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JPS6360856B2 - - Google Patents
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JPS6360856B2 - - Google Patents

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Publication number
JPS6360856B2
JPS6360856B2 JP21715982A JP21715982A JPS6360856B2 JP S6360856 B2 JPS6360856 B2 JP S6360856B2 JP 21715982 A JP21715982 A JP 21715982A JP 21715982 A JP21715982 A JP 21715982A JP S6360856 B2 JPS6360856 B2 JP S6360856B2
Authority
JP
Japan
Prior art keywords
measured
liquid
turbidity
water quality
propagation signal
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
JP21715982A
Other languages
Japanese (ja)
Other versions
JPS59107240A (en
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 filed Critical
Priority to JP21715982A priority Critical patent/JPS59107240A/en
Publication of JPS59107240A publication Critical patent/JPS59107240A/en
Publication of JPS6360856B2 publication Critical patent/JPS6360856B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N21/00Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
    • G01N21/17Systems in which incident light is modified in accordance with the properties of the material investigated
    • G01N21/59Transmissivity

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図は従来の光学式濁度計の一例を示す断面
図であり、第2図はその斜視図である。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
を受光する第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、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, and FIG. 2 is a perspective view thereof. In the figure, 1 is the liquid to be measured, 2 is the light source, 3 is a lens for parallelizing the light beam ○a from the light source 2, and 4 is the transmitted light ○ out of the light beam ○a from the light source 2 that has passed through the liquid to be measured 1 5 is a second photocell that monitors the light intensity of the light source 2; 6 is the first photocell;
A computing unit 7 is a measuring tube which performs predetermined computing processing using the outputs X and Y of the second photocells 4 and 5 and sends out a turbidity proportional signal Z.

上記のように構成した濁度計の作用は以下のと
おりである。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。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される。透過光の○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(1)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 the liquid to be measured 1
incident on . The light beams ○ and ○ 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 ◯◯ of transmitted light, is expressed by the following equation (1) in accordance with Beer-Lambert's 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。
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.

(1)式から濁度xは、次の(2)式で表わされる。 From equation (1), turbidity x is expressed by equation (2) below.

x=1/εl・lnY/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と置ける。そこで、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のフオドセル出力Yから濁度比例値Zが
(3)式のように求まる。
x=1/εl·lnY/X (2) Here, since the extinction coefficient ε and the measurement length l usually do not change, they can be set as a constant C. Therefore, the turbidity proportional value Z is determined from the output X of the first photocell 4 and the output Y of the second photocell that monitors the light intensity of the light source 2.
It can be found as shown in equation (3).

Z=C・lnY/X …(3) 演算器は(3)式に示す演算を行ない濁度比例値Z
を出力する。しかしながらこの場合は、測定長l
が固定されているため、測定のダイナミツクレン
ジが狭いという欠点があつた。
Z=C・lnY/X...(3) The calculator performs the calculation shown in equation (3) and calculates the turbidity proportional value Z.
Output. However, in this case, the measurement length l
Since it is fixed, the measurement dynamic range is narrow.

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が可変できる水質計器を得る
ことを目的とするものである。
The present invention was made in order to solve the above-mentioned drawbacks, and an object of the present invention is to obtain a water quality meter whose measurement length can be varied.

本発明は上記の目的を達成するためになされた
もので、被測定体を通過する光、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、
被測定液をサンプリングする測定管の一部を蛇腹
状に構成したことを特徴とする水質計器を提供す
るものである。さらに本発明は、被測定体を通過
する光、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、被測定液をサンプリングす
る測定管の一部を蛇腹状にし、測定長を調整する
手段として被測定体よりの透過信号が常に一定の
範囲内に入るよう測定長を制御し、測定長の値を
参照することにより濁度比例値を出力することを
特徴とする水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 was made to achieve the above object, and measures the turbidity, MLSS (activated sludge concentration), organic pollution, etc. of the object to be measured by the transmittance of light, ultrasonic waves, etc. passing through the object. In water quality instruments,
The present invention provides a water quality meter characterized in that a part of a measurement tube for sampling a liquid to be measured is configured in a bellows shape. Furthermore, the present invention provides a water quality instrument that measures the turbidity, MLSS (activated sludge concentration), organic pollution, etc. of a measured object based on the transmittance of light, ultrasonic waves, etc. passing through the measured object. A part of the measurement tube is made into a bellows shape, and as a means of adjusting the measurement length, the measurement length is controlled so that the transmitted signal from the object to be measured is always within a certain range, and the turbidity can be determined by referring to the measurement length value. The present invention provides a water quality meter characterized by outputting a proportional value. The present invention will be explained below using the drawings.

第3図a,bは本発明の一実施例を示す断面図
である。図において、被測定液1から第2のフオ
トセル5までは、従来の濁度計の説明で述べたも
のと同様であるが、測定管7は管の一部が自由に
伸縮できるように蛇腹状となつている点が異な
る。8は第1、第2のフオトセル4,5の出力
X,Yおよび光源ヘツド9の位置に対応した電気
出力を発生する位置検出器11の出力Lを入力
し、所定の演算処理をおこない、濁度比例値Zと
モーター10の制御信号を発生する演算器であ
る。9は光源2、レンズ3、第2のフオトセル5
を塔載し、モータ10によつて移動される光源ヘ
ツド9を移動させるモータである。
FIGS. 3a and 3b are cross-sectional views showing one embodiment of the present invention. In the figure, the structure from the liquid to be measured 1 to the second photocell 5 is the same as that described in the explanation of the conventional turbidity meter, but the measuring tube 7 has a bellows shape so that a part of the tube can freely expand and contract. The difference is that it is . Reference numeral 8 inputs the outputs X and Y of the first and second photocells 4 and 5 and the output L of the position detector 11 that generates an electrical output corresponding to the position of the light source head 9, performs predetermined arithmetic processing, and This is an arithmetic unit that generates a degree proportional value Z and a control signal for the motor 10. 9 is a light source 2, a lens 3, and a second photocell 5
This is a motor that moves the light source head 9 which is mounted on the head and is moved by the motor 10.

次に上記のように構成した本発明の作用を説明
する。従来の濁度計の説明で述べたように、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。
Next, the operation of the present invention configured as described above will be explained. As described in the description of the conventional turbidity meter, the light beam ○I 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 .

また、光束○イの透過量を検出する第1のフオト
セル4の出力が前記(1)式に示す関係式で表わされ
ることも全く同様である。本発明による濁度計で
は、測定管7の一部分を蛇腹状としているの
で、光源ヘツド9の位置が測定管7の長手方向に
自由に移動できる。光源ヘツド9の位置は測定長
lに対応しており、位置検出器11の出力Lで検
知できる。演算器8は第1、第2のフオトセル
4,5の出力X,Yと上記Lとを入力し、次の(4)
式によつて濁度比例値Zを演算して出力する。
Furthermore, it is exactly the same that the output of the first photocell 4 that detects the amount of transmission of the luminous flux ○i is expressed by the relational expression shown in the above equation (1). In the turbidity meter according to the present invention, since a portion of the measuring tube 7 is bellows-shaped, the position of the light source head 9 can be freely moved in the longitudinal direction of the measuring tube 7. The position of the light source head 9 corresponds to the measurement length l and can be detected by the output L of the position detector 11. The arithmetic unit 8 inputs the outputs X and Y of the first and second photocells 4 and 5 and the above L, and calculates the following (4)
The turbidity proportional value Z is calculated and output using the formula.

Z=C/L・lnY/X …(4) また、演算器8は第1のフオトセル出力Xをモ
ニタリングし、適正な出力が得られるようモータ
10を制御して測定長を変える。
Z=C/L·lnY/X (4) Further, the computing unit 8 monitors the first photocell output X, and controls the motor 10 to change the measurement length so as to obtain an appropriate output.

第3図aは被測定液1の濁度が低い場合を示し
ており、出力Xが大きい分だけ光源ヘツド9が後
退し測定長l1が長くなる。また、第3図bは濁度
の高い場合を示しており、前述のl1では出力Xが
小さい場合光源ヘツド9を前進させ測定長l2を短
かくすることにより出力Xを増大させる。このよ
うに、測定長lが常に最適制御された状態で(4)式
による濁度比例値を出力することができる。
FIG. 3a shows a case where the turbidity of the liquid 1 to be measured is low, and the light source head 9 is moved back as the output X is large, so that the measurement length l1 becomes longer. Further, FIG. 3b shows a case where the turbidity is high, and when the output X is small in the aforementioned l1 , the output X is increased by advancing the light source head 9 and shortening the measurement length l2 . In this way, the turbidity proportional value according to equation (4) can be output while the measurement length l is always optimally controlled.

以上、本発明を濁度計に実施した実施例につい
て説明したが、測定長の効果が生じるMLSS計や
有機汚濁計等の水質計、および煙濃度計等であつ
てもよく、また光学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、両方のフオトセル
を移動させてもよく、移動方式はモータに限らな
いことは言うまでもない。
The embodiments in which the present invention is applied to a turbidity meter have been described above, but the present invention may also be applied to water quality meters such as MLSS meters and organic turbidity meters, which have the effect of measuring length, and smoke concentration meters, or only optical type meters. It can also be applied to ultrasonic methods, etc. Furthermore, the light source head may be fixed and either the first photocell side or both photocells may be moved, and it goes without saying that the moving method is not limited to the motor.

以上の説明から明らかなように、本発明に係る
水質計器によれば、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、安定した出
力が得られる等、実施による効果大である。
As is clear from the above explanation, the water quality meter according to the present invention has great effects when implemented, such as expanding the dynamic range of measurement, improving the S/N of the detection signal, and obtaining stable output. It is.

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

第1図は従来の濁度計の一例を示す断面図、第
2図はその要部を示す斜視図、第3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…測定管、8…演
算器、9…光源ヘツド、10…モータ、11…位
置検出器。
FIG. 1 is a sectional view showing an example of a conventional turbidity meter, FIG. 2 is a perspective view showing the main parts thereof, and FIGS. 3a and 3b 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...Measuring tube, 8...Calculator, 9...Light source head, 10...Motor, 11...Position detector.

Claims (1)

【特許請求の範囲】 1 被測定液を通過する光、超音波等の伝搬信号
の透過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
の上記伝搬信号を発生する発生源と上記被測定液
を通過した上記伝搬信号を受ける受信素子の間の
一部及び上記測定管の上記発生源と受信素子の間
を除く一部を蛇腹状に構成したことを特徴とする
水質計器。 2 被測定液を通過する光、超音波等の伝搬信号
の透過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
の上記伝搬信号を発生する発生源と上記被測定液
を通過した上記伝搬信号を受ける受信素子の間の
一部及び上記測定管の上記発生源と受信素子の間
を除く一部を蛇腹状にし、上記発生源及び受信素
子間の測定長を調整する手段として前記被測定液
の透過信号が常に一定範囲内に入るよう前記測定
長を制御し、前記測定長の値を参照することによ
り濁度比例値を出力することを特徴とする水質計
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 a propagation signal such as light or ultrasonic waves passing through the liquid to be measured, A part between the generation source that generates the propagation signal of the measurement tube that samples the liquid to be measured and a receiving element that receives the propagation signal that has passed through the liquid to be measured, and a part between the generation source of the measurement tube and the reception element. A water quality meter characterized by having a bellows-shaped portion except for the gap. 2. The liquid to be measured is sampled with a water quality instrument that measures the turbidity, MLSS (activated sludge concentration), organic pollution, etc. of the liquid to be measured based on the transmittance of propagation signals such as light and ultrasonic waves passing through the liquid to be measured. a part of the measurement tube between the source that generates the propagation signal and a receiving element that receives the propagation signal that has passed through the liquid to be measured, and a part of the measurement tube other than the part between the generation source and the reception element. The measuring length is controlled so that the transmission signal of the liquid to be measured is always within a certain range, and the value of the measuring length is referred to as a means for adjusting the measuring length between the source and the receiving element. A water quality meter characterized by outputting a turbidity proportional value.
JP21715982A 1982-12-10 1982-12-10 Water quality measuring instrument Granted JPS59107240A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP21715982A JPS59107240A (en) 1982-12-10 1982-12-10 Water quality measuring instrument

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP21715982A JPS59107240A (en) 1982-12-10 1982-12-10 Water quality measuring instrument

Publications (2)

Publication Number Publication Date
JPS59107240A JPS59107240A (en) 1984-06-21
JPS6360856B2 true JPS6360856B2 (en) 1988-11-25

Family

ID=16699774

Family Applications (1)

Application Number Title Priority Date Filing Date
JP21715982A Granted JPS59107240A (en) 1982-12-10 1982-12-10 Water quality measuring instrument

Country Status (1)

Country Link
JP (1) JPS59107240A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH01272686A (en) * 1988-04-26 1989-10-31 Nippon Denso Co Ltd Heat generator
JPH01274838A (en) * 1988-04-25 1989-11-02 Nok Corp Device for optionally solidifying supercooled liquid

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP2182105B1 (en) * 2008-11-04 2014-05-07 Electrolux Home Products Corporation N.V. Turbidity sensor

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH01274838A (en) * 1988-04-25 1989-11-02 Nok Corp Device for optionally solidifying supercooled liquid
JPH01272686A (en) * 1988-04-26 1989-10-31 Nippon Denso Co Ltd Heat generator

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Publication number Publication date
JPS59107240A (en) 1984-06-21

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