JPH06137947A - High amplification measuring equipment of intensity of specific received pulse light - Google Patents

High amplification measuring equipment of intensity of specific received pulse light

Info

Publication number
JPH06137947A
JPH06137947A JP28895992A JP28895992A JPH06137947A JP H06137947 A JPH06137947 A JP H06137947A JP 28895992 A JP28895992 A JP 28895992A JP 28895992 A JP28895992 A JP 28895992A JP H06137947 A JPH06137947 A JP H06137947A
Authority
JP
Japan
Prior art keywords
output
light
pulse light
intensity
specific
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
Application number
JP28895992A
Other languages
Japanese (ja)
Other versions
JP2896547B2 (en
Inventor
Toshiaki Ishise
俊明 石瀬
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.)
Takenaka Komuten Co Ltd
Original Assignee
Takenaka Komuten Co Ltd
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 Takenaka Komuten Co Ltd filed Critical Takenaka Komuten Co Ltd
Priority to JP28895992A priority Critical patent/JP2896547B2/en
Publication of JPH06137947A publication Critical patent/JPH06137947A/en
Application granted granted Critical
Publication of JP2896547B2 publication Critical patent/JP2896547B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Abstract

PURPOSE:To provide a high amplification measuring equipment for measuring the intensity of specific received pulse light while tuning and amplifying and employed in means for detecting position, traveling direction or traveling speed of a specific pulse light source. CONSTITUTION:The high amplification measuring equipment of the intensity of specific received pulse light comprises a photoelectric converting element 1 which produces current upon receiving light, a tuning amplifier 2 for tuning/amplifying an output from the photoelectric converting element 1 produced upon receiving a pulse light of specific period, a comparator 3 for comparing an amplified output from the tuning amplifier 2 with a preset decision reference value and producing an ON output when the output from the tuning amplifier 2 is higher than the decision reference value otherwise producing an OFF output, and a unit for calculating the rate of ON output for a predetermined time as the intensity of received pulse light having specific period. This equipment alloxys great amplification of pulse light having specific period and high sensitivity catching of light emitting source and thereby employed generally in photometer, distance measuring equipment, direction measuring equipment, and the like.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】この発明は、特定パルス光を高感
度に受光し、その受光強度も測定し、例えば目標とする
移動体(特定パルス光源)の位置(発光源位置)や進行
方向・進行速度などを検出する手段に使用される、特定
パルス光の受光強度の高増幅測定装置に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention receives a specific pulsed light with high sensitivity and also measures the intensity of the received light. For example, a target position of a moving body (specific pulsed light source) and a traveling direction, The present invention relates to a high-amplification measuring device for the received light intensity of a specific pulsed light, which is used as a means for detecting the traveling speed.

【0002】[0002]

【従来の技術】目標物を追尾しようとする場合、目標物
の方向,目標物までの距離を測定することが必要とな
る。そこで従来、目標物の方向や距離を把握する手段と
しては、例えば距離については、超音波やレーザー光の
対象物からの反射時間を利用する技術が主流である。ま
た、目標物の方向を定める手段には、目標物に特定パル
ス光源をセットし、それをPSD(ポジショニングセン
サ)やCCD(電荷結合素子)で測定することが主に用
いられている。
2. Description of the Related Art In order to track a target object, it is necessary to measure the direction of the target object and the distance to the target object. Therefore, conventionally, as a means for grasping the direction and distance of a target, for example, with respect to the distance, a technique in which the reflection time of an ultrasonic wave or a laser beam from the object is mainly used. Further, as a means for determining the direction of the target object, it is mainly used to set a specific pulse light source on the target object and measure it with a PSD (positioning sensor) or a CCD (charge coupled device).

【0003】[0003]

【本発明が解決しようとする課題】超音波やレーザ光を
利用した距離測定装置は、コストが高い上に、異なる目
標物別に反射波を区別することができないし、目標物を
特定するのが困難である。また、PSDを利用した方向
測定装置は、増幅率をあまり大きくできず、感度が低い
ので、受光の高感度化の要請に反する。
A distance measuring device using ultrasonic waves or laser light is high in cost, cannot distinguish reflected waves for different target objects, and specifies a target object. Have difficulty. Further, since the direction measuring device using PSD cannot increase the amplification factor so much and has low sensitivity, it is against the demand for high sensitivity of light reception.

【0004】従って、本発明の目的は、発光源を高感度
でキャッチするために、特定周期パルス光の高増幅を可
能にし、光度計や距離測定装置、方向測定装置などに広
く利用できる、特定パルス光の受光強度高増幅測定装置
を提供することである。
Therefore, an object of the present invention is to enable a high amplification of a pulse light having a specific period in order to catch a light emitting source with high sensitivity, and can be widely used in photometers, distance measuring devices, direction measuring devices, etc. An object of the present invention is to provide a high-amplification measuring device for the received light intensity of pulsed light.

【0005】[0005]

【課題を解決するための手段】上記の課題を解決するた
めの手段として、本発明に係る特定パルス光の受光強度
高増幅測定装置は、受光することにより電流を出力する
光電変換素子1と、特定周期のパルス光による前記光電
変換素子1からの出力を同調・増幅する同調増幅器2
と、前記同調増幅器2により増幅された出力Vo(電
圧)と、予め設定された判定基準Vc(電圧)とを比較
し、前記同調増幅器2の出力Voが前記判定基準値Vc
より大きいとオン出力し、小さいとオフ出力するコンパ
レータ3と、前記オン・オフ出力の一定時間におけるオ
ン出力状態の割合を特定周期パルス光の受光強度として
算定する装置(パルスカウンタ)5とで構成されている
ことを特徴とする。
As means for solving the above-mentioned problems, a measuring apparatus for highly amplifying received light intensity of a specific pulsed light according to the present invention comprises a photoelectric conversion element 1 which outputs a current by receiving light. Tuning amplifier 2 for tuning / amplifying the output from the photoelectric conversion element 1 by pulsed light of a specific cycle
And the output Vo (voltage) amplified by the tuning amplifier 2 and a preset determination reference Vc (voltage) are compared, and the output Vo of the tuning amplifier 2 is determined as the determination reference value Vc.
It is composed of a comparator 3 that outputs ON when it is larger, and outputs OFF when it is smaller, and a device (pulse counter) 5 that calculates the ratio of the ON output state of the ON / OFF output in a certain period of time as the received light intensity of pulse light of a specific cycle. It is characterized by being.

【0006】[0006]

【作用】光電変換素子1は受光した光量に応じた大きさ
の電流を出力し、同調増幅器2は前記光電変換素子1の
出力の中から特定周期パルス光の出力を増幅し、応答電
圧(又は電流)として出力する。コンパレータ3は増幅
された前記の受光応答電圧Voを判定基準電圧Vcと比
較し、受光応答電圧Voが判定基準電圧Vcを超えると
きはオン出力し、それ以下のときオフ出力する。パルス
カウンタ5は、前記オン出力の割合を算定してデジタル
出力する。
The photoelectric conversion element 1 outputs a current having a magnitude corresponding to the amount of received light, and the tuning amplifier 2 amplifies the output of the pulse light having a specific period from the output of the photoelectric conversion element 1 to obtain a response voltage (or Current). The comparator 3 compares the amplified light reception response voltage Vo with the determination reference voltage Vc, and outputs ON when the light reception response voltage Vo exceeds the determination reference voltage Vc, and outputs OFF when it is less than that. The pulse counter 5 calculates the ratio of the ON output and digitally outputs it.

【0007】[0007]

【実施例】次に、図示した本発明の実施例を説明する。
図1に示した高増幅測定装置を構成する光電変換素子の
一つであるフォトダイオード1は、受光した光量に応じ
た(比例した)大きさの電流を発生(光電変換)する。
同調増幅器2は、前記フォトダイオード1で発生した特
定周期パルス光による出力を同調増幅し、受光応答電圧
Voとして出力する。コンパレータ3は、前記の同調増
幅器2から出力された前記受光応答電圧Voと、判定基
準電圧電源4から供給された判定基準電圧Vcとを比較
し、受光応答電圧Voの方が大きいとオン(Vccボル
ト)として出力し、小さいとオフ(ゼロボルト)として
出力する。なお、判定基準電圧電源4は、判定基準電圧
Vcを任意の電圧値に設定できる可変タイプとして構成
されている。パルスカウンタ5は、コンパレータ3から
変換出力された前記のオン・オフ出力から、一定時間の
間で一定回数を読みに行き、オン状態の割合を算定し、
このオン状態の割合をもって特定周期パルス光の受光強
度のデジタル出力とする。
EXAMPLE An example of the present invention shown in the drawings will be described below.
The photodiode 1 which is one of the photoelectric conversion elements constituting the high-amplification measuring device shown in FIG. 1 generates (photoelectric conversion) a current having a magnitude (proportional) corresponding to the amount of received light.
The tuned amplifier 2 tunes and amplifies the output of the pulse light having the specific period generated in the photodiode 1, and outputs the amplified output as a light reception response voltage Vo. The comparator 3 compares the light reception response voltage Vo output from the tuning amplifier 2 with the determination reference voltage Vc supplied from the determination reference voltage power supply 4, and is turned on (Vcc) when the light reception response voltage Vo is higher. Volt), and if it is small, it is output as off (zero volt). The judgment reference voltage power supply 4 is configured as a variable type capable of setting the judgment reference voltage Vc to an arbitrary voltage value. The pulse counter 5 reads a certain number of times from the above-mentioned on / off output converted and output from the comparator 3 in a certain period of time to calculate the on-state ratio,
The ratio of this ON state is used as a digital output of the received light intensity of the specific cycle pulsed light.

【0008】次に、上述した高増幅測定装置の動作状態
例を図2と図3を参照して説明する。例えば、電圧利得
が80dBを越えるような高増幅を行う場合、図2に示し
たように、入射光の光度が安定していても、フォトダイ
オード1の出力が同調増幅器2によって共振増幅された
後には時間的に激しく変動している。受光応答電圧Vo
の一例をあげると、図3Aに示したグラフのようにな
る。本実施例の同調増幅器2は、飽和電圧が5Vに設定
されている。コンパレータ3での比較動作によって、図
3Aに示した判定基準電圧値Vcのラインを超えたもの
は、オン出力としてVcc=5V(オン状態)を出力
し、判定基準電圧値Vcのライン以下のものは、オフ出
力として0V(オフ状態)を出力する。その結果、図3
Aの受光応答電圧Voは、図3Bに示したオン・オフ状
態変換図のように出力変換される。この出力変換に対し
て、パルスカウンタ5が、一定時間内に例えば1000
回読みに行き650回オン状態(割合)をカウントした
とすると、この場合「650」の受光強度としてデジタ
ル出力が出力されることになる。
Next, an example of the operating state of the above-mentioned high amplification measuring apparatus will be described with reference to FIGS. 2 and 3. For example, in the case of performing high amplification such that the voltage gain exceeds 80 dB, after the output of the photodiode 1 is resonance-amplified by the tuning amplifier 2 even if the intensity of the incident light is stable, as shown in FIG. Fluctuates wildly over time. Light reception response voltage Vo
As an example, the graph shown in FIG. 3A is obtained. The saturation voltage of the tuning amplifier 2 of this embodiment is set to 5V. Those that exceed the line of the judgment reference voltage value Vc shown in FIG. 3A by the comparison operation of the comparator 3 output Vcc = 5V (ON state) as an ON output and are below the line of the judgment reference voltage value Vc. Outputs 0 V (off state) as an off output. As a result,
The light reception response voltage Vo of A is output-converted as in the ON / OFF state conversion diagram shown in FIG. 3B. In response to this output conversion, the pulse counter 5 outputs 1000
Assuming that the ON state (ratio) is counted 650 times by going through the reading, the digital output will be output as the received light intensity of "650" in this case.

【0009】以上のように出力されたデジタル出力を光
度計に利用する場合は、図示を省略した演算装置によっ
て、ある一定時間内におけるオン状態の割合を百分率で
表すことができる。例えば、100パーセント受光状態
のオン回数を基にして、図4に示したキャリブレーショ
ンカーブが求められる。このキャリブレーションカーブ
を読み出し表示装置によって受光強度が表示されれば、
上述した高増幅測定装置全体が光度計として利用され
る。自然空間には、通常外乱光が満ちているが、本発明
の測定装置は特定周期のパルス光のみに反応するので、
太陽光等の外乱光の下でも十分に高感度の受光強度測定
が可能となる。また、後述する距離測定装置や方向測定
装置なども同様に受光の高感度化が可能である。
When the digital output output as described above is used for a photometer, an arithmetic unit (not shown) can express a percentage of the ON state within a certain fixed time as a percentage. For example, the calibration curve shown in FIG. 4 is obtained based on the number of times the 100% light receiving state is turned on. If this calibration curve is read and the received light intensity is displayed by the display device,
The entire high-amplification measuring device described above is used as a photometer. The natural space is usually filled with ambient light, but since the measuring device of the present invention responds only to pulsed light of a specific period,
It is possible to measure the received light intensity with a sufficiently high sensitivity even under ambient light such as sunlight. Further, a distance measuring device, a direction measuring device, and the like, which will be described later, can similarly increase the sensitivity of light reception.

【0010】次に、距離測定装置として利用する場合、
一般に光の強度は光源から離れる程小さくなる。一例と
して、図5に示したグラフのように、前記の受光強度と
距離との関係を予め求めておけば、フォトダイオード1
から光源までの距離を推定することができ距離測定装置
として利用できる。また、方向測定装置としては、図6
Aに示したように、フォトダイオード1を備えたセンサ
6と、そのすぐ後ろに焦点を合わせたレンズ7とで構成
することができる。あるいは、図6Bに示したように、
センサ6を底面に設置した有底円筒形状のカバー8とし
て構成することもできる。いずれも入射光Aに対して角
度をもって入射する入射光Bのセンサ6への入射面積
を、入射光Aのセンサ6への入射面積と比較すると、図
6Aでは横にずれた焦点のため、図6Bではカバー8の
円筒のため、入射光Bのセンサ6への入射面積の方が小
さい。入射面積が小さいので入射光量も小さくなり、入
射角度と入射光量との間に反比例関係が成立する。従っ
て、ある方向からの受光強度を本発明の測定装置でデジ
タル出力させ演算することにより、方位角を測定でき、
方向測定装置として利用することができる。
Next, when used as a distance measuring device,
Generally, the intensity of light decreases as the distance from the light source increases. As an example, if the relationship between the received light intensity and the distance is obtained in advance as shown in the graph of FIG.
The distance from the light source to the light source can be estimated and it can be used as a distance measuring device. Further, as a direction measuring device, FIG.
As shown in A, it can consist of a sensor 6 with a photodiode 1 and a focused lens 7 directly behind it. Alternatively, as shown in FIG. 6B,
The sensor 6 may be configured as a bottomed cylindrical cover 8 installed on the bottom surface. In both cases, when the incident area of the incident light B incident on the sensor 6 with respect to the incident light A is compared with the incident area of the incident light A on the sensor 6, in FIG. In 6B, since the cover 8 is a cylinder, the incident area of the incident light B on the sensor 6 is smaller. Since the incident area is small, the amount of incident light is also small, and an inverse proportional relationship is established between the incident angle and the incident light amount. Therefore, the azimuth angle can be measured by digitally outputting the received light intensity from a certain direction with the measuring device of the present invention and performing calculation,
It can be used as a direction measuring device.

【0011】[0011]

【本発明が奏する効果】本発明に係る特定パルス光の受
光強度の高増幅測定装置は、フォトダイオード1で受光
した光量に応じた大きさの出力(電流)が高増幅され、
その強さをさらにデジタル出力するので、特定周期パル
ス光の大増幅した強度測定が可能であり、発光源を高感
度でキャッチでき、光度計・距離測定装置・方向測定装
置などに広く利用できる。
In the highly amplified measuring apparatus for the received light intensity of the specific pulsed light according to the present invention, the output (current) having a magnitude corresponding to the amount of light received by the photodiode 1 is highly amplified,
Since the intensity is further digitally output, it is possible to measure the intensity of highly amplified specific period pulsed light, the light emission source can be caught with high sensitivity, and it can be widely used in photometers, distance measuring devices, direction measuring devices, and the like.

【図面の簡単な説明】[Brief description of drawings]

【図1】本実施例に係る特定パルス光の受光強度の高増
幅測定装置の構成図である。
FIG. 1 is a configuration diagram of a high-amplification measuring device for a received light intensity of specific pulsed light according to the present embodiment.

【図2】同上のフォトダイオードの出力の同調増幅後の
受光応答出力の時間による変化を示したグラフである。
FIG. 2 is a graph showing a change with time of a light reception response output after tuning and amplifying the output of the photodiode of the above.

【図3】Aは同上の同調増幅器による増幅後の受光応答
電圧を示し、Bはコンパレータによって受光応答電圧が
オン・オフ出力に変換される関係を示したグラフであ
る。
FIG. 3A is a graph showing a light reception response voltage after being amplified by the above tuning amplifier, and B is a graph showing a relationship in which the light reception response voltage is converted into an ON / OFF output by a comparator.

【図4】コンパレータのオン出力の百分率と受光強度と
の関係を示したキャリブレーションカーブである。
FIG. 4 is a calibration curve showing the relationship between the percentage of ON output of the comparator and the received light intensity.

【図5】フォトダイオード・光源間の距離とパルスカウ
ンタのカウント百分率との関係を示した曲線図である。
FIG. 5 is a curve diagram showing the relationship between the distance between the photodiode and the light source and the count percentage of the pulse counter.

【図6】Aはレンズを用いた場合の概要構成図であり、
Bはカバーを用いた場合の概要構成図である。
FIG. 6A is a schematic configuration diagram when a lens is used,
B is a schematic block diagram when a cover is used.

【符号の説明】[Explanation of symbols]

1 フォトダイオード 2 同調増幅器 3 コンパレータ 4 判定基準電圧電源 5 パルスカウンタ 1 Photodiode 2 Tuning amplifier 3 Comparator 4 Judgment reference voltage power supply 5 Pulse counter

───────────────────────────────────────────────────── フロントページの続き (51)Int.Cl.5 識別記号 庁内整理番号 FI 技術表示箇所 // G01P 3/36 Z 9010−2F ─────────────────────────────────────────────────── ─── Continuation of the front page (51) Int.Cl. 5 Identification number Office reference number FI technical display location // G01P 3/36 Z 9010-2F

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】受光することにより電流を出力する光電変
換素子と、 特定周期のパルス光による前記光電変換素子からの出力
を同調・増幅する同調増幅器と、 前記同調増幅器により増幅された出力と、予め設定され
た判定基準値とを比較し、前記同調増幅器の出力が前記
判定基準値より大きいとオン出力し、小さいとオフ出力
するコンパレータと、 前記オン・オフ出力の一定時間の間におけるオン出力状
態の割合を特定周期パルス光の受光強度として算定する
装置とで構成されていることを特徴とする、特定パルス
光の受光強度の高増幅測定装置。
1. A photoelectric conversion element that outputs a current by receiving light, a tuning amplifier that tunes and amplifies the output from the photoelectric conversion element by pulsed light of a specific period, and an output amplified by the tuning amplifier. A comparator that compares a preset judgment reference value, outputs ON when the output of the tuning amplifier is larger than the judgment reference value, and outputs OFF when the output is smaller than the judgment reference value, and an ON output during a certain time of the ON / OFF output. An apparatus for highly amplifying the received light intensity of a specific pulsed light, comprising: a device for calculating a ratio of states as a received light intensity of a specific cycled pulsed light.
JP28895992A 1992-10-27 1992-10-27 High-amplification measuring device for receiving light intensity of specific pulse light Expired - Fee Related JP2896547B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP28895992A JP2896547B2 (en) 1992-10-27 1992-10-27 High-amplification measuring device for receiving light intensity of specific pulse light

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP28895992A JP2896547B2 (en) 1992-10-27 1992-10-27 High-amplification measuring device for receiving light intensity of specific pulse light

Publications (2)

Publication Number Publication Date
JPH06137947A true JPH06137947A (en) 1994-05-20
JP2896547B2 JP2896547B2 (en) 1999-05-31

Family

ID=17737019

Family Applications (1)

Application Number Title Priority Date Filing Date
JP28895992A Expired - Fee Related JP2896547B2 (en) 1992-10-27 1992-10-27 High-amplification measuring device for receiving light intensity of specific pulse light

Country Status (1)

Country Link
JP (1) JP2896547B2 (en)

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS62142234A (en) * 1985-12-16 1987-06-25 Hamamatsu Photonics Kk High speed pulse repeating light measuring device
JPH04110619A (en) * 1990-08-30 1992-04-13 Topcon Corp Photometric apparatus

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS62142234A (en) * 1985-12-16 1987-06-25 Hamamatsu Photonics Kk High speed pulse repeating light measuring device
JPH04110619A (en) * 1990-08-30 1992-04-13 Topcon Corp Photometric apparatus

Also Published As

Publication number Publication date
JP2896547B2 (en) 1999-05-31

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