JPH03220444A - Measuring method of absorbing state and measuring apparatus of absorption - Google Patents

Measuring method of absorbing state and measuring apparatus of absorption

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Publication number
JPH03220444A
JPH03220444A JP1583590A JP1583590A JPH03220444A JP H03220444 A JPH03220444 A JP H03220444A JP 1583590 A JP1583590 A JP 1583590A JP 1583590 A JP1583590 A JP 1583590A JP H03220444 A JPH03220444 A JP H03220444A
Authority
JP
Japan
Prior art keywords
light
measurement
window
fluid
measured
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
JP1583590A
Other languages
Japanese (ja)
Inventor
Masataka Shichiri
雅隆 七里
Hitoshi Ishibashi
石橋 仁志
Masaaki Tsuchimoto
土本 正明
Ryoji Suzuki
良治 鈴木
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.)
Kubota Corp
Original Assignee
Kubota 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 Kubota Corp filed Critical Kubota Corp
Priority to JP1583590A priority Critical patent/JPH03220444A/en
Publication of JPH03220444A publication Critical patent/JPH03220444A/en
Pending legal-status Critical Current

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  • Investigating Or Analysing Materials By Optical Means (AREA)
  • Optical Measuring Cells (AREA)

Abstract

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、測定光を照射窓から測定対象流体中に入射さ
せ、その測定対象流体を透過した後に受光窓に受け入れ
た測定光を用いて前記測定対象流体の吸光状態を測定す
る吸光状態測定方法、および、測定対象流体に光源から
の測定光を入射させるための照射窓と、その照射窓から
射出されて前記測定対象流体中を透過した測定光を受け
入れて吸光状態測定用の受光手段に受光させるための受
光窓とを、離隔させて設けてある吸光測定装置に関する
[Detailed Description of the Invention] [Industrial Application Field] The present invention makes measurement light enter a fluid to be measured from an irradiation window, and uses the measurement light that is received by a light receiving window after passing through the fluid to be measured. A light absorption state measuring method for measuring the light absorption state of the fluid to be measured, an irradiation window for allowing measurement light from a light source to enter the fluid to be measured, and a light emitted from the irradiation window and transmitted through the fluid to be measured. The present invention relates to an absorption measuring device in which a light receiving window for receiving measurement light and allowing a light receiving means for measuring the state of light absorption to receive the light is provided at a distance.

〔従来の技術〕[Conventional technology]

上述した流体の吸光状態の測定は、例えば、得られる吸
収係数からそれに比例する測定対象流体の濃度を求めた
り、或いは、受光窓に受け入れた測定光をスペクトル分
析して測定対象流体の成分の同定を行ったりするための
ものである。ところが、この測定は、測定光を照射窓か
ら測定対象流体中に入射させ、その後、測定対象流体を
透過した測定光を受光窓から取り出すものであり、測定
に際して、照射窓と受光窓とがともに測定対象流体に接
触しているから、長期間に亘って測定を続けていると、
それら照射窓および受光窓に汚れが付着したり疵が付い
たりすることに起因してその照射窓および受光窓の部分
での光の吸収に変化が生じ、同じ吸収係数の測定対象流
体であっても、得られる測定光の強度が汚れや疵のない
時点としては異なることとなってしまう。そこで、従来
、定期的に照射窓や受光窓の清掃を行ったり、汚れ等が
ひどくなると照射窓や受光窓を新品に取り替えたり、と
いったメンテナンス作業を行うとか、或いは、そのよう
な経年変化による影響を除去するために、測定を開始す
る前に、例えば、汚れや疵のない時点で得た測定光の強
度に基づいて、測定系を較正(キャリブレーション)す
ることが−船釣に行われている。
The above-mentioned measurement of the light absorption state of a fluid can be carried out, for example, by determining the concentration of the fluid to be measured that is proportional to the absorption coefficient obtained, or by analyzing the spectrum of the measurement light received by the light receiving window to identify the components of the fluid to be measured. It is for doing things. However, in this measurement, the measurement light enters the fluid to be measured through the irradiation window, and then the measurement light that has passed through the fluid to be measured is extracted from the light reception window. Since it is in contact with the fluid to be measured, if measurements are continued for a long period of time,
Due to dirt or scratches on the irradiation window and the light receiving window, the absorption of light at the irradiation window and the light receiving window changes. However, the intensity of the measurement light obtained will be different from the point at which there is no dirt or flaw. Therefore, conventionally, maintenance work has been carried out such as cleaning the irradiation window and light receiving window on a regular basis, and replacing the irradiating window and light receiving window with new ones when they become dirty, or the effects of such changes over time. In order to eliminate this, the measuring system must be calibrated before starting the measurement, for example on the basis of the intensity of the measuring light obtained at a time when there are no stains or scratches - as is done when fishing on a boat. There is.

〔発明が解決しようとする課題〕[Problem to be solved by the invention]

しかし、上述した従来の測定においては、つまり、従来
の吸光状態測定方法による測定、或いは、従来の吸光測
定装置を用いた吸光状態の測定においては、前者のメン
テナンス作業を行う場合にはその作業に多大の労力を要
するとともに流体の流れを中断しなければならないので
操業率が低下するものであり、特に、扱う流体が汚泥や
或いは濁度の高いものである場合には汚れ等がつき易く
そのメンテナンス作業を頻繁に行う必要があって効率的
でなく、また、後者のキャリブレーション作業を行う場
合には、測定の度に、それに先立って必要となるキャリ
ブレーションの作業が煩わしく、かつ、そのキャリブレ
ーションのために吸収係数が既知である流体を用いて測
定光の基準強度を得る必要があることからその作業に手
間が掛かる問題があった。
However, in the conventional measurement described above, that is, in the measurement using the conventional light absorption state measurement method or in the measurement of the light absorption state using a conventional light absorption measuring device, when performing maintenance work for the former, it is difficult to perform the maintenance work. This requires a great deal of labor and requires interruption of the fluid flow, which lowers the operating rate.Especially when the fluid being handled is sludge or something with high turbidity, it tends to get dirty and maintenance is difficult. It is not efficient as it requires frequent calibration work, and when performing the latter calibration work, the calibration work that is required prior to each measurement is troublesome, and the calibration work is troublesome. Therefore, it is necessary to obtain the reference intensity of the measurement light using a fluid whose absorption coefficient is known, which poses a problem in that the work is time-consuming.

本発明の目的は、上記実情に鑑み、長期間にわたって測
定を行っても汚れや疵等による影響を受けることなく、
かつ、測定対象流体の流れを中断することなく測定を継
続して行うことのできる吸光状態測定方法および吸光測
定装置を提供することにある。
In view of the above-mentioned circumstances, the purpose of the present invention is to provide a system that is not affected by dirt, scratches, etc. even when measurements are carried out over a long period of time.
Another object of the present invention is to provide a light absorption state measuring method and a light absorption measuring device that allow continuous measurement without interrupting the flow of the fluid to be measured.

〔課題を解決するための手段〕[Means to solve the problem]

上記目的を達成するために講じた第1の手段である本発
明による吸光状態測定方法の特徴は、測定対象流体に光
源からの測定光を入射させるための照射窓と、この照射
窓から射出されて前記測定対象流体中を透過した測定光
を受け入れて吸光状態測定用の受光手段に受光させるた
めの受光窓とを設定距離を隔てて位置させた第1の測定
状態で前記受光窓に受け入れた第1の測定光の強度、及
び、この第1の測定状態とは異なる設定距離を隔てて前
記照射窓と受光窓とを位置させた第2の測定状態で前記
受光窓に受け入れた第2の測定光の強度とを用いて、k
−(1/ΔL)l!oga Iout/I′out)た
だし、k:測定対象流体での吸収係数ΔL:2つの測定
状態間の照射窓と受光窓との離隔距離の差 Iout:第1の測定光の強度 I′out:第2の測定光の強度 の式により前記測定対象流体(S)の吸収係数を求める
ことにある。
The light absorption state measuring method according to the present invention, which is the first means taken to achieve the above object, is characterized by an irradiation window for allowing measurement light from a light source to enter the fluid to be measured, and a light emitted from the irradiation window. and a light-receiving window for receiving the measurement light transmitted through the fluid to be measured and having it received by the light-receiving means for measuring the light absorption state, in a first measurement state in which the light-receiving window is positioned at a set distance. The intensity of the first measurement light and the second measurement light received by the light reception window in a second measurement state in which the irradiation window and the light reception window are positioned apart from each other by a set distance different from the first measurement state. Using the intensity of the measurement light, k
-(1/ΔL)l! oga Iout/I'out) where, k: Absorption coefficient ΔL in the fluid to be measured: Difference in the separation distance between the irradiation window and the light receiving window between the two measurement states Iout: Intensity of the first measurement light I'out: The purpose is to obtain the absorption coefficient of the fluid (S) to be measured using the second measurement light intensity equation.

また、前記目的を達成するために講じた第2の手段であ
る本発明による吸光測定装置の特徴構成は、照射窓と受
光窓とを測定光の透過方向に沿って相対移動自在に設け
、それら照射窓と受光窓とを相対移動させて離隔距離を
変更する測定距離変更手段と、この測定距離変更手段に
より互いに離隔距離を異ならせた2つの測定状態で前記
受光手段が各別に受光した第1および第2の測定光の強
度を用いて、 k= (1/ΔL)・fogs Iout/I′out
)ただし、k:測定対象流体の吸収係数 ΔL=2つの測定状態間での照射窓と受光窓との離隔距
離の差 Iout:第1の測定光の強度 I′out:第2の測定光の強度 の式により前記測定対象流体の吸収係数を求める演算手
段とを設けたことにある。
Further, the characteristic configuration of the absorption measuring device according to the present invention, which is the second means taken to achieve the above object, is that the irradiation window and the light receiving window are provided so as to be relatively movable along the transmission direction of the measurement light. measurement distance changing means for changing the separation distance by relatively moving the irradiation window and the light receiving window; and the intensity of the second measurement light, k= (1/ΔL)・fogs Iout/I'out
) where k: absorption coefficient of the fluid to be measured ΔL = difference in separation distance between the irradiation window and the light receiving window between the two measurement states Iout: intensity of the first measurement light I'out: intensity of the second measurement light The present invention further includes a calculation means for determining the absorption coefficient of the fluid to be measured using an intensity formula.

〔作 用〕[For production]

つまり、この種の吸光状態の測定においては、測定が面
倒なこと、および、測定系の感度の影響があることから
、測定光の強度の絶対値を測定するのではなく、一般に
、測定対象流体に入射した測定光(以下、入射光と称す
る)の強度と測定対象流体を透過した後に受光された測
定光(以下、出射光と称する)の強度との比を求めこと
が行われる。そして、上述の比と測定対象流体の吸収係
数との間には、ランハート−ヘールの法則によって、次
の■弐の関係があることが知られている。すなわち、 Iout/1.、=e−”L      ■ただし、I
ou t :出射光の強度 11)1:入射光の強度 に:測定対象流体の吸収係数 L:照射窓と受光窓との離隔距離 である。一般には、この0式により、吸収係数を求める
のである。
In other words, in measuring this type of light absorption state, the measurement is complicated and the sensitivity of the measurement system is affected, so instead of measuring the absolute value of the intensity of the measurement light, it is generally The ratio of the intensity of the measurement light incident on the fluid (hereinafter referred to as incident light) to the intensity of the measurement light received after passing through the fluid to be measured (hereinafter referred to as output light) is determined. It is known that the following relationship exists between the above-mentioned ratio and the absorption coefficient of the fluid to be measured, according to the Langhardt-Helle law. That is, Iout/1. ,=e−”L ■However, I
out: intensity of emitted light 11) 1: intensity of incident light: absorption coefficient of the fluid to be measured L: separation distance between the irradiation window and the light receiving window. Generally, the absorption coefficient is determined using this equation.

ここで、上掲の0式に照射窓および受光窓等による吸収
を導入すると、 Iout/IB=e−”°1゛1′       ■た
だし、a:照射窓と受光窓等による吸収となる。そして
、それら照射窓ならびに受光窓に汚れや疵が付くと、上
掲の0式における[a]の値が変化するため、吸収係数
を正確に求めることができなくなるのである。
Here, if absorption by the irradiation window and the light receiving window is introduced into the above equation 0, then Iout/IB=e-"°1゛1' ■However, a: Absorption by the irradiating window and the light receiving window, etc. If the irradiation window and the light receiving window become dirty or scratched, the value of [a] in the above equation 0 will change, making it impossible to accurately determine the absorption coefficient.

しかし、この吸収は、長期間に亘る使用では変化するが
、はぼ同時期に照射窓と受光窓との位置関係が変わって
も変化するものではない。
However, although this absorption changes over a long period of use, it does not change even if the positional relationship between the irradiation window and the light receiving window changes at approximately the same time.

そこで、照射窓と受光窓との離隔距離を異ならせた第2
の測定状態で測定を行うと、この場合に得られる出射光
の強度と測定対象流体の吸収係数との関係は、 I′out/I、、−e−(k”’ ”’      
■ただし、I′out:第2の測定状態での出射光の強
度 L゛:第2の測定状態での照射窓と 受光窓との離隔距離 (=L+ΔL) となる。
Therefore, the second
When measurement is carried out under the measurement conditions, the relationship between the intensity of the emitted light obtained in this case and the absorption coefficient of the fluid to be measured is I'out/I,, -e-(k''''''
(2) However, I'out: Intensity of emitted light in the second measurement state L': Separation distance between the irradiation window and the light receiving window in the second measurement state (=L+ΔL).

従って、0式と0式とを連立させて[k]について解く
と、 (Iou t/ I I N)バI′out/ItN)
  = e(”°l−+all  /(e−1°L’ 
on+ ) ■out/f’。ut=e(−に−L−a〉−(−に’
L’ −a)=ek−(1−1’) となり、両辺の対数をとって、 log、Iout/I′out)=に、(L’−L)=
k・ΔL となるから、結局、 k=(1/ΔL)・l Ig、(Iout/I′out
)■ の弐のよって、測定対象流体の吸収係数を求めることが
できる。そして、この式から明らかなように、吸収係数
を求めるにあたって、照射窓ならびに受光窓による吸収
の要素が除去されており、また、照射窓と受光窓との離
隔距離は必要でなく2つの測定状態でそれらの離隔距離
の差が分かればよく、さらに、測定対象流体へ入射され
る測定光の強度は分がっていなくてもよい 要約すると、設定距離を互いに異ならせた2つの測定状
態で得た2つの測定光の強度を用いて前掲の0式に基づ
いて計算すると、照射光や受光窓についた汚れや疵の影
響を受けることなく、測定系の経年変化に拘らず、常に
正確に測定対象流体の吸収係数を求めることができるの
である。
Therefore, when equations 0 and 0 are combined and solved for [k], (Iout/ I I N) I'out/ItN)
= e(”°l-+all /(e-1°L'
on+) ■out/f'. ut=e(-ni-L-a〉-(-ni'
L'-a)=ek-(1-1'), taking the logarithm of both sides, log, Iout/I'out)=, (L'-L)=
Since k・ΔL, in the end, k=(1/ΔL)・l Ig, (Iout/I′out
)■ The absorption coefficient of the fluid to be measured can be determined. As is clear from this equation, when calculating the absorption coefficient, the elements of absorption by the irradiation window and the light reception window are removed, and the separation distance between the irradiation window and the light reception window is not necessary, and the two measurement conditions are It is only necessary to know the difference in their separation distances, and the intensity of the measurement light incident on the fluid to be measured does not need to be known. Calculation based on the formula 0 above using the intensities of the two measurement lights allows accurate measurement at all times, regardless of age-related changes in the measurement system, without being affected by dirt or scratches on the irradiation light or the light receiving window. This allows the absorption coefficient of the target fluid to be determined.

また、請求項2記載のように、上述のような吸収係数を
求めるアルゴリズムを組み込んだ測定手段を備えた吸光
測定装置においては、照射窓と受光窓とのM隔距離を異
ならせる測定距離変更手段による2つの測定状態の切替
えと相俟って、上記演算手段が、自動的に測定対象流体
の吸収係数を求めるから、測定を極めて簡略かつ迅速に
行うことができる。
Further, as claimed in claim 2, in an absorption measuring device equipped with a measuring means incorporating an algorithm for determining an absorption coefficient as described above, a measuring distance changing means for varying the distance M between the irradiation window and the light receiving window is provided. Coupled with the switching between the two measurement states, the calculation means automatically calculates the absorption coefficient of the fluid to be measured, making it possible to perform measurements extremely simply and quickly.

〔発明の効果] その結果、本発明の吸光状態測定方法によれば、測定系
の経年変化に拘らず、照射窓や受光窓等による吸収の影
響を受けない状態で、常に、正確に測定対象流体の吸収
係数を求めることができるから、多大の労力を要し操業
率を低下させる虞のあるメンテナンス作業を煩雑に行う
必要なく、或いは、煩わしく手間の掛かるキャリブレー
ション作業を測定の度に行う必要なく、長期間にわたっ
て測定を行うことができ、しかも、その測定に際して測
定対象流体の流れを中断させることをなくせるから、全
体として、流体の吸光状態の測定を、手際よく行えるよ
うになった。
[Effects of the Invention] As a result, according to the light absorption state measuring method of the present invention, the measurement target can be accurately measured at all times without being affected by absorption by the irradiation window, the light receiving window, etc., regardless of the aging of the measurement system. Since the absorption coefficient of the fluid can be determined, there is no need to perform troublesome maintenance work that requires a lot of effort and may reduce the operating rate, or it is no longer necessary to perform troublesome and time-consuming calibration work every time a measurement is made. Since the measurement can be carried out over a long period of time, and the flow of the fluid to be measured is not interrupted during the measurement, the light absorption state of the fluid can be measured easily as a whole.

さらに、照射窓と受光窓との離隔距離は必要でなく、そ
れらの2つの測定状態間での差が分かη、ばよいから、
例えば、照射窓と受光窓とが分割されていて、それらを
流路径が不明な流路に通用する場合に、何れが一方の窓
の位置のみを正確に把握すればよく、測定系の流路への
設置が容易に行える利点もある。また、測定対象流体へ
の入射光の強さは必要でないから、測定光の強さを測る
ための構成を受光側だけに設けらればよく、測定系の簡
素化を図ることができる利点もある。
Furthermore, the separation distance between the irradiation window and the light receiving window is not necessary, and the difference between the two measurement states only needs to be η.
For example, when the irradiation window and the light reception window are divided and they are used to connect a flow path with an unknown flow path diameter, it is only necessary to accurately know the position of one window, and the flow path of the measurement system It also has the advantage of being easy to install. In addition, since the intensity of the light incident on the fluid to be measured is not required, a configuration for measuring the intensity of the measurement light only needs to be provided on the light receiving side, which has the advantage of simplifying the measurement system. .

また、本発明の吸光測定装置によれば、本発明の吸光状
態測定方法を具現した一例であり、上述した効果に加え
て、測定の手順を自動化することで、より一層の測定作
業の簡略化ならびに迅速化を図ることができる。
In addition, the absorbance measuring device of the present invention is an example of implementing the absorbance state measuring method of the present invention, and in addition to the above-mentioned effects, it further simplifies the measurement work by automating the measurement procedure. In addition, it is possible to speed up the process.

〔実施例〕〔Example〕

以下、図面に基づいて本発明の詳細な説明する。なお、
本発明の吸光状態測定方法の一例は本発明の吸光測定装
置によって具現されるものであるから、本発明の詳細な
説明は、吸光測定装置の説明を以って、両発明の説明を
兼ねて行う。
Hereinafter, the present invention will be described in detail based on the drawings. In addition,
Since an example of the method for measuring the light absorption state of the present invention is realized by the light absorption measuring device of the present invention, the detailed description of the present invention will include a description of the light absorption measuring device, and will also serve as a description of both inventions. conduct.

第1図および第2図に示すように、測定対象流体(S)
が流れる輸送管(p)の管壁の互いに対向する箇所に、
光源(1)から出射されコリメータレンズ(2)で平行
光線束に整形された測定光を測定対象流体(S)に入射
させる照射窓(3)と、その照射窓(3)から射出され
て前記測定対象流体(S)中を透過した測定光を受け入
れて集光レンズ(4)で集光させた後に吸光状態測定用
の受光手段である受光素子(S)に受光させるための受
光窓(6)とを、振り分けて配設し、前記受光素子(5
)により受光されて光電変換された光電流を用いて測定
対象流体(S)の吸光状態を測定するための演算手段(
7)を設けて、吸光測定装置を構成しである。
As shown in Figures 1 and 2, the fluid to be measured (S)
At mutually opposing locations on the pipe wall of the transport pipe (p) through which
An irradiation window (3) through which the measurement light emitted from the light source (1) and shaped into a parallel beam by the collimator lens (2) enters the fluid to be measured (S); A light-receiving window (6) receives the measurement light transmitted through the fluid to be measured (S), condenses it with a condenser lens (4), and then causes the light-receiving element (S), which is a light-receiving means for measuring the light absorption state, to receive the light. ) are distributed and arranged, and the light receiving element (5
) for measuring the light absorption state of the measurement target fluid (S) using the photocurrent received and photoelectrically converted by
7) to constitute an absorption measuring device.

前記受光窓(6)が設けられた流路の部分に、側方に膨
出する形状の補助室(8)を形成してあり、その補助室
(8)内に、前記受光窓(6)・集光レンズ(4)・受
光素子(5)からなる受光ユニット(R)を、ダイヤフ
ラム(9)を介して前記管壁に支持させた状態で収容し
、その受光ユニ7ト(R)を輸送管([〕)の径方向に
沿って位置変更させるように前記ダイヤフラム(9)を
伸縮させる一対のフリツプ(lO)を設けてある。
An auxiliary chamber (8) having a shape that bulges out laterally is formed in the part of the flow path where the light receiving window (6) is provided, and the light receiving window (6) is provided in the auxiliary chamber (8). - A light receiving unit (R) consisting of a condensing lens (4) and a light receiving element (5) is housed in a state supported by the tube wall via a diaphragm (9), and the light receiving unit (R) is A pair of flips (lO) are provided for expanding and contracting the diaphragm (9) so as to change its position along the radial direction of the transport pipe ([]).

この一対のフリツプ(10)は、前記演算手段(7)を
含む制御装置(C)からの制御信号によって伸縮駆動さ
れるように構成しである。そして、前記演算手段(7)
は、測定距離変更手段である上述したフリツプ(10)
に対する制御信号に応して自動的に前記受光ユニ7ト(
R)の移動で照射窓(3)と受光窓(6)との離隔距離
を互いに異ならせた2つの測定状態で前記受光素子(5
)が各別に受光した第1および第2の測定光の強度を用
いて、下記の式により前記測定対象流体(S)の吸収係
数を求めるように構成しである。すなわち、 k−(1/ΔL)l!og* Iout/I′out)
ただし、k:測定対象流体の吸収係数 ΔL:2つの測定状態間での照射窓と受光窓との離隔距
離の差 rout:第1の測定光の強度 I′out:第2の測定光の強度 つまり、流体の吸光状態に関わるランヘルドヘールの法
則から、測定対象流体(S)への入射光の強度CIIN
]と、測定対象流体(S)を透過した後の出射光の強度
[Iout]の比は、測定対象流体(S)の吸収係数[
k]ならびに照射窓(3)と受光窓(6)との離隔距離
[L]とに応して変化し、その関係式は、 Iout/I+s=e −”’ で表せる。そして、測定対象流体(S)による吸収以外
の照射窓(3)と受光窓(6)等による吸収[a]を含
めて考えると、上式は、 Iout/11H=e −”°1゛1 と表せるから、照射窓(3)と受光窓(6)との離隔距
離を互いに異ならせて得た2つの出射光の強度[Iou
t、 I′out]を用いて、各別に、Iout/I+
N=e−””a) I′out/I+N=e−”°1″+まただし、L’=
L+ΔL の関係式を得、それらを連立させて吸収係数[k]につ
いて解くことで、経年変化が生しる照射窓(3)と受光
窓(6)等による吸収fa]の影響を除去して、長期間
に亘って連続的な吸光状態の測定を簡単にかつ迅速に行
えるようにしである。すなわち、 k−(1/ΔL)l!og、 Iout/I′out)
Oこよって吸収係数Fk]を求めるのである。
This pair of flips (10) is configured to be driven to expand and contract by control signals from a control device (C) including the calculation means (7). and the calculation means (7)
is the above-mentioned flip (10) which is the measurement distance changing means.
The light receiving unit 7 (
The light receiving element (5) was measured in two measurement states in which the separation distance between the irradiation window (3) and the light receiving window (6) was changed by moving the light receiving element (5).
) is configured to determine the absorption coefficient of the fluid to be measured (S) using the following equation using the intensities of the first and second measurement lights received separately. That is, k-(1/ΔL)l! og* Iout/I'out)
where, k: Absorption coefficient of the fluid to be measured ΔL: Difference in separation distance between the irradiation window and the light receiving window between the two measurement states rout: Intensity of the first measurement light I'out: Intensity of the second measurement light In other words, from Langheld-Herr's law related to the light absorption state of the fluid, the intensity CIIN of the incident light on the fluid to be measured (S)
] and the intensity [Iout] of the emitted light after passing through the fluid to be measured (S) is the absorption coefficient [Iout] of the fluid to be measured (S).
k] and the separation distance [L] between the irradiation window (3) and the light receiving window (6), and the relational expression can be expressed as Iout/I+s=e −”'. Considering absorption [a] by the irradiation window (3) and the light receiving window (6) other than absorption by (S), the above equation can be expressed as Iout/11H=e −”°1゛1, so the irradiation The intensity of the two emitted lights [Iou
t, I'out], Iout/I+
N=e-""a) I'out/I+N=e-"°1"+ straight, L'=
By obtaining the relational expression L + ΔL, combining them and solving for the absorption coefficient [k], we can remove the influence of the absorption fa due to the irradiation window (3) and the light reception window (6), etc., which change over time. This makes it possible to easily and quickly measure the state of light absorption continuously over a long period of time. That is, k-(1/ΔL)l! og, Iout/I'out)
Therefore, the absorption coefficient Fk] is determined.

〔別実施例〕[Another example]

次に、本発明の別の実施例を列記する。 Next, another example of the present invention will be listed.

くl〉吸光状態測定方法において、第1の測定光の強度
ならびに第2の測定光の強度を測定した後、それから手
計算或いは計算機へ入力することによって、吸収係数[
k]を求めてもよい。
In the absorption state measuring method, after measuring the intensity of the first measurement light and the intensity of the second measurement light, the absorption coefficient [
k] may also be obtained.

〈2〉吸光測定装置において、照射窓(3)と受光窓(
6)とを輸送管(P)の管壁に設ける構成に替えて、照
射窓(3)と受光窓(6)のほか光源(1)や受光素子
(5)や測定手段(7)等を一体化して携帯も可能な構
成とし、測定に際して、その照射芯(3)と受光窓(6
)との部分を測定対象流体(S)中に浸漬して測定を行
えるようにしてもよい。
<2> In the absorption measurement device, the irradiation window (3) and the light reception window (
6) is installed on the pipe wall of the transport pipe (P), and in addition to the irradiation window (3) and the light receiving window (6), the light source (1), the light receiving element (5), the measuring means (7), etc. It has an integrated and portable configuration, and when measuring, the irradiation core (3) and light receiving window (6)
) may be immersed in the fluid to be measured (S) to perform the measurement.

く3〉吸光測定装置において、受光窓(6)を移動させ
ることに替えて照射窓(3)を移動させてもよく、要す
るに、照射窓(3)と受光窓(6)とを、測定光の透過
方向に沿って移動させるものであれば、測定距離変更手
段の具体的構成は適宜変更自在で、例えば、手動操作す
るものであっても、2つの測定状態間の照射窓(3)と
受光窓(6)との離隔距離の差が測定手段において検出
できる構成であれば構わない。
3) In the absorption measuring device, the irradiation window (3) may be moved instead of moving the light receiving window (6). In short, the irradiating window (3) and the light receiving window (6) are The specific configuration of the measurement distance changing means can be changed as appropriate as long as it moves along the transmission direction of Any configuration may be used as long as the difference in separation distance from the light receiving window (6) can be detected by the measuring means.

く4〉光源(1)の種類或いは受光手段(5)の形式等
は任意である。また、測定対象流体(S)の種類は特に
限定されるのではない。
(4) The type of light source (1), the type of light receiving means (5), etc. are arbitrary. Further, the type of fluid to be measured (S) is not particularly limited.

〈5〉本発明による測定は、単に全波長に亘る吸収係数
を測定する場合だけでなく、各種の単色光を用いて異な
る波長毎に得た測定結果から、スペクトル分析を行うも
のであってもよい。
<5> Measurements according to the present invention are not limited to simply measuring absorption coefficients over all wavelengths, but also include performing spectral analysis from measurement results obtained at different wavelengths using various monochromatic lights. good.

4 面、特許請求の範囲の項に図面との対照を便利にする為
に符号を記すが、該記入により本発明は添付図面の構造
に限定されるものではない。
4. Reference numerals are written in the claims section for convenience of comparison with the drawings, but the present invention is not limited to the structure shown in the accompanying drawings by these markings.

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

図面は本発明に係る吸光状態測定方法および吸光測定装
置の実施例を示し、第1図及び第2図はそれぞれ異なる
測定状態での吸光測定装置の概略構成図である。 (1)・・・・・・光源、(3)・・・・・・照射窓、
(5)・・・・・・受光手段、(6)・・・・・・受光
窓、(7)・・・・・・演算手段、(lO)・・・・・
・測定距離変更手段、(S)・・・・・・測定対象流体
The drawings show embodiments of the light absorption state measuring method and the light absorption measuring device according to the present invention, and FIGS. 1 and 2 are schematic configuration diagrams of the light absorption measuring device in different measurement states. (1)...Light source, (3)...Irradiation window,
(5)... Light receiving means, (6)... Light receiving window, (7)... Calculating means, (lO)...
・Measurement distance changing means, (S)...Fluid to be measured.

Claims (1)

【特許請求の範囲】 1、測定光を照射窓(3)から測定対象流体(S)中に
入射させ、その測定対象流体(S)を透過した後に受光
窓(6)に受け入れた測定光を用いて前記測定対象流体
(S)の吸光状態を測定する吸光状態測定方法であって
、前記照射窓(3)と受光窓(6)とを設定距離を隔て
て位置させた第1の測定状態で前記受光窓(6)に受け
入れた第1の測定光の強度、及び、この第1の測定状態
とは異なる設定距離を隔てて前記照射窓(3)と受光窓
(6)とを位置させた第2の測定状態で前記受光窓(6
)に受け入れた第2の測定光の強度とを用いて、 k=(1/ΔL)・log_eIout/I′out)
ただし、k:測定対象流体の吸収係数 ΔL:2つの測定状態間での照射窓と 受光窓との離隔距離の差 Iout:第1の測定光の強度 I′out:第2の測定光の強度 の式により前記測定対象流体(S)の吸収係数を求める
吸光状態測定方法。 2、測定対象流体(S)に光源(1)からの測定光を入
射させるための照射窓(3)と、この照射窓(3)から
射出されて前記測定対象流体(S)中を透過した測定光
を受け入れて吸光状態測定用の受光手段(5)に受光さ
せるための受光窓(6)とを、離隔させて設けてある吸
光測定装置において、前記照射窓(3)と受光窓(6)
とを測定光の透過方向に沿って相対移動自在に設け、そ
れら照射窓(3)と受光窓(6)とを相対移動させて離
隔距離を変更する測定距離変更手段(10)と、この測
定距離変更手段(10)により互いに離隔距離を異なら
せた2つの測定状態で前記受光手段(5)が各別に受光
した第1および第2の測定光の強度を用いて、 k=(1/ΔL)・log_eIout/I′out)
ただし、k:測定対象流体の吸収係数 ΔL:2つの測定状態間での照射窓と 受光窓との離隔距離の差 Iout:第1の測定光の強度 I′out:第2の測定光の強度 の式により前記測定対象流体(S)の吸収係数を求める
演算手段(7)とを設けてある吸光測定装置。
[Claims] 1. The measurement light is made to enter the fluid to be measured (S) through the irradiation window (3), and after passing through the fluid to be measured (S), the measurement light is received by the light receiving window (6). A first measurement state in which the irradiation window (3) and the light reception window (6) are located apart from each other by a set distance. the intensity of the first measurement light received by the light receiving window (6), and positioning the irradiation window (3) and the light receiving window (6) at a set distance different from this first measurement state. In the second measurement state, the light receiving window (6
) and the intensity of the second measurement light received in k=(1/ΔL)・log_eIout/I′out)
where, k: Absorption coefficient of the fluid to be measured ΔL: Difference in separation distance between the irradiation window and the light receiving window between the two measurement states Iout: Intensity of the first measurement light I'out: Intensity of the second measurement light A light absorption state measuring method for determining the absorption coefficient of the fluid to be measured (S) using the following equation. 2. An irradiation window (3) for allowing the measurement light from the light source (1) to enter the fluid to be measured (S), and the light emitted from the irradiation window (3) and transmitted through the fluid to be measured (S). In an absorption measuring device, a light receiving window (6) for receiving measurement light and allowing the light receiving means (5) for measuring the light absorption state to receive the light is provided separately from the light receiving window (6). )
and a measurement distance changing means (10) which is provided so as to be relatively movable along the transmission direction of the measurement light, and which changes the separation distance by relatively moving the irradiation window (3) and the light reception window (6); Using the intensities of the first and second measurement lights separately received by the light receiving means (5) in two measurement states with different distances from each other by the distance changing means (10), k=(1/ΔL )・log_eIout/I'out)
where, k: Absorption coefficient of the fluid to be measured ΔL: Difference in separation distance between the irradiation window and the light receiving window between the two measurement states Iout: Intensity of the first measurement light I'out: Intensity of the second measurement light An absorption measuring device comprising: calculation means (7) for determining the absorption coefficient of the fluid to be measured (S) according to the equation.
JP1583590A 1990-01-25 1990-01-25 Measuring method of absorbing state and measuring apparatus of absorption Pending JPH03220444A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1583590A JPH03220444A (en) 1990-01-25 1990-01-25 Measuring method of absorbing state and measuring apparatus of absorption

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1583590A JPH03220444A (en) 1990-01-25 1990-01-25 Measuring method of absorbing state and measuring apparatus of absorption

Publications (1)

Publication Number Publication Date
JPH03220444A true JPH03220444A (en) 1991-09-27

Family

ID=11899897

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1583590A Pending JPH03220444A (en) 1990-01-25 1990-01-25 Measuring method of absorbing state and measuring apparatus of absorption

Country Status (1)

Country Link
JP (1) JPH03220444A (en)

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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
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Cited By (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2001228079A (en) * 2000-02-15 2001-08-24 Jasco Corp Variable optical path length cell
JPWO2008105146A1 (en) * 2007-02-28 2010-06-03 サントリーホールディングス株式会社 Liquid-type absorbance sensor element and absorptiometer using the same
JP2012255806A (en) * 2007-02-28 2012-12-27 Suntory Holdings Ltd Absorptiometer using liquid immersion type absorbance sensor element
JP2013513783A (en) * 2009-12-10 2013-04-22 フォス アナリティカル エー/エス Variable path length probe
US8873057B2 (en) 2009-12-10 2014-10-28 Foss Analytical A/S Variable path length probe
WO2014170985A1 (en) * 2013-04-18 2014-10-23 ニプロ株式会社 Fluid concentration measuring device
US9562858B2 (en) 2013-04-18 2017-02-07 Nipro Corporation Fluid concentration measuring device
JPWO2014170985A1 (en) * 2013-04-18 2017-02-16 ニプロ株式会社 Fluid concentration measuring device
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