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JPS6024411B2 - Photometric conversion device - Google Patents
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JPS6024411B2 - Photometric conversion device - Google Patents

Photometric conversion device

Info

Publication number
JPS6024411B2
JPS6024411B2 JP3762777A JP3762777A JPS6024411B2 JP S6024411 B2 JPS6024411 B2 JP S6024411B2 JP 3762777 A JP3762777 A JP 3762777A JP 3762777 A JP3762777 A JP 3762777A JP S6024411 B2 JPS6024411 B2 JP S6024411B2
Authority
JP
Japan
Prior art keywords
light
digital
amount
signal
converter
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
Application number
JP3762777A
Other languages
Japanese (ja)
Other versions
JPS53123183A (en
Inventor
芳夫 前田
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.)
Hitachi Ltd
Original Assignee
Hitachi 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 Hitachi Ltd filed Critical Hitachi Ltd
Priority to JP3762777A priority Critical patent/JPS6024411B2/en
Priority to US05/888,655 priority patent/US4201472A/en
Priority to DE2814358A priority patent/DE2814358C3/en
Publication of JPS53123183A publication Critical patent/JPS53123183A/en
Publication of JPS6024411B2 publication Critical patent/JPS6024411B2/en
Expired legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01JMEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
    • G01J1/00Photometry, e.g. photographic exposure meter
    • G01J1/42Photometry, e.g. photographic exposure meter using electric radiation detectors
    • G01J1/44Electric circuits

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Spectroscopy & Molecular Physics (AREA)
  • Spectrometry And Color Measurement (AREA)
  • Photometry And Measurement Of Optical Pulse Characteristics (AREA)

Abstract

PURPOSE:To obtain a digital quantity, which is correctly proportional to the quantity of incident light, even in the case of weak light by effecting conversion to the digital quantity with the use of an AD converter after a preset quantity of electric signals are added to the either signals which are produced by photoelectric converting means.

Description

【発明の詳細な説明】 本発明は光量をディジタル量に変換する頚9光量変換装
置に係り、特に入射光量が微弱な場合においても入射光
量に正しく比例したディジタル量を与える脚光量変換装
置に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a neck light amount converting device that converts a light amount into a digital amount, and particularly to a leg light amount converting device that provides a digital amount that is accurately proportional to the incident light amount even when the incident light amount is weak.

例えば分光光度計のように光を用いて試料の分折を行な
う装置などにおいては、光量を光電変換手段(例えば光
電管や半導体光検知器など)によって電気信号に変換し
、電気信号処理によって例えば試料の透過率や吸光度を
求めることが行なわれる。
For example, in a device such as a spectrophotometer that uses light to analyze a sample, the amount of light is converted into an electrical signal by a photoelectric conversion means (for example, a phototube or a semiconductor photodetector), and the electrical signal processing is performed to analyze the sample. The transmittance and absorbance of the light are determined.

ところで近年のディジタル技術の発展に伴ない、上記し
た電気信号処理をアナログ回路によって行なうより、デ
ィジタル量で取扱う方が便利な場合があり、脚光量をデ
ィジタル量に変換する頚。光量変換が良く用いられるよ
うになって来た。このような場合、前記した光電変換手
段からのアナログ電気信号量をディジタル量に変換する
アナログーディジタル変換器(以下A−D変換器と略記
する。)が利用される。A一D変換器としては必要な精
度や回路の簡単さなどに見合った計数方式のものや比較
方式のものが良く用いられるが、いずれの場合も光量を
取り扱うには光量に比例した絶対値のディジタル量を得
る必要がある。また特に高濃度試料の吸光度測定やラマ
ン分光、蛍光分光欄光などにおいては、広いダイナミッ
クレンジが必要であり、かつ微弱光においても直線性良
く変換することが要求される。このように要求に対し、
従釆より用いられているA−D変換器には以下のような
幾つかの不都合な問題点があった。特に微弱光を取扱う
場合には、微弱信号城での良い直線性が必要であるが、
一般にA−D変換器では、良く用いられる電圧一周波数
変換器などのように入力が小さいところで直線性の悪い
ことが多い。電圧一周波腐変換器を用いるA−D変換器
の直線性のよい範囲は、変換されたパルスの周波数に依
存し、入力のフル・スケールの約1%までである。また
、二重積分形のA−D変換器の直線性が良い範囲は、レ
ベル比較器の精度に依存し、入力のフル・スケールに対
して約0.5%乃至5%程度である。すなわち、フル・
スケールが10VのA−○変換器においては、直線性の
よい範囲は、約1胸hV乃至10Vであり、1仇hV以
下の微弱信号は、正確にディジタル電気信号に変換でき
ない。また微弱光を例えば光電子増倍管などによって電
気信号に変換する場合、光電変換素子自体の発生する雑
音や周辺回路での雑音などにより、光蟹変換手段から得
られる電気信号は多くの雑音を含んでいることがある。
これに対し正の電気信号を取扱うA−D変換器では雑音
を多く含んだ零しベル近くの電気信号に対しては零しベ
ル以下の電気信号を無視してしまうため、光量に正しく
比例したディジタル量を得ることができない。尚、雑音
の信号レベルは条件によっても異るが、約lmV乃至I
Vである。 また負の電気信号をも含めてA−○変換す
るため、入力にバイアスを与える形式のA−○変換器で
は、雑音分を忠実に含んだディジタル信号が得られるも
のの光量に比例しなくなる不都合が生ずる。さらにまた
電圧一時間変換形A−D変換器のようにのこぎり波電圧
と入力電圧を比較して両者が一致するまでの時間を測定
する場合や、入力電圧を一定時間積分器で積分した後入
力電圧と逆極性の基準電圧を該積分器に加えてその出力
電圧が基準レベルに戻るまでの時間を測定する場合には
、雑音などにより入力信号がA一D変換中に零しベルを
越えない時にはしベル検出器が動作しないという動作不
止が生じ甚だ不都合である。
However, with the development of digital technology in recent years, it is sometimes more convenient to handle the above-mentioned electrical signal processing in digital quantities rather than using analog circuits, and it has become necessary to convert the amount of attention to digital quantities. Light amount conversion has come into widespread use. In such a case, an analog-to-digital converter (hereinafter abbreviated as an AD converter) is used that converts the analog electrical signal amount from the photoelectric conversion means to a digital amount. Counting type and comparison type converters are often used as A-D converters, depending on the required accuracy and simplicity of the circuit, but in either case, in order to handle the amount of light, it is necessary to calculate the absolute value proportional to the amount of light. It is necessary to obtain digital quantities. Furthermore, particularly in absorbance measurement of high-concentration samples, Raman spectroscopy, fluorescence spectroscopy, etc., a wide dynamic range is required, and even weak light is required to be converted with good linearity. In this way, in response to the request,
The conventional A/D converters have some disadvantages as follows. Particularly when dealing with weak light, good linearity is required at weak signal levels.
In general, A-D converters often have poor linearity when the input is small, such as in commonly used voltage-to-frequency converters. The range of good linearity of an A-to-D converter using a voltage single-frequency rotor converter depends on the frequency of the converted pulses and is up to about 1% of the full scale of the input. Further, the range in which the double integral type A-D converter has good linearity depends on the accuracy of the level comparator, and is about 0.5% to 5% of the full scale of the input. That is, full
In an A-○ converter with a scale of 10V, the range of good linearity is about 1 hV to 10V, and a weak signal of 1 hV or less cannot be accurately converted into a digital electrical signal. Furthermore, when weak light is converted into an electrical signal using, for example, a photomultiplier tube, the electrical signal obtained from the photoconversion means contains a lot of noise due to noise generated by the photoelectric conversion element itself and noise in peripheral circuits. There are times when I am.
On the other hand, an A-D converter that handles positive electrical signals ignores electrical signals that are close to the zero bell and contain a lot of noise, and therefore ignores electrical signals that are below the zero bell. Digital quantities cannot be obtained. Note that the noise signal level varies depending on the conditions, but is about lmV to I
It is V. In addition, because A-○ conversion is performed including negative electrical signals, an A-○ converter that applies a bias to the input can obtain a digital signal that faithfully contains noise, but has the disadvantage that it is not proportional to the amount of light. arise. Furthermore, when comparing the sawtooth voltage and the input voltage and measuring the time until the two match, such as in a one-time voltage conversion type A-D converter, or when inputting the input voltage after integrating it with an integrator for a certain period of time, When applying a reference voltage with the opposite polarity to the integrator and measuring the time it takes for the output voltage to return to the reference level, the input signal may drop during A-to-D conversion due to noise and do not exceed the level. Sometimes the bell detector does not work, which is a serious inconvenience.

また、光電変換手段から得られる電気信号には好ましく
ない直流信号成分が重畳している。
Further, an undesirable DC signal component is superimposed on the electric signal obtained from the photoelectric conversion means.

この直流信号成分は、光電管や光電子増倍管においては
暗電流であり、P瓜セルのような光導電素子においては
晴抵抗があり、しかも温度変換によって変化する。また
、増中器においては、オフセット電圧やその温度ドリフ
トがある。尚、階抵抗の温度変化は、10qoの温度変
化に対して20〜30%である。この直流信号成分によ
り、光量に正しく比例したディジタル信号を得ることが
できない。本発明は上記したような不都合を解決し、入
射光量に正しく比例したディジタル量を得る側光量変換
装置を提供することを目的としてなされたものである。
本発明の要点は、A−D変換手段に入力する電気信号に
一定量の信号を加算した後、A−D変換手段にてディジ
タル量に変換換することにより、微弱光の場合において
も常にA−D変換手段を直線性の良好な領域にて使用す
ると共に、前記した低レベル入力信号域での不安定動作
領域を避けること、および入射光量に忠実に比例したデ
ィジタル量を得るために、入射光を遮断する手段を設け
、該遮断手段により入射光が遮断されているステップに
おいて得られたディジタル信号量と、入射光が遮断され
ていないステップにおいて得られたディジタル信号量と
を、ディジタル量にて減算し、前記加算された一定量の
電気信号を相殺することである。
This DC signal component is a dark current in a phototube or a photomultiplier tube, and has a clear resistance in a photoconductive element such as a Pumpkin cell, and changes due to temperature conversion. Additionally, intensifiers have offset voltages and temperature drifts. Incidentally, the temperature change in the floor resistance is 20 to 30% for a temperature change of 10 qo. This DC signal component makes it impossible to obtain a digital signal that is accurately proportional to the amount of light. The present invention has been made for the purpose of solving the above-mentioned disadvantages and providing a side light amount conversion device that obtains a digital amount that is accurately proportional to the amount of incident light.
The key point of the present invention is to add a certain amount of signal to the electric signal input to the A-D conversion means, and then convert it into a digital quantity by the A-D conversion means, so that even in the case of weak light, the signal is always A - In order to use the D conversion means in a region with good linearity, to avoid the unstable operation region in the low-level input signal region mentioned above, and to obtain a digital amount that is faithfully proportional to the amount of incident light, A means for blocking light is provided, and the digital signal amount obtained in the step in which the incident light is blocked by the blocking means and the digital signal amount obtained in the step in which the incident light is not blocked are converted into digital quantities. The method is to cancel the added electric signal of a certain amount by subtracting the electric signal.

以下本発明の望ましい一実施例に基づいて本発明を詳述
する。
The present invention will be described in detail below based on a preferred embodiment of the present invention.

第1図は本発明の望ましい一実施例を示す機能説明図で
ある。
FIG. 1 is a functional explanatory diagram showing a preferred embodiment of the present invention.

光電子増情管などの光電変換素子1 1、増幅器12、
図示していない光電変換素子11への供給電源などから
なる光電変換手段1は、入射光を検知して光量を電圧な
どの電気量に変換し加算器2へ入力する。加算器2では
定電圧源+Vより抵抗R2を通して一定電圧を入力電圧
に加算し、A−D変換器3に入力する。A−D変換器3
は入力電圧をディジタル量に変換し、ディジタル記憶装
置52に与える。一方光電変換素子11への入射光10
は、例えばロータリーソレノィダやモーターなどで構成
される駆動装置42によって駆動されるシャッター41
により光東が遮断される。第1図では実線で示したシャ
ッター41の位置では光東10が非遮断状態にあり、点
線で示した位置では光東10が遮断された状態を表わし
ている。シャッター41が光電変換素子への入射光10
を遮断している状態か否かは、駆動装置42もしくは図
示していないシャッター位薄検出器などによって判定さ
れ弁別信号発生装置43を駆動する。弁別信号発生装置
43はシャッター41が入射光10を遮断しているか否
かの信号をアドレスレジスタ51に与え、アドレスレジ
スタ51は該信号に基づいてディジタル記憶装置52の
記憶アドレスを制御し、A−D変換器3より入力された
ディジタル側光信号は入射光10が遮断状態にあるか否
かによってそれぞれディジタル記憶装置52の異なるア
ドレスへ記憶される。ディジタル演算装置53は、ディ
ジタル記憶装置52に記憶された入射光10が遮断され
ていない状態の側光ディジタル信号Sと入射光10が遮
断されている状態の脚光ディジタル信号Zとを読み出し
、(S−Z)の減算を行なってその結果を出力する。本
発明の一実施例によればディジタル演算装置53より得
られるディジタル量(S−Z)は、加算器2により加算
された電圧あるいは増幅器12などにおいて親。
A photoelectric conversion element 1 1 such as a photoelectron intensifier tube, an amplifier 12,
A photoelectric conversion means 1 including a power supply to a photoelectric conversion element 11 (not shown) detects incident light, converts the amount of light into an electrical amount such as voltage, and inputs the converted amount to an adder 2. The adder 2 adds a constant voltage to the input voltage from the constant voltage source +V through the resistor R2, and inputs the added voltage to the AD converter 3. A-D converter 3
converts the input voltage into a digital quantity and provides it to the digital storage device 52. On the other hand, incident light 10 to the photoelectric conversion element 11
is a shutter 41 driven by a drive device 42 composed of, for example, a rotary solenoid or a motor.
Due to this, Koto is cut off. In FIG. 1, the light east 10 is in a non-blocking state at the position of the shutter 41 shown by a solid line, and the light east 10 is in a blocked state at a position shown by a dotted line. The shutter 41 prevents incident light 10 from entering the photoelectric conversion element.
It is determined by the driving device 42 or a shutter thinness detector (not shown), etc., and the discrimination signal generating device 43 is driven. The discrimination signal generator 43 gives a signal indicating whether or not the shutter 41 is blocking the incident light 10 to the address register 51, and the address register 51 controls the storage address of the digital storage device 52 based on the signal. The digital side optical signals input from the D converter 3 are stored in different addresses of the digital storage device 52 depending on whether or not the incident light 10 is in a blocked state. The digital arithmetic unit 53 reads out the side light digital signal S in a state in which the incident light 10 is not blocked and the footlight digital signal Z in a state in which the incident light 10 is blocked, which are stored in the digital storage device 52. -Z) and outputs the result. According to one embodiment of the present invention, the digital quantity (S-Z) obtained from the digital arithmetic unit 53 is applied to the voltage summed by the adder 2 or the parent value in the amplifier 12 or the like.

光信号に加わるオフセット電圧などを相殺し、入射光量
に比例したディジタル絶対値を得ることができる。加算
器2より加算する電圧は、光電変換素子11の時電流お
よび増中器12のオフセット電圧あるいはドリフト等お
よびA−D変換器の直線性のよい範囲によって決定され
る。入力ナフルスケールが10VのA−D変換器で直線
性の良い範囲が1肌hVから10Vであるならば、加算
される電圧は10仇hV以上であればよい。A−D変換
器3への入力電圧は増幅器2の出力電圧に加算器2によ
り一定電圧が加わった電圧であるため、前述したA−D
変換器の低レベル入力時の動作不良を排除することがで
きると共に常にA−D変換器3を直線性の良い領域で動
作させることができるため、入射光10が極めて微弱な
場合においても入射光量に忠実に比例したディジタル量
を安定に得ることが可能である。更に加えてA−D変換
器3によりディジタル量に変換された洩り光値には、入
射光10が遮断状態にあるか否かに拘らず発生する光電
変換素子11の情電流分や増幅器12のオフセット電圧
分なども含まれているが、これらの量はディジタル演算
装置53における減算において相殺されるという特徴を
も得ることができる。第2図は本発明になる狼。
By canceling out the offset voltage applied to the optical signal, it is possible to obtain a digital absolute value proportional to the amount of incident light. The voltage added by the adder 2 is determined by the current of the photoelectric conversion element 11, the offset voltage or drift of the intensifier 12, and the range of good linearity of the A-D converter. If an A-D converter has an input voltage scale of 10V and the range of good linearity is from 1 hV to 10V, the added voltage may be 10 hV or more. Since the input voltage to the A-D converter 3 is the output voltage of the amplifier 2 plus a constant voltage by the adder 2, the above-mentioned A-D
It is possible to eliminate malfunctions when the converter is input at low levels, and it is also possible to always operate the A-D converter 3 in a region with good linearity, so even when the incident light 10 is extremely weak, the amount of incident light can be controlled. It is possible to stably obtain a digital quantity that is faithfully proportional to . In addition, the leakage light value converted into a digital quantity by the A-D converter 3 includes the information current of the photoelectric conversion element 11 and the amplifier 12, which are generated regardless of whether or not the incident light 10 is blocked. , offset voltage, etc. are also included, but it is also possible to obtain the feature that these amounts are canceled out during subtraction in the digital arithmetic unit 53. Figure 2 shows the wolf of the present invention.

光量変換装置の一構成要素である加算回路とA−D変換
器の一実施例を示す回路説明図であり、A−D変換回路
はいわゆる二重積分形A−D変換器を用いている。光電
変換手段よりのアナログ入力Ainは抵抗R,を通し、
定電圧源十Vから抵抗又2を経た一定電圧が加算されて
積分器31にて積分される。制御回路33は積分器31
への入力電圧を一定時間積分した後、スイッチSW,を
切替え、入力電圧とは逆極性の定電圧源32から抵抗R
3を通して積分器31へ供給される電圧により積分器3
1を逆積分する。比較器34は積分器31に積分された
アナログ入力電圧が、定電圧源32による一定割合での
逆積分により雫電位に戻るのを検出して信号を発生する
。ゲート36は制御回路33と比較器34からの信号に
より、積分器31が逆積分されている間だけゲートを開
き、発振器35からの一定周波数のクロックパルスを計
数器37に送り、計数器37がこのクロックパルスを計
数することにより、アナログ入力電圧に比例したディジ
タル出力D側を得ることができる。第2図の実施例のよ
うに加算回路2はA−D変換器と組合わせて極めて容易
に達成することができる。第2図における実施例では、
積分器31に用いる増幅器や比較器34でのオフセット
電圧は、光電変換手段1への入射光10が遮断状態にあ
るか否かに拘らず一定であるので、ディジタル変換後の
減算において相殺することができる。第3図aは本発明
になる脚光量変換装置の一構成要素である光遮断手段の
一実施例を示す機能説明図である。
FIG. 2 is a circuit explanatory diagram showing an embodiment of an addition circuit and an AD converter that are one component of a light amount conversion device, and the AD conversion circuit uses a so-called double integral type AD converter. The analog input Ain from the photoelectric conversion means is passed through the resistor R,
A constant voltage from a constant voltage source of 10 V passes through a resistor 2 and is added and integrated by an integrator 31. The control circuit 33 is an integrator 31
After integrating the input voltage for a certain period of time, switch SW is switched to connect the constant voltage source 32, which has the opposite polarity to the input voltage, to the resistor R.
3 to the integrator 31 by the voltage supplied to the integrator 31 through 3.
Inversely integrate 1. The comparator 34 detects that the analog input voltage integrated by the integrator 31 returns to a drop potential due to inverse integration at a constant rate by the constant voltage source 32, and generates a signal. The gate 36 opens only while the integrator 31 is inversely integrating according to the signals from the control circuit 33 and the comparator 34, and sends a constant frequency clock pulse from the oscillator 35 to the counter 37. By counting these clock pulses, a digital output D proportional to the analog input voltage can be obtained. As in the embodiment of FIG. 2, the adder circuit 2 can be very easily achieved in combination with an A/D converter. In the example in FIG.
The offset voltage in the amplifier and comparator 34 used in the integrator 31 is constant regardless of whether the incident light 10 to the photoelectric conversion means 1 is blocked or not, so it can be canceled out in the subtraction after digital conversion. I can do it. FIG. 3a is a functional explanatory diagram showing an embodiment of a light blocking means which is a component of the spotlight amount converting device according to the present invention.

光電変換素子1 1への入射光1川まチョッパ44によ
り一定周期で断続されて光電変換素子1 1へ入射する
。チョッパ44は例えば第3図bにその側面図を示すよ
うに入射光10を遮断する部分と透過する部分が設けら
れ、モータ45によって回転することにより入射光10
を断続する。かくして入射光10‘ま一定周期にて断続
的に光電変換素子11へ入射するが、この断続の状態は
例えば光源46、光電素子47(例えばフオトトランジ
スタなどが用いられる。)によって検知され、弁別信号
としてアドレスレジスタを制御すると共に、第2図にお
ける制御回路33をコントロールして積分器における積
分と逆積分のタイミングをコントロールする。第3図の
実施例では、光電変換素子11への入射光10を一定周
期で断続し、その度にディジタル演算装置において減算
を行なうことができるので、光電変換素子11における
時電流や光電変換手段1に用いる増幅器のドリフト、加
算器2やA−D変換器に用いる積分器などのドリフトな
どを常に補償することができ、入射光量に忠実に比例し
たディジタル量を得ることが可能できる。第1図におけ
るディジタル記憶装置52、アドレスレジスタ51、デ
ィジタル演算装置53は例えばディジタル計算器などを
用いても容易に達成することが可能である。
The light incident on the photoelectric conversion element 11 is interrupted at regular intervals by the chopper 44, and then enters the photoelectric conversion element 11. The chopper 44 is provided with a part that blocks the incident light 10 and a part that transmits the incident light 10, as shown in a side view in FIG.
Intermittent. In this way, the incident light 10' enters the photoelectric conversion element 11 intermittently at a constant period, but this intermittent state is detected by, for example, the light source 46 and the photoelectric element 47 (for example, a phototransistor or the like is used), and a discrimination signal is generated. It controls the address register as well as the control circuit 33 in FIG. 2 to control the timing of integration and inverse integration in the integrator. In the embodiment shown in FIG. 3, the incident light 10 to the photoelectric conversion element 11 can be interrupted at regular intervals, and subtraction can be performed in the digital arithmetic unit each time. It is possible to always compensate for the drift of the amplifier used in the amplifier 1, the drift of the integrator used in the adder 2 and the AD converter, etc., and it is possible to obtain a digital quantity that is faithfully proportional to the amount of incident light. The digital storage device 52, address register 51, and digital arithmetic device 53 in FIG. 1 can be easily achieved by using, for example, a digital calculator.

ム次上のように本発明によれば、微弱な光の場合におい
ても、光量に直線性良く比例した絶対値のディジタル量
を得ることができ、更に光電変換手段や、A−D変換器
などで発生するドリフトなどを補償すると共にA−D変
換器を安定に動作させることが可能である。
As described above, according to the present invention, even in the case of weak light, it is possible to obtain a digital amount with an absolute value that is linearly proportional to the amount of light, and furthermore, it is possible to obtain a digital amount with an absolute value that is linearly proportional to the amount of light, and furthermore, it is possible to obtain a digital amount with an absolute value that is linearly proportional to the amount of light. It is possible to compensate for drifts and the like occurring in the A-D converter, and to operate the A-D converter stably.

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

第1図は本発明になる側光量変換装置の望ましい一実施
例を示す機能説明図、第2図は本発明の一構成要素であ
る加算手段とA−D変換器の一実施例を示す回路説明図
、第3図aは本発明の他の構成要素である光遮断手段の
一実施施例を示す機能説明図、第3図bは第3図aにお
けるチョッパの側面図である。 1・・・・・・光電変換手段、2・・・・・・加算器、
3・・・・・・A−D変換器、41・・・・・・シャツ
夕、44・・・・・・チョッパ、53・・・・・・ディ
ジタル演算装置。 弟/図第2図 第3図
FIG. 1 is a functional explanatory diagram showing a preferred embodiment of the side light amount conversion device according to the present invention, and FIG. 2 is a circuit diagram showing an embodiment of an adding means and an A-D converter which are one component of the present invention. 3A is a functional explanatory diagram showing an embodiment of a light blocking means which is another component of the present invention, and FIG. 3B is a side view of the chopper in FIG. 3A. 1...Photoelectric conversion means, 2...Adder,
3... A-D converter, 41... Shirtless, 44... Chopper, 53... Digital calculation device. Younger brother/Figure 2 Figure 3

Claims (1)

【特許請求の範囲】 1 光量を電気信号に変換する光電変換手段と、上記光
電変換手段からの電気信号をデイジタル量に変換するア
ナログ−デイジタル変換手段とを備えた測光量変換装置
において上記アナログ−デイジタル変換手段に入力する
電気信号に一定量の信号を加算する手段と、上記光電変
換手段に入射する光を遮断する光遮断手段と、上記アナ
ログ−デイジタル変換手段の出力信号のうち上記光遮断
手段が光を遮断している間に得られた信号量と、上記光
遮断手段が光を遮断していない間に得られた信号量とを
減算する手段を備えたことを特徴とする測光量変換装置
。 2 特許請求の範囲第1項記載の測光量変換装置におい
て、前記光遮断手段は、前記光電変換手段に入射する光
を一定周期にて断続する光断続器であることを特徴とす
る測光量変換装置。
[Scope of Claims] 1. In the photometric quantity conversion device comprising a photoelectric conversion means for converting a light quantity into an electrical signal, and an analog-to-digital conversion means for converting the electrical signal from the photoelectric conversion means into a digital quantity, means for adding a certain amount of signal to the electrical signal input to the digital conversion means; a light blocking means for blocking light incident on the photoelectric conversion means; and a light blocking means among the output signals of the analog-to-digital conversion means. A photometric amount conversion characterized by comprising means for subtracting a signal amount obtained while the light blocking means is blocking light and a signal amount obtained while the light blocking means is not blocking light. Device. 2. The photometric amount conversion device according to claim 1, wherein the light blocking means is a light interrupter that interrupts the light incident on the photoelectric conversion means at a constant cycle. Device.
JP3762777A 1977-04-04 1977-04-04 Photometric conversion device Expired JPS6024411B2 (en)

Priority Applications (3)

Application Number Priority Date Filing Date Title
JP3762777A JPS6024411B2 (en) 1977-04-04 1977-04-04 Photometric conversion device
US05/888,655 US4201472A (en) 1977-04-04 1978-03-21 Apparatus for converting light signals into digital electrical signals
DE2814358A DE2814358C3 (en) 1977-04-04 1978-04-03 Photoelectric converter arrangement

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP3762777A JPS6024411B2 (en) 1977-04-04 1977-04-04 Photometric conversion device

Publications (2)

Publication Number Publication Date
JPS53123183A JPS53123183A (en) 1978-10-27
JPS6024411B2 true JPS6024411B2 (en) 1985-06-12

Family

ID=12502865

Family Applications (1)

Application Number Title Priority Date Filing Date
JP3762777A Expired JPS6024411B2 (en) 1977-04-04 1977-04-04 Photometric conversion device

Country Status (1)

Country Link
JP (1) JPS6024411B2 (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE3138879A1 (en) * 1981-09-30 1983-04-14 Boehringer Mannheim Gmbh, 6800 Mannheim METHOD FOR DETECTING PHOTOMETRIC SIGNALS AND ARRANGEMENT FOR IMPLEMENTING THE METHOD
KR20190091970A (en) * 2018-01-30 2019-08-07 주식회사 엘지화학 Adapter for changing connector pitch and method for manufacturing the same

Also Published As

Publication number Publication date
JPS53123183A (en) 1978-10-27

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