JPS6379010A - Distance measuring apparatus - Google Patents

Distance measuring apparatus

Info

Publication number
JPS6379010A
JPS6379010A JP61224179A JP22417986A JPS6379010A JP S6379010 A JPS6379010 A JP S6379010A JP 61224179 A JP61224179 A JP 61224179A JP 22417986 A JP22417986 A JP 22417986A JP S6379010 A JPS6379010 A JP S6379010A
Authority
JP
Japan
Prior art keywords
light
distance measurement
distance
noise
pulse
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP61224179A
Other languages
Japanese (ja)
Inventor
Juichi Yoneyama
米山 寿一
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Nikon Corp
Original Assignee
Nikon Corp
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Nikon Corp filed Critical Nikon Corp
Priority to JP61224179A priority Critical patent/JPS6379010A/en
Publication of JPS6379010A publication Critical patent/JPS6379010A/en
Pending legal-status Critical Current

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  • Automatic Focus Adjustment (AREA)
  • Length Measuring Devices By Optical Means (AREA)
  • Measurement Of Optical Distance (AREA)
  • Focusing (AREA)

Abstract

PURPOSE:To enable accurate measurement of distance regardless of pulse-like noise received, by a method wherein the measurement of distance by the emission of light beam is repeated twice continuously and the third distance measurement is performed at a timing avoiding the incidence of noise light when the results of the measurement differ. CONSTITUTION:When a shutter release of a camera is depressed, a clock pulse is supplied from a terminal 7 and a decoder 4 generates an emission driving pulse 8 at a specified timing to emit light with a driving circuit 2 from a light emitting element 1. Then, the decoder 4 generates a driving pulse 9 at a timing after the passage of a specified time to emit second pulse light from the element 1. On the other hand, a light receiving element 11 receives reflected light of the emission light from an object to compute 13 distance and the results of the measurement is latched by latch circuits 14 and 15 respectively. Outputs of the circuits 14 and 15 are applied to a coincidence judging circuit 16 and outputs an H level to make an AND gate 6 for passage when non-coincidence is judged and a driving pulse 10 is generated from the decoder 4 at a specified timing avoiding the incidence of noise light. The results of the third distance measurement are latched by the circuit 14 to be a distance measurement output 17.

Description

【発明の詳細な説明】 (産業上の利用分野〉 本発明は、カメラのオートフォーカス等に用いられる測
距装置に関する。
DETAILED DESCRIPTION OF THE INVENTION (Industrial Field of Application) The present invention relates to a distance measuring device used for autofocus of a camera and the like.

(従来技術) 従来、カメラ等で用いられる測距装置に市っては、三角
測距方式に基づき発光素子からパルス光を被写体に発射
し、被写体からの反則光を発光素子に対し基線長だけ離
れた位置に配置した受光素子で受光し、反射光の受光位
置によって被写体までの距離を測定するようにしている
(Prior Art) Conventionally, distance measuring devices used in cameras, etc., use a triangular distance measuring method to emit pulsed light from a light-emitting element to a subject, and then direct the reflected light from the subject to the light-emitting element by a baseline length. Light is received by a light-receiving element placed at a distant position, and the distance to the subject is measured based on the receiving position of the reflected light.

(発明が解決しようとする問題点) しかしながら、このような従来の測距装置に必っては、
被写体が蛍光灯等で照明されている場合には、照明光も
受光素子に入射され、蛍光灯の場合、照明光も一種のパ
ルス光となるため、測距用のパルス光と照明によるパル
ス光のタイミングが重なると、測距用の受光信号と照明
光による雑音信号との分離が不可能であり、照明光によ
って誤った測距結果を生ずるという問題がおった。
(Problems to be solved by the invention) However, such conventional distance measuring devices always have the following problems:
When the subject is illuminated with a fluorescent lamp, etc., the illumination light also enters the light receiving element, and in the case of fluorescent lamps, the illumination light also becomes a kind of pulsed light, so the pulsed light for distance measurement and the pulsed light from the illumination are separated. If the timings of the two overlap, it is impossible to separate the light reception signal for distance measurement from the noise signal caused by the illumination light, and a problem arises in that the illumination light causes erroneous distance measurement results.

(問題点を解決するための手段〉 本発明は、このような従来の問題点に鑑みてなされたも
ので、照明等によりパルス性のノイズ光の入射を受けて
も正確に被写体までの距離を測定できるようにしだ測距
装置を提供することを目的とする。
(Means for Solving the Problems) The present invention has been made in view of such conventional problems, and it is possible to accurately measure the distance to an object even when pulsed noise light is incident from illumination or the like. The object of the present invention is to provide a distance measuring device that can perform measurements.

この目的を達成するため本発明におっては、発光素子か
ら光ビームを発射し、被写体からの反射光を受光素子で
受光して受光信号から被写体までの距離を演算する測距
装置において、光ビームの発射による測距を連続して2
回行ない、第1回目と第2回目の測距結果が異なったと
きには、ノイズ光により誤った測距が行なわれたものと
判断して、第3回目の測距をノイズ光の入射を受けない
所定のタイミングで行なうようにしたものである。
To achieve this objective, the present invention provides a distance measuring device that emits a light beam from a light emitting element, receives reflected light from a subject with a light receiving element, and calculates the distance to the subject from the received light signal. Continuous distance measurement by beam firing 2 times
If the first and second distance measurement results are different, it is determined that the distance measurement was incorrect due to noise light, and the third distance measurement is performed without receiving the noise light. This is done at a predetermined timing.

(作用) このような本発明の構成によれば、第1回目と第2回目
の測距結果が異なっていれば、いずれかの測距で蛍光灯
等の照明光によるノイズ光の受光による誤った測距が行
なわれたことが判定でき、この場合には、例えば蛍光灯
の照明光についてはノイズ光のパルス幅及び周期が予め
分っていることから、ノイズ光の入射を受けない所定の
タイミングで第3回目の測距を行なうこととなり、第3
回目の測距によりノイズ光の影響を受けない正しい測距
結果が得られる。
(Function) According to the configuration of the present invention, if the first and second distance measurement results are different, an error due to reception of noise light due to illumination light such as a fluorescent lamp may be detected in one of the distance measurements. In this case, for example, since the pulse width and period of the noise light are known in advance for the illumination light of a fluorescent lamp, a predetermined distance measurement that is not subject to the incidence of noise light can be determined. It was decided to conduct the third distance measurement at the timing, and the third distance measurement was carried out.
Correct distance measurement results that are not affected by noise light can be obtained by the second distance measurement.

勿論、第1回目と第2回目の測距結果が一致していれば
、いずれの測距結果も正しいものと判定して第3回目の
測距は行なわないこととなる。
Of course, if the first and second distance measurement results match, both distance measurement results will be determined to be correct and the third distance measurement will not be performed.

(実施例) 第1図は本発明の一実施例を示したブロック図でおる。(Example) FIG. 1 is a block diagram showing one embodiment of the present invention.

まず構成を説明すると、1は発光素子であり、駆動回路
2に対する発光駆動パルスに基づいて被写体に向けて所
定パルス幅TWのパルス光を発射する。この駆動回路2
による発光素子1の発光駆動はカウンタ3、デコーダ4
、ORゲート5及びANDゲート6で成る回路部で行な
われる。
First, the configuration will be described. Reference numeral 1 denotes a light emitting element, which emits pulsed light having a predetermined pulse width TW toward a subject based on a light emission drive pulse sent to a drive circuit 2. This drive circuit 2
The light emission drive of the light emitting element 1 is performed by a counter 3 and a decoder 4.
, an OR gate 5 and an AND gate 6.

即ち、カメラのシャッターレリーズ釦を押すと測距制御
が囲始され、カウンタ3に対し端子7よりタロツクパル
スが供給され、カウンタ3がこのクロックパルスの計数
を行なう。カウンタ3の計数値はデコーダ4で解読され
、デコーダ4は所定のタイミングとなる時刻toでパル
ス幅Twの発光駆動パルス8を発生し、ORゲート5を
介して駆動回路2により発光素子1を発光して第1回目
の発光駆動を行なう。また、デコーダ4には時刻toに
おける第1回目の発光駆動から所定時間T1を経過した
時刻t1のタイミングで同じくパルス幅TWの駆動パル
ス9を発生し、ORゲート5を介して駆動回路2を作動
することで発光素子1により第2回目のパルス光を被写
体に発射する。
That is, when the shutter release button of the camera is pressed, distance measurement control is started, and a clock pulse is supplied to the counter 3 from the terminal 7, and the counter 3 counts this clock pulse. The count value of the counter 3 is decoded by a decoder 4, and the decoder 4 generates a light emission drive pulse 8 with a pulse width Tw at a predetermined timing to, and causes the light emitting element 1 to emit light by the drive circuit 2 via an OR gate 5. Then, the first light emission drive is performed. Further, the decoder 4 generates a drive pulse 9 having the same pulse width TW at the timing t1, which is a predetermined time T1 after the first light emission drive at the time to, and activates the drive circuit 2 via the OR gate 5. By doing so, the light emitting element 1 emits the second pulsed light to the subject.

更に、デコーダ4には時刻t1の第2回目のパルス発光
から例えば照明によるノイズ光として螢光灯を例にとる
と、螢光灯の発光パルス幅及び繰り返し周期に基づいて
予め設定したT2時間経過後の時刻t2のタイミングで
パルス幅Twとなる第3回目の発光駆動パルス10を出
力するようになり、゛この第3回目の発光駆動パルス1
0はANDゲート6が許容状態におることを条件にOR
ゲート5を介して駆動回路2に供給され、駆動回路2に
より発光素子1を駆動して第3回目の発光駆動を行なう
ようになる。
Further, the decoder 4 records the elapsed time T2, which is preset based on the emission pulse width and repetition period of the fluorescent lamp, from the second pulse emission at time t1, for example, in the case of a fluorescent lamp as noise light caused by illumination. At the later timing t2, the third light emission drive pulse 10 having the pulse width Tw is outputted, and 'this third light emission drive pulse 1
0 is OR on the condition that AND gate 6 is in the allowable state.
The light is supplied to the drive circuit 2 through the gate 5, and the drive circuit 2 drives the light emitting element 1 to perform the third light emission drive.

一方、発光素子1に対し基線長離れた位置には受光素子
11が配置され、発光素子1から発射された光パルスの
被写体による反射光を受光し、増幅器12で信号増幅を
行なった後、演算回路13に増幅信号を与えて被写体ま
での距離を演算するようにしている。演算回路13て演
算された測距結果は、第1回目の発光駆動による測距結
果についてはラッチ回路14にラッチされる。ラッチ回
路14のラッチ駆動はORゲート20と単安定マルチバ
イブレータ21で行なわれ、デコーダ4より出力される
第1回目の発光駆動パルスを所定時間遅延したラッチパ
ルスをラッチ回路14に与え、演算回路13から得られ
た第1回目の測距結果をラッチする。また、演算回路1
3の出力はラッチ回路15にも与えられており、ラッチ
回路15は第2回目の発光駆動で得られた測距結果をラ
ッチする。そのためラッチ回路15に対してデコーダ4
から得られた第2回目の発光駆動パルス9が単安定マル
チバイブレータ22で所定の時間遅延を受けてラッチパ
ルスとして与えられている。ラッチ回路14及び15の
出力は一致判定回路16に与えられており、ラッチ回路
′14と15にラッチされた第1回目と第2回目の測距
結果が一致したときには一致判定回路6はLレベル出力
を生じ、この一致判定回路16の出力はANDゲート6
に入力されていることから、ANDゲート6が禁止状態
となり、デコーダ4からの第3回目の発光駆動パルス1
0の駆動回路2に対する出力を禁止するようになる。一
方、一致判定回路16で第1回目と第2回目の測距結果
の不一致を判定したときには、一致判定回路16の出力
はHレベルとなり、ANDゲート6を許容状態としてデ
コーダ4から出力される第3回目の発光駆動パルスの出
力を許容し、発光素子1による第3回目の発光駆動を行
なわせるようになる。このように一致判定回路16が第
1回目と第2回目の測距結果の不一致を判別して第3回
目の発光駆動を行なわせたときに演算回路13から得ら
れた第3回目の測距結果は、ラッチ回路14にラッチさ
れる。こQラッチ回路14に対する第3回目の測距結果
のラッチのため、ANDゲート6の出力はORゲート2
0に入力されてあり、第3回目の発光駆動パルス10の
出力時にも単安定マルチバイブレータ21よりラッチ回
路14にラッチパルスが与えられて演算回路13で得ら
れた第3回目の測距結果をラッチするようになる。
On the other hand, a light-receiving element 11 is arranged at a position separated from the light-emitting element 1 by a baseline length, and receives the light reflected by the object of the light pulse emitted from the light-emitting element 1. After signal amplification is performed by an amplifier 12, calculation is performed. An amplified signal is given to the circuit 13 to calculate the distance to the subject. The distance measurement results calculated by the calculation circuit 13 are latched by the latch circuit 14 for the distance measurement results obtained by the first light emission drive. Latch driving of the latch circuit 14 is performed by an OR gate 20 and a monostable multivibrator 21, and a latch pulse obtained by delaying the first light emission driving pulse outputted from the decoder 4 by a predetermined time is given to the latch circuit 14, and the arithmetic circuit 13 The first distance measurement result obtained from the first distance measurement is latched. In addition, the arithmetic circuit 1
The output of No. 3 is also given to the latch circuit 15, and the latch circuit 15 latches the distance measurement result obtained in the second light emission drive. Therefore, for the latch circuit 15, the decoder 4
The second light emission driving pulse 9 obtained from the above is given as a latch pulse after being delayed by a predetermined time in the monostable multivibrator 22. The outputs of the latch circuits 14 and 15 are given to a coincidence judgment circuit 16, and when the first and second ranging results latched by the latch circuits 14 and 15 match, the coincidence judgment circuit 6 goes to L level. The output of the match judgment circuit 16 is outputted to the AND gate 6.
, the AND gate 6 becomes inhibited, and the third light emission drive pulse 1 from the decoder 4
Output to the drive circuit 2 of 0 is prohibited. On the other hand, when the coincidence determination circuit 16 determines that there is a discrepancy between the first and second distance measurement results, the output of the coincidence determination circuit 16 becomes H level, and the AND gate 6 is set to the permissible state and the second distance measurement result is output from the decoder 4. The output of the third light emission drive pulse is allowed, and the light emitting element 1 is caused to perform the third light emission drive. In this way, when the coincidence determination circuit 16 determines the discrepancy between the first and second distance measurement results and performs the third light emission drive, the third distance measurement obtained from the calculation circuit 13 The result is latched into latch circuit 14. In order to latch the third distance measurement result to the Q latch circuit 14, the output of the AND gate 6 is output to the OR gate 2.
0, and when the third light emission drive pulse 10 is output, a latch pulse is given to the latch circuit 14 from the monostable multivibrator 21, and the third distance measurement result obtained by the arithmetic circuit 13 is It will latch.

更に、ラッチ回路14の出力17及び一致判定回路の出
力18は図示しないカメラのオートフォーカス制御回路
等に与えられており、第1回目と第2回目の測距結果が
一致したときにはラッチ回路14にラッチしている第1
回目の測距結果を測距出力とし、一方、第1回目と第2
回目の測距結果が異なっていたときには、ラッチ回路1
4にラッチされた第3回目の測距結果を測距出力とする
Furthermore, the output 17 of the latch circuit 14 and the output 18 of the coincidence determination circuit are given to an autofocus control circuit of a camera (not shown), and when the first and second distance measurement results match, the output 17 is sent to the latch circuit 14. The first latched
The distance measurement result of the first time is used as the distance measurement output, while the first and second
If the second distance measurement result is different, latch circuit 1
The third distance measurement result latched at 4 is taken as the distance measurement output.

次に、被写体が蛍光灯による照明を受けていた場合を例
にとって本発明の測距原理を作用と共に説明する。
Next, the distance measuring principle of the present invention will be explained along with its operation, taking as an example a case where the subject is illuminated by a fluorescent lamp.

第2図は蛍光灯等によるノイズ人の入射を受けないとき
の測距動作による発光パルスP、受光信号VO及び測距
演算のタイミングTを示したタイムチャートである。
FIG. 2 is a time chart showing the light emitting pulse P, the light reception signal VO, and the timing T of the distance measurement operation during the distance measurement operation when there is no noise or human incident from a fluorescent lamp or the like.

即ち、時刻toでパルス幅TWをもって第1回目の発光
を行ない、更に所定時間T1後に同じくパルス幅TWで
第2回目の発光を行なう。この連続した第1回目と第2
回目の発光パルスPの発射により各発光タイミングで受
光素子11の受光信号を増幅器12で増幅した受光信号
Voがそれぞれ得られ、時刻to、tlの各発光開始か
らTS経過後に測距演算を実行して被写体までの距離を
演算する。この被写体までの距離の演算方式については
、例えば公開特許公報昭和56−29112@等の演算
原理に従って求められる。
That is, the first light emission is performed with the pulse width TW at time to, and the second light emission is performed with the same pulse width TW after a predetermined time T1. This consecutive first and second
By emitting the second light emitting pulse P, a light receiving signal Vo is obtained by amplifying the light receiving signal of the light receiving element 11 with the amplifier 12 at each light emitting timing, and distance measurement calculation is executed after TS has elapsed from the start of each light emission at times to and tl. to calculate the distance to the subject. The method of calculating the distance to the object is determined according to the calculation principle of, for example, Japanese Patent Publication No. 1983-29112@.

このような第1回目と第2回目の発光駆動による測距演
算で得られた測距結果は、第2図の場合には蛍光灯等の
ノイズ光の受光がないことから、第1回目と第2回目の
測距結果が等しく、正確な測距が行なわれたものと判定
される。
The distance measurement results obtained by such distance measurement calculations using the first and second light emission drives are similar to those of the first time because in the case of Fig. 2, there is no reception of noise light such as fluorescent lamps. The second distance measurement results are equal, and it is determined that accurate distance measurement has been performed.

第3図は測距動作を行なった際に被写体が蛍光灯で照明
されていたり、或いは受光素子に蛍光灯からの光が直接
入射した場合の信号波形を示す。
FIG. 3 shows signal waveforms when the object is illuminated with a fluorescent lamp or when light from a fluorescent lamp directly enters the light receiving element when performing a distance measuring operation.

例えば、時刻↑1の第2回目の発光駆動のタイミングで
蛍光灯による受光ノイズ成分VNが重なったとすると、
ノイズ光VNがないときの受光信号VSとの重ね合わせ
により、実際に得られる受光信号はVOに示すようにな
る。このため、第1回目の測距結果と第2回目の測距結
果が異なる。そこで本発明にあっては、第1回目と第2
回目の測距結果が異なったときには、ノイズ光のないタ
イミングで第3回目の測距を行なうことで正確な測距結
果を得るようにしている。
For example, if the light reception noise component VN from the fluorescent lamp overlaps at the timing of the second light emission drive at time ↑1,
By superimposing the received light signal VS with the received light signal VS when there is no noise light VN, the actually obtained received light signal becomes as shown in VO. Therefore, the first distance measurement result and the second distance measurement result are different. Therefore, in the present invention, the first and second
If the distance measurement results are different, the third distance measurement is performed at a timing free of noise light to obtain accurate distance measurement results.

ここで蛍光灯は50H2或いは60トIZて点灯してい
ても光示の時間的な変化は正弦的なものではなく、繰り
返し周期が商用交流周期の2倍のパルス波形となり、こ
の間にノイズの小ざい期間がある。即ち、第3図のノイ
ズ信号VNに示すように、繰り返し周期Tcをもってパ
ルス幅TNのパルス波形を生じ、繰り返し周期Tc内の
TMの11!]間中は雑音がない。そこで、この雑音が
ないTHの期間中に第3回目の測距を行なえばよい。
Here, even if the fluorescent lamp is lit at 50H2 or 60T IZ, the temporal change in the light display is not sinusoidal, and the repetition period is a pulse waveform twice the commercial AC period, and during this period, the noise is small. There is a rough period. That is, as shown in the noise signal VN of FIG. 3, a pulse waveform of pulse width TN is generated with a repetition period Tc, and 11! of TM within the repetition period Tc! ] There is no noise during this time. Therefore, the third distance measurement may be performed during this noise-free TH period.

尚、第3図にあっては、第2回目の測距時にノイズによ
って測距誤差を発生した場合を示すが、現実には第1回
目のみに測距誤差を生ずる場合、第2回目に測距誤差を
生ずる場合、更に第1回目及び第2回目共に測距誤差を
生する3つの場合がある。
Although Fig. 3 shows a case where a distance measurement error occurs due to noise during the second distance measurement, in reality, if a distance measurement error occurs only during the first distance measurement, the second distance measurement When a distance error occurs, there are three cases in which a distance measurement error occurs both in the first measurement and in the second measurement.

第3図のように第2回目に測距誤差を発生したとぎには
、発光パルスPの発光終了から第3回目の発光パルスま
での期間(T2−Tw>をノイズ光のノイズ期間Tnよ
り大きくしておけば第3回目の測距を雑音のない期間1
’−mで正しく行なうことができる。
As shown in Fig. 3, when a distance measurement error occurs for the second time, the period from the end of the light emission pulse P to the third light emission pulse (T2-Tw>) should be made larger than the noise period Tn of the noise light. If you do this, the third distance measurement will be performed during noise-free period 1.
'-m can be used correctly.

一方、第1回目の測距時にノイズ光による誤差を発生し
たときには、発光パルスPの第1回目と第2回目及び第
2回目と第3回目の周期の和(T1+T2>がノイズ光
のノイズの小さい期間Tmより小さい期間に第3回目の
発光を行なえば、次の雑音を受ける前に第3回目の測距
を行なうことができる。即ち、 T2−Tw>Tn  −−・(1) T1+T2<Tm  −−−(2> が成立するように発光パルスPの周期T1.T2及びパ
ルス幅Twを選んでおけば、第3回目の測距時には雑音
を受けることはない。
On the other hand, when an error occurs due to noise light during the first distance measurement, the sum of the periods of the first and second and second and third pulses P (T1+T2> is the noise of the noise light). If the third light emission is performed in a period smaller than the short period Tm, the third distance measurement can be performed before receiving the next noise. That is, T2-Tw>Tn -- (1) T1+T2< If the period T1, T2 and pulse width Tw of the light emitting pulse P are selected so that Tm ---(2> holds true), noise will not occur during the third distance measurement.

具体的には、螢光対の場合7−n=2m5. Tc=8
.3ms (60Hzの場合)、または10m5(50
H2の場合〉程度である。T1−1−T2に関しては、
短い方の3.3msを考えれば良いから、Tw=0.5
msST1=2msとして前記第(1)、(2>式に代
入すると、 T2−0.5ms>2ms  =13>TI+T2< 
(8,3−2>ms  −−−(4)となり、第(3)
式より、 T2>2.5mS となり、また第(4)式より、 T2<6.3−2=4.3ms となることから、第3回目の発光を行なう周lII]T
2として、T2=3mS2=3設定すれば、第1回目ま
たは第2回目、或いは第1回目と第2回目の両方でノイ
ズ光を受けて誤った測距結果が得られたとしても、第3
回目についてはノイズ光を回避した正しい測距結果を得
ることができる。
Specifically, in the case of a fluorescent pair, 7-n=2m5. Tc=8
.. 3ms (at 60Hz), or 10m5 (50
In the case of H2>. Regarding T1-1-T2,
Just consider the shorter 3.3ms, so Tw=0.5
Substituting msST1=2ms into equations (1) and (2> above, T2-0.5ms>2ms =13>TI+T2<
(8,3-2>ms---(4), and the (3rd)
From the formula, T2 > 2.5 mS, and from formula (4), T2 < 6.3-2 = 4.3 ms.
2, if you set T2=3mS2=3, even if an incorrect distance measurement result is obtained due to noise light in the first or second measurement, or in both the first and second measurements, the third
For the second time, it is possible to obtain a correct distance measurement result that avoids noise light.

従って、第1図の実施例に示すデコーダ4に例えば螢光
対によるノイズ光を例にとると、時刻to、t2及びT
3の各タイミングでパルス幅Tw=Q、5msの発光駆
動パルスを発生するように回路条件を設定し、且つ第1
回目と第2回目の発光パルスの周期T1をT1=2mS
となるように設定し、更に第2回目と第3回目の発光周
期T2をT2=3mSと設定することで、第1回目また
は第2回目、或いは第1回目と第2回目の両方でノイズ
光による誤った測距結果が得られたとしても、第3回目
については常に正しい測距結果を得ることができる。
Therefore, if noise light from a fluorescent pair is applied to the decoder 4 shown in the embodiment of FIG.
The circuit conditions are set so that a light emission drive pulse of pulse width Tw=Q, 5 ms is generated at each timing of 3.
The period T1 of the first and second light emission pulses is T1=2mS.
By setting the emission period T2 of the second and third times to T2=3mS, noise light can be eliminated in the first or second time, or in both the first and second time. Even if an incorrect distance measurement result is obtained, a correct distance measurement result can always be obtained the third time.

尚、上記の実施例は螢光対によるノイズ光を例にとるも
のであったが、本発明はこれに限定されず、測距時にお
けるノイズ光が連続的なノイズ光でなく、ノイズ光の低
い期間を周期的に生ずるノイズ光については、螢光対の
場合と同様ノイズ光の繰り返し周期とノイズ期間及びノ
イズなし期間に基づいた発光パルス幅TW、第1回目と
第2回目の発光周期T1及び第2回目と第3回目の発光
周期T2を前記第(’I)、(2>式に示した条件とな
るように設定することで、第1回目と第2回目のいずれ
か一方、若しくは両方でノイズ光による誤った測距結果
を生じても、第3回目の測距についてはノイズ光を受け
ることなく正確な測距結果を得ることができる。
Although the above embodiment takes noise light caused by a fluorescent pair as an example, the present invention is not limited to this, and the noise light during distance measurement is not continuous noise light, but noise light. Regarding the noise light that periodically generates low periods, as in the case of the fluorescent pair, the emission pulse width TW is based on the repetition period of the noise light, the noise period, and the no-noise period, and the first and second emission periods T1. And by setting the second and third light emitting periods T2 to meet the conditions shown in formula ('I) and (2>), either one of the first and second light emitting times, or Even if erroneous distance measurement results occur in both cases due to noise light, accurate distance measurement results can be obtained in the third distance measurement without receiving noise light.

(発明の効果) 以上説明してきたように本発明によれば、光ビームの発
射による測距を連続して2回行ない、第1回目と第2回
目の測距結果が異なったときにはノイズ光により誤った
測距か行なわれたものと判断して第3回目の測距をノイ
ズ光の入射を受けない所定のタイミングで行なうように
したため、被写体が螢光対等の外乱光源により照明され
ていたり、外乱光源からの光が直接受光素子に入射した
場合にも、常に正確な被写体までの距離測定を行なうこ
とかでき、距離測定の信頼性を大幅に向上することがで
きる。
(Effects of the Invention) As explained above, according to the present invention, distance measurement by emitting a light beam is performed twice in succession, and when the first and second distance measurement results are different, noise light is Because it was determined that an erroneous distance measurement had been performed and the third distance measurement was performed at a predetermined timing when no noise light was incident, the subject may have been illuminated by a disturbance light source such as a fluorescent pair. Even when light from a disturbance light source directly enters the light receiving element, the distance to the object can always be accurately measured, and the reliability of distance measurement can be greatly improved.

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

第1図は本発明の一実施例を示したブロック図、第2図
はノイズ光がないときの信号・波形図、第3図はノイズ
光を受けたときの信号波形図である。 1:発光素子 2:駆動回路 3:カウンタ 4:デコーダ 5.20:ORゲート 6:ANDゲート 7:端子(クロック入力) 8.9,10:発光駆動パルス 11:受光素子 12:増幅器 13:演算回路 14.15:ラッチ回路 16:一致判定回路
FIG. 1 is a block diagram showing an embodiment of the present invention, FIG. 2 is a signal/waveform diagram when there is no noise light, and FIG. 3 is a signal waveform diagram when noise light is received. 1: Light emitting element 2: Drive circuit 3: Counter 4: Decoder 5.20: OR gate 6: AND gate 7: Terminal (clock input) 8.9, 10: Light emission drive pulse 11: Light receiving element 12: Amplifier 13: Operation Circuit 14.15: Latch circuit 16: Match determination circuit

Claims (1)

【特許請求の範囲】[Claims] 被写体に向けて光ビームを発射する発光手段と、被写体
よりの反射光を受光する受光手段と、該受光手段の受光
信号に基づいて被写体までの距離を演算する演算手段と
を備えた測距装置に於いて、前記光ビームの発射による
被写体の測距を連続して2回行ない、第1回目と第2回
目の測距結果が異なったときに第3回目の測距を行なう
測距制御手段を設けたことを特徴とする測距装置。
A distance measuring device comprising a light emitting means for emitting a light beam toward a subject, a light receiving means for receiving reflected light from the subject, and a calculation means for calculating a distance to the subject based on a light reception signal of the light receiving means. Distance measurement control means that measures the distance of the subject twice in succession by emitting the light beam, and performs the third distance measurement when the results of the first and second distance measurements are different. A distance measuring device characterized by being provided with.
JP61224179A 1986-09-22 1986-09-22 Distance measuring apparatus Pending JPS6379010A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP61224179A JPS6379010A (en) 1986-09-22 1986-09-22 Distance measuring apparatus

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61224179A JPS6379010A (en) 1986-09-22 1986-09-22 Distance measuring apparatus

Publications (1)

Publication Number Publication Date
JPS6379010A true JPS6379010A (en) 1988-04-09

Family

ID=16809763

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61224179A Pending JPS6379010A (en) 1986-09-22 1986-09-22 Distance measuring apparatus

Country Status (1)

Country Link
JP (1) JPS6379010A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH02201327A (en) * 1989-01-30 1990-08-09 Minolta Camera Co Ltd Camera with automatic zooming mechanism
WO2012127671A1 (en) * 2011-03-24 2012-09-27 北陽電機株式会社 Signal processing device of scanning-type distance measurement device, signal processing method, and scanning-type distance measurement device

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH02201327A (en) * 1989-01-30 1990-08-09 Minolta Camera Co Ltd Camera with automatic zooming mechanism
WO2012127671A1 (en) * 2011-03-24 2012-09-27 北陽電機株式会社 Signal processing device of scanning-type distance measurement device, signal processing method, and scanning-type distance measurement device
JPWO2012127671A1 (en) * 2011-03-24 2014-07-24 北陽電機株式会社 Scanning distance measuring device signal processing device, signal processing method, and scanning distance measuring device
JP6040444B2 (en) * 2011-03-24 2016-12-07 北陽電機株式会社 Scanning distance measuring device signal processing device, signal processing method, and scanning distance measuring device
US9797711B2 (en) 2011-03-24 2017-10-24 Hokuyo Automatic Co., Ltd. Signal processing device of scanning-type distance measurement device, signal processing method, and scanning-type distance measurement device

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