JPS6360857B2 - - Google Patents
Info
- Publication number
- JPS6360857B2 JPS6360857B2 JP21716082A JP21716082A JPS6360857B2 JP S6360857 B2 JPS6360857 B2 JP S6360857B2 JP 21716082 A JP21716082 A JP 21716082A JP 21716082 A JP21716082 A JP 21716082A JP S6360857 B2 JPS6360857 B2 JP S6360857B2
- Authority
- JP
- Japan
- Prior art keywords
- measured
- liquid
- turbidity
- light source
- water quality
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired
Links
- 238000005259 measurement Methods 0.000 claims description 20
- 239000007788 liquid Substances 0.000 claims description 17
- XLYOFNOQVPJJNP-UHFFFAOYSA-N water Substances O XLYOFNOQVPJJNP-UHFFFAOYSA-N 0.000 claims description 8
- 239000010802 sludge Substances 0.000 claims description 3
- 238000002834 transmittance Methods 0.000 claims description 2
- 238000005070 sampling Methods 0.000 claims 1
- 238000002604 ultrasonography Methods 0.000 claims 1
- 238000000034 method Methods 0.000 description 3
- 239000000463 material Substances 0.000 description 2
- 230000003287 optical effect Effects 0.000 description 2
- 230000008033 biological extinction Effects 0.000 description 1
- 230000005540 biological transmission Effects 0.000 description 1
- 238000001514 detection method Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 239000013013 elastic material Substances 0.000 description 1
- 230000001151 other effect Effects 0.000 description 1
- 239000010865 sewage Substances 0.000 description 1
- 239000000779 smoke Substances 0.000 description 1
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
- G01N21/17—Systems in which incident light is modified in accordance with the properties of the material investigated
- G01N21/59—Transmissivity
Landscapes
- Physics & Mathematics (AREA)
- Health & Medical Sciences (AREA)
- Life Sciences & Earth Sciences (AREA)
- Chemical & Material Sciences (AREA)
- Analytical Chemistry (AREA)
- Biochemistry (AREA)
- General Health & Medical Sciences (AREA)
- General Physics & Mathematics (AREA)
- Immunology (AREA)
- Pathology (AREA)
- Investigating Or Analysing Materials By Optical Means (AREA)
Description
【発明の詳細な説明】
本発明は、上水場あるいは下水処理場で用いら
れる濁度、MLSS(活性汚泥濃度)、有機汚濁等の
水質計器に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a water quality meter for measuring turbidity, MLSS (activated sludge concentration), organic pollution, etc. used in water supply plants or sewage treatment plants.
第1図は従来の光学式の濁度計の一例を示す断
面図である。図において、1は被測定液、2は光
源、3は光源2からの光束○イを平行光束○ロにする
ためのレンズ、4は光源2からの光束○イのうち被
測定液1を通過してきた透過光○ハの受光する第1
のフオトセル、5は光源2の光強度をモニターす
る第2のフオトセルである。6は第1、第2のフ
オトセル4,5の出力X,Yにより所定の演算処
理を行い、濁度比例信号Zを送出する演算器、7
は測定管である。 FIG. 1 is a sectional view showing an example of a conventional optical turbidity meter. In the figure, 1 is the liquid to be measured, 2 is the light source, 3 is a lens for converting the light beam ○a from the light source 2 into a parallel beam ○b, and 4 is the light beam ○a from the light source 2 that passes through the liquid to be measured 1 The first to receive the transmitted light
The photocell 5 is a second photocell that monitors the light intensity of the light source 2. 6 is a computing unit that performs predetermined computing processing using the outputs X and Y of the first and second photocells 4 and 5 and sends out a turbidity proportional signal Z;
is the measuring tube.
上記のように構成した濁度計の作用は次の通り
である。レンズ3の焦点位置に置かれた光源2か
らの光束○イは平行光束○ロとなつて被測定液1に入
射する。平行光束○ロは被測定液1の濁度成分によ
つて吸収あるいは散乱する。透過光○ハを検出する
第1のフオトセル4の出力Xは、ランベルト−ベ
ールの法則に従つて次の式で示される。 The operation of the turbidity meter configured as described above is as follows. The light beam ○a from the light source 2 placed at the focal position of the lens 3 becomes a parallel light beam ○b and enters the liquid to be measured 1. The parallel light beams (○) and (b) are absorbed or scattered by the turbidity component of the liquid to be measured 1. The output X of the first photocell 4, which detects the transmitted light ○, is expressed by the following equation according to the Lambert-Beer law.
X=Y exp〔−εlx〕 …(1)
ここに、Yは光源2の光強度、εは被測定液1
の吸光係数、lは被測定液1の測定長、xは濁度
である。(1)式から濁度xは、次のように表わされ
る。 X=Y exp [−εlx] …(1) Here, Y is the light intensity of light source 2, and ε is the measured liquid 1.
, l is the measurement length of the liquid to be measured 1, and x is the turbidity. From equation (1), turbidity x is expressed as follows.
x=1/εl・loY/X …(2)
ここで、吸光係数εと測定長lは、通常変化し
ないので、定数Cと置く。第1のフオトセル4の
出力Xと光源2の光強度をモニタしている第2の
フオトセル5の出力Yから濁度比例値Zは次のよ
うに求まる。 x=1/εl·l o Y/X (2) Here, since the extinction coefficient ε and the measurement length l do not normally change, they are set as a constant C. The turbidity proportional value Z is determined from the output X of the first photocell 4 and the output Y of the second photocell 5 that monitors the light intensity of the light source 2 as follows.
Z=C・loY/X …(3)
演算器6は(3)式に示す演算を行ない濁度比例値
Zを出力する。以上のように従来の濁度計は、測
定長を固定にすれば測定ダイナミツクレンジが狭
くなるため、測定長の異なる測定管を複数個用意
する必要があり、さらに測定管の交換に入手と時
間がかかるなどの欠点があつた。 Z=C·l o Y/X (3) The calculator 6 performs the calculation shown in equation (3) and outputs the turbidity proportional value Z. As mentioned above, with conventional turbidity meters, if the measurement length is fixed, the measurement dynamic range becomes narrower, so it is necessary to prepare multiple measurement tubes with different measurement lengths, and it is also necessary to obtain measurement tubes to replace them. It had drawbacks such as being time consuming.
本発明は、上記のような欠点を解決するために
なされたもので、測定長を自由に変えることがで
きる濁度計を得ることを目的とする。 The present invention was made to solve the above-mentioned drawbacks, and an object of the present invention is to obtain a turbidity meter whose measurement length can be freely changed.
本発明は、上記のような目的を達成するために
なされたもので、被測定体を透過する光、または
超音波等の透過率により被測定体の濁度、MLSS
(活性汚泥濃度)、有機汚濁等を計測する水質計器
において、被測定体をサンプリングする測定管の
一部に弾性を有する弾性部を設け外力により弾性
部を変形させ被測定液の測定長を調整できるよう
にしたことを特徴とする氷質計器を提供するもの
である。以下図面をもちいて本発明を説明する。 The present invention has been made to achieve the above-mentioned objects, and it is possible to measure the turbidity and MLSS of a measured object using the transmittance of light or ultrasonic waves passing through the measured object.
In water quality meters that measure activated sludge concentration, organic pollution, etc., an elastic part is installed in a part of the measurement tube that samples the object to be measured, and the elastic part is deformed by external force to adjust the measurement length of the liquid to be measured. The present invention provides an ice quality meter characterized by the ability to The present invention will be explained below using the drawings.
第2図a,bは、それぞれ本発明の一実施例を
示す断面図である。被測定液1から第2のフオト
セル5までは先に述べたものと同一である。7a
は管の一部分がゴム等の弾力性を有する物質Aで
構成される測定管、8は光源2、レンズ3、第2
のフオトセル5を搭載した光源ヘツドである。な
お9は、光源ヘツド8を移動させるためのモー
タ、10は、光源ヘツド8の位置に対応した電気
出力を発生する位置検出器である。11は、第
1、第2のフオトセル4,5の出力X,Yおよび
位置検出器10の出力Lを入力し、所定の演算処
理を行い濁度比例値Zとモータ9の制御信号を発
生する演算器である。 FIGS. 2a and 2b are sectional views each showing an embodiment of the present invention. The components from the liquid to be measured 1 to the second photocell 5 are the same as those described above. 7a
8 is a measuring tube in which a part of the tube is made of elastic material A such as rubber; 8 is a light source 2, a lens 3, and a second tube;
This is a light source head equipped with a photocell 5. Note that 9 is a motor for moving the light source head 8, and 10 is a position detector that generates an electrical output corresponding to the position of the light source head 8. 11 inputs the outputs X and Y of the first and second photocells 4 and 5 and the output L of the position detector 10, performs predetermined arithmetic processing, and generates a turbidity proportional value Z and a control signal for the motor 9. It is a computing device.
上記のように構成した本発明の作用を説明すれ
ば次の通りである。光源2からの光束○イはレンズ
3により平行光束○ロとなり被測定液1に照射され
る。この場合、平行光束○ロの透過量を検出する第
1のフオトセル4の出力が(1)式に示す関係式で表
わされることは先に述べたことと同様である。し
かしながら、本発明においては、測定管7aの一
部分に弾力性を有するゴム等の材質Aを用い、材
質Aよりなる部分に光源ヘツド8を押し当てるこ
とにより、光源ヘツド8の移動に従つて測定長l
を変えることができる。光源ヘツド8の移動、す
なわち測定長lの調整は演算器11により第1の
フオトセル4の出力Xが常に適正範囲内になるよ
うモータ9を制御することにより行なわれる。 The operation of the present invention configured as described above will be explained as follows. The light beam ○a from the light source 2 is converted into a parallel light beam ○b by the lens 3 and is irradiated onto the liquid to be measured 1. In this case, as described above, the output of the first photocell 4 that detects the amount of transmission of the parallel light beam ◯◯ is expressed by the relational expression shown in equation (1). However, in the present invention, a part of the measuring tube 7a is made of material A such as elastic rubber, and by pressing the light source head 8 against the part made of material A, the measurement length is adjusted as the light source head 8 moves. l
can be changed. The movement of the light source head 8, that is, the adjustment of the measurement length l, is performed by controlling the motor 9 using the computing unit 11 so that the output X of the first photocell 4 is always within a proper range.
第2図aは被測定液1の濁度が低い場合を示し
ており、光源ヘツド8を後退させることによつて
測定長l1が長く取られている。第2図bは被測定
液1の濁度が高い場合を示し、光源ヘツド8の前
進により測定長l2が短かくなつている。位置検出
器10は光源ヘツド8の位置から測定長lに対す
る比例値Lを演算器11に送出する。演算器11
は上記Lと、第1、第2のフオトセル4,5の出
力X,Yを入力し次の式により濁度比例値Zを算
出して出力する。 FIG. 2a shows a case where the turbidity of the liquid 1 to be measured is low, and the measurement length l1 is made longer by retracting the light source head 8. FIG. 2b shows a case where the turbidity of the liquid to be measured 1 is high, and the measurement length l2 is shortened by the advancement of the light source head 8. The position detector 10 sends a proportional value L to the measurement length l from the position of the light source head 8 to the calculator 11. Arithmetic unit 11
inputs the above L and the outputs X and Y of the first and second photocells 4 and 5, calculates and outputs the turbidity proportional value Z using the following formula.
Z=C/L・loY/X …(4)
このようにして、測定長lが可変の濁度計が得
られる。 Z=C/L·l o Y/X (4) In this way, a turbidity meter with variable measurement length l is obtained.
以上の実施例で濁度計について説明したが、測
定長の効果が生じるMLSS計や有機汚濁等の水質
計、または煙濃度計等であつても同様である。ま
た、本発明は光学方式のみならず超音波方式等に
も適用することができる。さらに、光源ヘツドを
固定し第1のフオトセル側か、両方を移動させて
もよく移動方式はモータに限らない。 In the above embodiments, a turbidity meter has been described, but the same applies to a MLSS meter, a water quality meter for organic pollution, etc., or a smoke concentration meter, etc., in which the effect of the measurement length occurs. Further, the present invention can be applied not only to an optical method but also to an ultrasonic method. Furthermore, the light source head may be fixed and either the first photocell side or both may be moved, and the movement method is not limited to the motor.
以上のべたように、本発明によれば、測定のダ
イナミツクレンジが拡大し、検出信号のS/Nが
向上し出力が安定する等、実施による効果大であ
る。 As described above, according to the present invention, the dynamic range of measurement is expanded, the S/N of the detection signal is improved, the output is stabilized, and other effects can be achieved through implementation.
第1図は従来の濁度計の一例を示す断面図、第
2図a,bはそれぞれ本発明の実施例を示す断面
図である。
1…被測定液、2…光源、4…第1のフオトセ
ル、5…第2のフオトセル、7,7a…測定管、
8…光源ヘツド、9…モータ、10…位置検出
器、11…演算器。
FIG. 1 is a sectional view showing an example of a conventional turbidimeter, and FIGS. 2a and 2b are sectional views showing an embodiment of the present invention. DESCRIPTION OF SYMBOLS 1... Liquid to be measured, 2... Light source, 4... First photocell, 5... Second photocell, 7, 7a... Measuring tube,
8...Light source head, 9...Motor, 10...Position detector, 11...Arithmetic unit.
Claims (1)
率により前記被測定液の濁度、MLSS(活性汚泥
濃度)、有機汚濁等を計測する水質計器において、
前記被測定液をサンプリングする測定管の一部に
弾性を有する弾性部を設け、外力により前記弾性
部を変形させ、前記被測定液の測定長を調整する
ようにしたことを特徴とする水質計器。 2 弾性部を変形させる手段として被測定液から
の透過信号が一定の範囲に入るように前記弾性部
に外力を印加するモータを制御し、測定長を含ん
た関係式より濁度比例値を得るようにしたことを
特徴とする特許請求の範囲第1項記載の水質計
器。[Scope of Claims] 1. A water quality meter that measures the turbidity, MLSS (activated sludge concentration), organic pollution, etc. of a liquid to be measured based on the transmittance of light or ultrasound transmitted through the liquid to be measured,
A water quality meter characterized in that a part of the measuring tube for sampling the liquid to be measured is provided with an elastic part having elasticity, and the elastic part is deformed by an external force to adjust the measurement length of the liquid to be measured. . 2. As a means of deforming the elastic part, a motor that applies an external force to the elastic part is controlled so that the transmitted signal from the liquid to be measured falls within a certain range, and a turbidity proportional value is obtained from a relational expression including the measurement length. A water quality meter according to claim 1, characterized in that the water quality meter is configured as follows.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP57217160A JPS59107241A (en) | 1982-12-10 | 1982-12-10 | Water quality measuring instrument |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP57217160A JPS59107241A (en) | 1982-12-10 | 1982-12-10 | Water quality measuring instrument |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS59107241A JPS59107241A (en) | 1984-06-21 |
| JPS6360857B2 true JPS6360857B2 (en) | 1988-11-25 |
Family
ID=16699791
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP57217160A Granted JPS59107241A (en) | 1982-12-10 | 1982-12-10 | Water quality measuring instrument |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS59107241A (en) |
Families Citing this family (7)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH01229940A (en) * | 1987-11-19 | 1989-09-13 | Nippon Koden Corp | Cuvet for optical analysis |
| JPH02196946A (en) * | 1989-01-25 | 1990-08-03 | Kurabo Ind Ltd | Method for measuring absorbancy |
| JP3792374B2 (en) * | 1997-10-29 | 2006-07-05 | 倉敷紡績株式会社 | Optical density measuring device |
| EP1010975A1 (en) * | 1998-12-14 | 2000-06-21 | SCITEX DIGITAL PRINTING, Inc. | Liquid concentration optical sensor |
| JP5010180B2 (en) * | 2006-05-31 | 2012-08-29 | 京セラドキュメントソリューションズ株式会社 | Liquid developer concentration measuring apparatus and wet image forming apparatus having the same |
| ITRM20080428A1 (en) * | 2008-08-05 | 2010-02-06 | Anova S A S Di Giovanni Mappa | DEVICE FOR IN-LINE DETERMINATION OF THE QUANTITY OF COLOR AND / OR TURBIDITY UNDER THE TREATMENT AND DISCHARGE OF WASTE OF INDUSTRIAL AND / OR CIVIL WATERS. |
| JP6503230B2 (en) * | 2015-05-29 | 2019-04-17 | ニプロ株式会社 | Transmitted light intensity measurement unit |
-
1982
- 1982-12-10 JP JP57217160A patent/JPS59107241A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS59107241A (en) | 1984-06-21 |
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