JPH06273330A - Turbidimeter - Google Patents

Turbidimeter

Info

Publication number
JPH06273330A
JPH06273330A JP5843893A JP5843893A JPH06273330A JP H06273330 A JPH06273330 A JP H06273330A JP 5843893 A JP5843893 A JP 5843893A JP 5843893 A JP5843893 A JP 5843893A JP H06273330 A JPH06273330 A JP H06273330A
Authority
JP
Japan
Prior art keywords
light
intensity
transmitted
transmitted light
turbidity
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP5843893A
Other languages
Japanese (ja)
Inventor
Akihiro Suga
章宏 菅
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.)
Yokogawa Electric Corp
Original Assignee
Yokogawa Electric Corp
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Yokogawa Electric Corp filed Critical Yokogawa Electric Corp
Priority to JP5843893A priority Critical patent/JPH06273330A/en
Publication of JPH06273330A publication Critical patent/JPH06273330A/en
Pending legal-status Critical Current

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  • Investigating Or Analysing Materials By Optical Means (AREA)

Abstract

PURPOSE:To provide a highly accurate turbidimeter. CONSTITUTION:The turbidimeter for measuring the turbidity of a solution by measuring the intensity of light transmitted through the solution comprises a lens 10 for focusing the light transmitted straightly through the solution and the light scattered by the solution, an optical detector 11 for detecting the intensities of the transmitted light and the scattered light focused by the lens 10, and a shutter 12 for cutting the transmitted light. Turbidity is then determined based on the intensity of scattered light when the transmitted light is cut by means of the shutter 12 and the total intensity of the transmitted and scattered lights when the transmitted light is not cut.

Description

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

【0001】[0001]

【産業上の利用分野】本発明は、被測定溶液の濁度を測
定する濁度測定装置に関し、更に詳しくは、セルを透過
する散乱光と透過光の強度を同一の検出器で検出し、検
出器に用いられるフォトダイオード固有の温度特性の影
響を受けず、精度よく被測定溶液の濁度を測定すること
のできる濁度測定装置に関するものである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a turbidity measuring device for measuring the turbidity of a solution to be measured. More specifically, the scattered light transmitted through the cell and the intensity of the transmitted light are detected by the same detector, The present invention relates to a turbidity measuring device capable of accurately measuring the turbidity of a solution to be measured without being affected by the temperature characteristics peculiar to a photodiode used in a detector.

【0002】[0002]

【従来の技術】図4は、従来の濁度測定装置の構成図で
ある。図中、1は光源であるランプ、2はランプ1から
の光を平行光束にするコリメータレンズ、3は絞りで、
コリメータレンズ2から出射された平行光束を適切な光
束径Dに絞る。4は光路面にガラス窓4Aを有したセル
で、被測定溶液が入口側から供給され、出口側から送出
される。5はセル4を透過した平行光束(透過光)の強
度Ipを測定する透過光検出器、6はセル4を透過した
散乱光の強度Idを測定する散乱光検出器である。尚、
これらの検出器は、フォトダイオード等によって構成さ
れる。
2. Description of the Related Art FIG. 4 is a block diagram of a conventional turbidity measuring device. In the figure, 1 is a lamp which is a light source, 2 is a collimator lens for collimating the light from the lamp 1, and 3 is a diaphragm,
The parallel light flux emitted from the collimator lens 2 is narrowed down to an appropriate light flux diameter D. Reference numeral 4 denotes a cell having a glass window 4A on the optical path surface. The solution to be measured is supplied from the inlet side and delivered from the outlet side. Reference numeral 5 is a transmitted light detector that measures the intensity I p of the parallel light flux (transmitted light) that has passed through the cell 4, and 6 is a scattered light detector that measures the intensity I d of the scattered light that has passed through the cell 4. still,
These detectors are composed of photodiodes or the like.

【0003】7は増幅回路で、透過光検出器5と散乱光
検出器6から入力した光の強度Ip、Idを増幅し演算回
路8に出力する。演算回路8は、増幅回路7から入力し
た散乱光信号Sdと透過光信号Spに基づいて濁度Tを算
出する。
An amplification circuit 7 amplifies the intensities I p and I d of the light input from the transmitted light detector 5 and the scattered light detector 6, and outputs the amplified light intensities to the arithmetic circuit 8. The arithmetic circuit 8 calculates the turbidity T based on the scattered light signal S d and the transmitted light signal S p input from the amplifier circuit 7.

【0004】[0004]

【発明が解決しようとする課題】このような従来の濁度
測定装置は、検出器に用いられているフォトダイオード
がそれぞれ固有の温度特性を有しているため、濁度を正
確に測定するためには透過光検出器と散乱光検出器のフ
ォトダイオードを同じ温度特性のものにする必要があっ
た。又は、透過光検出器と散乱光検出器のフォトダイオ
ードの温度特性の違いを補正するための演算を行う必要
があった。
In such a conventional turbidity measuring device, since the photodiodes used in the detector have their own temperature characteristics, the turbidity can be accurately measured. It was necessary to make the photodiodes of the transmitted light detector and the scattered light detector have the same temperature characteristics. Alternatively, it is necessary to perform a calculation for correcting the difference in temperature characteristics between the photodiodes of the transmitted light detector and the scattered light detector.

【0005】本発明は、このような点に鑑みて成された
もので、セルを透過する散乱光と透過光の強度を一つの
検出器で測定するようにしたもので、フォトダイオード
の温度特性の影響を受けないで、被測定溶液の濁度を精
度良く測定することのできる濁度測定装置を提供するこ
とを目的としている。
The present invention has been made in view of the above point, and is one in which the intensity of scattered light transmitted through a cell and the intensity of the transmitted light are measured by one detector, and the temperature characteristic of the photodiode is measured. It is an object of the present invention to provide a turbidity measuring device capable of accurately measuring the turbidity of a solution to be measured without being affected by.

【0006】[0006]

【課題を解決するための手段】このような目的を達成す
るために、本発明は、被測定溶液を透過した光の強度を
測定し、被測定溶液の濁度を測定する濁度測定装置にお
いて、前記被測定溶液を直進する透過光と前記被測定溶
液によって散乱される散乱光とを結像するレンズと、こ
のレンズで結像した透過光と散乱光の強度を検出する光
検出器と、前記被測定溶液の透過光をカットするシャッ
タと、を設け、前記シャッタによって透過光をカットし
た場合の散乱光の強度と透過光をカットしない場合の透
過光と散乱光の強度の和に基づいて濁度値を求めること
を特徴としている。
In order to achieve such an object, the present invention provides a turbidity measuring apparatus for measuring the intensity of light transmitted through a solution to be measured and measuring the turbidity of the solution to be measured. A lens that forms an image of the transmitted light that travels straight through the solution to be measured and the scattered light that is scattered by the solution to be measured, and a photodetector that detects the intensity of the transmitted light and the scattered light formed by the lens, A shutter for cutting the transmitted light of the solution to be measured is provided, and based on the sum of the intensity of the scattered light when the transmitted light is cut by the shutter and the intensity of the transmitted light and the scattered light when the transmitted light is not cut. It is characterized by determining the turbidity value.

【0007】[0007]

【作用】光検出器は、シャッタを開いた場合の信号と閉
じた場合の信号とから(散乱光)/(散乱光及び透過
光)の強度を得る。そして、光検出器が得た(散乱光)
/(散乱光及び透過光)の強度から散乱光と透過光との
強度比を求め、濁度を得る。
The photodetector obtains the intensity of (scattered light) / (scattered light and transmitted light) from the signal when the shutter is opened and the signal when the shutter is closed. And the photodetector got (scattered light)
The intensity ratio of scattered light and transmitted light is calculated from the intensity of / (scattered light and transmitted light) to obtain turbidity.

【0008】[0008]

【実施例】以下、図面を用いて本発明の一実施例を詳細
に説明する。図1は本発明の濁度測定装置の一実施例を
示した構成図、図2は、本発明の濁度測定装置のシャッ
タが開かれた状態の要部構成図である。図中、図4と同
一作用をするものは同一符号を付けて説明する。10は
平行光束の延長上に設けらた焦点距離fのレンズ、11
はレンズ10の光軸上に設けられた光検出器である。
An embodiment of the present invention will be described in detail below with reference to the drawings. FIG. 1 is a configuration diagram showing an embodiment of the turbidity measuring device of the present invention, and FIG. 2 is a configuration diagram of a main part of the turbidity measuring device of the present invention in a state where a shutter is opened. In the figure, components having the same functions as those in FIG. Reference numeral 10 is a lens having a focal length f provided on the extension of the parallel light flux, and 11
Is a photodetector provided on the optical axis of the lens 10.

【0009】レンズ10は、レンズ10からの距離aで
平行光束より発する散乱光をレンズ10からの距離bに
位置する光検出器11に結像すると共に、セル4を透過
した平行光束(以下、透過光という)を一旦焦点fに像
を結び、光検出器11に結像する。
The lens 10 forms an image of scattered light emitted from a parallel light flux at a distance a from the lens 10 on a photodetector 11 located at a distance b from the lens 10 and also transmits a parallel light flux (hereinafter, The transmitted light) is once focused on the focal point f, and then focused on the photodetector 11.

【0010】12はセル4とレンズ10間に設けられた
円形形状をしたシャッタで、モータ13によって開閉が
制御され、透過光のレンズ10への入射を制御する。1
3Aは円形形状をした位置検出板で、モータ軸13Bに
取り付けられていて、モータ13の回転に伴って回転す
る。14は位置検出器で、位置検出板13Aの外周から
中心方向に向かって設けられたスリット(図省略)をフ
ォトセンサ(図省略)で検知し、シャッタ12の開閉状
態を認識する。
Reference numeral 12 denotes a circular shutter provided between the cell 4 and the lens 10, the opening and closing of which is controlled by the motor 13 to control the incident of the transmitted light on the lens 10. 1
3A is a circular position detecting plate, which is attached to the motor shaft 13B and rotates with the rotation of the motor 13. A position detector 14 detects a slit (not shown) provided from the outer periphery of the position detection plate 13A toward the center with a photo sensor (not shown) to recognize the open / closed state of the shutter 12.

【0011】増幅回路7は、光検出器11から入力した
信号S1を増幅し、サンプルホールド回路15に出力す
る。サンプルホールド回路15は、位置検出器14の出
力するラッチ信号S2に基づいて増幅回路15から入力
した信号S3を保持する。この場合は、シャッタ12を
開いた場合の信号(散乱光と透過光との強度Id、Ip
基づいた信号)と閉じた場合の信号(透過光が遮蔽され
散乱光のみの強度Idに基づいた信号)が保持される。
The amplifier circuit 7 amplifies the signal S 1 input from the photodetector 11 and outputs it to the sample hold circuit 15. The sample hold circuit 15 holds the signal S 3 input from the amplifier circuit 15 based on the latch signal S 2 output from the position detector 14. In this case, a signal when the shutter 12 is opened (a signal based on the intensities I d and I p of the scattered light and the transmitted light) and a signal when the shutter 12 is closed (the intensity of the scattered light only I d Signal based on the above) is held.

【0012】このサンプルホールド回路15に保持され
た信号S3は、演算回路8に出力され、散乱光と透過光
の比が求められ、濁度信号Tとなる。
The signal S 3 held in the sample-hold circuit 15 is output to the arithmetic circuit 8 and the ratio of scattered light to transmitted light is obtained and becomes a turbidity signal T.

【0013】次に、本発明の濁度測定装置の動作につい
て説明する。ランプ1から出射された光は、コリメータ
レンズ2と絞り3とによって平行光束にされ、セル4に
出射される。このセル4に出射された光は、散乱あるい
は反射されるので被測定溶液を透過する全透過光の強度
tは、 It=Id+Ip となる。尚、Idは散乱光の強度、Ipは透過光(セル4
を透過した平行光束)の強度である。
Next, the operation of the turbidity measuring device of the present invention will be described. The light emitted from the lamp 1 is collimated by the collimator lens 2 and the diaphragm 3 and emitted to the cell 4. Since the light emitted to the cell 4 is scattered or reflected, the intensity I t of the total transmitted light that passes through the solution to be measured is I t = I d + I p . Incidentally, I d is the intensity of scattered light, and I p is the transmitted light (cell 4
Is the intensity of the parallel light flux that has passed through.

【0014】レンズ10からの距離aにおける散乱光
は、レンズ10で光検出器11にd1の大きさに結像さ
れる。この時d1はd1=DX(b/a)の関係になって
いる。一方、透過光は、一旦、レンズ10によって焦点
fで像を結び、光検出器11にd2の大きさに結像され
る。d2はDX(b−f)/fで表され、(1/f)=
(1/a)+(1/b)の関係より、d2=DX(b/
a)、即ち、d1と同じ大きさで光検出器11に結像さ
れる。
The scattered light at a distance a from the lens 10 is imaged by the lens 10 on the photodetector 11 to have a size of d 1 . At this time, d 1 has a relationship of d 1 = D X (b / a). On the other hand, the transmitted light forms an image at the focal point f by the lens 10 and is formed on the photodetector 11 in the size of d 2 . d 2 is represented by D X (b−f) / f, and (1 / f) =
From the relationship of (1 / a) + (1 / b), d 2 = D X (b /
a) That is, the image is formed on the photodetector 11 in the same size as d 1 .

【0015】シャッタ12がオンされた場合(透過光が
遮蔽される場合) 光検出器11には、散乱光のみがレンズ10によって集
光され、d1の大きさで結像される。光検出器11によ
って検出された散乱光の強度Idは、増幅回路7で増幅
された後、位置検出器14がシャッタ12の動作に基づ
いて得たラッチ信号Sによりサンプルホールド回路15
に保持され、演算回路8に出力される。
When the shutter 12 is turned on (transmitted light is
Only the scattered light is focused on the photodetector 11 by the lens 10 ( when it is shielded) , and is imaged in the size of d 1 . The intensity I d of the scattered light detected by the photodetector 11 is amplified by the amplifier circuit 7, and then the sample-hold circuit 15 is operated by the latch signal S obtained by the position detector 14 based on the operation of the shutter 12.
And is output to the arithmetic circuit 8.

【0016】シャッタ12がオフされた場合(透過光が
遮蔽されない場合) 光検出器11には、散乱光と透過光がレンズ10によっ
て集光され、d1の大きさで結像される。光検出器11
によって検出された散乱光と透過光の強度Id、Ipは、
増幅回路7で増幅された後、位置検出器14がシャッタ
の動作に基づいて得たラッチ信号S2によりサンプルホ
ールド回路15に保持され、演算回路8に出力される。
When the shutter 12 is turned off (transmitted light is
The scattered light and the transmitted light are converged by the lens 10 on the photodetector 11 ( when not shielded) , and are imaged in the size of d 1 . Photodetector 11
The scattered light and transmitted light intensities I d and I p detected by
After being amplified by the amplifier circuit 7, the position detector 14 is held in the sample hold circuit 15 by the latch signal S 2 obtained based on the operation of the shutter and is output to the arithmetic circuit 8.

【0017】図3は、光検出器の信号から得たスペクト
ルを示した図である。最大値Aが散乱光と透過光との強
度Id、Ipに基づいた信号、最小値Bが透過光が遮蔽さ
れ散乱光のみの強度Idに基づいた信号である。演算回
路8は、シャッタ12のオン/オフで得た(散乱光)/
(散乱光及び透過光)の強度から散乱光と透過光との強
度比を求め、濁度Tを得る。
FIG. 3 is a diagram showing a spectrum obtained from the signal of the photodetector. The maximum value A is a signal based on the intensities I d and I p of the scattered light and the transmitted light, and the minimum value B is a signal based on the intensity I d of the scattered light in which the transmitted light is shielded. The arithmetic circuit 8 is obtained by turning on / off the shutter 12 (scattered light) /
The intensity ratio of scattered light and transmitted light is obtained from the intensity of (scattered light and transmitted light) to obtain the turbidity T.

【発明の効果】以上、詳細に説明したように本発明の濁
度測定装置は、透過光と散乱光の強度を同一の検出器で
測定するようにしたもので、フォトダイオードの温度特
性の影響を受けないで、被測定溶液の濁度を精度良く測
定することができる。
As described above in detail, the turbidity measuring device of the present invention is designed to measure the intensity of transmitted light and scattered light with the same detector, and the influence of the temperature characteristic of the photodiode. The turbidity of the solution to be measured can be accurately measured without receiving the turbidity.

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

【図1】本発明の濁度測定装置の一実施例を示した構成
図である。
FIG. 1 is a configuration diagram showing an embodiment of a turbidity measuring device of the present invention.

【図2】本発明の濁度測定装置のシャッタが開かれた状
態の要部構成図である。
FIG. 2 is a main part configuration diagram of a turbidity measuring device of the present invention in a state where a shutter is opened.

【図3】光検出器の信号から得たスペクトルを示した図
である。
FIG. 3 is a diagram showing a spectrum obtained from a signal of a photodetector.

【図4】従来の濁度測定装置の構成図である。FIG. 4 is a configuration diagram of a conventional turbidity measuring device.

【符号の説明】[Explanation of symbols]

10 レンズ 11 光検出器 13 モータ 14 位置検出器 15 サンプルホールド回路 10 Lens 11 Photodetector 13 Motor 14 Position Detector 15 Sample Hold Circuit

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】 被測定溶液を透過した光の強度を測定
し、被測定溶液の濁度を測定する濁度測定装置におい
て、 前記被測定溶液を直進する透過光と前記被測定溶液によ
って散乱される散乱光とを結像するレンズと、 このレンズで結像した透過光と散乱光の強度を検出する
光検出器と、 前記被測定溶液の透過光をカットするシャッタと、 を設け、前記シャッタによって透過光をカットした場合
の散乱光の強度と透過光をカットしない場合の透過光と
散乱光の強度の和とに基づいて濁度値を求めることを特
徴とした濁度測定装置。
1. A turbidity measuring device for measuring the intensity of light transmitted through a solution to be measured to measure the turbidity of the solution to be measured, wherein the transmitted light traveling straight through the solution to be measured and scattered by the solution to be measured. The shutter for cutting the transmitted light of the solution to be measured, a lens for forming an image of the scattered light formed by the lens, a photodetector for detecting the intensity of the transmitted light and the scattered light formed by the lens, and the shutter A turbidity measuring device characterized by obtaining a turbidity value based on the intensity of scattered light when the transmitted light is cut by and the sum of the intensity of the transmitted light and the intensity of the scattered light when the transmitted light is not cut.
JP5843893A 1993-03-18 1993-03-18 Turbidimeter Pending JPH06273330A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP5843893A JPH06273330A (en) 1993-03-18 1993-03-18 Turbidimeter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP5843893A JPH06273330A (en) 1993-03-18 1993-03-18 Turbidimeter

Publications (1)

Publication Number Publication Date
JPH06273330A true JPH06273330A (en) 1994-09-30

Family

ID=13084408

Family Applications (1)

Application Number Title Priority Date Filing Date
JP5843893A Pending JPH06273330A (en) 1993-03-18 1993-03-18 Turbidimeter

Country Status (1)

Country Link
JP (1) JPH06273330A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2008064594A (en) * 2006-09-07 2008-03-21 Yokogawa Electric Corp Turbidimeter
JP2012098282A (en) * 2010-10-29 2012-05-24 F Hoffmann-La Roche Ag System for performing scattering and absorption spectrometry
CN107831099A (en) * 2017-11-23 2018-03-23 北京是卓科技有限公司 The detection means and detection method of air particle

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2008064594A (en) * 2006-09-07 2008-03-21 Yokogawa Electric Corp Turbidimeter
JP2012098282A (en) * 2010-10-29 2012-05-24 F Hoffmann-La Roche Ag System for performing scattering and absorption spectrometry
CN107831099A (en) * 2017-11-23 2018-03-23 北京是卓科技有限公司 The detection means and detection method of air particle

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