JPH0358475B2 - - Google Patents
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- Publication number
- JPH0358475B2 JPH0358475B2 JP59011349A JP1134984A JPH0358475B2 JP H0358475 B2 JPH0358475 B2 JP H0358475B2 JP 59011349 A JP59011349 A JP 59011349A JP 1134984 A JP1134984 A JP 1134984A JP H0358475 B2 JPH0358475 B2 JP H0358475B2
- Authority
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- Japan
- Prior art keywords
- light
- output
- circuit
- detection
- detected
- Prior art date
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- 238000001514 detection method Methods 0.000 claims abstract description 53
- 230000007423 decrease Effects 0.000 claims abstract description 7
- 230000003321 amplification Effects 0.000 claims description 21
- 238000003199 nucleic acid amplification method Methods 0.000 claims description 21
- 229920006395 saturated elastomer Polymers 0.000 claims description 10
- 101000736368 Homo sapiens PH and SEC7 domain-containing protein 4 Proteins 0.000 abstract description 6
- 102100036232 PH and SEC7 domain-containing protein 4 Human genes 0.000 abstract description 6
- 230000003287 optical effect Effects 0.000 description 10
- 238000010586 diagram Methods 0.000 description 6
- 238000005259 measurement Methods 0.000 description 4
- 230000007257 malfunction Effects 0.000 description 3
- 230000010355 oscillation Effects 0.000 description 2
- 230000002159 abnormal effect Effects 0.000 description 1
- 230000008094 contradictory effect Effects 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000005070 sampling Methods 0.000 description 1
- 239000004065 semiconductor Substances 0.000 description 1
- XUIMIQQOPSSXEZ-AKLPVKDBSA-N silicon-31 atom Chemical compound [31Si] XUIMIQQOPSSXEZ-AKLPVKDBSA-N 0.000 description 1
- 230000001360 synchronised 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
- G01S17/00—Systems using the reflection or reradiation of electromagnetic waves other than radio waves, e.g. lidar systems
- G01S17/02—Systems using the reflection of electromagnetic waves other than radio waves
- G01S17/06—Systems determining position data of a target
- G01S17/46—Indirect determination of position data
- G01S17/48—Active triangulation systems, i.e. using the transmission and reflection of electromagnetic waves other than radio waves
-
- 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
- G01S17/00—Systems using the reflection or reradiation of electromagnetic waves other than radio waves, e.g. lidar systems
- G01S17/02—Systems using the reflection of electromagnetic waves other than radio waves
- G01S17/04—Systems determining the presence of a target
-
- 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
- G01S7/491—Details of non-pulse systems
- G01S7/4912—Receivers
Landscapes
- Physics & Mathematics (AREA)
- Engineering & Computer Science (AREA)
- Electromagnetism (AREA)
- Computer Networks & Wireless Communication (AREA)
- General Physics & Mathematics (AREA)
- Radar, Positioning & Navigation (AREA)
- Remote Sensing (AREA)
- Measurement Of Optical Distance (AREA)
- Geophysics And Detection Of Objects (AREA)
- Electronic Switches (AREA)
- Optical Radar Systems And Details Thereof (AREA)
Abstract
Description
(技術分野)
本発明は予め設定された検知エリア内に被検知
物体が存在するかどうかを判別して出力回路を制
御する反射型光電スイツチに関するものである。
(背景技術)
第1図乃至第3図はこの種の反射型光電スイツ
チの基本例を示すもので、図中1は被検知物体X
に対してパルス変調光よりなる光ビームPを投光
する投光手段であり、投光タイミングを設定する
同期信号を発生する発振回路10と、ドライブ回
路11と、発光ダイオード、レーザーダイオード
などの投光素子12と、光ビームPを形成するコ
ンデンサレンズよりなる投光用光学系13とで形
成されている。2は投光手段1から所定間隔l0を
もつて並置された受光手段であり、投、受光手段
1,2は被検知物体Xに対して三角測量的に配置
されている。この受光手段2は被検知物体Xによ
る反射光を集光するための凸レンズよりなる集光
手段3と、集光手段3の集光面に配設され集光ス
ポツトSの位置に対応した位置信号を出力する位
置検出手段4とで構成されており、この位置検出
手段4は、凸レンズよりなる集光手段3の集光面
内に配設され、集光スポツトSの一方向の移動に
際して光量に比例しかつその移動量に応じて増加
する第1の検知信号IAを出力するとともに光量
に比例しかつ移動量に応じて減少する第2の検知
信号IBを出力する。ここに、基本例では、この
位置検出手段4は、1次元位置検知素子(以下
PSD4と称する)にて形成され、このPSD4は
第3図aに示すように、平板状シリコン31の表
面にP層31a、裏面にN層31b、中間にI層
31cを形成したものであり、集光スポツトSの
位置に対応した信号電流IA,IBが出力されるよ
うになつている。この信号電流IAは集光スポツ
トSの一方向の移動に際してその移動量に比例し
て増加する信号であり、信号電流IBは移動量に
比例して減少する信号である。もちろん、信号電
流IA,IBが光量に比例することは言うまでもな
い。第3図bは位置検知素子4の等価回路を示す
もので、図中Piは電流源、Doは理想的ダイオー
ド、Coは接合容量、Ptは並列抵抗、Roは電極間
抵抗である。
なお位置検出手段4として距離lが変化した場
合における集光スポツトSの移動に応じて相反す
る信号電流IA,IBが得られるものであれば何で
も良く、例えば移動方向(矢印M)に連設された
2個の受光素子にて形成しても良く、受光素子と
してホトトランジスタ、ホトダイオード、太陽電
池、CdSなどが用いられる。5は判別制御手段で
あり、位置検出手段4出力に基いて被検知物体X
が所定の検知エリアDE内に存在するかどうかを
判別して出力回路6を制御するようになつてい
る。この判別制御手段5は、位置検出手段4から
の信号電流IA,IBを信号電圧VA,VBに増巾変
換する受光回路21a,21bと、対数増巾回路
22a,22bと、対数増巾回路22a出力
lnVAから対数増巾回路22b出力lnVBを減算す
る減算回路23と、減算回路23出力lnVA/
VBと検知エリア設定用ボリウム24aにて設定
された動作レベルVsとを比較して減算回路23
出力lnVA/VBが動作レベルVs以下のときHレ
ベルを出力する比較回路24と、投光素子12か
らの光ビームPの投光タイミング(発振回路10
から出力される同期信号)に同期して比較回路2
4出力をサンプリングすることにより、被検知物
体Xが検知エリアDE内に存在するかどうかを確
実に判別するようにした信号処理回路25とで形
成され、信号処理回路25出力にて負荷制御用の
リレー、負荷制御用の半導体スイツチ素子などよ
りなる出力回路6を制御するようになつている。
なお、受光回路21a,21bはパルス光信号の
みを通し直流光信号をカツトしたり、特定の周波
数のみを通すバンドパスフイルタ回路を含むもの
である。
いま、被検知物体Xが第4図aに示すように反
射型光電スイツチYから距離l1,l2,l3の位置に
存在する場合において、集光面内に配設された素
子PSD4に対する集光スポツトSの位置はそれ
ぞれ第4図bのようになり、被検知物体Xの位置
が光ビームPの投光方向に変化すると、集光ビー
ムSが矢印M方向に移動してPSD4から出力さ
れる信号電流IA,IBは集光スポツトSの位置に
対応した位置信号となる。判別制御手段5では受
光回路21a,21bにてこの信号電流IA,IB
に比例した信号電圧VA,VBを形成し、対数増
巾回路22a,22bにて対数増巾した電圧
lnVA,lnVBを減算回路23にて減算することに
より、減算回路23から信号電圧VA,VBのレ
ベル比の対数値lnVA/VBが出力されることに
なる。この減算回路23出力lnVA/VBは反射
型光電スイツチYから被検知物体Xまでの距離l
に応じて変化し、距離lに対する減算回路23出
力lnVA/VBは第5図に示すようになる。した
がつて、比較回路24の検知エリア設定ボリウム
24aにて動作レベルVsを適当に設定すること
により、正確な検知エリアDEが容易に設定でき、
減算回路23出力lnVA/VBが動作レベルVs以
下となつたとき比較回路24出力がHレベルとな
り、信号処理回路25を介して出力回路6が作動
されるようになつている。なお、対数増巾回路2
2a,22bに代えて、リニア増巾回路を用いる
とともに減算回路23に代えて除算回路を用いて
増巾手段および演算手段を形成しても良い。
ここに、上述のような基本例において、判別制
御手段5はPSD4から出力される信号電流IA,
IBを増巾した信号のレベル比の対数値を演算し
てその演算値が所定の検知範囲か否かによつて被
検知物体Xが検知エリアDE内にあるかどうかを
判別して出力回路6を作動させているので、被検
知物体Xの光反射率に関係なく検知エリアDEを
設定でき、さらに投、受光用光学系13,3の汚
れの影響を受けることがないようになつている。
ところで、このような基本例において、被検知
物体Xの光反射率あるいは被検知物体Xまでの距
離lが大巾に変化して受光量が大巾に変動した場
合にあつても誤動作が生じないようにするには、
受光回路21a,21bおよび対数増巾回路22
a,22bよりなる信号電流IA,IBの増巾手段
のダイナミツクレンジを広くしておく必要があ
り、被検知物体Xの光反射率の変化に加えて検知
エリアDEの設定可能範囲を考慮すれば上記増巾
手段のダイナミツクレンジは4〜5桁以上にする
必要がある。しかしながら、このような広いダイ
ナミツクレンジを実現することは非常に難しいの
で、通常は3桁程度のダイナミツクレンジを有す
る増巾手段を用いている。したがつて、被検知物
体Xが高反射率を有するものであり、かつ検知エ
リアDEを近くに設定したとき、信号電流IA,IB
の増巾手段が飽和して測距誤差が生じ、出力回路
6が誤動作する場合があるという問題があつた。
第6図は上記問題点を示す図であり、距離lに対
する減算回路23出力lnVA/VB、対数増巾回
路22a,22bの出力lnVA,lnVBの変化を示
している。いま、同図bに示すように信号電流
IBの増巾手段21b,22bが距離lβで飽和し、
信号電流IAの増巾手段21a,22aが距離lα
で飽和するものとすれば、距離lβ〜lαの区間にお
いて、減算回路23出力lnVA/VBが距離lに
対応しなくなつて測距誤差が生じ、距離lβ以下の
区間においては減算回路23出力lnVA/VBが
「0」(IA/IB=1)となつて測距不能になる。
但し、減算回路23出力lnVA/VBの「0」は
集光スポツトSがPSD4の中央に結像され信号
電流比IA,IBが「1」となる距離lcに対応する。
同図aの実線は受光回路21a,21bあるいは
対数増巾回路22a,22bの飽和が発生した場
合、点線は飽和が発生しない場合を示している。
ここに動作レベルVsを第5図に想像線で示すう
に「0」以下に設定し、比較回路23による検知
範囲として「0」を含まないように設定した場合
において、高反射率の被検知物体Xが検知エリア
DE′に存在して信号電流IA,IBの増巾手段が共
に飽和すると、減算回路23出力lnVA/VBが
「0」になり、出力回路6は作動しない。したが
つて、検知エリアDE′内に被検知物体Xが存在し
ているにも拘らず被検知物体Xが検知されないと
いう不都合があつた。つまり、増巾手段の飽和に
よつて、被検知物体Xが恰も距離lcの位置(信号
電流比IA/IB=1の位置)に存在しているかの
ように判別され、被検知物体Xを見落すことにな
り、このような検知ミスが発生すると、出力回路
6にて制御される機器が異常動作して危険である
という問題があつた。
(発明の目的)
本発明は上記の点に鑑みて為されたものであ
り、その目的とするところは、増巾手段が飽和し
た場合における被検知物体の飽和ミスを防止する
ことができる光電スイツチを提供することにあ
る。
(発明の開示)
実施例 1
第7図は本発明一実施例を示すもので、前述の
基本例と同様の光電スイツチにおいて、検知エリ
ア設定用ボリウム24aによる比較回路24の動
作レベルVsを「0」以上で設定自在にする設定
制御手段24bを設けたものであり、比較判別手
段の検知範囲は増巾手段たる受光回路21a,2
1b、対数増巾回路22a,22bが飽和したと
きの演算手段出力、すなわち減算回路23出力で
あるところの「0」を含んで設定自在となつてい
る。つまり、検知エリアDEの遠限点Aの設定可
能範囲A1〜A2の最近点A1の距離la1を第8図に示
すように、PSD4および集光手段3により決定
される中央点Cの距離lcよりも大きく(la1lc)
なるようにしたものである。
而して、遠限点Aの距離laをla1〜la2に設定し
た検知エリアDEに光反射率の高い被検知物体X
が存在して強い反射光Rが受光されると、PSD
4から出力される検知信号すなわち信号電流IA,
IBが大きくなつて受光回路21a,21b、対
数増巾回路22a,22bが飽和し、信号電流比
IA/IBが「1」になつて減算回路24出力
lnVA/VBが「0」となり測距不能状態となる
が、実施例1にあつては、設定制限手段24bに
より比較回路24の動作レベルVsが常に0以上
に設定されるようにしているので、被検知物体X
が存在するものと判断され出力回路6が作動され
る。したがつて、増巾手段の飽和に起因する被検
知物体Xの検知ミスが防止され、出力回路6にて
制御される機器が異常動作する危険が発生しない
ことになる。すなわち、本発明にあつては増巾手
段が飽和した場合に被検知物体Xが検知エリア
DE内に存在するものと判断して出力回路6を作
動させるように検知エリアDEが設定されるので、
いわゆるフエールセーフ機能が付加されたことに
なつて危険が回避されるようになつているわけで
ある。
ところで、このような三角測量方式の光電スイ
ツチにおけるPSD4上の集光スポツトSの中心
位置Zは、第8図に示すように凸レンズよりなる
集光手段3の集光手段3とPSD4間の距離をF
とすれば、Z=l0×F/lとなり、距離lが大きく
なると距離変化Δlに対するZの変化は第9図に
示すようにΔZ1からΔZ2まで小さくなつてゆく。
一方、ZとPSD4から出力される信号電流比
IA/IBの関係は、PSD4の長さをLとすれば
lnlA/IB=ln(L/Z−1)となり、Zの変化ΔZ1〜
ΔZ2が小さくなるとIA/IBの変化も小さくなり
測距精度が低下する。しかしながら、PSD4の
端部に光が当るときの信号電流比IA/IBは第1
0図に示すようにに急峻となるので、この部分を
使えば精度の低下が少なくなる。つまり、検知エ
リアDEの設定可能範囲の最遠点A2に存在する被
検知物体Xの反射光Rの集光スポツトS′を第8図
に示すようにできるだけPSD4の端部に結像さ
せるような光学系を設計すれば良いことになる。
ここに、第8図において最遠点A2と集光手段3
の中心とを結ぶ直線上にPSD4の一方の端部が
位置するようにしているが、実際にはPSD4上
での集光スポツトSはある程度の大きさをもつて
いるので、集光スポツトSの中心はPSD4の端
部よりも少々内側に位置させている。したがつ
て、上記条件および前記条件に基いて、PSD4
の中心が検知エリアDEの設定可能範囲の最近点
A1と集光手段3の中心とを結ぶ直線上に位置し、
PSD4の一方の端部4aが検知エリアDEの設定
可能範囲の最遠点A2と集光手段3の中心とを結
ぶ直線上に位置するように光学系およびPSD4
の長さを設計すれば良いことになる。したがつ
て、PSD4の長さは決まつてきて、PSD4の他
方の端部4bと集光手段3の中心を結ぶ直線が投
光手段1の光軸と交わる点が検知エリアDEに理
論的近限点Bとなる。すなわち、この近限点Bの
距離lbよりも被検知物体Xまでの距離lが小さく
なると、集光スポツトSがPSD4の他方の端部
4bから外れてしまうため、検知動作が行なえな
くなつて不感応部分ができる。この近限点Bの距
離lbはlb=la2×lc/2la2−lcとなる。ところが、光電
スイ
ツチとしては、近限点Bよりも近い部分(投光用
光学系13の近傍まで)を検知エリアDEに含め
る必要があるので、この不感応部分の存在が問題
となる。しかしながら、実際にはPSD4上の集
光スポツトSは点ではなくある程度の大きさを持
つており、集光ビームをぼかしてPSD4の端部
4bにおける集光スポツトSを適当に大きくする
ことにより、集光スポツトSの中心がPSD4の
端部4bから外れてもPSD4上にある程度の反
射光が集光されるようにでき、上記不感応部分を
なくすことが可能となる。しかしながら、集光ビ
ームをぼかして集光スポツトSを大きくする場合
において、あまり大きくすると、集光スポツトS
内での反射ムラの影響が大きくなり、著しく精度
が低下するので、集光スポツトSをあまり大きく
しなくても良いようにするには近限点Bを適当に
設定する必要がある。以上の点を考慮して色々な
系について実験を行つた結果、少くともlb2/3
lcの関係をもつて近限点Bを設定すれば良いこと
がわかつた。ここに、近限点Bはla2×lc/2la2−lcで
あ
るので、Ra22Rcという関係を満足すれば良い
ことになる。
一方、上述の考察は、光電スイツチ本体の大き
さ(例えば投、受光手段1,2の間隔l0)を無視
しているが、実際には検知エリアDEの距離A1,
A,A2と光電スイツチ本体の大きさとは使いや
すさの点から経験的におよそ決まつたものであ
り、このことを考慮してl0とlcとの望ましい関係
を実験的に求めたところlc/lo20が得られた。下
表はPSD4の長さLを3mmとして上述の条件に
基いて各部の寸法を設計した具体例を示してい
る。但し、fは凸レンズよりなる集光手段3の焦
点距離、dはレンズ径である。
(Technical Field) The present invention relates to a reflective photoelectric switch that controls an output circuit by determining whether or not a detected object exists within a preset detection area. (Background Art) Figures 1 to 3 show basic examples of this type of reflective photoelectric switch.
It is a light projecting means for projecting a light beam P made of pulse modulated light onto a target, and includes an oscillation circuit 10 that generates a synchronization signal for setting the light projection timing, a drive circuit 11, and a light emitting diode, laser diode, etc. It is formed by an optical element 12 and a light projecting optical system 13 consisting of a condenser lens that forms a light beam P. Reference numeral 2 denotes a light receiving means juxtaposed with a predetermined distance l 0 from the light projecting means 1, and the projecting and light receiving means 1 and 2 are arranged in a triangular manner with respect to the object X to be detected. This light receiving means 2 includes a condensing means 3 made of a convex lens for condensing the light reflected by the object to be detected The position detecting means 4 is arranged within the condensing plane of the condensing means 3 made of a convex lens, and the position detecting means 4 is arranged in the condensing plane of the condensing means 3 made of a convex lens, and changes the amount of light when the condensing spot S moves in one direction. It outputs a first detection signal IA that increases in proportion to the amount of movement and outputs a second detection signal IB that increases in proportion to the amount of light and decreases in accordance with the amount of movement. Here, in the basic example, this position detection means 4 is a one-dimensional position detection element (hereinafter referred to as
As shown in FIG. 3a, this PSD 4 is formed by forming a P layer 31a on the front surface of a flat silicon 31, an N layer 31b on the back surface, and an I layer 31c in the middle. Signal currents IA and IB corresponding to the position of the condensing spot S are output. This signal current IA is a signal that increases in proportion to the amount of movement of the condensing spot S in one direction, and the signal current IB is a signal that decreases in proportion to the amount of movement. Of course, it goes without saying that the signal currents IA and IB are proportional to the amount of light. FIG. 3b shows an equivalent circuit of the position sensing element 4, where Pi is a current source, Do is an ideal diode, Co is a junction capacitance, Pt is a parallel resistance, and Ro is an interelectrode resistance. The position detecting means 4 may be any device as long as it can obtain contradictory signal currents IA and IB according to the movement of the condensing spot S when the distance l changes; It may be formed by two light receiving elements, and a phototransistor, a photodiode, a solar cell, CdS, etc. are used as the light receiving element. 5 is a discrimination control means, which detects the detected object X based on the output of the position detection means 4.
The output circuit 6 is controlled by determining whether or not the detection area DE exists within a predetermined detection area DE. The discrimination control means 5 includes light receiving circuits 21a and 21b that amplify and convert signal currents IA and IB from the position detection means 4 into signal voltages VA and VB, logarithmic amplification circuits 22a and 22b, and a logarithmic amplification circuit 22a. output
A subtraction circuit 23 that subtracts the logarithmic amplification circuit 22b output lnVB from lnVA, and a subtraction circuit 23 output lnVA/
The subtraction circuit 23 compares VB with the operation level Vs set by the detection area setting volume 24a.
A comparator circuit 24 that outputs an H level when the output lnVA/VB is lower than the operating level Vs, and the emission timing of the light beam P from the light emission element 12 (the oscillation circuit 10
The comparison circuit 2 is synchronized with the synchronization signal output from the
It is formed with a signal processing circuit 25 that reliably determines whether or not the detected object X exists within the detection area DE by sampling the four outputs. It is designed to control an output circuit 6 consisting of a relay, a semiconductor switch element for load control, etc.
Note that the light receiving circuits 21a and 21b include a bandpass filter circuit that passes only a pulsed optical signal and cuts out a DC optical signal, or that passes only a specific frequency. Now, when the detected object X exists at distances l 1 , l 2 , l 3 from the reflective photoelectric switch Y as shown in FIG. The positions of the condensing spots S are as shown in Fig. 4b, and when the position of the detected object X changes in the projection direction of the light beam P, the condensed beam S moves in the direction of the arrow M and is output from the PSD 4. The signal currents IA and IB thus generated become position signals corresponding to the position of the condensing spot S. In the discrimination control means 5, the signal currents IA and IB are detected by the light receiving circuits 21a and 21b.
Signal voltages VA and VB are formed proportional to
By subtracting lnVA and lnVB in the subtraction circuit 23, the subtraction circuit 23 outputs a logarithmic value lnVA/VB of the level ratio of the signal voltages VA and VB. The output lnVA/VB of this subtraction circuit 23 is the distance l from the reflective photoelectric switch Y to the detected object X.
The output lnVA/VB of the subtraction circuit 23 with respect to the distance l becomes as shown in FIG. Therefore, by appropriately setting the operating level Vs with the detection area setting volume 24a of the comparison circuit 24, an accurate detection area DE can be easily set.
When the output lnVA/VB of the subtraction circuit 23 becomes lower than the operating level Vs, the output of the comparison circuit 24 becomes H level, and the output circuit 6 is activated via the signal processing circuit 25. Note that the logarithmic amplification circuit 2
In place of 2a and 22b, a linear amplification circuit may be used, and in place of the subtraction circuit 23, a division circuit may be used to form the amplification means and the calculation means. Here, in the above-mentioned basic example, the discrimination control means 5 uses the signal current IA output from the PSD 4,
The output circuit 6 calculates the logarithm of the level ratio of the signal with IB amplified and determines whether the detected object X is within the detection area DE based on whether the calculated value is within the predetermined detection range. is activated, the detection area DE can be set regardless of the light reflectance of the object to be detected X, and furthermore, it is not affected by dirt on the optical systems 13 and 3 for projecting and receiving light. By the way, in such a basic example, even if the light reflectance of the detected object X or the distance l to the detected object X changes widely, and the amount of received light fluctuates widely, no malfunction will occur. To do this,
Light receiving circuits 21a, 21b and logarithmic amplification circuit 22
It is necessary to widen the dynamic range of the amplification means for the signal currents IA and IB consisting of a and 22b, and in addition to the change in the light reflectance of the detected object X, the range in which the detection area DE can be set must be considered. For example, the dynamic range of the width increasing means needs to be 4 to 5 orders of magnitude or more. However, since it is very difficult to achieve such a wide dynamic range, amplifying means having a dynamic range of about three digits is usually used. Therefore, when the detected object X has a high reflectance and the detection area DE is set nearby, the signal currents IA and IB
There has been a problem in that the amplifying means of the sensor becomes saturated and a distance measurement error occurs, which may cause the output circuit 6 to malfunction.
FIG. 6 is a diagram illustrating the above-mentioned problem, and shows changes in the output lnVA/VB of the subtraction circuit 23 and the outputs lnVA and lnVB of the logarithmic amplification circuits 22a and 22b with respect to the distance l. Now, as shown in figure b, the signal current
IB amplification means 21b and 22b are saturated at distance lβ,
The amplifying means 21a and 22a of the signal current IA are at a distance lα
If it is assumed that the subtraction circuit 23 output lnVA/VB no longer corresponds to the distance l in the interval from distance lβ to lα, a distance measurement error will occur, and in the interval below the distance lβ, the subtraction circuit 23 output lnVA /VB becomes "0" (IA/IB=1) and distance measurement becomes impossible.
However, "0" of the output lnVA/VB of the subtraction circuit 23 corresponds to the distance lc at which the condensing spot S is imaged at the center of the PSD 4 and the signal current ratios IA and IB are "1".
The solid line in FIG. 1A shows the case where saturation occurs in the light receiving circuits 21a, 21b or the logarithmic amplification circuits 22a, 22b, and the dotted line shows the case where saturation does not occur.
Here, when the operating level Vs is set to "0" or less as shown by the imaginary line in FIG. X is the detection area
When the amplification means of the signal currents IA and IB are saturated at DE', the output lnVA/VB of the subtraction circuit 23 becomes "0" and the output circuit 6 does not operate. Therefore, there was an inconvenience that the object to be detected X was not detected even though the object to be detected X existed within the detection area DE'. In other words, due to the saturation of the amplification means, the detected object If such a detection error occurs, the equipment controlled by the output circuit 6 may operate abnormally, which is dangerous. (Object of the Invention) The present invention has been made in view of the above points, and its object is to provide a photoelectric switch that can prevent the saturation error of the detected object when the amplification means is saturated. Our goal is to provide the following. (Disclosure of the Invention) Embodiment 1 FIG. 7 shows an embodiment of the present invention. In a photoelectric switch similar to the basic example described above, the operation level Vs of the comparison circuit 24 is set to "0" by the detection area setting volume 24a. A setting control means 24b that can be set freely is provided, and the detection range of the comparison and discrimination means is limited to the light receiving circuits 21a and 2, which are amplifying means.
1b and "0", which is the arithmetic means output when the logarithmic amplification circuits 22a and 22b are saturated, that is, the subtraction circuit 23 output. In other words, as shown in FIG. 8, the distance la 1 of the nearest point A 1 of the settable range A 1 to A 2 of the far limit point A of the detection area DE is determined by the center point C determined by the PSD 4 and the condensing means 3. distance greater than lc (la 1 lc)
It was made so that it would become so. Therefore , a detected object
exists and strong reflected light R is received, the PSD
The detection signal output from 4, that is, the signal current IA,
As IB increases, the light receiving circuits 21a and 21b and the logarithmic amplification circuits 22a and 22b become saturated, and the signal current ratio
IA/IB becomes “1” and subtraction circuit 24 outputs
lnVA/VB becomes "0" and distance measurement becomes impossible, but in the first embodiment, the operating level Vs of the comparator circuit 24 is always set to 0 or higher by the setting limiting means 24b. Detected object X
is determined to exist, and the output circuit 6 is activated. Therefore, detection errors of the detected object X due to saturation of the amplification means are prevented, and there is no risk that the equipment controlled by the output circuit 6 will malfunction. In other words, in the present invention, when the amplifying means is saturated, the detected object
Since the detection area DE is set so that it is determined that it exists within DE and the output circuit 6 is activated,
With the addition of a so-called fail-safe function, danger can now be avoided. By the way, the center position Z of the condensing spot S on the PSD 4 in such a triangulation type photoelectric switch is determined by the distance between the condensing means 3 of the convex lens and the PSD 4, as shown in FIG. F
Then, Z=l 0 ×F/l, and as the distance l increases, the change in Z with respect to the distance change Δl decreases from ΔZ 1 to ΔZ 2 as shown in FIG.
On the other hand, the signal current ratio output from Z and PSD4
The relationship between IA/IB is, if the length of PSD4 is L,
lnlA/IB=ln(L/Z-1), and as the change in Z ΔZ 1 to ΔZ 2 becomes smaller, the change in IA/IB also becomes smaller and the ranging accuracy decreases. However, when light hits the edge of PSD4, the signal current ratio IA/IB is the first
As shown in Figure 0, the curve becomes steep, so if this part is used, the drop in accuracy will be reduced. In other words, the focus spot S ' of the reflected light R of the detected object All you have to do is design a suitable optical system.
Here, in Fig. 8, the farthest point A 2 and the condensing means 3
One end of the PSD 4 is positioned on a straight line connecting the center of The center is located slightly inside the edge of PSD4. Therefore, based on the above conditions and conditions, PSD4
The center of is the nearest point of the settable range of the detection area DE
Located on the straight line connecting A 1 and the center of the condensing means 3,
The optical system and PSD 4 are arranged so that one end 4a of the PSD 4 is located on a straight line connecting the farthest point A 2 of the settable range of the detection area DE and the center of the condensing means 3.
All you have to do is design the length. Therefore, the length of the PSD 4 is determined, and the point where the straight line connecting the other end 4b of the PSD 4 and the center of the condensing means 3 intersects with the optical axis of the light projecting means 1 is theoretically close to the detection area DE. This is the limit point B. In other words, when the distance l to the detected object Sensitive parts are formed. The distance lb of this near limit point B is lb=la 2 ×lc/2la 2 −lc. However, since the photoelectric switch needs to include a portion closer than the near limit point B (up to the vicinity of the light projecting optical system 13) in the detection area DE, the existence of this insensitive portion poses a problem. However, in reality, the condensing spot S on the PSD 4 is not a point but has a certain size, and by blurring the condensed beam and making the condensing spot S at the end 4b of the PSD 4 appropriately large, it is possible to Even if the center of the light spot S deviates from the end 4b of the PSD 4, a certain amount of reflected light can be focused on the PSD 4, making it possible to eliminate the above-mentioned insensitive portion. However, when blurring the focused beam to enlarge the focused spot S, if it is made too large, the focused spot S
Since the influence of reflection unevenness within the lens becomes large and the accuracy is significantly reduced, it is necessary to set the near limit point B appropriately in order to avoid making the focal spot S so large. As a result of conducting experiments on various systems in consideration of the above points, it was found that the near limit point B should be set with a relationship of at least lb2/3lc. Here, since the near limit point B is la 2 ×lc/2la 2 −lc, it is sufficient to satisfy the relationship Ra 2 2Rc. On the other hand, the above consideration ignores the size of the photoelectric switch body (for example, the distance l 0 between the emitter and light receiver means 1 and 2), but in reality, the distance A 1 of the detection area DE,
A, A 2 and the size of the photoelectric switch body are approximately determined empirically from the point of view of ease of use, and taking this into account, we experimentally determined the desirable relationship between l 0 and lc. lc/lo20 was obtained. The table below shows a specific example in which the length L of the PSD 4 is 3 mm and the dimensions of each part are designed based on the above conditions. However, f is the focal length of the condensing means 3 made of a convex lens, and d is the lens diameter.
【表】
上記具体例(A−1)乃至(A−3)によるl
−lnIA/IB特性はそれぞれ第11図乃至第13図と
なる。
(発明の効果)
本発明は上述のように、移動する被検知物体に
対して光ビームを投光する投光手段と、投光手段
の側方に所定間隔をもつて配設され、被検知物体
による光ビームの反射光を集光する集光手段と、
集光手段の集光面に配設され集光スポツトの一方
向の移動に際して光量に比例しかつその移動量に
応じて増加する第1の検知信号を出力するととも
に光量に比例しかつ移動量に応じて減少する第2
の検知信号を出力する位置検出手段と、両検知信
号をそれぞれ増幅する増巾手段と、増巾手段出力
に基いて検知信号のレベル比を演算する演算手段
と、演算手段出力が予め設定された検知範囲かど
うかを比較判別して該検知範囲内のとき出力回路
を作動させる比較判別手段とよりなる光電スイツ
チであるので、被検知物体の光反射率に関係なく
検知エリアを設定できるとともに投、受光用光学
系の汚れの影響を受けることがないという利点が
あり、また上記検知範囲を両増巾手段が飽和した
ときの演算手段出力を含んで設定自在とする設定
制限手段を設けたので、両増巾手段が飽和した場
合には必ず出力回路が作動され、増巾手段の飽和
に起因する被検知物体の検知ミスが防止され、出
力回路にて制御される機器が異常動作する危険が
ないという利点がある。[Table] l according to the above specific examples (A-1) to (A-3)
-lnIA/IB characteristics are shown in FIGS. 11 to 13, respectively. (Effects of the Invention) As described above, the present invention includes a light projecting means for projecting a light beam onto a moving detected object, and a light projecting means disposed at a predetermined interval on the side of the light projecting means. a condensing means for condensing light reflected from the light beam by the object;
A first detection signal is provided on the light collecting surface of the light collecting means, and outputs a first detection signal that is proportional to the amount of light and increases in accordance with the amount of movement when the light focusing spot moves in one direction, and is proportional to the amount of light and increases in accordance with the amount of movement. The second decreases accordingly
position detecting means for outputting a detection signal of It is a photoelectric switch that includes a comparison and discrimination means that compares and discriminates whether or not it is within the detection range and activates the output circuit when it is within the detection range, so it is possible to set the detection area regardless of the light reflectance of the object to be detected, and also to It has the advantage of not being affected by dirt on the light receiving optical system, and also has a setting restriction means that allows the detection range to be freely set to include the output of the calculation means when both amplification means are saturated. When both amplifying means are saturated, the output circuit is always activated, preventing misdetection of the object to be detected due to saturation of the amplifying means, and there is no risk of abnormal operation of equipment controlled by the output circuit. There is an advantage.
第1図は本発明に係る基本例の構成を示す図、
第2図は同上のブロツク回路図、第3図は同上に
用いる位置検出素子の構成および等価回路を示す
図、第4図乃至第6図は同上の動作説明図、第7
図は本発明一実施例のブロツク回路図、第8図乃
至第13図は同上の動作説明図である。
1は投光手段、3は集光手段、4は位置検出手
段、6は出力回路、22a,22bは対数増巾回
路、23は減算回路、24は比較回路、24bは
設定制限手段である。
FIG. 1 is a diagram showing the configuration of a basic example according to the present invention,
Fig. 2 is a block circuit diagram of the same as above, Fig. 3 is a diagram showing the configuration and equivalent circuit of the position detection element used in the above, Figs.
The figure is a block circuit diagram of one embodiment of the present invention, and FIGS. 8 to 13 are explanatory diagrams of the same operation. 1 is a light projection means, 3 is a condensing means, 4 is a position detection means, 6 is an output circuit, 22a, 22b are logarithmic amplification circuits, 23 is a subtraction circuit, 24 is a comparison circuit, and 24b is a setting restriction means.
Claims (1)
する投光手段と、投光手段の側方に所定間隔をも
つて配設され、被検知物体による光ビームの反射
光を集光する集光手段と、集光手段の集光面に配
設され集光スポツトの一方向の移動に際して光量
に比例しかつその移動量に応じて増加する第1の
検知信号を出力するとともに光量に比例しかつ移
動量に応じて減少する第2の検知信号を出力する
位置検出手段と、両検知信号をそれぞれ増幅する
増巾手段と、増巾手段出力に基いて検知信号のレ
ベル比を演算する演算手段と、演算手段出力が予
め設定された検知範囲かどうかを比較判別して該
検知範囲内のとき出力回路を作動させる比較判別
手段とよりなる光電スイツチであつて、上記検知
範囲を両増巾手段が飽和したときの演算手段出力
を含んで設定自在とする設定制御手段を設けたこ
とを特徴とする光電スイツチ。1. A light projecting means for projecting a light beam onto a moving object to be detected, and a condenser disposed at a predetermined interval on the side of the light projecting means to collect light reflected from the light beam by the object to be detected. A first detection signal is provided on the light collecting surface of the light means and the light collecting means, and outputs a first detection signal which is proportional to the amount of light and increases in accordance with the amount of movement when the light collecting spot moves in one direction, and which is proportional to the amount of light. and a position detection means that outputs a second detection signal that decreases in accordance with the amount of movement, an amplification means that amplifies both detection signals, and a calculation means that calculates a level ratio of the detection signals based on the output of the amplification means. and a comparison/discrimination means for comparing and discriminating whether the output of the arithmetic means is within a preset detection range and operating an output circuit when the output is within the detection range, the photoelectric switch comprising a means for amplifying the detection range. A photoelectric switch characterized in that it is provided with a setting control means that can freely set the output of the calculation means when the output of the calculation means is saturated.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59011349A JPS60154176A (en) | 1984-01-25 | 1984-01-25 | Photoelectric switch |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59011349A JPS60154176A (en) | 1984-01-25 | 1984-01-25 | Photoelectric switch |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS60154176A JPS60154176A (en) | 1985-08-13 |
| JPH0358475B2 true JPH0358475B2 (en) | 1991-09-05 |
Family
ID=11775559
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP59011349A Granted JPS60154176A (en) | 1984-01-25 | 1984-01-25 | Photoelectric switch |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS60154176A (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US5369462A (en) * | 1992-06-09 | 1994-11-29 | Olympus Optical Co., Ltd. | Inclination detecting apparatus and camera for detecting hand shake using the same |
-
1984
- 1984-01-25 JP JP59011349A patent/JPS60154176A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS60154176A (en) | 1985-08-13 |
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|---|---|---|---|
| EXPY | Cancellation because of completion of term |