JPH08114546A - Liquid concentration measuring device - Google Patents

Liquid concentration measuring device

Info

Publication number
JPH08114546A
JPH08114546A JP24786594A JP24786594A JPH08114546A JP H08114546 A JPH08114546 A JP H08114546A JP 24786594 A JP24786594 A JP 24786594A JP 24786594 A JP24786594 A JP 24786594A JP H08114546 A JPH08114546 A JP H08114546A
Authority
JP
Japan
Prior art keywords
light
liquid
measured
reflected
concentration
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
JP24786594A
Other languages
Japanese (ja)
Inventor
Fuminori Kobayashi
史典 小林
Yoshiharu Igawa
義春 井川
Joji Nonoyama
錠治 野々山
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.)
Shiroki Corp
Original Assignee
Shiroki 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 Shiroki Corp filed Critical Shiroki Corp
Priority to JP24786594A priority Critical patent/JPH08114546A/en
Publication of JPH08114546A publication Critical patent/JPH08114546A/en
Pending legal-status Critical Current

Links

Landscapes

  • Investigating Or Analysing Materials By Optical Means (AREA)

Abstract

PURPOSE: To accurately measure the liquid concentration even in the case where a scattering light source is used or even in the case where the liquid at a little quantity is measured by providing a shading member in the measuring surface of the translucent medium except for an area, in which the total reflection of the incident light is generated in the case of the specified concentration of the liquid to be measured. CONSTITUTION: In the case where the liquid (f) to be measured at the specified concentration is dropped onto the measuring surface 24a, a part of the outgoing light from a light emitting diode 20 is reflected by the boundary surface and goes in nearly parallel with the boundary surface, and does not enter a photo diode 21 because almost of the optical component thereof is refracted and goes inside of the liquid (f) to be measured, and discharged outside or because the incident angle does not exceeds the maximum critical angle. The measuring surface 24a is provided with a shading film 32 in the area, in which total reflection of the incident light is to be generated, except for a transmitting hole 32a, and the light c4 , which enters the transmitting hole 32a, is reflected all in the condition that the light c4 exceeds the maximum critical angle, and all the optical component enters the diode 21. Light receiving quantity at this time is compared with the previously stored reference data showing the relation of the reflectance index with concentration, and concentration of the liquid to be measured can be thereby easily obtained.

Description

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

【0001】[0001]

【技術分野】本発明は、被測定液の濃度を測定するため
の液体濃度測定装置に関する。
TECHNICAL FIELD The present invention relates to a liquid concentration measuring device for measuring the concentration of a liquid to be measured.

【0002】[0002]

【従来技術及びその問題点】従来より、液体の濃度(体
積率)と該液体の屈折率との間に一定の相関関係がある
という液体の性質を利用して、濃度を測定する液体濃度
センサが知られている。この液体濃度センサは、LED
等の発光素子からの光束を光ファイバを介して被測定液
中に照射し、該光ファイバ先端に設けた反射膜で該光束
の一部を反射させ、上記光ファイバ内を戻して光検出器
に入射させ、この入射光に基づいて被測定液の濃度を検
出するように構成されている。
2. Description of the Related Art Conventionally, a liquid concentration sensor for measuring the concentration by utilizing the property of the liquid that there is a certain correlation between the concentration (volume ratio) of the liquid and the refractive index of the liquid. It has been known. This liquid concentration sensor is an LED
A light beam from a light-emitting element such as a light source is irradiated through an optical fiber into the liquid to be measured, a part of the light beam is reflected by a reflection film provided at the tip of the optical fiber, and the optical fiber is returned to the photodetector. And the concentration of the liquid to be measured is detected based on the incident light.

【0003】しかしこの従来の液体濃度センサは、発光
素子から照射される光束が、指向性を持たずに放射状に
広がる光束である場合には、光ファイバ中で伝搬される
光束同士が干渉しあうため、反射膜で反射した反射光が
効率よく光検出部内のフォトセンサに伝搬されず、正確
な濃度測定が極めて困難となる。また被測定液の量が少
なくて、光ファイバ先端のコア部を浸漬できない場合に
も、正確な測定が困難となる。
However, in this conventional liquid concentration sensor, when the luminous flux emitted from the light emitting element is a luminous flux which has no directivity and spreads radially, the luminous fluxes propagating in the optical fiber interfere with each other. Therefore, the reflected light reflected by the reflective film is not efficiently propagated to the photosensor in the photodetection section, and accurate density measurement becomes extremely difficult. Further, even when the amount of the liquid to be measured is small and the core portion at the tip of the optical fiber cannot be immersed, accurate measurement becomes difficult.

【0004】[0004]

【発明の目的】本発明は、上記従来の液体濃度センサに
関する問題点に基づき成されたもので、発光素子に発散
光を発する光源を使用した場合でも、被測定液が少量の
場合でも、液体濃度の測定を正確に行うことが可能な液
体濃度測定装置を提供することを目的とする。
SUMMARY OF THE INVENTION The present invention has been made in view of the above-mentioned problems associated with the conventional liquid concentration sensor, and can be applied to a liquid crystal even when a light source that emits divergent light is used for the light emitting element or when the liquid to be measured is small. An object of the present invention is to provide a liquid concentration measuring device capable of accurately measuring the concentration.

【0005】[0005]

【発明の概要】上記目的を達成するための本発明は、被
測定液の屈折率より高い屈折率を有し、該被測定液を接
触させる測定面を備えた透光性媒体と;この透光性媒体
を透過させて、上記測定面に向けて発散光を照射する発
光素子と;該発光素子から照射され、上記測定面と該測
定面上の被測定液との境界面で反射された反射光を受光
する受光素子と;を備えた液体濃度測定装置において、
上記透光性媒体の測定面に、上記発光素子から発光され
て該測定面で反射する光のうち、少なくとも被測定液が
特定濃度のとき該測定面で全反射が生じる領域を残して
遮光部材を設けたことを特徴としている。
SUMMARY OF THE INVENTION To achieve the above object, the present invention provides a translucent medium having a refractive index higher than that of a liquid to be measured and having a measuring surface for contacting the liquid to be measured; A light-emitting element that transmits an optical medium and emits divergent light toward the measurement surface; is emitted from the light-emitting element and is reflected by the boundary surface between the measurement surface and the liquid to be measured on the measurement surface. A liquid concentration measuring device comprising: a light receiving element that receives reflected light;
Of the light emitted from the light emitting element and reflected on the measurement surface of the light-transmissive medium, at least a region where total reflection occurs on the measurement surface when the liquid to be measured has a specific concentration is shielded. It is characterized by the provision of.

【0006】上記受光素子の前面には、発光素子から発
光されて上記測定面で反射する光のうち、特定濃度のと
き全反射が生じる上記領域で反射した光が入射する位置
に、第2の遮光部材を設けることができる。
On the front surface of the light receiving element, of the light emitted from the light emitting element and reflected by the measuring surface, the light reflected in the area where total reflection occurs at a specific density is incident on the second light receiving element. A light blocking member can be provided.

【0007】また本発明は、被測定液の屈折率より高い
屈折率を有し、該被測定液を接触させる測定面を備えた
透光性媒体と;この透光性媒体を透過させて、上記測定
面に向けて発散光を照射する発光素子と;該発光素子か
ら照射され、上記測定面と該測定面上の被測定液との境
界面で反射された反射光を受光する受光素子と;を備え
た液体濃度測定装置において、上記受光素子の前面に、
上記発光素子から発光された光のうち、少なくとも被測
定液が特定濃度のとき上記測定面で全反射が生じる領域
での反射光を受光する透光部と;この透光部の周縁の遮
光部と;を有する遮光部材を設けたこと、を特徴として
いる。
The present invention also provides a translucent medium having a refractive index higher than that of the liquid to be measured and having a measuring surface for contacting the liquid to be measured; A light emitting element for irradiating the measurement surface with divergent light; and a light receiving element for receiving reflected light emitted from the light emitting element and reflected at the boundary surface between the measurement surface and the liquid to be measured on the measurement surface. In a liquid concentration measuring device including;
Among the light emitted from the light-emitting element, a light-transmitting portion that receives reflected light at least in a region where total reflection occurs on the measurement surface when the liquid to be measured has a specific concentration; And a light-shielding member having; are provided.

【0008】[0008]

【発明の実施例】以下図示実施例について本発明を説明
する。先ず、本発明の理解を容易にするために、本発明
者等によって案出された液体濃度測定装置11′につい
て、図8により説明する。この液体濃度測定装置11′
は、本発明による液体濃度測定装置11の基礎となる。
BEST MODE FOR CARRYING OUT THE INVENTION The present invention will be described below with reference to illustrated embodiments. First, in order to facilitate understanding of the present invention, a liquid concentration measuring device 11 'devised by the present inventors will be described with reference to FIG. This liquid concentration measuring device 11 '
Is the basis of the liquid concentration measuring device 11 according to the invention.

【0009】液体濃度測定装置11′は、円筒状のケー
シング30を有している。このケーシング30の上部壁
30cの中心には、円形の測定孔30aと、この測定孔
30aと同心状のリング嵌込部30bとが形成されてい
る。ケーシング30の内方には、プリズム24を保持す
るプリズムホルダ13が固定されている。
The liquid concentration measuring device 11 'has a cylindrical casing 30. A circular measurement hole 30a and a ring fitting portion 30b concentric with the measurement hole 30a are formed at the center of the upper wall 30c of the casing 30. A prism holder 13 that holds the prism 24 is fixed inside the casing 30.

【0010】検査部10′の一部をなす上記プリズムホ
ルダ13は、図5、図6及び図8に示されるように、側
面視略台形状に形成され、所定角度に傾斜された対向す
る支持面13a、13e、及び底部13dを有してい
る。これらの支持面13a、13eには、円筒状の支持
部18、19がそれぞれに設けられている。この支持部
18は、発光ダイオード(LED)20を実装するため
の中空部18aを有し、支持部19は、フォトダイオー
ド21を実装するための中空部19aを有している。ま
たプリズムホルダ13の上部四隅には、このプリズムホ
ルダ13をケーシング30に固定するための固定用突起
13bが設けられ、該4個の固定用突起13bは、それ
ぞれにボルト孔13cを有している。
As shown in FIGS. 5, 6 and 8, the prism holder 13 forming a part of the inspection unit 10 'is formed into a substantially trapezoidal shape in a side view, and is opposed to and supported by a predetermined angle. It has surfaces 13a and 13e and a bottom portion 13d. Cylindrical supporting portions 18 and 19 are provided on these supporting surfaces 13a and 13e, respectively. The supporting portion 18 has a hollow portion 18a for mounting the light emitting diode (LED) 20, and the supporting portion 19 has a hollow portion 19a for mounting the photodiode 21. Fixing protrusions 13b for fixing the prism holder 13 to the casing 30 are provided at the four corners of the prism holder 13, and the four fixing protrusions 13b each have a bolt hole 13c. .

【0011】上記プリズム24は、被測定液fの屈折率
より高い屈折率を有するガラス等の透光性媒体からな
り、被測定液fを接触させる測定面24aと、プリズム
ホルダ13の支持面13aと同角度に傾斜された光入射
面24bと、支持面13eと同角度に傾斜された光出射
面24dと、切欠24cとを有している。
The prism 24 is made of a translucent medium such as glass having a refractive index higher than that of the liquid to be measured f, and has a measuring surface 24a with which the liquid to be measured f comes into contact and a supporting surface 13a of the prism holder 13. It has a light incident surface 24b inclined at the same angle, a light emitting surface 24d inclined at the same angle as the support surface 13e, and a notch 24c.

【0012】プリズムホルダ13は、内方に保持したプ
リズム24の測定面24aを測定孔30aに対向させた
状態で、固定ボルト33を介して上壁部30c裏面に固
定されている。さらに上壁部30cと、ケーシング30
裏面に当接する測定面24aとの間には、リング嵌込部
30bに嵌着されたOリング31が縮設されている。こ
れにより、測定孔30aと測定面24aとの間の水密が
保持され、被測定液fを留めるための凹部が構成されて
いる。
The prism holder 13 is fixed to the rear surface of the upper wall portion 30c via a fixing bolt 33 in a state where the measuring surface 24a of the prism 24 held inside faces the measuring hole 30a. Further, the upper wall portion 30c and the casing 30
An O-ring 31 fitted to the ring fitting portion 30b is contracted between the measurement surface 24a that contacts the back surface. As a result, the watertightness between the measurement hole 30a and the measurement surface 24a is maintained, and a concave portion for holding the liquid to be measured f is formed.

【0013】発光ダイオード20は、発散光である射出
光束の略中心部の光c3 を、プリズム24の屈折率と測
定面24a上の被測定液fとの屈折率に基づき求められ
る最大臨界角θc程度となる入射角で測定面24aに照
射できる角度で設けられている。フォトダイオード21
は、被測定液fとプリズム24とでなす境界面Iで反射
された反射光を、できるだけ有効に集光できる角度とな
るように設けられている。
The light emitting diode 20 has a maximum critical angle at which the light c 3 at the substantially central portion of the emitted light flux, which is divergent light, is obtained based on the refractive index of the prism 24 and the measured liquid f on the measurement surface 24a. The measurement surface 24a is provided with an angle of incidence of about θc. Photodiode 21
Is provided so that the reflected light reflected by the boundary surface I formed by the liquid to be measured f and the prism 24 can be focused as effectively as possible.

【0014】また発光ダイオード20、フォトダイオー
ド21の端子20a、21aは、ケーシング30の内方
空間15に配置された基板17に対し、リード線22、
23を介してそれぞれに接続されている。この基板17
には、発光ダイオード20を駆動する駆動回路37、フ
ォトダイオード21の受光アナログ信号をデジタル信号
に変換するA/D変換回路38、ROM39、各種演算
を行うCPU40、液晶表示部駆動回路41等が設けら
れている。該ROM39は、被測定液fの異なる濃度に
応じた境界面Iでの反射率変化によって変わる、フォト
ダイオード21によって受光される測定光の受光光量
と、被測定液fの濃度との関係をテーブルデータとして
記憶している。CPU40は、測定面24a上に滴下さ
れた被測定液fの濃度によって変わるフォトダイオード
21の受光光量と、ROM39のテーブルデータとに基
づき、被測定液fの濃度を検出する。CPU40の該検
出結果は、ケーシング30の側面に設けられた液晶表示
部25(図4参照)に表示される。図8中の符号16
は、バッテリーである。
The terminals 20a, 21a of the light emitting diode 20 and the photodiode 21 are connected to the substrate 17, which is disposed in the inner space 15 of the casing 30, with lead wires 22,
They are connected to each other via 23. This board 17
A drive circuit 37 for driving the light emitting diode 20, an A / D conversion circuit 38 for converting the received light analog signal of the photodiode 21 into a digital signal, a ROM 39, a CPU 40 for performing various calculations, a liquid crystal display drive circuit 41, etc. Has been. The ROM 39 is a table showing the relationship between the received light amount of the measurement light received by the photodiode 21 and the concentration of the measured liquid f, which changes depending on the change in the reflectance on the boundary surface I according to the different concentrations of the measured liquid f. It is stored as data. The CPU 40 detects the concentration of the liquid to be measured f based on the received light amount of the photodiode 21 which changes depending on the concentration of the liquid to be measured f dropped on the measurement surface 24a and the table data of the ROM 39. The detection result of the CPU 40 is displayed on the liquid crystal display unit 25 (see FIG. 4) provided on the side surface of the casing 30. Reference numeral 16 in FIG.
Is the battery.

【0015】ところで、一定の屈折率を有する媒質(媒
体)M1 中を進む光束が、この媒質M1 より低い屈折率
を有する媒質(媒体)M2 との境界面に入射する場合、
入射側の媒質M1 及び屈折側の媒質M2 の屈折率をそれ
ぞれn1 、n2 (n1 >n2)とすると、光束はその入
射角が臨界角θc (=sin-1(n2 /n1 ))より大
きいとき全反射する。また光束の入射角が臨界角θc
り小さいとき、光束の一部が両媒質の屈折率比(n2
1 )に応じた反射率で媒質M2 側に透過し、残りは反
射する。
By the way, when a light beam traveling through a medium (medium) M 1 having a constant refractive index is incident on a boundary surface with a medium (medium) M 2 having a lower refractive index than the medium M 1 ,
Assuming that the refractive indices of the medium M 1 on the incident side and the medium M 2 on the refractive side are n 1 and n 2 (n 1 > n 2 ), the incident angle of the light beam is a critical angle θ c (= sin −1 (n 2 / n 1 )) is greater than total reflection. When the incident angle of the light beam is smaller than the critical angle θ c , a part of the light beam has a refractive index ratio (n 2 /
It transmits to the medium M 2 side with a reflectance according to n 1 ) and reflects the rest.

【0016】従って、図5において、境界面Iに一定量
の光束を照射する場合、反射光の光量は、媒質M1 、M
2 の屈折率に応じて変化する。すなわち、媒質M1 を既
知の屈折率n1 を有するガラス材等からなるプリズム2
4とし、媒質M2 を屈折率が未知である被測定液fとす
ると、フォトダイオード21によって反射光の光量を測
定することにより、被測定液fの屈折率n2 を検出する
ことができ、これに基づき被測定液fの濃度を検出する
ことができる。
Therefore, in FIG. 5, when the boundary surface I is irradiated with a certain amount of light flux, the amount of reflected light is equal to that of the mediums M 1 and M.
It changes according to the refractive index of 2 . That is, the prism 2 made of a glass material or the like having a known refractive index n 1 is used as the medium M 1.
4, and the medium M 2 is the liquid to be measured f whose refractive index is unknown, the refractive index n 2 of the liquid to be measured f can be detected by measuring the amount of reflected light by the photodiode 21. Based on this, the concentration of the liquid to be measured f can be detected.

【0017】図5において、測定面24上に特定濃度の
被測定液fを滴下した場合、発光ダイオード20からの
出射光c1 、c2 、c3 のうち、例えば光c1 はその光
成分の殆どが被測定液f内を屈折して進んで外方に放出
されるため、被測定液fの測定に寄与しない。また光c
2 は、入射角が最大臨界角に近いがこの角度を越えない
ため、境界面Iで反射して該境界面Iと略平行な方向に
進み、フォトダイオード21には入射されない。このた
め、光c1 と同様、測定に寄与しない。
In FIG. 5, when the liquid to be measured f having a specific concentration is dropped on the measurement surface 24, for example, the light c 1 among the light emitted from the light emitting diode c 1 , c 2 , c 3 is its light component. Since most of them are refracted in the liquid to be measured f and proceed to be released to the outside, they do not contribute to the measurement of the liquid to be measured f. Also light c
In No. 2 , since the incident angle is close to the maximum critical angle but does not exceed this angle, it is reflected by the boundary surface I, travels in a direction substantially parallel to the boundary surface I, and is not incident on the photodiode 21. Therefore, like the light c 1 , it does not contribute to the measurement.

【0018】さらに光c3 は、最大臨界角を越える状態
となって全反射を起こすため、光成分の全てがフォトダ
イオード21に向けて照射される。このときのフォトダ
イオード21による受光量は最大であるから、この受光
量と、被測定液fの屈折率と、算出された該被測定液f
の濃度との関係を基準データとしてROM39に記憶し
ておく。さらに、この基準データから所定量ずつ段階的
に減少する受光光量と、この受光光量に対応させた被測
定液fの屈折率と、この被測定液fの濃度との関係を諸
データとして、ROM39に記憶させておく。このよう
に、ROM39に、フォトダイオード21の受光光量毎
に各データの関係を定義したテーブルデータを格納して
おけば、被測定液fの測定時に、CPU40がこのテー
ブルデータのうちの対応するものを呼び出すことによ
り、被測定液fの濃度を容易に検出することができる。
さらにCPU40は、その検出結果(数値)を、液晶表
示部25に表示する。
Further, the light c 3 is in a state of exceeding the maximum critical angle and causes total reflection, so that all the light components are irradiated toward the photodiode 21. Since the amount of light received by the photodiode 21 at this time is the maximum, this amount of light received, the refractive index of the measured liquid f, and the calculated measured liquid f
The relationship with the density of is stored in the ROM 39 as reference data. Further, the relationship between the received light amount that gradually decreases from the reference data by a predetermined amount, the refractive index of the measured liquid f corresponding to the received light amount, and the concentration of the measured liquid f is stored as various data in the ROM 39. To remember. In this way, if the ROM 39 stores the table data defining the relation of each data for each received light amount of the photodiode 21, the CPU 40 corresponds to this table data at the time of measuring the liquid to be measured f. By calling, the concentration of the liquid to be measured f can be easily detected.
Further, the CPU 40 displays the detection result (numerical value) on the liquid crystal display unit 25.

【0019】上記構成の液体濃度測定装置11′は、次
のように作動する。先ず、測定孔30aに囲繞された測
定面24a上に被測定液fを適当量滴下する。この状態
において、図示しないメインスイッチをオンし、発光ダ
イオード20を発光させ、光束を境界面Iに向けて照射
すると、光c3 等がフォトダイオード21により受光さ
れる。フォトダイオード21によって受光された光は、
その受光光量がCPU40によって演算され、さらに該
CPU40が、この受光光量と対応するテーブルデータ
をROM39から呼び出して、対応する濃度を検出し、
その数値を液晶表示部25に表示する。
The liquid concentration measuring device 11 'having the above structure operates as follows. First, an appropriate amount of the liquid to be measured f is dropped on the measurement surface 24a surrounded by the measurement hole 30a. In this state, a main switch (not shown) is turned on, the light emitting diode 20 is caused to emit light, and the light flux is irradiated toward the boundary surface I, so that the light c 3 or the like is received by the photodiode 21. The light received by the photodiode 21 is
The received light amount is calculated by the CPU 40, and the CPU 40 further reads out the table data corresponding to the received light amount from the ROM 39 to detect the corresponding density,
The numerical value is displayed on the liquid crystal display unit 25.

【0020】液体濃度測定装置11′は、上記のように
作動するが、研究の結果、濃度測定に関し以下のような
問題点を有することが分かった。すなわち、被測定液f
の濃度測定に寄与する光束は光c3 等ごく限られたもの
であるが、屈折して被測定液f側に出射された光が測定
孔30aの壁面や水泡b等で反射してプリズム24側に
戻り、フォトダイオード21に入射される場合に、この
入射光は、液体濃度測定装置11′外方からの外乱光a
と共に測定に悪影響を与える。つまり、フォトダイオー
ド21が、本来濃度測定に寄与する光と共に不要な光ま
で受光するため、測定誤差を小さくすることが困難にな
る。
The liquid concentration measuring device 11 'operates as described above, but as a result of research, it has been found that it has the following problems regarding the concentration measurement. That is, the measured liquid f
The light flux that contributes to the concentration measurement is extremely limited such as the light c 3 , but the light that is refracted and emitted to the measured liquid f side is reflected by the wall surface of the measurement hole 30a, the water bubble b, and the like, and the prism 24 When the light returns to the side and enters the photodiode 21, this incident light is the disturbance light a from the outside of the liquid concentration measuring device 11 ′.
Along with this, it adversely affects the measurement. That is, the photodiode 21 receives not only the light that originally contributes to the concentration measurement but also the unnecessary light, so that it is difficult to reduce the measurement error.

【0021】本発明による液体濃度測定装置11は、そ
の基礎的構成を有する液体濃度測定装置11′において
の上記問題点を解決するため完成されたものである。以
下その構成を、図1〜図4により説明する。同図に示す
液体濃度測定装置11において、上記液体濃度測定装置
11′と共通する部分には同一符号を付している。
The liquid concentration measuring device 11 according to the present invention has been completed in order to solve the above problems in the liquid concentration measuring device 11 'having the basic structure. The configuration will be described below with reference to FIGS. In the liquid concentration measuring device 11 shown in the figure, the same parts as those of the liquid concentration measuring device 11 'are designated by the same reference numerals.

【0022】本測定装置11の検査部10は、上記測定
装置11′の検査部10′と同様に、ケーシング30の
上壁部30cの裏面に、測定孔30aと対向させて固定
されたプリズムホルダ13、このプリズムホルダ13内
に収納されたプリズム24、及び、該プリズムホルダ1
3に実装された発光ダイオード20とフォトダイオード
21を有している。これらの発光ダイオード20とフォ
トダイオード21は、液体濃度測定装置11′の場合と
同様の角度でプリズムホルダ13に実装されている。
The inspection unit 10 of the measurement device 11 is, like the inspection unit 10 'of the measurement device 11', a prism holder fixed to the back surface of the upper wall portion 30c of the casing 30 so as to face the measurement hole 30a. 13, a prism 24 housed in the prism holder 13, and the prism holder 1
3 has a light emitting diode 20 and a photodiode 21 mounted thereon. The light emitting diode 20 and the photodiode 21 are mounted on the prism holder 13 at the same angle as in the liquid concentration measuring device 11 '.

【0023】プリズム24の測定面24aには、発光ダ
イオード20からの発散光をフォトダイオード21に対
して最も効果的に反射できる箇所に、所定径の透過孔3
2aが形成されている。つまり、測定面24aには、発
光ダイオード20から発光されて該測定面24aで反射
する光のうち、少なくとも被測定液fが特定濃度のとき
該測定面24aで全反射が生じる領域(透過孔32a)
を残して遮光膜(遮光部材)32がシルク印刷によって
形成されている。上記透過孔32aは、測定孔30aと
同心状の所定径、例えばφ3mmとされている。図1中、
遮光膜32は、内容の理解を助けるため大分厚く描かれ
ているが、実際は0.15mm程度の厚さである。
On the measurement surface 24a of the prism 24, a transmission hole 3 having a predetermined diameter is provided at a position where the divergent light from the light emitting diode 20 can be most effectively reflected by the photodiode 21.
2a is formed. That is, in the measurement surface 24a, of the light emitted from the light-emitting diode 20 and reflected by the measurement surface 24a, at least when the measured liquid f has a specific concentration, total reflection occurs on the measurement surface 24a (transmission hole 32a). )
The light-shielding film (light-shielding member) 32 is formed by silk-printing except the above. The transmission hole 32a has a predetermined diameter concentric with the measurement hole 30a, for example, φ3 mm. In Figure 1,
The light-shielding film 32 is drawn to be thick in order to facilitate understanding of the contents, but it is actually about 0.15 mm thick.

【0024】また、フォトダイオード21の前面には、
支持面13eと同一平面に位置された遮光部材35が設
けられている。この遮光部材35の中心には、透過孔3
2aで反射して略スポット状とされた測定光c4 を入射
する入射制限孔35aを有する遮光部材35が設けられ
ている。すなわち、該遮光部材35は、支持部19の中
空部19aと略同径に構成され、発光ダイオード20か
ら発光されて測定面24aで反射する光のうち、特定濃
度のとき全反射が生じる上記透過孔32aで反射した光
が入射する位置に、入射制限孔35aを位置させるよう
に設けられている。この遮光部材35は、入射制限孔
(透光部)35aと共に、この入射制限孔35aの周縁
に位置する遮光部35bを有している。
On the front surface of the photodiode 21,
A light blocking member 35 is provided which is located on the same plane as the support surface 13e. At the center of the light shielding member 35, the transmission hole 3
A light blocking member 35 having an entrance limiting hole 35a through which the measurement light c 4 reflected by 2a and made into a substantially spot shape is made incident is provided. That is, the light shielding member 35 is configured to have substantially the same diameter as the hollow portion 19a of the supporting portion 19, and out of the light emitted from the light emitting diode 20 and reflected by the measurement surface 24a, total reflection occurs at a specific density. The entrance limiting hole 35a is provided at a position where the light reflected by the hole 32a enters. The light blocking member 35 has an entrance limiting hole (light transmitting portion) 35a and a light blocking portion 35b located at the periphery of the entrance limiting hole 35a.

【0025】フォトダイオード21は、前面に上記遮光
部材35を有することにより、透過孔32aで反射した
もの以外の、測定に寄与しない光をカットし、この透過
孔32aで反射した、濃度測定に寄与する測定光c4
できる限り入射するように構成されている。
The photodiode 21 has the above-mentioned light-shielding member 35 on the front surface, so that it cuts off the light which does not contribute to the measurement except the light reflected by the transmission hole 32a and contributes to the concentration measurement reflected by the transmission hole 32a. The measuring light c 4 which is used is made to enter as much as possible.

【0026】このような検査部10を有する液体濃度測
定装置11は、次のように作動する。すなわち、測定孔
30aに囲繞された凹部に被測定液fを適当量滴下し
て、メインスイッチ(図示せず)をオンし、発光ダイオ
ード20を発光させると、境界面Iにおいての極狭い範
囲(φd)の透過孔32aで反射した測定光c4 は、φ
eのスポットとして遮光部材35の入射制限孔35aか
らフォトダイオード21に入射する。
The liquid concentration measuring device 11 having such an inspection section 10 operates as follows. That is, when an appropriate amount of the liquid to be measured f is dropped in the concave portion surrounded by the measurement hole 30a, the main switch (not shown) is turned on, and the light emitting diode 20 is caused to emit light, an extremely narrow range on the boundary surface I ( The measurement light c 4 reflected by the transmission hole 32a of φd) is φ
As a spot of e, the light enters the photodiode 21 through the entrance limiting hole 35a of the light shielding member 35.

【0027】この場合、凹部に滴下する被測定液fの濃
度によって、透過孔32aと対応する境界面Iでの反射
率が変わる。すなわち、被測定液fが比較的濃度の低い
ものであれば、境界面Iでの反射率が高くなり、フォト
ダイオード21によって受光される受光光量が大きくな
る。また、被測定液fの濃度が比較的高い場合には、境
界面Iでの反射率が低くなって、被測定液f側に屈折す
る光成分が増加し、よってフォトダイオード21が受光
する受光光量が小さくなる。さらに、被測定液fの濃度
によっては全反射となり、透過孔32aと対応する境界
面Iに到達した光成分の全てがフォトダイオード21に
受光されるため、このときの受光光量が最大となる。
In this case, the reflectance at the boundary surface I corresponding to the transmission hole 32a changes depending on the concentration of the liquid to be measured f dropped on the concave portion. That is, if the measured liquid f has a relatively low concentration, the reflectance at the boundary surface I becomes high, and the amount of light received by the photodiode 21 becomes large. Further, when the concentration of the liquid to be measured f is relatively high, the reflectance at the boundary surface I becomes low, and the light component refracted toward the liquid to be measured f increases, so that the light received by the photodiode 21 is received. The amount of light decreases. Further, total reflection occurs depending on the concentration of the liquid to be measured f, and all the light components reaching the boundary surface I corresponding to the transmission hole 32a are received by the photodiode 21, so the amount of received light at this time becomes maximum.

【0028】そして、測定光c4 がフォトダイオード2
1によって受光されると、その受光光量がCPU40に
よって検出され、さらに該CPU40が、この受光光量
と対応するテーブルデータをROM39から呼び出し
て、対応する濃度を検出しその数値を液晶表示部25に
表示する。
Then, the measuring light c 4 is emitted from the photodiode 2
When the light is received by 1, the amount of the received light is detected by the CPU 40, and the CPU 40 calls the table data corresponding to the received light amount from the ROM 39, detects the corresponding density, and displays the numerical value on the liquid crystal display unit 25. To do.

【0029】このように本液体濃度測定装置11は、所
定の出射角度及び入射角度に配置された発光ダイオード
20とフォトダイオード21を有し、この発光ダイオー
ド20からの出射光を測定光c4 として制限する透過孔
32aを設け、受光する光を、透過孔32aと対応する
境界面Iで反射した測定光c4 に限るための入射制限孔
35aを設けたから、光源に発光ダイオード20のよう
な発散光を発するものを光源に用いた場合でも、被測定
液fが少量の場合でも、液体濃度の測定を正確に行うこ
とができる。そして、測定値のバラツキを抑えて、濃度
測定の高精度化を可能とすることができる。
As described above, the liquid concentration measuring device 11 has the light emitting diode 20 and the photodiode 21 arranged at a predetermined emission angle and incidence angle, and the emission light from this light emitting diode 20 is used as the measurement light c 4. the transmission hole 32a to restrict provided, the received light, from the incident restriction hole 35a to limit the measuring beam c 4 reflected by the transmission holes 32a corresponding interface I provided, such as a light emitting diode 20 as a light source divergence The liquid concentration can be accurately measured even when a light source that emits light is used as the light source or when the measured liquid f is small. Further, it is possible to suppress the variation of the measured value and to improve the accuracy of the concentration measurement.

【0030】因に、本発明の液体濃度測定装置11にお
いて、例えば3000〔mV〕で使用される発光ダイオード2
0とフォトダイオード21を用いる場合、本発明の基礎
となる液体濃度測定装置11′のフォトダイオード21
付近で受光される受光光量によるセンサ出力が2.059
〔mV〕だったのに対し、入射制限孔35aを通って受光
される受光光量によるセンサ出力は0.848 〔mV〕とな
る。また本発明の液体濃度測定装置11において、その
基礎となる液体濃度測定装置11′の測定面24aで反
射された光によるセンサ出力が20.341〔mV〕だったのに
対し、透過孔32aで反射された光によるセンサ出力は
4.093 〔mV〕となる。
Incidentally, in the liquid concentration measuring device 11 of the present invention, the light emitting diode 2 used at 3000 [mV], for example.
0 and the photodiode 21 are used, the photodiode 21 of the liquid concentration measuring device 11 'which is the basis of the present invention is used.
The sensor output is 2.059 depending on the amount of light received in the vicinity.
While it was [mV], the sensor output due to the amount of received light received through the entrance limiting hole 35a is 0.848 [mV]. Further, in the liquid concentration measuring device 11 of the present invention, the sensor output due to the light reflected by the measuring surface 24a of the liquid concentration measuring device 11 'which is the base is 20.341 [mV], while it is reflected by the transmission hole 32a. The sensor output by the emitted light is
It becomes 4.093 [mV].

【0031】なお、本実施例では、ROM39に、各デ
ータの関係を予め定義したテーブルデータを格納する構
成としたが、これに限らず、CPU40が、演算した受
光光量を基に所定の条件式によって被測定液の濃度をそ
の都度算出するように構成してもよい。
In this embodiment, the ROM 39 stores the table data in which the relation of each data is defined in advance. However, the present invention is not limited to this, and the CPU 40 calculates a predetermined conditional expression based on the calculated received light amount. Alternatively, the concentration of the liquid to be measured may be calculated each time.

【0032】[0032]

【発明の効果】以上のように本発明の液体濃度測定装置
によれば、発光素子に発散光を発する光源を使用した場
合でも、被測定液が少量の場合でも、液体濃度の測定を
正確に行うことが可能となる。
As described above, according to the liquid concentration measuring apparatus of the present invention, it is possible to accurately measure the liquid concentration even when a light source that emits divergent light is used for the light emitting element or when the liquid to be measured is a small amount. It becomes possible to do.

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

【図1】本発明を適用した液体濃度測定装置を示す要部
の正面断面図である。
FIG. 1 is a front sectional view of essential parts showing a liquid concentration measuring device to which the present invention is applied.

【図2】同液体濃度測定装置に用いられるプリズムホル
ダを示す斜視図である。
FIG. 2 is a perspective view showing a prism holder used in the liquid concentration measuring apparatus.

【図3】同液体濃度測定装置に用いられるプリズムを示
す斜視図である。
FIG. 3 is a perspective view showing a prism used in the liquid concentration measuring apparatus.

【図4】同液体濃度測定装置を示す斜視外観図である。FIG. 4 is a perspective external view showing the same liquid concentration measuring device.

【図5】本発明による液体濃度測定装置の基礎となる液
体濃度測定装置の要部を示す正面断面図である。
FIG. 5 is a front sectional view showing a main part of a liquid concentration measuring device which is a basis of the liquid concentration measuring device according to the present invention.

【図6】同本発明の基礎となる液体濃度測定装置に用い
られるプリズムホルダを示す斜視図である。
FIG. 6 is a perspective view showing a prism holder used in the liquid concentration measuring device which is the basis of the present invention.

【図7】同本発明の基礎となる液体濃度測定装置に用い
られるプリズムを示す斜視図である。
FIG. 7 is a perspective view showing a prism used in the liquid concentration measuring device which is the basis of the present invention.

【図8】同本発明の基礎となる液体濃度測定装置の全体
を示す正面断面図である。
FIG. 8 is a front cross-sectional view showing the entire liquid concentration measuring device which is the basis of the present invention.

【符号の説明】[Explanation of symbols]

11 液体濃度測定装置 20 発光ダイオード(発光素子) 21 フォトダイオード(受光素子) 24 プリズム(透光性媒体) 24a 測定面 32 遮光膜(遮光部材) 32a 透過孔(透光部) 35 遮光部材(第2の遮光部材) 35a 入射制限孔 35b 遮光部 f 被測定液 I 境界面 11 Liquid Concentration Measuring Device 20 Light-Emitting Diode (Light-Emitting Element) 21 Photodiode (Light-Receiving Element) 24 Prism (Translucent Medium) 24a Measurement Surface 32 Light-Shielding Film (Light-shielding Member) 32a Transmission Hole (Light-transmitting Part) 35 Light-shielding Member (No. 1) 2 light blocking member) 35a entrance limiting hole 35b light blocking portion f measured liquid I boundary surface

Claims (3)

【特許請求の範囲】[Claims] 【請求項1】 被測定液の屈折率より高い屈折率を有
し、該被測定液を接触させる測定面を備えた透光性媒体
と;この透光性媒体を透過させて、上記測定面に向けて
発散光を照射する発光素子と;該発光素子から照射さ
れ、上記測定面と該測定面上の被測定液との境界面で反
射された反射光を受光する受光素子と;を備えた液体濃
度測定装置において、 上記透光性媒体の測定面に、上記発光素子から発光され
て該測定面で反射する光のうち、少なくとも被測定液が
特定濃度のとき該測定面で全反射が生じる領域を残して
遮光部材を設けた、ことを特徴とする液体濃度測定装
置。
1. A translucent medium having a refractive index higher than that of a liquid to be measured and provided with a measurement surface for contacting the liquid to be measured; A light-emitting element that emits divergent light toward the light source; and a light-receiving element that receives the reflected light emitted from the light-emitting element and reflected by the boundary surface between the measurement surface and the liquid to be measured on the measurement surface. In the liquid concentration measuring device, the total reflection on the measurement surface of the transparent medium is at least when the liquid to be measured has a specific concentration among the light emitted from the light emitting element and reflected on the measurement surface. A liquid concentration measuring device, characterized in that a light-shielding member is provided while leaving a generated region.
【請求項2】 請求項1において、受光素子の前面に
は、発光素子から発光されて上記測定面で反射する光の
うち、特定濃度のとき全反射が生じる上記領域で反射し
た光が入射する位置に、第2の遮光部材が設けられてい
ることを特徴とする液体濃度測定装置。
2. The front surface of the light-receiving element according to claim 1, of the light emitted from the light-emitting element and reflected by the measurement surface, the light reflected in the region where total reflection occurs at a specific density. A liquid concentration measuring device, wherein a second light shielding member is provided at the position.
【請求項3】 被測定液の屈折率より高い屈折率を有
し、該被測定液を接触させる測定面を備えた透光性媒体
と;この透光性媒体を透過させて、上記測定面に向けて
発散光を照射する発光素子と;該発光素子から照射さ
れ、上記測定面と該測定面上の被測定液との境界面で反
射された反射光を受光する受光素子と;を備えた液体濃
度測定装置において、 上記受光素子の前面に、 上記発光素子から発光された光のうち、少なくとも被測
定液が特定濃度のとき上記測定面で全反射が生じる領域
での反射光を受光する透光部と;この透光部の周縁の遮
光部と;を有する遮光部材を設けたこと、を特徴とする
液体濃度測定装置。
3. A translucent medium having a refractive index higher than that of the liquid to be measured and having a measurement surface for contacting the liquid to be measured; A light-emitting element that emits divergent light toward the light source; and a light-receiving element that receives the reflected light emitted from the light-emitting element and reflected by the boundary surface between the measurement surface and the liquid to be measured on the measurement surface. In the liquid concentration measuring apparatus, the front surface of the light receiving element receives, of the light emitted from the light emitting element, reflected light at least in a region where total reflection occurs on the measurement surface when the liquid to be measured has a specific concentration. A liquid concentration measuring device comprising: a light-transmitting portion; and a light-shielding member having a light-shielding portion on the periphery of the light-transmitting portion.
JP24786594A 1994-10-13 1994-10-13 Liquid concentration measuring device Pending JPH08114546A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP24786594A JPH08114546A (en) 1994-10-13 1994-10-13 Liquid concentration measuring device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP24786594A JPH08114546A (en) 1994-10-13 1994-10-13 Liquid concentration measuring device

Publications (1)

Publication Number Publication Date
JPH08114546A true JPH08114546A (en) 1996-05-07

Family

ID=17169792

Family Applications (1)

Application Number Title Priority Date Filing Date
JP24786594A Pending JPH08114546A (en) 1994-10-13 1994-10-13 Liquid concentration measuring device

Country Status (1)

Country Link
JP (1) JPH08114546A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2008241549A (en) * 2007-03-28 2008-10-09 Hitachi High-Technologies Corp Fluorescence detector and method, and prism body used for the same
JP2010008099A (en) * 2008-06-24 2010-01-14 National Institute Of Advanced Industrial & Technology Optical measuring instrument of liquid or molten material and optical measuring method
JP2011112598A (en) * 2009-11-30 2011-06-09 Shimadzu Corp Refractometer

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2008241549A (en) * 2007-03-28 2008-10-09 Hitachi High-Technologies Corp Fluorescence detector and method, and prism body used for the same
JP2010008099A (en) * 2008-06-24 2010-01-14 National Institute Of Advanced Industrial & Technology Optical measuring instrument of liquid or molten material and optical measuring method
JP2011112598A (en) * 2009-11-30 2011-06-09 Shimadzu Corp Refractometer

Similar Documents

Publication Publication Date Title
JP5016677B2 (en) Tilt sensor with optoelectronic level
US5917605A (en) Fluorescence sensing device
JP2009150690A (en) Reflection-type optical sensor
JP2005186388A (en) Inkjet printer
US6885455B2 (en) Self-calibration of an optical-based sensor using a total internal reflection (TIR) signature
JPH08114546A (en) Liquid concentration measuring device
JPH1151861A (en) Apparatus for measuring concentration of liquid
JP2006300793A (en) Optical liquid-level sensor
JPS6269111A (en) Reflection type inclination detecting element
JP3347542B2 (en) Concentration sensor
JP2500995Y2 (en) Liquid concentration meter
KR20050009155A (en) Missing die detection
JP3016168B2 (en) Optical liquid level detector
JPH11166892A (en) Liquid concentration measuring device
JP2569611Y2 (en) Optical system holding device
JP2992943B2 (en) Small tilt angle detector
JP2002148102A (en) Detector and method for detecting liquid
JPH10176927A (en) Inclination sensor
JPH0629725Y2 (en) Liquid concentration meter
SU1265822A1 (en) Smoke detector
JPS587986Y2 (en) battery
JPH0750030B2 (en) Liquid concentration sensor
JP2001317984A (en) Liquid level detector
JP2507666Y2 (en) Liquid concentration sensor
JPH04198843A (en) Liquid densitometer