して図7の受信パルス波信号25aと同様の波形を得
るように構成する。この構成は、上記の第1の構成と第
2の構成のような距離計測方法において、1つの搬送波
の全振幅を所要の周期をもつパルスで振幅変調した送信
波を用い、このパルスの部分を上記の計測距離値を得る
ための送信波とし、また、このパルスの中に含まれる搬
送波を上記の計測変移量を得るための送信波として用い
るようにした距離計測方法を構成していることになる。(7) The modulation of the transmission wave A1 by the pulse p1 in the second embodiment is full amplitude modulation, that is, 100% modulation, and the pulse width t1 of the pulse p1 is set by the sample hold signals 23a and 24a. Change the configuration so that the time is long enough to achieve the purpose.
Further, in the case of this configuration, the short wave t1 in the transmission wave A1 of FIG. 7 is formed so as to have no amplitude,
The received pulse wave signal 25a shown in FIG. 7 is configured to have a reverse waveform to detect the time ta, or the received signal 18a is reversely detected to obtain the same waveform as the received pulse wave signal 25a shown in FIG. . In this configuration, in the distance measuring method as in the first configuration and the second configuration described above, a transmission wave in which the total amplitude of one carrier is amplitude-modulated with a pulse having a required period is used, and a part of this pulse is used. To configure a distance measuring method that uses a transmission wave for obtaining the above-mentioned measured distance value and uses a carrier wave included in this pulse as a transmission wave for obtaining the above-mentioned measurement displacement amount. Become.
【0075】(8)距離計測部1から送波する送信波
を、繰り返し周期Tを複数分割した区間毎に、順次に、
または、所定の順序で周波数を変化して得られる周波数
変調波形にするとともに、距離計測部1では、周波数変
調波形の周波数の変化点などを距離計測のための規定点
として検出することにより計測距離値を得るようにし、
また、変移計測部2では、周波数の変化している所定の
周波数または各周波数に対する受信信号中の周波数変化
量または位相変化量を検出することにより計測変移量を
得るように構成する。(8) The transmission wave transmitted from the distance measuring unit 1 is sequentially divided into a plurality of intervals of the repetition cycle T,
Alternatively, the measured distance is obtained by changing the frequency in a predetermined order to obtain a frequency-modulated waveform, and the distance measuring unit 1 detects a frequency change point of the frequency-modulated waveform as a specified point for distance measurement. To get the value,
Further, the shift measuring unit 2 is configured to obtain the measurement shift amount by detecting the amount of frequency change or the amount of phase change in the received signal for a predetermined frequency whose frequency is changing or each frequency.
【0076】(9)第2実施例または上記(8)の構成
において、反射波の受信信号の周波数を周波数変換して
得られる周波数の信号、例えば、スーパーヘテロダイン
増幅回路による中間周波数の信号を受信信号18aとし
て得るようにし、受信信号中の周波数変化量または位相
変化量を検出するための周波数信号または90°/2相
信号を得るための周期をもつ信号を、送信波の周波数か
ら周波数変換して得た信号または独立の発信器の周波数
の信号から得るように構成する。(9) In the configuration of the second embodiment or the above (8), a signal of a frequency obtained by frequency-converting the frequency of the received signal of the reflected wave, for example, an intermediate frequency signal by the superheterodyne amplifier circuit is received. The signal 18a is obtained, and the frequency signal for detecting the frequency change amount or the phase change amount in the received signal or the signal having the cycle for obtaining the 90 ° / 2-phase signal is frequency-converted from the frequency of the transmitted wave. It is configured to be obtained from the signal obtained by the above or a signal of the frequency of an independent oscillator.
【0077】(10)送信波の周期などを制御している
第1分周回路12・第2分周回路13・90°/2相回
路22に代えて、これらによる分周部分などを、CPU
32による計数処理で行うように構成する。また、この
場合、必要に応じて、発振回路11の発振信号11aに
代えて、CPU32のクロック信号を用いるように構成
する。この構成によれば、第7の構成のような距離計測
装置において、上記の送信波の周期の制御と、上記の変
移量計測手段と、距離値計測手段と、最適推定演算手段
とを1つのCPUにより演算する演算手段を設けた距離
計測装置を構成していることになる。(10) Instead of the first frequency dividing circuit 12, the second frequency dividing circuit 13, and the 90 ° / 2-phase circuit 22 which control the period of the transmitted wave, the frequency dividing portion by these is controlled by the CPU.
The counting process by 32 is performed. Further, in this case, the clock signal of the CPU 32 is used instead of the oscillation signal 11a of the oscillation circuit 11 as necessary. According to this configuration, in the distance measuring device as in the seventh configuration, the control of the cycle of the transmission wave, the displacement amount measuring means, the distance value measuring means, and the optimum estimation calculating means are combined into one unit. This constitutes a distance measuring device provided with a computing means for computing by the CPU.
【0078】(11)計測距離値を得る演算部分と、計
測変移量を得る演算部分と、最適推定演算処理を行う演
算部分とを、各別個のCPUを用いて演算するように構
成する。(11) The calculation part for obtaining the measured distance value, the calculation part for obtaining the measurement displacement amount, and the calculation part for performing the optimum estimation calculation process are configured to perform calculation using separate CPUs.
【0079】(12)計測距離値を得るための送信波
と、計測変移量を得るための送信波とを、別個の送信波
で行うともに、計測距離値を得るための回路部分と計測
偏移量を得るための回路部分とを独立した別個の回路に
して構成する。(12) The transmission wave for obtaining the measurement distance value and the transmission wave for obtaining the measurement displacement amount are performed by separate transmission waves, and the circuit portion and the measurement deviation for obtaining the measurement distance value are used. The circuit portion for obtaining the quantity is configured as an independent separate circuit.
【0080】[0080]
【発明の効果】この発明によれば、上記のように、パル
ス反射型距離計測とドップラー変移量計測とを係合する
とともに、最適推定に逐次型最小二乗法による収束演算
を行っているため、複雑な方程式を解くための非常に長
い演算が不要になるので、移動体の速度変化が速い場合
や移動データを綿密に得たい場合に対しても、オンライ
ン式の構成で行わせることができるなどの特長がある。According to the present invention, as described above, the pulse reflection type distance measurement and the Doppler displacement amount measurement are engaged, and the convergence calculation by the recursive least squares method is performed for the optimum estimation. Since an extremely long calculation for solving a complicated equation is not required, it is possible to use an online configuration even when the speed of the moving body changes rapidly or when you want to obtain detailed movement data. There is a feature of.
図面中、図1〜図9はこの発明の実施例を、また、図1
0〜図13は従来技術を示し、各図の内容は次のとおり
である。1 to 9 show an embodiment of the present invention, and FIG.
0 to 13 show the prior art, and the contents of each figure are as follows.
【図1】ブロック構成図FIG. 1 is a block diagram
【図2】計測結果のプロット図[Fig. 2] Plot diagram of measurement results
【図3】計測結果のプロット図[Fig. 3] Plot diagram of measurement results
【図4】計測結果のプロット図[Fig. 4] Plot diagram of measurement results
【図5】回路ブロック構成図FIG. 5 is a circuit block configuration diagram.
【図6】要部の信号波形図FIG. 6 is a signal waveform diagram of essential parts.
【図7】要部の信号波形図FIG. 7 is a signal waveform diagram of essential parts.
【図8】要部の信号波形図FIG. 8 is a signal waveform diagram of essential parts.
【図9】位相変化の極座標表示図FIG. 9: Polar coordinate display diagram of phase change
【図10】要部の信号波形図FIG. 10 is a signal waveform diagram of essential parts.
【図11】要部の信号波形図FIG. 11 is a signal waveform diagram of essential parts.
【図12】計測結果のプロット図FIG. 12: Plot diagram of measurement results
【図13】要部の信号波形図FIG. 13 is a signal waveform diagram of essential parts.
1 距離計測部 2 変移計測部 3 修正距離値演算部 4 表示部 11 発振回路 11a 発振信号 12 第1分周回路 12a 第1分周信号 13 第2分周回路 13a 第2分周信号 14 変調回路 14a 変調波信号 15 送信回路 16 送波器 17 受波器 18 増幅回路 18a 受信信号 20 振幅制限回路 21 濾波回路 21a 受信位相信号 22 90°/2相回路 22a サンプル時点信号 22b サンプル時点信号 23 サンプルホールド回路 23a サンプルホールド信号・sin成分信号 24 サンプルホールド回路 24a サンプルホールド信号・cos成分信号 25 検波回路 25a 受信パルス波信号 26 比較回路 26a 比較検出信号 27 ゲート回路 27a 時間量信号 31 A/D変換回路 32 CPU 41 プリンタ 42 D/A変換回路 43 表示器 A 送信パルス波 A1 送信波 B 受信パルス波 B1 反射波 C 送信波 D 受信波 T 周期 t0 周期 t1 パルス幅 p1 パルス p2 パルス 1 distance measuring unit 2 displacement measuring unit 3 corrected distance value calculating unit 4 display unit 11 oscillation circuit 11a oscillation signal 12 first frequency dividing circuit 12a first frequency dividing signal 13 second frequency dividing circuit 13a second frequency dividing signal 14 modulation circuit 14a Modulated wave signal 15 Transmitter circuit 16 Transmitter 17 Receiver 18 Amplifier circuit 18a Received signal 20 Amplitude limiting circuit 21 Filtering circuit 21a Received phase signal 22 90 ° / 2-phase circuit 22a Sample time point signal 22b Sample time point signal 23 Sample hold Circuit 23a Sample and hold signal / sin component signal 24 Sample and hold circuit 24a Sample and hold signal / cos component signal 25 Detection circuit 25a Received pulse wave signal 26 Comparison circuit 26a Comparison detection signal 27 Gate circuit 27a Time amount signal 31 A / D conversion circuit 32 CPU 41 Printer 42 D / A Circuit 43 display A transmitted pulse wave A1 transmission wave B receiving pulse wave B1 reflected wave C transmission wave D received wave T period t0 period t1 pulse width p1 pulse p2 pulse
Claims (10)
とともに、前記送信波の各周期の規定点から前記反射波
の前記規定点に対応する規定点までの時間量の測定値に
もとづいて得られる計測距離値を、送信波の周波数に対
する反射波の周波数変化量または位相変化量の測定値に
もとづいて得られる計測変移量で修正することにより修
正距離値を得る距離測定方法であって、 前記修正を行うための最適推定の演算を、逐次型最小二
乗法による収束を用いて演算することを特徴とする距離
計測方法。1. A reflected wave of a periodically repeated transmission wave is obtained, and based on a measured value of a time amount from a specified point of each cycle of the transmitted wave to a specified point corresponding to the specified point of the reflected wave. A distance measuring method for obtaining a corrected distance value by correcting the obtained measured distance value with a measured displacement amount obtained based on the measured value of the frequency change amount or the phase change amount of the reflected wave with respect to the frequency of the transmitted wave, A distance measuring method, characterized in that the calculation of the optimum estimation for performing the correction is performed by using the convergence by the recursive least squares method.
所定時点以後に得られる毎回の計測変移量をr(i)、
毎回の計測距離値をR(i)、また、修正距離値をR
c、誤差の二乗和が最小となる計測距離値の推定値を
「R(0,i)」として、演算式 Rc=「R(i)」=「R(0,i)」+r(i) により修正距離値を得る演算を行うことを特徴とする距
離計測方法。2. The distance measuring method according to claim 1, wherein an initial measured distance value obtained at a predetermined time point is R (0), and a measurement displacement amount obtained every time after the predetermined time point is r (i). ,
R (i) is the measured distance value for each time, and R is the corrected distance value.
c, the estimated value of the measured distance value that minimizes the sum of squared error is “R (0, i)”, and the arithmetic expression Rc = “R (i)” = “R (0, i)” + r (i) A distance measuring method, characterized in that a calculation for obtaining a corrected distance value is performed.
であって、 1つの連続波の振幅を所要の周期で部分的にパルス状に
振幅変調した送信波を用い、前記パルス状の部分を前記
計測距離値を得るための送信波とし、前記連続波を前記
計測変移量を得るための送信波として用いることを特徴
とする距離計測方法。3. The distance measuring method according to claim 1, wherein the amplitude of one continuous wave is partly pulse-modulated at a required period to form a pulse wave, and the pulse wave part is used. Is used as a transmission wave for obtaining the measurement distance value, and the continuous wave is used as a transmission wave for obtaining the measurement displacement amount.
ことを特徴とする距離計測方法。4. The distance measuring method according to claim 3, wherein a transmission wave obtained by modulating the amplitude modulation with an intermediate modulation rate is used.
であって、 1つの搬送波の全振幅を所要の周期をもつパルスで振幅
変調した送信波を用い、前記パルスの部分を前記計測距
離値を得るための送信波とし、前記パルスの中に含まれ
る前記搬送波を前記計測変移量を得るための送信波とし
て用いることを特徴とする距離計測方法。5. The distance measuring method according to claim 1 or 2, wherein a transmission wave in which the total amplitude of one carrier is amplitude-modulated with a pulse having a required period is used, and a portion of the pulse is used as the measured distance. A distance measuring method, wherein a transmission wave for obtaining a value is used, and the carrier wave included in the pulse is used as a transmission wave for obtaining the measurement displacement amount.
を用いる距離計測装置であって、 前記計測距離値を得るための時間量を測定する距離計測
部と、 前記計測変移量を得るための周波数変化量または位相変
化量を測定する変移計測部と、 前記時間量と、前記周波数変化量または位相変化量とに
もとづいて前記計測距離値と前記変化量とを計測すると
ともに、前記演算式にもとづく演算を行なって前記修正
距離値を得る修正距離値演算部とを具備することを特徴
とする距離計測装置。6. A distance measuring device using the distance measuring method according to claim 1 or 2, wherein a distance measuring section for measuring an amount of time for obtaining the measured distance value, and for obtaining the measured displacement amount. Of the displacement measurement unit that measures the amount of frequency change or the amount of phase change, the amount of time, and the measurement distance value and the amount of change based on the amount of frequency change or the amount of phase change, the arithmetic expression A distance measuring device, comprising: a corrected distance value calculation unit that performs a calculation based on the corrected distance value calculation unit.
5の距離計測方法を用いる距離計測装置であって、 前記計測距離値を得るための時間量を測定する距離計測
部と、 前記計測変移量を得るための周波数変化量または位相変
化量を測定する変移計測部と、 前記時間量と、前記周波数変化量または位相変化量とに
もとづいて前記計測距離値と前記変化量とを計測すると
ともに、前記演算式にもとづく演算を行なって前記修正
距離値を得る修正距離値演算部とを具備することを特徴
とする距離計測装置。7. A distance measuring device using the distance measuring method according to claim 3, 4, or 5, wherein a distance measuring unit for measuring an amount of time for obtaining the measured distance value; A displacement measuring unit that measures the amount of frequency change or the amount of phase change to obtain the amount, while measuring the time distance and the measured distance value and the amount of change based on the amount of frequency change or the amount of phase change. A distance measuring device for calculating a corrected distance value by performing a calculation based on the calculation formula.
って、 前記送信波を送信するための送信回路と、 前記送信波による反射波を受信する受信回路と、 前記送信波の周波数をもつ正弦波信号と余弦波信号とを
得る基準波回路と、 前記受信回路により得られる反射波の周波数信号を、前
記正弦波信号と前記余弦波信号とにもとづいて検出する
ことにより、前記計測変移量を得る変移量計測手段と、 前記受信回路により得られる前記反射波のパルス信号と
前記送信波のパルス信号との間の時間量にもとづいて前
記計測距離値を得る距離値計測手段と、 前記計測変移量と前記計測距離値とにもとづいて、前記
演算式による演算を行うことにより前記修正距離値を得
る最適推定演算手段とを具備することを特徴とする距離
計測装置。8. The distance measuring device according to claim 6, wherein the transmitting circuit transmits the transmitting wave, the receiving circuit receives the reflected wave of the transmitting wave, and the frequency of the transmitting wave. A reference wave circuit for obtaining a sine wave signal and a cosine wave signal having a frequency signal of a reflected wave obtained by the receiving circuit, based on the sine wave signal and the cosine wave signal, the measurement A displacement amount measuring unit for obtaining a displacement amount, a distance value measuring unit for obtaining the measured distance value based on the amount of time between the pulse signal of the reflected wave and the pulse signal of the transmitted wave obtained by the receiving circuit, A distance measuring device comprising: an optimum estimation calculation means for obtaining the corrected distance value by performing a calculation by the calculation formula based on the measured displacement amount and the measured distance value.
適推定演算手段とを1つのCPUにより演算する演算手
段を具備することを特徴とする距離計測装置。9. The distance measuring device according to claim 8, further comprising arithmetic means for arithmetically operating the displacement amount measuring means, the distance value measuring means, and the optimum estimation arithmetic means by one CPU. A characteristic distance measuring device.
記距離値計測手段と、前記最適推定演算手段とを1つの
CPUにより演算する演算手段を具備することを特徴と
する距離計測装置。10. The distance measuring device according to claim 8, wherein the control of the cycle of the transmitted wave, the displacement amount measuring means, the distance value measuring means, and the optimum estimation calculating means are performed by one CPU. A distance measuring device comprising a calculating means for calculating.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP14429093A JP3256332B2 (en) | 1993-05-24 | 1993-05-24 | Distance measuring method and distance measuring device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP14429093A JP3256332B2 (en) | 1993-05-24 | 1993-05-24 | Distance measuring method and distance measuring device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH06331733A true JPH06331733A (en) | 1994-12-02 |
| JP3256332B2 JP3256332B2 (en) | 2002-02-12 |
Family
ID=15358635
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP14429093A Expired - Fee Related JP3256332B2 (en) | 1993-05-24 | 1993-05-24 | Distance measuring method and distance measuring device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP3256332B2 (en) |
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| JP3256332B2 (en) | 2002-02-12 |
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