JPH0875854A - Distance measuring device - Google Patents
Distance measuring deviceInfo
- Publication number
- JPH0875854A JPH0875854A JP21504994A JP21504994A JPH0875854A JP H0875854 A JPH0875854 A JP H0875854A JP 21504994 A JP21504994 A JP 21504994A JP 21504994 A JP21504994 A JP 21504994A JP H0875854 A JPH0875854 A JP H0875854A
- Authority
- JP
- Japan
- Prior art keywords
- distance
- time
- distance measurement
- waveform
- distance measuring
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Granted
Links
- 230000000630 rising effect Effects 0.000 claims abstract description 18
- 238000005259 measurement Methods 0.000 claims description 64
- 238000012937 correction Methods 0.000 claims description 37
- 230000006870 function Effects 0.000 claims description 10
- 239000003990 capacitor Substances 0.000 description 6
- 238000000034 method Methods 0.000 description 6
- 238000010586 diagram Methods 0.000 description 5
- 229920006395 saturated elastomer Polymers 0.000 description 5
- 230000000694 effects Effects 0.000 description 2
- 230000003287 optical effect Effects 0.000 description 2
- 230000003321 amplification Effects 0.000 description 1
- 239000013256 coordination polymer Substances 0.000 description 1
- 230000007423 decrease Effects 0.000 description 1
- 238000001514 detection method Methods 0.000 description 1
- 230000004069 differentiation Effects 0.000 description 1
- 238000012544 monitoring process Methods 0.000 description 1
- 238000003199 nucleic acid amplification method Methods 0.000 description 1
- 230000001960 triggered effect Effects 0.000 description 1
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- Optical Radar Systems And Details Thereof (AREA)
Abstract
Description
【0001】[0001]
【産業上の利用分野】本発明は、測距信号の受信時刻判
定に伴う誤差を補正して計測精度を高めるようにした測
距装置に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a distance measuring device which corrects an error associated with a reception time determination of a distance measuring signal to improve measurement accuracy.
【0002】[0002]
【従来の技術】物体までの距離すなわち対物距離を計測
する場合に、距離計測対象に向けて照射した光が距離計
測対象にて反射されて戻るまでの時間を計測し、この時
間に光速を乗じて往復距離を求める光学式測距装置がよ
く用いられる。2. Description of the Related Art When measuring the distance to an object, that is, the object distance, the time until the light emitted toward the distance measurement target is reflected back by the distance measurement target is measured, and this time is multiplied by the speed of light. Optical rangefinders are often used to determine the round trip distance.
【0003】図4に示す光学式測距装置1は、光源であ
るレーザダイオード2を駆動回路3にて所定周期で間欠
発光させ、送光レンズ4を介してレーザ光を前方照射
し、同時にまたレーザダイオード2に対向配置したモニ
タ用のフォトダイオード5により発光タイミングすなわ
ち送光時刻を検知させる。モニタ用フォトダイオード5
の受光出力はコンパレータ6にてしきい値判別され、コ
ンパレータ6のしきい値判別出力をもって測距時間計数
用のカウンタ7が計数を開始する。レーザダイオード2
から出射されたレーザ光線は、距離計測対象である前方
車両等の物体8の表面で反射されて戻り、受光レンズ9
を通りフォトダイオード10にて受光される。フォトダ
イオード10の受光出力は、受信アンプ回路11にて増
幅された後、しきい値判別のためコンパレータ12に送
り込まれる。フォトダオード10の受光出力、厳密には
受信アンプ回路11の出力が、しきい値設定回路13に
よりコンパレータ12に設定されたしきい値Rfを越え
ると、レーザ光線の受光時刻に符合させてコンパレータ
12からカウンタ7に対し計数停止信号が供給され、こ
れにより測距信号であるレーザ光線が物体8までを往復
する間にカウンタ7が計数した計数値Nが得られる。カ
ウンタ7は、高精度のクロック周期τで発振するクロッ
ク信号に基づいて計数動作を行っており、計数値Nにク
ロック周期τを乗算することにより、レーザ光線が測距
装置1と物体8を往復するのに要した往復時間T(=N
τ)が求まる。本例の場合、この乗算はCPU14が行
うが、CPU14はまた乗算により得られた往復時間N
τに測距信号であるレーザ光の進行速度すなわち光速c
を乗算し、得られた往復距離Nτcを1/2倍して物体
8までの距離Nτc/2を求める。In an optical distance measuring apparatus 1 shown in FIG. 4, a laser diode 2 which is a light source is made to intermittently emit light by a driving circuit 3 at a predetermined cycle, and laser light is irradiated forward through a light transmitting lens 4 and at the same time. A light emitting timing, that is, a light sending time is detected by a monitoring photodiode 5 arranged opposite to the laser diode 2. Monitor photodiode 5
The received light output of is detected by the comparator 6 as a threshold value, and the counter 7 for counting the distance measurement time starts counting with the threshold value determination output of the comparator 6. Laser diode 2
The laser beam emitted from is reflected by the surface of an object 8 such as a vehicle in front of which the distance is to be measured and returns to the receiving lens 9
The light is received by the photodiode 10 through. The received light output of the photodiode 10 is amplified by the receiving amplifier circuit 11 and then sent to the comparator 12 for threshold value determination. When the light receiving output of the photo diode 10, strictly speaking, the output of the receiving amplifier circuit 11 exceeds the threshold value Rf set in the comparator 12 by the threshold value setting circuit 13, the light receiving time of the laser beam is matched with the comparator. A count stop signal is supplied from 12 to the counter 7, whereby a count value N counted by the counter 7 is obtained while the laser beam, which is a distance measurement signal, travels back and forth to the object 8. The counter 7 performs a counting operation based on a clock signal that oscillates at a highly accurate clock cycle τ, and a laser beam reciprocates between the distance measuring device 1 and the object 8 by multiplying the count value N by the clock cycle τ. Round-trip time T (= N
τ) is obtained. In the case of this example, this multiplication is performed by the CPU 14, but the CPU 14 also returns the round trip time N obtained by the multiplication.
In τ, the traveling speed of the laser light which is the distance measurement signal, that is, the speed of light c
The obtained round trip distance Nτc is multiplied by 1/2 to obtain the distance Nτc / 2 to the object 8.
【0004】[0004]
【発明が解決しようとする課題】上記従来の測距装置1
は、レーザ光線の発光時刻については、モニタ用フォト
ダオード5の出力に基づいて常に正確に把握できるが、
受光時刻については、フォトダイオード10の受光出力
を受信アンプ回路11で増幅して得られる受信信号をコ
ンパレータ12にてしきい値判別して決定する関係上、
同一距離にある物体8からの反射波であっても、照射さ
れたレーザ光線の全照射面積が図4に実線で示したよう
にすべて物体8に含まれるか、又は同図に点線で示した
ようにレーザ光線の照射面積の一部のみが物体8に照射
されるかによって受光波形が異なり、この受光波形の違
いが災いして受光時刻判別に誤差が避けられなかった。
例えば、図5に対比した送光波形と受光波形からも明ら
かなように、同じ送光波形のレーザ光線を用いて測距し
ても、測距装置1から同じ距離に置かれた物体8に照射
されるレーザ光線の照射面積が異なる場合、受光波形に
物体形状の影響が現れる。すなわち、同図に示す3種類
の波高値を有する受光波形は、同距離にある同一物体8
からの反射波形であり、最大の波高値を有する受光波形
は、物体8にレーザ光線すべてが入射して反射された場
合、すなわちレーザ光線の照射面積がすべて物体8に含
まれる場合の受光波形であり、基準波形に該当する。そ
こで、この基準波形がコンパレータ12に設定されたし
きい値を横切る点が測距時間誤差補正の基準点Toを与
えるものとしたときに、中間波高値の受光波形と最小波
高値の受光波形がコンパレータ12のしきい値Rfを横
切る点と前述の基準点Toとの間には、立ち上がり波形
の相違に基づく時間差ΔTa,ΔTbが歴然として存在
し、この差が受光時刻の判定ひいては距離計測の誤差原
因となっていた。DISCLOSURE OF THE INVENTION The above conventional distance measuring device 1
Can always accurately grasp the emission time of the laser beam based on the output of the monitor photodiode 5.
Regarding the light receiving time, because the received signal obtained by amplifying the light receiving output of the photodiode 10 by the receiving amplifier circuit 11 is determined by the threshold value judgment by the comparator 12,
Even for the reflected waves from the object 8 at the same distance, the entire irradiation area of the irradiated laser beam is all included in the object 8 as shown by the solid line in FIG. 4, or is shown by the dotted line in FIG. As described above, the received light waveform differs depending on whether only a part of the irradiation area of the laser beam is applied to the object 8, and the difference in the received light waveform damages the light reception time, and an error cannot be avoided.
For example, as is clear from the light-transmitting waveform and the light-receiving waveform which are compared with FIG. When the irradiation area of the irradiated laser beam is different, the influence of the object shape appears on the received light waveform. That is, the received light waveforms having the three types of peak values shown in the figure are the same object 8 at the same distance.
The received light waveform having a maximum peak value is the received light waveform when all the laser beams are incident on the object 8 and reflected, that is, when the irradiation area of the laser beam is entirely included in the object 8. Yes, it corresponds to the reference waveform. Therefore, when it is assumed that the point where this reference waveform crosses the threshold value set in the comparator 12 provides the reference point To for the distance measurement time error correction, the received light waveform of the intermediate peak value and the received light waveform of the minimum peak value are Between the point crossing the threshold value Rf of the comparator 12 and the above-mentioned reference point To, there are obvious time differences ΔTa and ΔTb based on the difference in the rising waveform, and this difference is an error in the determination of the light reception time and thus in the distance measurement error. It was the cause.
【0005】一方、受光波形の強度すなわち波高値に応
じてカウンタ7の計数値Nを補正し、しかも受光波形の
波高値による補正内容が適時修正できるようにした測距
装置が、特開昭63−266382号「レーザ測距装
置」に開示されている。このものは、反射信号の強度と
カウンタ7の計数値との関係を随時書き換え可能な特性
マップに保持するため、ドリフト等が発生した場合に特
性マップを書き換えて精度補償できるようになってい
る。しかしながら、例えば反射信号の強度が過大である
ためにフォトダイオード10が飽和してしまった場合、
反射信号の強度が正確には把握できなくなるために、距
離補正に有効な手掛かりが全く得られず、それ故に測距
精度を改善することができないといった課題があった。On the other hand, there is disclosed a distance measuring device in which the count value N of the counter 7 is corrected according to the intensity of the received light waveform, that is, the crest value, and the correction content based on the crest value of the received light waveform can be corrected in a timely manner. -266382 "Laser range finder". Since this one holds the relationship between the intensity of the reflected signal and the count value of the counter 7 in a rewritable characteristic map at any time, the characteristic map can be rewritten and accuracy can be compensated when a drift or the like occurs. However, for example, when the photodiode 10 is saturated because the intensity of the reflected signal is excessive,
Since the intensity of the reflected signal cannot be accurately grasped, no effective clue can be obtained for the distance correction, and therefore the ranging accuracy cannot be improved.
【0006】また、受光時刻の判定を鋸歯状波に近い受
光波形の頂点で行う構成の測距装置が、特開平3−73
880号「レーザ測距器」に開示されている。このもの
は、受光波形の頂点を判別するため、反射光のパワーが
最大となる点をもって受光波形の頂点と判定するもので
あるが、受光波形が鋸歯状波であるとの前提でパワー最
大点を求める構成であるため、鋸歯状波が鈍ってしまっ
たり飽和により台形波と化してしまった場合に、正確な
距離補正が困難である等の課題があった。また、パワー
最大点検出の導入契機となった前提技術として、受光波
形の時間微分値が正から負に反転する時点をもって受光
波形の頂点を検出する方法が記述され、距離計測対象ま
での距離が長くなったときに微分回路の出力が低下して
実用精度を割り込みやすい欠点が指摘されている。しか
しながら、こうした微分回路の出力反転を検出する方法
は、微分出力自体がさほど変化しない入力レベルの低迷
に対して弱いのは当然であり、またその反対に出力飽和
して微分値が零をとり続けたようなときは、微分値の極
性反転点の捕捉が困難になるために受光波形の頂点が正
確に検出できず、測距精度が落ちる欠点があった。Further, a distance measuring device having a structure in which the light receiving time is determined at the apex of a light receiving waveform close to a sawtooth wave is disclosed in Japanese Patent Laid-Open No. 3-73.
No. 880, "Laser Range Finder". This discriminates the apex of the received light waveform, so that the point where the power of the reflected light is maximum is determined as the apex of the received light waveform. However, it is assumed that the received light waveform is a sawtooth wave. However, when the sawtooth wave becomes dull or becomes a trapezoidal wave due to saturation, there is a problem that accurate distance correction is difficult. Also, as a prerequisite technology that triggered the introduction of the maximum power point detection, a method of detecting the peak of the received light waveform at the time when the time derivative of the received light waveform is inverted from positive to negative is described, and the distance to the distance measurement target is described. It has been pointed out that the output of the differentiating circuit is reduced when it becomes long and it is easy to interrupt the practical accuracy. However, it is natural that the method of detecting the output inversion of such a differentiating circuit is weak against the slump of the input level where the differential output itself does not change so much. On the contrary, the output is saturated and the differential value continues to take zero. In such a case, it is difficult to capture the polarity reversal point of the differential value, so that the apex of the received light waveform cannot be accurately detected, and there is a drawback that the distance measurement accuracy decreases.
【0007】[0007]
【課題を解決するための手段】本発明は、上記課題を解
決したものであり、距離計測対象に向けて送信した測距
信号が該距離計測対象で反射されて受信されるまでの往
復時間を計測し、該往復時間と該測距信号の進行速度と
から前記距離計測対象までの距離を演算する測距装置に
おいて、前記受信した測距信号を時間微分する微分回路
と、該微分回路の出力をピークホールドするピークホー
ルド回路と、該ピークホールド回路の出力に基づき、前
記往復時間の計測に及ぼす前記受信信号の立ち上がり波
形の影響を補正する測距時間誤差補正手段とを具備する
ことを特徴とするものである。DISCLOSURE OF THE INVENTION The present invention has solved the above-mentioned problems and provides a round-trip time until a distance-measuring signal transmitted to a distance-measuring object is reflected and received by the distance-measuring object. In a distance measuring device for measuring and calculating the distance to the distance measurement object from the round trip time and the traveling speed of the distance measuring signal, a differential circuit for time differentiating the received distance measuring signal, and an output of the differentiating circuit. A peak hold circuit for peak-holding, and a distance measurement time error correction means for correcting the influence of the rising waveform of the received signal on the round trip time measurement based on the output of the peak hold circuit. To do.
【0008】また、本発明は、前記測距時間誤差補正手
段が、前記ピークホールド回路の出力及び前記往復時間
との関数として規定された演算式に基づき、前記受信信
号の立ち上がり波形の影響を補正する補正データを演算
するCPUを含むこと、或いは前記ピークホールド回路
の出力と前記往復時間とをアドレスとし、前記受信信号
の立ち上がり波形の影響を補正する補正データが格納さ
れたメモリと、測距のつど前記メモリを読み出し制御す
るCPUとを含むこと等を、他の特徴とするものであ
る。Further, according to the present invention, the distance measuring time error correcting means corrects the influence of the rising waveform of the received signal on the basis of an arithmetic expression defined as a function of the output of the peak hold circuit and the round trip time. Or a memory for storing correction data for correcting the influence of the rising waveform of the received signal by using the output of the peak hold circuit and the round trip time as an address, and a distance measuring unit. Another feature is that it includes a CPU that controls the reading of the memory each time.
【0009】[0009]
【実施例】以下、本発明の実施例について、図1ないし
図3を参照して説明する。図1は、本発明の測距装置の
一実施例を示す回路構成図、図2は、図1に示したCP
Uが測距時間誤差の演算に用いる演算式をグラフ化して
示す図である。DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS An embodiment of the present invention will be described below with reference to FIGS. FIG. 1 is a circuit configuration diagram showing an embodiment of a distance measuring device of the present invention, and FIG. 2 is a CP shown in FIG.
It is a figure which shows in a graph the arithmetic expression which U uses for calculation of a ranging time error.
【0010】図1に示す測距装置21は、受信アンプ回
路11とCPU14の間に微分回路22とピークホール
ド回路23とAD変換器24を縦列接続し、CPU25
に受光波形の立ち上がり情報を取り込ませ、レーザ光線
の照射面積との関係に基づく測距時間誤差ΔTを補正す
る構成としたものである。CPU25は、往復時間Tの
計測に及ぼす受信信号の立ち上がり波形の影響を補正す
る測距時間誤差補正手段を構成しており、ピークホール
ド回路23の出力すなわち微分ピーク値Dpと往復時間
Tとの関数として規定された演算式ΔT=f(T,D
p)に基づき、受信信号の立ち上がり波形に付随する測
距時間誤差ΔTを演算し、これを補正データとして用い
る。In the distance measuring device 21 shown in FIG. 1, a differentiating circuit 22, a peak hold circuit 23 and an AD converter 24 are cascade-connected between the receiving amplifier circuit 11 and the CPU 14, and a CPU 25 is provided.
The rising information of the received light waveform is taken in to correct the distance measurement time error ΔT based on the relationship with the irradiation area of the laser beam. The CPU 25 constitutes a distance measurement time error correction means for correcting the influence of the rising waveform of the received signal on the measurement of the round trip time T, and is a function of the output of the peak hold circuit 23, that is, the differential peak value Dp and the round trip time T. Is defined as ΔT = f (T, D
Based on p), the distance measurement time error ΔT associated with the rising waveform of the received signal is calculated, and this is used as correction data.
【0011】微分回路22は、受信アンプ回路11の出
力を時間微分するものであり、出力端子と反転入力端子
が帰還抵抗R0を介して接続された演算増幅器22aの
非反転入力端子を接地し、受信アンプ回路11の出力を
微分コンデンサC0を介して反転入力端子に入力する構
成をとる。この微分回路22は、1/2πR0C0に折
点周波数を有し、入力信号の極性を反転して微分出力す
る反転型時間微分を行う。ピークホールド回路23は、
非反転入力端子を接地した演算増幅器23aの反転入力
端子に入力抵抗R1と帰還抵抗R2を接続して構成され
た反転増幅器(増幅率R2/R1)の出力を、整流用ダ
イオードDを介してホールドコンデンサC1に保持さ
せ、測距のつどCPU25により事後閉成されるリセッ
ト用スイッチSによりホールドコンデンサC1を放電さ
せる構成としたものであり、ホールドコンデンサC1に
は微分ピーク値Dpが保持される。AD変換器24は、
CPU25のビット数に対応した分解能を有しており、
ホールドコンデンサC1が保持する微分ピーク値Dpを
ディジタルデータに変換してCPU25に送り込む。C
PU25は、AD変換器24から送り込まれる微分ピー
ク値Dpから、受光波形の前縁部すなわち立ち上がり波
形がコンパレータ12のしきい値Rfを横切る点と、基
準波形に関する基準点Toとのずれすなちわ測距時間誤
差ΔTを、所定の演算式ΔT=f(T,Dp)に従って
割り出し、この測距時間誤差ΔTを補正データとして測
距値Nτc/2を(Nτ−ΔT)c/2のごとく補正す
る。The differentiating circuit 22 differentiates the output of the receiving amplifier circuit 11 with respect to time, and grounds the non-inverting input terminal of the operational amplifier 22a whose output terminal and inverting input terminal are connected via the feedback resistor R0. The configuration is such that the output of the reception amplifier circuit 11 is input to the inverting input terminal via the differential capacitor C0. The differentiating circuit 22 has an inversion frequency at 1 / 2πR0C0, and performs an inversion-type time differentiation in which the polarity of the input signal is inverted and differentially output. The peak hold circuit 23 is
The output of an inverting amplifier (amplification factor R2 / R1) configured by connecting an input resistor R1 and a feedback resistor R2 to the inverting input terminal of an operational amplifier 23a whose non-inverting input terminal is grounded is held via a rectifying diode D. The hold capacitor C1 is held by the capacitor C1, and the hold capacitor C1 is discharged by the reset switch S that is closed later by the CPU 25 each time the distance is measured. The hold capacitor C1 holds the differential peak value Dp. The AD converter 24 is
It has a resolution corresponding to the number of bits of the CPU 25,
The differential peak value Dp held by the hold capacitor C1 is converted into digital data and sent to the CPU 25. C
The PU 25 shifts the differential peak value Dp sent from the AD converter 24 from the point where the leading edge of the received light waveform, that is, the rising waveform, crosses the threshold value Rf of the comparator 12 and the reference point To related to the reference waveform. The distance measuring time error ΔT is calculated according to a predetermined arithmetic expression ΔT = f (T, Dp), and the distance measuring value Nτc / 2 is calculated as (Nτ−ΔT) c / 2 using this distance measuring time error ΔT as correction data. to correct.
【0012】測距時間誤差ΔTと微分ピーク値Dpの関
係は、図2に示したように、往復時間T(T1<T
2...<Tn)をパラメータにグラフ化することがで
き、実測値に基づいて作成した図2のグラフから、測距
時間誤差ΔTと往復時間T及び微分ピーク値Dpの間
に、 ΔT=f(T,Dp) なる関数関係を抽出することができる。この演算式が規
定する関係は、図2のグラフからも明らかなように、微
分ピーク値Dpが大きな値をとるほど、すなわち受光波
形の立ち上がりが急峻なほど基準波形に対する測距時間
誤差ΔTは小さな値で済み、また同じ微分ピーク値Dp
が得られる場合でも、測距装置21から物体8までの距
離が大となるほど(すなわち、往復時間Tが大となるほ
ど)、往復に伴う光減衰の影響をより強く受けるために
測距時間誤差ΔTは小さく抑えられる。As shown in FIG. 2, the relationship between the distance measurement time error ΔT and the differential peak value Dp is the round trip time T (T1 <T
2. . . <Tn) can be graphed as a parameter, and from the graph of FIG. 2 created based on the measured values, ΔT = f (T, T, f) between the distance measurement time error ΔT, the round trip time T and the differential peak value Dp. Dp) can be extracted. As is clear from the graph of FIG. 2, the relationship defined by this arithmetic expression is such that the larger the differential peak value Dp is, that is, the steeper the rising edge of the received light waveform, the smaller the distance measurement time error ΔT with respect to the reference waveform. Value, and the same differential peak value Dp
Even when the distance is obtained, as the distance from the distance measuring device 21 to the object 8 increases (that is, as the round trip time T increases), the distance measurement time error ΔT increases because the light attenuation due to the round trip is more strongly influenced. Can be kept small.
【0013】ここで、測距装置から同じ距離だけ離れた
位置にある同一物体8で、レーザ光線の照射面積が異な
る場合、図1に実線で示したように、レーザ光線がすべ
て物体8に照射されるときは、図5に示した最大波高値
を有する受光波形すなわち基準波形が得られるため、測
距時間誤差ΔTは零であり、測距値Nτc/2がそのま
ま距離データとして採用される。これに対し、図1に点
線で示したように、レーザ光線の照射面積の1/4又は
1/2しか物体8に照射されないときは、図5に示した
中以下の受光波形しか得られず、この受光波形がコンパ
レータ12のしきい値Rfと交差する点と基準点Toと
の間の時間ずれΔTa,ΔTbに相当する測距時間誤差
が、演算式ΔT=f(T,Dp)から求まる。こうして
得られた測距時間誤差ΔTa,ΔTbは往復時間Tに対
する補正データとして用いられ、CPU25はレーザ光
線の照射面積が1/2の場合は、(Nτ−ΔTa)c/
2のごとく測距補正を行い、レーザ光線の照射面積が1
/4の場合は、(Nτ−ΔTb)c/2のごとく測距補
正を行う。Here, when the same object 8 located at the same distance from the distance measuring device has a different irradiation area of the laser beam, as shown by the solid line in FIG. In this case, since the received light waveform having the maximum peak value shown in FIG. 5, that is, the reference waveform, is obtained, the distance measurement time error ΔT is zero, and the distance measurement value Nτc / 2 is directly used as the distance data. On the other hand, as shown by the dotted line in FIG. 1, when the object 8 is irradiated with only 1/4 or 1/2 of the irradiation area of the laser beam, only the light receiving waveforms in the middle and below shown in FIG. 5 are obtained. , The distance measurement time error corresponding to the time difference ΔTa, ΔTb between the point where this light receiving waveform intersects the threshold value Rf of the comparator 12 and the reference point To is obtained from the arithmetic expression ΔT = f (T, Dp). . The distance measurement time errors ΔTa and ΔTb thus obtained are used as correction data for the round trip time T, and when the irradiation area of the laser beam is ½, the CPU 25 (Nτ−ΔTa) c /
Distance correction is performed as shown in 2, and the irradiation area of the laser beam is 1
In the case of / 4, distance measurement correction is performed as in (Nτ-ΔTb) c / 2.
【0014】このように、上記測距装置21によれば、
物体8を往復する測距信号の往復時間Tに測距信号の進
行速度cを乗算して距離計測するときに、距離計測対象
で反射されて受信した測距信号を時間微分してピーク値
を保持し、この微分ピーク値Dpに基づき、往復時間T
の計測に及ぼす受光信号の立ち上がり波形の影響を補正
する構成としたから、同じ距離にありながらレーザ光線
の照射面積が異なるために受光波形に違いを見せる物体
8までの距離を、受光波形の違いによる測距時間誤差Δ
Tを補正して正確に計測することができ、受光波形が飽
和するほど近距離にある距離計測対象に関しても、受光
波形が立ち上がって飽和するまでの過程で得られる微分
ピーク値Dpから距離補正に必要なデータが確実に得ら
れるため、飽和に関係なく測距時間誤差の補正が可能で
あり、また受光波形の波高値が低く微分値もさほど変化
しない場合でも、微分ピーク値Dpから距離補正に必要
なデータが得られるため、相応の距離補正が可能であ
る。As described above, according to the distance measuring device 21,
When measuring the distance by multiplying the round-trip time T of the distance measurement signal that reciprocates the object 8 by the traveling speed c of the distance measurement signal, the distance measurement signal reflected and received by the distance measurement target is time differentiated to obtain the peak value. Hold, and based on this differential peak value Dp, round trip time T
Since the influence of the rising waveform of the received light signal on the measurement of is received is corrected, the distance to the object 8 that shows the difference in the received light waveform due to the different irradiation area of the laser beam at the same distance is the difference in the received light waveform. Distance measurement error due to Δ
It is possible to correct T and perform accurate measurement, and for a distance measurement target that is as close as the received light waveform is saturated, the differential peak value Dp obtained during the process until the received light waveform rises and becomes saturated is used for distance correction. Since the necessary data can be reliably obtained, the distance measurement time error can be corrected regardless of saturation, and even if the peak value of the received light waveform is low and the differential value does not change so much, the differential peak value Dp can be used for distance correction. Since the necessary data can be obtained, it is possible to perform appropriate distance correction.
【0015】また、測距時間誤差補正手段であるCPU
25が、ピークホールド回路23の出力Dpと往復時間
Tとの関数として規定された演算式ΔT=f(T,D
p)に基づき、受光信号の立ち上がり波形の影響を補正
する補正データを演算する構成としたから、関数f
(T,Dp)を、実測に基づいて経験値から割り出し、
演算式として最初から用意しておくことで、定式化され
た補正方式とCPU25の数値演算機能とにより短時間
で正確な補正が可能である。Further, a CPU which is a distance measuring time error correcting means.
25 is an arithmetic expression ΔT = f (T, D defined as a function of the output Dp of the peak hold circuit 23 and the round trip time T.
Since the correction data for correcting the influence of the rising waveform of the received light signal is calculated based on p), the function f
(T, Dp) is calculated from the empirical value based on the actual measurement,
By preparing the calculation formula from the beginning, it is possible to perform accurate correction in a short time by the formulated correction method and the numerical calculation function of the CPU 25.
【0016】なお、上記実施例では、微分ピーク値Dp
に対応する測距時間誤差ΔTを、CPU25が所定の演
算式ΔT=f(T,Dp)に従って演算する構成とした
が、図3に示す測距装置31のごとく、微分ピーク値D
pに対応する測距時間誤差ΔTを、時間微分値Dpと往
復時間TをアドレスとしてROM等のメモリ32に書き
込んでおき、測距のつどCPU14からの指令でメモリ
32を読み出し制御する構成とすることもできる。この
場合、特別な演算式は不要となり、メモリ32から機械
的に測距時間誤差ΔTを読み出すことで補正データが得
られるため、CPU25の演算負担を軽減し、なおかつ
迅速かつ確実な距離補正が可能となる。In the above embodiment, the differential peak value Dp
The CPU 25 calculates the distance measurement time error ΔT in accordance with the predetermined calculation formula ΔT = f (T, Dp). However, as in the distance measurement device 31 shown in FIG.
The distance measurement time error ΔT corresponding to p is written in the memory 32 such as a ROM by using the time differential value Dp and the round trip time T as addresses, and the memory 32 is read out and controlled by a command from the CPU 14 each time the distance measurement is performed. You can also In this case, no special arithmetic expression is required, and the correction data can be obtained by mechanically reading the distance measurement time error ΔT from the memory 32. Therefore, the calculation load on the CPU 25 can be reduced, and quick and reliable distance correction can be performed. Becomes
【0017】さらにまた、上記両実施例では、微分回路
22やピークホールド回路23をアナログ回路で構成し
たが、これらアナログ回路の機能をソフトウェア処理に
よってCPU25に代替させることもできる。Furthermore, in both of the above embodiments, the differentiating circuit 22 and the peak hold circuit 23 are analog circuits, but the functions of these analog circuits can be replaced by the CPU 25 by software processing.
【0018】[0018]
【発明の効果】以上説明したように、本発明によれば、
距離計測対象を往復する測距信号の往復時間と測距信号
の進行速度とから距離計測するときに、距離計測対象で
反射されて受信した測距信号を時間微分してピーク値を
保持し、この微分ピーク値に基づき、前記往復時間の計
測に及ぼす前記受信信号の立ち上がり波形の影響を補正
する構成としたから、同じ距離にありながらレーザ光線
の照射面積が異なるために受信波形に違いを見せる物体
までの距離を、受信波形の違いによる測距時間誤差を補
正して正確に計測することができ、受信波形が飽和する
ほど近距離にある距離計測対象に関しても、受信波形が
立ち上がって飽和するまでの過程で得られる微分ピーク
値から距離補正に必要なデータが確実に得られるため、
飽和に関係なく測距時間誤差の補正が可能であり、また
受信波形の波高値が低く微分値もさほど変化しない場合
でも、微分ピーク値から距離補正に必要なデータが得ら
れるため、相応の距離補正が可能である等の優れた効果
を奏する。As described above, according to the present invention,
When measuring the distance from the round-trip time of the distance measurement signal that travels back and forth to the distance measurement target and the traveling speed of the distance measurement signal, the distance measurement signal reflected and received by the distance measurement target is time-differentiated to hold the peak value, Based on this differential peak value, the influence of the rising waveform of the received signal on the measurement of the round-trip time is corrected, so that the received waveform shows a difference because the irradiation area of the laser beam is different even at the same distance. The distance to the object can be measured accurately by correcting the distance measurement time error due to the difference in the received waveform, and the received waveform rises and saturates even for distance measurement targets that are as close as the received waveform is saturated. Since the data required for distance correction can be reliably obtained from the differential peak value obtained in the process up to
It is possible to correct the distance measurement time error regardless of saturation, and even if the peak value of the received waveform is low and the differential value does not change so much, the data required for distance correction can be obtained from the differential peak value. An excellent effect such as correction is possible.
【0019】また、本発明は、測距時間誤差補正手段
を、ピークホールド回路の出力と往復時間との関数とし
て規定された演算式に基づき、受信信号の立ち上がり波
形の影響を補正する補正データを演算するCPUで構成
したから、受信波形の時間微分値のピークすなわち微分
ピーク値と往復時間の関数を、実測に基づいて経験値か
ら割り出し、演算式として最初から用意しておくこと
で、定式化された補正方式とCPUの数値演算機能とに
より短時間で正確な補正が可能である等の効果を奏す
る。Further, according to the present invention, the distance measurement time error correction means uses the correction data for correcting the influence of the rising waveform of the received signal based on the arithmetic expression defined as a function of the output of the peak hold circuit and the round trip time. Since it is composed of a CPU for calculation, the peak of the time-differential value of the received waveform, that is, the function of the differential peak value and the round-trip time is calculated from the empirical value based on the actual measurement, and is prepared from the beginning as a calculation formula. The correction method and the numerical operation function of the CPU provide an effect that accurate correction can be performed in a short time.
【0020】さらにまた、本発明は、測距時間誤差補正
手段を、ピークホールド回路の出力と往復時間とをアド
レスとし、受信信号の立ち上がり波形の影響を補正する
補正データが格納されたメモリと、測距のつど該メモリ
を読み出し制御するCPUとから構成したから、受信波
形の時間微分値のピークすなわち微分ピーク値と往復時
間とをアドレスとして、実測に基づいて得られた経験値
から割り出された補正データを書き込んでおいたメモリ
を用意することにより、特別な演算式を用いることな
く、指定アドレスから機械的に補正データを読み出すこ
とができ、これによりCPUの演算負担を軽減し、なお
かつ迅速かつ確実な距離補正が可能である等の効果を奏
する。Further, according to the present invention, the distance measurement time error correction means has a memory in which correction data for correcting the influence of the rising waveform of the received signal is stored, with the output of the peak hold circuit and the round trip time as addresses. Each time the distance is measured, the memory is configured to read and control the CPU. Therefore, the peak of the time-differential value of the received waveform, that is, the differential peak value and the round-trip time is used as an address and is calculated from the empirical value obtained based on the actual measurement. By preparing the memory in which the correction data is written, the correction data can be mechanically read from the specified address without using a special calculation formula, thereby reducing the calculation load on the CPU and speedily. In addition, it is possible to perform a reliable distance correction.
【図1】本発明の測距装置の一実施例を示す回路構成図
である。FIG. 1 is a circuit configuration diagram showing an embodiment of a distance measuring device of the present invention.
【図2】図1に示したCPUが測距時間誤差の演算に用
いる演算式をグラフ化して示す図である。FIG. 2 is a graph showing an arithmetic expression used by a CPU shown in FIG. 1 for calculating a distance measurement time error.
【図3】本発明の測距装置の変形例を示す回路構成図で
ある。FIG. 3 is a circuit configuration diagram showing a modified example of the distance measuring device of the present invention.
【図4】従来の測距装置の一例を示す回路構成図であ
る。FIG. 4 is a circuit configuration diagram showing an example of a conventional distance measuring device.
【図5】測距信号の送光波形と受光波形を示す波形図で
ある。FIG. 5 is a waveform diagram showing a light transmitting waveform and a light receiving waveform of a distance measurement signal.
2 レーザダイオード 3 駆動回路 4 送光レンズ 5 フォトダイオード 6 コンパレータ 7 カウンタ 8 物体 9 受光レンズ 10 フォトダイオード 11 受信アンプ回路 12 コンパレータ 13 しきい値設定回路 21,31 測距装置 22 微分回路 23 ピークホールド回路 24 AD変換器 25 測距時間誤差補正手段(CPU) 32 測距時間誤差補正手段(メモリ) 2 laser diode 3 drive circuit 4 light transmitting lens 5 photo diode 6 comparator 7 counter 8 object 9 light receiving lens 10 photo diode 11 receiving amplifier circuit 12 comparator 13 threshold value setting circuit 21, 31 range finder 22 differentiating circuit 23 peak hold circuit 24 AD converter 25 Distance measuring time error correcting means (CPU) 32 Distance measuring time error correcting means (memory)
Claims (3)
が該距離計測対象で反射されて受信されるまでの往復時
間を計測し、該往復時間と該測距信号の進行速度とから
前記距離計測対象までの距離を演算する測距装置におい
て、前記受信した測距信号を時間微分する微分回路と、
該微分回路の出力をピークホールドするピークホールド
回路と、該ピークホールド回路の出力に基づき、前記往
復時間の計測に及ぼす前記受信信号の立ち上がり波形の
影響を補正する測距時間誤差補正手段とを具備すること
を特徴とする測距装置。1. A round trip time until a distance measurement signal transmitted to a distance measurement target is reflected and received by the distance measurement target is measured, and the round trip time and the traveling speed of the distance measurement signal are used to calculate the round trip time. In a distance measuring device that calculates a distance to a distance measurement target, a differentiating circuit that time-differentiates the received distance measuring signal,
A peak hold circuit for peak-holding the output of the differentiating circuit, and a distance-measuring time error correction means for correcting the influence of the rising waveform of the received signal on the measurement of the round-trip time based on the output of the peak-hold circuit. A distance measuring device characterized by:
クホールド回路の出力及び前記往復時間の関数として規
定された演算式に基づき、前記受信信号の立ち上がり波
形の影響を補正する補正データを演算するCPUを含む
ことを特徴とする請求項1記載の測距装置。2. The distance measurement time error correction means calculates correction data for correcting the influence of the rising waveform of the received signal based on an arithmetic expression defined as a function of the output of the peak hold circuit and the round trip time. The distance measuring apparatus according to claim 1, further comprising a CPU that operates.
クホールド回路の出力と前記往復時間とをアドレスと
し、前記受信信号の立ち上がり波形の影響を補正する補
正データが格納されたメモリと、測距のつど前記メモリ
を読み出し制御するCPUを含むことを特徴とする請求
項1記載の測距装置。3. The distance measurement time error correction means uses the output of the peak hold circuit and the round trip time as an address, and a memory that stores correction data for correcting the influence of the rising waveform of the received signal, The distance measuring device according to claim 1, further comprising a CPU that controls reading of the memory each time the distance is increased.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP21504994A JP3156518B2 (en) | 1994-09-08 | 1994-09-08 | Distance measuring device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP21504994A JP3156518B2 (en) | 1994-09-08 | 1994-09-08 | Distance measuring device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH0875854A true JPH0875854A (en) | 1996-03-22 |
| JP3156518B2 JP3156518B2 (en) | 2001-04-16 |
Family
ID=16665918
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| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP21504994A Expired - Fee Related JP3156518B2 (en) | 1994-09-08 | 1994-09-08 | Distance measuring device |
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| Country | Link |
|---|---|
| JP (1) | JP3156518B2 (en) |
Cited By (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2007093210A (en) * | 2005-09-26 | 2007-04-12 | Topcon Corp | Surveying device and surveying method |
| JP2010210522A (en) * | 2009-03-11 | 2010-09-24 | Sogo Keibi Hosho Co Ltd | Time stamp function adding apparatus for laser range sensor |
| WO2017042991A1 (en) * | 2015-09-07 | 2017-03-16 | ソニー株式会社 | Peak value detection apparatus and peak value detection method |
| WO2025115368A1 (en) * | 2023-11-30 | 2025-06-05 | パナソニックIpマネジメント株式会社 | Distance measuring device and distance measuring method |
-
1994
- 1994-09-08 JP JP21504994A patent/JP3156518B2/en not_active Expired - Fee Related
Cited By (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2007093210A (en) * | 2005-09-26 | 2007-04-12 | Topcon Corp | Surveying device and surveying method |
| JP2010210522A (en) * | 2009-03-11 | 2010-09-24 | Sogo Keibi Hosho Co Ltd | Time stamp function adding apparatus for laser range sensor |
| WO2017042991A1 (en) * | 2015-09-07 | 2017-03-16 | ソニー株式会社 | Peak value detection apparatus and peak value detection method |
| WO2025115368A1 (en) * | 2023-11-30 | 2025-06-05 | パナソニックIpマネジメント株式会社 | Distance measuring device and distance measuring method |
Also Published As
| Publication number | Publication date |
|---|---|
| JP3156518B2 (en) | 2001-04-16 |
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