JPS5842411B2 - distance measuring device - Google Patents
distance measuring deviceInfo
- Publication number
- JPS5842411B2 JPS5842411B2 JP55120417A JP12041780A JPS5842411B2 JP S5842411 B2 JPS5842411 B2 JP S5842411B2 JP 55120417 A JP55120417 A JP 55120417A JP 12041780 A JP12041780 A JP 12041780A JP S5842411 B2 JPS5842411 B2 JP S5842411B2
- Authority
- JP
- Japan
- Prior art keywords
- light
- light receiving
- amount
- distance
- measured
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired
Links
- 230000010355 oscillation Effects 0.000 claims description 16
- 230000001360 synchronised effect Effects 0.000 claims description 2
- 238000005259 measurement Methods 0.000 description 5
- 230000003287 optical effect Effects 0.000 description 5
- 230000000694 effects Effects 0.000 description 4
- 230000002411 adverse Effects 0.000 description 3
- 238000010586 diagram Methods 0.000 description 3
- 239000004065 semiconductor Substances 0.000 description 2
- 230000007423 decrease Effects 0.000 description 1
- 238000003384 imaging method Methods 0.000 description 1
- 230000010354 integration Effects 0.000 description 1
- 230000000087 stabilizing effect Effects 0.000 description 1
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01S—RADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
- G01S7/00—Details of systems according to groups G01S13/00, G01S15/00, G01S17/00
- G01S7/48—Details of systems according to groups G01S13/00, G01S15/00, G01S17/00 of systems according to group G01S17/00
- G01S7/483—Details of pulse systems
- G01S7/486—Receivers
Landscapes
- Engineering & Computer Science (AREA)
- Computer Networks & Wireless Communication (AREA)
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Radar, Positioning & Navigation (AREA)
- Remote Sensing (AREA)
- Measurement Of Optical Distance (AREA)
Description
【発明の詳細な説明】
本発明は被測定体との距離を光学的手段により測定する
距離測定装置に関するもので、その目的は、受光手段の
受光量が常に一定となるように投光手段の投光量をフィ
ードバック制御し得て、距離測定精度の変動の防止並び
に構造の簡単化を図り得ると共に、外乱光による悪影響
を抑制できる距離測定装置を提供するにある。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a distance measuring device for measuring the distance to an object to be measured by optical means, and its purpose is to adjust the light emitting means so that the amount of light received by the light receiving means is always constant. It is an object of the present invention to provide a distance measuring device capable of feedback controlling the amount of light projected, preventing fluctuations in distance measuring accuracy, simplifying the structure, and suppressing the adverse effects of ambient light.
以下、本発明の第1実施例について第1図乃至第4図を
参照しながら説明する。Hereinafter, a first embodiment of the present invention will be described with reference to FIGS. 1 to 4.
第1図において、1は発光ダイオード或はレーザ発生器
等より成る投光手段としての投光素子で、これは制御手
段たるパルス変調回路2により駆動されてパルス変調光
を発射する。In FIG. 1, reference numeral 1 denotes a light projecting element as a light projecting means consisting of a light emitting diode, a laser generator, etc., which is driven by a pulse modulation circuit 2, which is a control means, to emit pulse modulated light.
3はコンデンサレンズ等により構成された集光用光学系
で、前記パルス変調光はこの集光用光学系3を介して被
測定体4に投光される。Reference numeral 3 denotes a condensing optical system composed of a condenser lens, etc., and the pulse modulated light is projected onto the object to be measured 4 via this condensing optical system 3.
5は投光素子1と所定間隔を存するように並置した受光
手段としての半導体装置検出器(以下PSDと略称する
)であり、これの受光面5aには被測定体4で反射され
たパルス変調光が結像用光学系6を介して入射結像され
るようになっている。Reference numeral 5 denotes a semiconductor device detector (hereinafter abbreviated as PSD) as a light receiving means arranged in parallel with the light emitting element 1 at a predetermined interval, and a light receiving surface 5a of this device is provided with a pulse modulation device reflected by the object to be measured 4. The light is incident and imaged via the imaging optical system 6.
即ち、投光素子1及びPSD5は被測定体4に対して三
角測量的配置になされており、従ってPSD5は、被測
定体4で反射されたパルス変調光を該被測定体4との距
離Xに応じた受光点で受光する。That is, the light projecting element 1 and the PSD 5 are arranged in a triangular manner with respect to the object to be measured 4, and therefore the PSD 5 directs the pulse modulated light reflected by the object to be measured 4 to the distance X from the object to be measured 4. The light is received at a light receiving point according to the
ここで、上記PSD5は次に述べる機能を有するもので
ある。Here, the PSD 5 has the following functions.
つまり、PSD5は、バイアス用電源7によりバイアス
された状態で受光面5aに光が入射されると、その入射
光量に応じた値の光電流Iを生成すると共に、対をなす
電極A、Bより夫々次式で与えられる信号電流工え、I
B(但し、■よ+I、=I)を位置信号として出力する
。In other words, when light is incident on the light-receiving surface 5a while being biased by the bias power source 7, the PSD 5 generates a photocurrent I having a value corresponding to the amount of incident light, and also generates a photocurrent I from the pair of electrodes A and B. Signal current processing, I, given by the following formulas, respectively:
B (however, +I, =I) is output as a position signal.
即ち、第2図に示すようにPSD5の電極A、B間の距
離をL1電極Aから受光点までの距離をXとした場合、
の関係があり、従って信号電流■6゜
■8により
距離X(即ち受光点の位置)を知ることができ、この距
離Xに応じて被測定体4との距離Xを測定することがで
きる。That is, as shown in Fig. 2, when the distance between electrodes A and B of PSD 5 is defined as the distance from L1 electrode A to the light receiving point, there is the following relationship, and therefore, the signal current ■6゜■8 makes the distance X (that is, the position of the light receiving point), and the distance X to the object to be measured 4 can be measured according to this distance X.
8,9は夫々信号電流■え、■8に応じて単調増加する
、直流信号電圧vA、VBを出力する受光回路であり、
これらは第3図に示すような構成になっている。8 and 9 are light receiving circuits that output DC signal voltages vA and VB that monotonically increase in accordance with signal currents ① and ②8, respectively;
These have a configuration as shown in FIG.
尚、受光回路8,9は夫々同一構成であるから、第3図
においては一方の受光回路8のみ示し、他方の受光回路
9については受光回路8と同一構成部分に対応させて付
゛した(ト)内の符号を援用することによりその図示を
省略する。Note that since the light receiving circuits 8 and 9 have the same configuration, only one of the light receiving circuits 8 is shown in FIG. By using the reference numerals in (g), illustration thereof will be omitted.
即ち、第3図に示す受光回路8においで、10aは信号
電流■えを受ける電流入力増幅器で、その増幅出力が交
流増幅器11a並びに同期手段としてのゲート回路12
aを順に介して積分回路13aに入力され、この積分回
路13aからの積分出力が信号電圧■6をなす。That is, in the light receiving circuit 8 shown in FIG. 3, 10a is a current input amplifier that receives a signal current, and its amplified output is sent to an AC amplifier 11a and a gate circuit 12 as a synchronizing means.
A is sequentially inputted to an integrating circuit 13a through the input circuit 13a, and an integrated output from the integrating circuit 13a forms a signal voltage 6.
尚、上記ゲート回路12aは、前記パルス変調回路2か
ら出力される同期信号たる発振パルスP。Note that the gate circuit 12a receives an oscillation pulse P which is a synchronizing signal output from the pulse modulation circuit 2.
を受けたときのみ信号の通過を許容する構成である。The configuration allows the signal to pass only when the signal is received.
一方、14は信号電圧■6と■8との和即ち「■よ+V
8Jを演算する加算器で、その演算結果はパルス変調回
路2に送出される。On the other hand, 14 is the sum of the signal voltages ■6 and ■8, that is, "■yo+V
The adder calculates 8J, and the result of the calculation is sent to the pulse modulation circuit 2.
ここで、信号電圧■え、■8は夫々信号電流■え、■8
に対し単調増加するものであるから、「■よ+V3Jも
「■□十I8Jに対し単調増加するものになる。Here, the signal voltages ■e, ■8 are the signal currents ■e, ■8, respectively.
Since it increases monotonically with respect to ``■yo+V3J'', it also increases monotonically with respect to ``■□10I8J.
即ち、「IA+■8」は、PSD5が生成する光電流■
と等しいものであって該PSD5が受光する前記パルス
変調光の光量に応じた値になるから、「■え+■8」も
PSD5が受光する光量に応じた値になる。That is, "IA+■8" is the photocurrent ■ generated by PSD5.
Since the value is equal to the amount of light of the pulse modulated light that the PSD 5 receives, "■e+■8" also takes a value that corresponds to the amount of light that the PSD 5 receives.
しかして、前記パルス変調回路2は第4図に示すような
構成になっている。The pulse modulation circuit 2 has a configuration as shown in FIG. 4.
この第4図において、15は誤差増幅器で、これは加算
器14からの演算出力「■よ+■8」と基準電圧E8と
の差を増幅してその誤差出力電圧■。In FIG. 4, reference numeral 15 denotes an error amplifier, which amplifies the difference between the calculation output "■Yo+■8" from the adder 14 and the reference voltage E8 to produce an error output voltage ■.
を電圧コントロール発振器16に送出するものである。is sent to the voltage controlled oscillator 16.
この場合、上記誤差出力電圧■。In this case, the above error output voltage ■.
は rV、+V、Jに対して反比例的に変化するように
なっている。is designed to change in inverse proportion to rV, +V, and J.
そして、上記電圧コントロール発振器16は、入力され
る電圧V。The voltage control oscillator 16 receives the input voltage V.
に応じて単調増加する周波数の発振パルスP。An oscillation pulse P with a frequency that monotonically increases according to.
を出力するものである。従って該発振パルスP の周波
数は「■え+■8」に対して反比例的に変化する。This outputs the following. Therefore, the frequency of the oscillation pulse P changes in inverse proportion to "■e+■8".
また、上記発振パルスPoは、前述したように受光回路
8,9内のゲート回路12a 、12bに与えられると
共に、ドライブ回路17にも与えられるようになってお
り、このドライブ回路17は発振パルスP。Further, as mentioned above, the oscillation pulse Po is given to the gate circuits 12a and 12b in the light receiving circuits 8 and 9, and is also given to the drive circuit 17, which is connected to the oscillation pulse Po. .
を増幅してその増幅出力により前記投光素子1を駆動し
、以て該投光素子1からパルス変調光を発射させる。is amplified and the amplified output drives the light projecting element 1, thereby causing the light projecting element 1 to emit pulse modulated light.
さらに、第1図中、18は信号電圧■ と■ との差即
ちrV、−V8Jを演算する減算器、19は減算器18
による演算結果「vA−■8」に基づいて被測定体4と
の距離Xを演算する演算手段としての距離演算回路であ
る。Furthermore, in FIG. 1, 18 is a subtracter that calculates the difference between the signal voltages ■ and ■, that is, rV, -V8J, and 19 is a subtracter 18.
This is a distance calculation circuit as a calculation means for calculating the distance X to the object to be measured 4 based on the calculation result "vA-■8".
即ち、「■よ一■8」はPSD5の受光点の位置に対応
して出力される前記信号電流■よ、■8と一定の比関係
にあるものであり、従って、この「v −■ 」に基づ
いて被測定体4との距離Xの演算を行なうことができる
。That is, "■yoichi■8" has a constant ratio relationship with the signal current "■yoichi■8" outputted corresponding to the position of the light receiving point of the PSD 5, and therefore, this "v - ■" Based on this, the distance X to the object to be measured 4 can be calculated.
上記構成においては、投光素子1から発射され且つ被測
定体4で反射されたパルス変調光が、PSD5の受光面
5a上における上記被測定体4との距離Xに応じた受光
点で受光され、PSD5は斯ような受光点に対応した位
置信号として信号電流■え、■8を出力する。In the above configuration, the pulse modulated light emitted from the light projecting element 1 and reflected by the object to be measured 4 is received at a light receiving point on the light receiving surface 5a of the PSD 5 corresponding to the distance X from the object to be measured 4. , PSD5 outputs signal currents (1) and (8) as position signals corresponding to such light receiving points.
そして受光回路8゜9においては、ゲート回路12a、
12bが、前記パルス変調光と同期したタイミングで出
力される発振パルスP。In the light receiving circuit 8°9, the gate circuit 12a,
12b is an oscillation pulse P output at a timing synchronized with the pulse modulated light.
を与えられる毎に上記信号電流■え、■8に対応した交
流増幅器11a、11bからの増幅信号を周期的に通過
させ、且つ積分回路13a 、 13bが上記通過信号
を積分し、結果的に該受光回路8,9から連続的な信号
電圧■よ。The amplified signals from the AC amplifiers 11a and 11b corresponding to the signal current (1) and (8) are passed through periodically, and the integration circuits 13a, 13b integrate the passed signals, resulting in the corresponding signal current. Continuous signal voltage ■ from the light receiving circuits 8 and 9.
vBが夫々出力される。vB is output respectively.
すると、加算器14が「VA+■8」を演算してその演
算結果をパルス変調回路2内の誤差増幅器15に送出す
るため、電圧コントロール発振器16が「■よ+V8J
(即ち、PSD5の受光量に対応した値)に対して周波
数が反比例的に変化する発振パルスP。Then, the adder 14 calculates "VA+■8" and sends the result to the error amplifier 15 in the pulse modulation circuit 2, so the voltage control oscillator 16 calculates "VA+V8J".
(that is, a value corresponding to the amount of light received by the PSD 5), the oscillation pulse P whose frequency changes in inverse proportion to the amount of light received by the PSD 5.
を出力する。Output.
従って、PSD5の受光量が基準値より多い場合、換言
すればrv、+v、」が基準電圧E8より大なる値であ
った場合には発振パルスPoの周波数が低くなり、これ
とは逆にPSD5の受光量が基準値より少ない場合には
発振パルスPoの周波数が高くなる。Therefore, when the amount of light received by the PSD5 is greater than the reference value, in other words, when rv, +v, is greater than the reference voltage E8, the frequency of the oscillation pulse Po becomes lower; When the amount of received light is less than the reference value, the frequency of the oscillation pulse Po increases.
これにより、発振パルスP。As a result, the oscillation pulse P.
により駆動される投光素子1に対して所謂パルス数変調
(PNM)がかけられ、従って該投光素子1による投光
量は、PSD5の受光量が犬なるときに減少し且つPS
D5の受光量が小なるときに増大する方向にフィードバ
ック制御され、結果的に、パルス変調回路2はPSD5
の受光量が常に一定レベルとなるように保持する動作を
行なう。So-called pulse number modulation (PNM) is applied to the light emitting element 1 driven by the light emitting element 1, so that the amount of light emitted by the light emitting element 1 decreases when the amount of light received by the PSD 5 becomes small, and
Feedback control is performed in the direction of increasing the amount of light received by D5 when it becomes small, and as a result, the pulse modulation circuit 2
The amount of light received is always maintained at a constant level.
以上のような動作によって、被測定体4との距離Xが変
化した場合でもその変化に応動してPSD5の受光量が
一定に保持され、また、被測定体4のパルス変調光反射
面における明度2表面形状、PSD5に対する傾斜度合
等の如何に拘らずPSD5の受光量が一定に保持される
ものである。Through the above operations, even if the distance X to the object to be measured 4 changes, the amount of light received by the PSD 5 is kept constant in response to the change, and the brightness at the pulse modulated light reflecting surface of the object to be measured 4 is maintained constant. 2. The amount of light received by the PSD 5 is kept constant regardless of the surface shape, the degree of inclination to the PSD 5, etc.
従って、信号電流I 、I ひいては距離測定の基
礎となる減算器18の演算結果rV、V8Jは被測定体
4との距離Xに対して常に一定の関係を呈するようにな
り、以て距離測定精度が被測定体4の種類並びに該被測
定体4との距離の如何に拘らず変動しなくなるという優
れた効果が得られる。Therefore, the signal currents I, I, and the calculation results rV and V8J of the subtracter 18, which are the basis of distance measurement, always exhibit a constant relationship with the distance X from the object to be measured 4, which increases the accuracy of distance measurement. An excellent effect is obtained in that the distance does not vary regardless of the type of the object 4 to be measured and the distance from the object 4 to be measured.
また、受光回路8,9及びPSD5並びに加算器14.
減算器18等の動作レベルも略一定になすことができて
、これらのダイナミックレンジを小さく構成し得、以て
構造の簡単化を図ることができる。Further, the light receiving circuits 8 and 9, the PSD 5, and the adder 14.
The operating level of the subtracter 18 and the like can also be kept substantially constant, and the dynamic range of these components can be made small, thereby simplifying the structure.
そして、PSD5の受光量が一定であるということは、
該PSD5の性質上これが生成する光電流■も一定であ
るということであるから、距離演算回路19での演算時
に上記光電流■の変化による影響を無視することができ
る。And, since the amount of light received by PSD5 is constant,
Due to the nature of the PSD 5, the photocurrent (2) generated by the PSD 5 is also constant, so that the influence of changes in the photocurrent (2) can be ignored during calculation in the distance calculation circuit 19.
即ち、光電流■の変化によるスケールファクタの変動が
なくなるため、PSD5からの信号電流I、、I、を規
格化するための演算が不要である。That is, since there is no variation in the scale factor due to changes in the photocurrent (2), there is no need for calculations to normalize the signal currents I, , I, from the PSD 5.
従って距離演算回路19は、単純に「■□−■8」を距
離Xに変換するだけの機能があれば良く、この面からも
構造の簡単化を図り得る。Therefore, the distance calculation circuit 19 only needs to have the function of simply converting "■□-■8" into distance X, and from this point of view as well, the structure can be simplified.
さらに、距離測定のための光学系にパルス変調光を用い
たから、外乱光による悪影響を極力抑制でき、以て距離
測定精度のより一層の安定化を図り得る。Furthermore, since pulse modulated light is used in the optical system for distance measurement, the adverse effects of disturbance light can be suppressed as much as possible, thereby further stabilizing the accuracy of distance measurement.
尚、上記実施例中におけるパルス変調回路2並びに受光
回路8,9に代えて、夫々第5図に示す構成の制御手段
たるパルス変調回路20並びに第6図に示す構成の受光
回路21を適用しても良い。Incidentally, in place of the pulse modulation circuit 2 and the light receiving circuits 8 and 9 in the above embodiment, a pulse modulation circuit 20 serving as a control means having the structure shown in FIG. 5 and a light receiving circuit 21 having the structure shown in FIG. 6 are applied, respectively. It's okay.
即ち、第5図において、22は加算器14からの演算出
力rV +V Jと基準電圧Esとの差をB
増幅してその誤差出力電圧■ (但し、■oは「■よ+
VB」に対して反比例的に変化する)をFET23のゲ
ートに与える誤差増幅器、24は同期信号たる発振パル
スP。That is, in FIG. 5, 22 amplifies the difference between the calculation output rV+VJ from the adder 14 and the reference voltage Es to produce an error output voltage .
24 is an oscillation pulse P which is a synchronizing signal.
を出力する自励式の発振回路、25は発振パルスP。25 is a self-excited oscillation circuit that outputs an oscillation pulse P.
の立ち下がり期間のみオンされるトランジスタであり、
このトランジスタ25はそのオン時にFET23のゲー
トを接地する。It is a transistor that is turned on only during the falling period of
This transistor 25 grounds the gate of FET 23 when it is on.
そして、FET23は、そのドレイン・ソース間が電源
+■と接地端子との間に投光素子1(この場合発光ダイ
オード)を介して接続されている。The drain and source of the FET 23 are connected between the power supply +■ and the ground terminal via the light emitting element 1 (in this case, a light emitting diode).
斯かるパルス変調回路20は、「V1+ V2J =
E sとなるように投光素子1に流れる電流のピーク値
を制御し、以て該投光素子1の投光量を制御してPSD
5の受光量を一定レベルになす。Such a pulse modulation circuit 20 has "V1+V2J=
The peak value of the current flowing through the light emitting element 1 is controlled so that E
5. Keep the amount of light received at a constant level.
また、第6図において、26は信号電流■A(若しくは
より)を受ける電流入力増幅器、27は利得可変交流増
幅器、28は同期手段としてのゲート回路、29は積分
回路、30は誤差増幅器であり、この誤差増幅器30の
出力は利得可変信号として利得可変交流増幅器27にフ
ィードバックされる。Further, in FIG. 6, 26 is a current input amplifier receiving signal current ■A (or more), 27 is a variable gain AC amplifier, 28 is a gate circuit as a synchronizing means, 29 is an integrating circuit, and 30 is an error amplifier. The output of this error amplifier 30 is fed back to the variable gain AC amplifier 27 as a variable gain signal.
斯かる構成の受光回路21においても信号電流■ (若
しくは■B)と所定の比関係にある信号電圧V (若し
くはVB)が誤差増幅器30から出力されるものであり
、特にこの構成によればダイナミックレンジが大になる
利点がある。Even in the light receiving circuit 21 having such a configuration, a signal voltage V (or VB) having a predetermined ratio relationship with the signal current ■ (or ■B) is output from the error amplifier 30, and especially with this configuration, a dynamic It has the advantage of having a large range.
本発明によれば以上の説明によって明らかなように、被
測定体との距離、該被測定体の表面状態の如何に拘らず
受光手段の受光量が常に一定となるように投光手段の投
光量をフィードバック制御し得て、距離測定精度の変動
の防止並びに構造の簡単化を図り得ると共に、外乱光に
よる悪影響を小ならしめ得る等の効果を奏する距離測定
装置を提供することができる。According to the present invention, as is clear from the above description, the light emitting means emits light so that the amount of light received by the light receiving means is always constant regardless of the distance to the object to be measured or the surface condition of the object to be measured. It is possible to provide a distance measuring device that can perform feedback control of the amount of light, prevent fluctuations in distance measurement accuracy, simplify the structure, and reduce the adverse effects of ambient light.
第1図乃至第4図は本発明の一実施例に関するもので、
第1図は全体の構成説明図、第2図は受光手段の機能説
明用の図、第3図及び第4図は夫夫異なる要部を示すブ
ロック図である。
また第5図及び第6図は夫々本発明の他の実施例を示す
第4図及び第5図相当図である。
図中、1は投光素子(投光手段)、2,20はパルス変
調回路(制御手段)、4は被測定体、5は半導体装置検
出器(受光手段)、8.9は受光回路、12a、12b
、28はゲート回路(同期手段)、16は電圧コントロ
ール発振器、19は距離演算回路(演算手段)である。1 to 4 relate to an embodiment of the present invention,
FIG. 1 is a diagram illustrating the overall configuration, FIG. 2 is a diagram illustrating the functions of the light receiving means, and FIGS. 3 and 4 are block diagrams showing different main parts. Further, FIGS. 5 and 6 are views corresponding to FIGS. 4 and 5, respectively, showing other embodiments of the present invention. In the figure, 1 is a light projecting element (light projecting means), 2 and 20 are pulse modulation circuits (control means), 4 is an object to be measured, 5 is a semiconductor device detector (light receiving means), 8.9 is a light receiving circuit, 12a, 12b
, 28 is a gate circuit (synchronization means), 16 is a voltage control oscillator, and 19 is a distance calculation circuit (calculation means).
Claims (1)
の投光手段と所定間隔を存するように配置されて前記被
測定体で反射されたパルス変調光を該被測定体との距離
に応じた受光点で受光するように設けられ、その受光点
の位置に対応した位置信号を出力する受光手段と、前記
位置信号に応じて前記被測定体との距離を演算する演算
手段と、前記パルス変調光に同期したタイミングで前記
位置信号を前記演算手段に与える同期手段と、前記受光
手段が受光するパルス変調光の光量に応じて前記投光手
段の投光量をフィードバック制御し以て該受光手段の受
光量が常に一定レベルとなるように保持する制御手段と
を具備したことを特徴とする距離測定装置。 2 制御手段は、受光手段の受光量に対応した周波数の
発振パルスを出力する発振器を有し、その発振パルスに
よるパルス数変調によって投光手段の投光量を制御する
と共に、該発振パルスを同期手段の同期信号として用い
るように構成されていることを特徴とする特許請求の範
囲第1項記載の距離測定装置。[Scope of Claims] 1. A light projecting means for emitting pulse modulated light onto an object to be measured; A light receiving means is provided to receive light at a light receiving point corresponding to a distance from the object to be measured, and outputs a position signal corresponding to the position of the light receiving point, and a distance to the object to be measured is calculated according to the position signal. a synchronizing means for supplying the position signal to the calculating means at a timing synchronized with the pulse modulated light; and a synchronizing means for feeding back the amount of light emitted by the light emitting means in accordance with the amount of the pulse modulated light received by the light receiving means. 1. A distance measuring device comprising: control means for controlling and maintaining the amount of light received by the light receiving means always at a constant level. 2. The control means has an oscillator that outputs an oscillation pulse of a frequency corresponding to the amount of light received by the light receiving means, controls the amount of light emitted by the light emitting means by modulating the number of pulses by the oscillation pulse, and transmits the oscillation pulse to the synchronizing means. 2. The distance measuring device according to claim 1, wherein the distance measuring device is configured to be used as a synchronization signal for.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP55120417A JPS5842411B2 (en) | 1980-08-28 | 1980-08-28 | distance measuring device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP55120417A JPS5842411B2 (en) | 1980-08-28 | 1980-08-28 | distance measuring device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5744809A JPS5744809A (en) | 1982-03-13 |
| JPS5842411B2 true JPS5842411B2 (en) | 1983-09-20 |
Family
ID=14785699
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP55120417A Expired JPS5842411B2 (en) | 1980-08-28 | 1980-08-28 | distance measuring device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5842411B2 (en) |
Families Citing this family (21)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5891111U (en) * | 1981-12-14 | 1983-06-20 | 日本電気ホームエレクトロニクス株式会社 | Tilt condition detection device |
| JPS5964805A (en) * | 1982-10-05 | 1984-04-12 | Konishiroku Photo Ind Co Ltd | Auto-focusing device |
| JPS6081610A (en) * | 1983-10-08 | 1985-05-09 | Nippon Yusoki Co Ltd | Device for detecting stopping position of constant point of omnidirectional movable truck |
| JPS6095318A (en) * | 1983-10-31 | 1985-05-28 | Matsushita Electric Ind Co Ltd | Optical distance measuring device |
| JPS60112113A (en) * | 1983-11-24 | 1985-06-18 | Toyota Central Res & Dev Lab Inc | Measuring device of position and/or azimuth of unattended car |
| JPS60117102A (en) * | 1983-11-30 | 1985-06-24 | Hitachi Ltd | Welding line tracing detection device |
| JPH0746052B2 (en) * | 1984-04-25 | 1995-05-17 | 三菱電機株式会社 | Optical displacement meter |
| JPH0752087B2 (en) * | 1984-10-26 | 1995-06-05 | 三菱電機株式会社 | Optical displacement meter |
| JPS61117407A (en) * | 1984-11-13 | 1986-06-04 | Kyocera Corp | Automatic range measuring circuit |
| JPS61178610A (en) * | 1985-02-01 | 1986-08-11 | Sankusu Kk | Reflection type distance sensor |
| JPS61226735A (en) * | 1985-04-01 | 1986-10-08 | Konishiroku Photo Ind Co Ltd | Automatic focus adjusting device for camera |
| JPS62293408A (en) * | 1986-06-12 | 1987-12-21 | Toyota Motor Corp | Work end driving control device |
| US5082363A (en) * | 1988-02-12 | 1992-01-21 | Omron Tateisi Electronics Co. | Optical distance measuring apparatus and method using light projection pulses |
| JPH01274010A (en) * | 1988-04-26 | 1989-11-01 | Mitsubishi Electric Corp | Optical displacement measuring apparatus |
| US5055664A (en) * | 1990-08-06 | 1991-10-08 | Eaton Corporation | Optical distance measuring system using a position sensitive device and a ramp generator driven light source |
| JPH06235646A (en) * | 1993-07-27 | 1994-08-23 | Harmonic Drive Syst Ind Co Ltd | Rotation angle detector |
| JP3215232B2 (en) * | 1993-08-03 | 2001-10-02 | 株式会社山武 | Photoelectric distance sensor |
| US5923427A (en) * | 1997-07-10 | 1999-07-13 | Banner Engineering Corporation | Optical triangulation distance sensing system and method using a position sensitive detector and an automatic power controlled light source |
| US6122039A (en) * | 1998-10-28 | 2000-09-19 | Banner Engineering Corp. | Method and apparatus to detect and report object displacement utilizing optical triangulation principles |
| JP2007322177A (en) * | 2006-05-30 | 2007-12-13 | Pulstec Industrial Co Ltd | Laser beam irradiation measuring device |
| JP2016102697A (en) * | 2014-11-27 | 2016-06-02 | パナソニックIpマネジメント株式会社 | Device, method, and program for creating distance image |
-
1980
- 1980-08-28 JP JP55120417A patent/JPS5842411B2/en not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5744809A (en) | 1982-03-13 |
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