JPS58103645A - Measuring apparatus of turbidity - Google Patents
Measuring apparatus of turbidityInfo
- Publication number
- JPS58103645A JPS58103645A JP56204420A JP20442081A JPS58103645A JP S58103645 A JPS58103645 A JP S58103645A JP 56204420 A JP56204420 A JP 56204420A JP 20442081 A JP20442081 A JP 20442081A JP S58103645 A JPS58103645 A JP S58103645A
- Authority
- JP
- Japan
- Prior art keywords
- light
- turbidity
- scattered
- lens
- light receiving
- 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
Links
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
- G01N21/84—Systems specially adapted for particular applications
- G01N21/85—Investigating moving fluids or granular solids
- G01N21/8507—Probe photometers, i.e. with optical measuring part dipped into fluid sample
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)
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】
本発明は溶液の濁シを測定する濁度測定装置に関し、光
源、受光素子、演算回路等の電気回路部の防水をはかシ
、かつ溶液の深い所での濁度測定においても光の減衰、
ノイズ等の問題が起らない濁度測定装置を提供するもの
である。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a turbidity measuring device for measuring turbidity in a solution, which is capable of waterproofing electric circuit parts such as a light source, a light receiving element, and an arithmetic circuit, and is capable of preventing turbidity in a deep place. Attenuation of light also occurs when measuring
The present invention provides a turbidity measuring device that does not cause problems such as noise.
以下に本発明の一実施例について図面とともに説明する
。第1図、第2図において、1は光学系の本体であり、
この本4体1は、発光側の筐体2と、受光側の筐体3と
を結合片4で結合した形状である。6は発光側の筐体2
の開口部に設けられた保護ガラスであシ、この保護ガラ
ス6の内側には屈折率分布型レンズ6が配置されている
。7は一端が上記発光側の筐体2内に導入された光ファ
イバである。8は受光側の筐体3の開1部に設けられた
保護ガラスであり、この保護ガラス8の内側の各面に対
応してレンズ9#10j11が設けられている。12,
13.14はそれぞれ一端が上記受光側の筐体3内に導
入された光ファイバであり、各光ファイバ12〜14は
上記レンズ9〜11で集光された光を筐体3の外部に導
出するものである。16は光ファイバ7を補強するだめ
の被覆チューブ、16は光ファイバ12〜14を補強す
るための被覆チューブである。上記被覆チューブ15.
16は、さらに他の被覆チューブ17で波節されている
。18は電気回路部であり、との電気回路部18には光
源191受光素子20,21が配置されている。An embodiment of the present invention will be described below with reference to the drawings. In FIGS. 1 and 2, 1 is the main body of the optical system,
This four-book body 1 has a shape in which a light-emitting side casing 2 and a light-receiving side casing 3 are connected by a connecting piece 4. 6 is the light emitting side housing 2
A refractive index gradient lens 6 is disposed inside the protective glass 6. Reference numeral 7 denotes an optical fiber whose one end is introduced into the casing 2 on the light emitting side. 8 is a protective glass provided in the opening 1 of the housing 3 on the light receiving side, and lenses 9#10j11 are provided corresponding to each inner surface of this protective glass 8. 12,
Reference numerals 13 and 14 each indicate an optical fiber whose one end is introduced into the housing 3 on the light receiving side, and each of the optical fibers 12 to 14 guides the light collected by the lenses 9 to 11 to the outside of the housing 3. It is something to do. 16 is a covering tube for reinforcing the optical fiber 7, and 16 is a covering tube for reinforcing the optical fibers 12-14. Said coated tube 15.
16 is further articulated with another covering tube 17. Reference numeral 18 denotes an electric circuit section, and a light source 191 and light receiving elements 20 and 21 are arranged in the electric circuit section 18 .
上記濁度測定装置の光学系の本体1は測定溶液内に挿入
され、電気回路部18は地上に置かれるものであシ、光
源19からの光は、光ファイバ7を介して屈折率分布型
レンズ6に達する。このレンズ6からの平行光は保護ガ
ラス6を介して測定溶液中に照射される。測定溶液中を
進んだ平行光束は測定溶液中の粒子により一部散乱を起
こす。The main body 1 of the optical system of the turbidity measuring device is inserted into the measurement solution, the electric circuit section 18 is placed on the ground, and the light from the light source 19 is transmitted through the optical fiber 7 into a refractive index gradient type. It reaches lens 6. The parallel light from this lens 6 is irradiated into the measurement solution through the protective glass 6. A part of the parallel light beam traveling through the measurement solution is scattered by particles in the measurement solution.
溶液中のム点で散乱した散乱光は受光側の筐体3の保護
ガラス8を介してレンズ10s11に入射する。一方、
測定溶液中で散乱を起さない透過光はそのまま直進し、
レンズ9に入射する。レンズ1ol 11で集光された
光はそれぞれ光ファイバ13.14を介して受光素子2
1に達する。一方、レンズ9で集光された光は光ファイ
バ12を介して他方の受光素子2oに達する。The scattered light scattered by the dots in the solution enters the lens 10s11 via the protective glass 8 of the housing 3 on the light receiving side. on the other hand,
Transmitted light that does not cause scattering in the measurement solution travels straight,
The light enters the lens 9. The light focused by the lens 1ol 11 is transmitted to the light receiving element 2 via the optical fibers 13 and 14, respectively.
Reach 1. On the other hand, the light focused by the lens 9 reaches the other light receiving element 2o via the optical fiber 12.
本実施例においては、溶液の濁りによる透過光と散乱光
を検知し、両者の割算(散乱光出力÷透過光出力)で溶
液中の濁シを検知している。In this embodiment, the transmitted light and scattered light due to the turbidity of the solution are detected, and the turbidity in the solution is detected by dividing the two (scattered light output/transmitted light output).
第3図は透過光受光素子2oの出力S1と散乱光受光素
子21の出力S2から濁度を算出する回路のブロック図
であシ、22は増巾器、23は割算演算回路である。FIG. 3 is a block diagram of a circuit that calculates turbidity from the output S1 of the transmitted light receiving element 2o and the output S2 of the scattered light receiving element 21, 22 is an amplifier, and 23 is a division calculation circuit.
第4図(A)は濁度の変化に対する透過光、散乱光の出
力の変化を示しており、散乱光出力は成る濁度を越すと
低下する。−しかし、透過光・散乱光出力を割算(82
÷8+=83)することにより、第4図(B)のように
変曲点のない曲線の濁度と演算出力の関係が得られる。FIG. 4(A) shows changes in the output of transmitted light and scattered light with respect to changes in turbidity, and the output of scattered light decreases when the turbidity is exceeded. - However, dividing the transmitted light/scattered light output (82
÷8+=83), a relationship between turbidity and calculation output of a curve without an inflection point as shown in FIG. 4(B) can be obtained.
また、このように両者の出力信号を割算することにより
、保護ガラス5,8の汚れによる影響が相殺できる。す
なわち、ガラス6.8による減光率をaとすれば、上記
の割算演算式は、となり、ガラス6.8の汚れが一様な
らば、汚れの影響は相殺されるものである。Further, by dividing both output signals in this manner, the influence of dirt on the protective glasses 5 and 8 can be canceled out. That is, if the light attenuation rate due to the glass 6.8 is a, the above division calculation formula becomes: If the dirt on the glass 6.8 is uniform, the influence of the dirt is canceled out.
本発明は上記のような構成であり、本発明によれば、光
学系部分と電気系部分を分離し、光学系を固化している
ため、発熱及び浸水の問題がなく光ファイバで光の伝達
を行うので、電気的なノイズの発生もなく、高感度の性
能をもつ濁度測定装置を提供することができる。The present invention has the above configuration, and according to the present invention, the optical system part and the electrical system part are separated and the optical system is solidified, so light can be transmitted through optical fibers without problems of heat generation and water intrusion. Therefore, it is possible to provide a turbidity measuring device that does not generate electrical noise and has highly sensitive performance.
第1図は本発明の一実施例における濁度測定装置の要部
の斜視図、第2図は同装置の要部の断面図、第3図は同
装置の電気回路部のブロック図、第4図(ム)、伊)は
同装置の特性図である。
1・・・・・・本体、2,3・・・・・・筐体、4・・
・・・・結合片、6・・・・・・保護ガラス、6・・・
・・・屈折率分布型レンズ、7・・・・・・光ファイバ
、8・・・・・・保護ガラス、9,10゜11・・・・
・・レンズ、12,13.14・・・・・・光ファイバ
、15,16,17・・・・・−被覆チェープ、1B・
・・・・・電気回路部、19・・・・・・光源、20,
21・・・・・・受光素子。
代理人の氏名 弁理士 中 尾 敏 男 ほか1名11
a1
183図
久9
第4因FIG. 1 is a perspective view of the main parts of a turbidity measuring device according to an embodiment of the present invention, FIG. 2 is a sectional view of the main parts of the device, and FIG. 3 is a block diagram of the electric circuit section of the device. Figure 4 (Mu) and Italy) are characteristic diagrams of the same device. 1... Main body, 2, 3... Housing, 4...
...Binding piece, 6...Protection glass, 6...
...gradient index lens, 7...optical fiber, 8...protective glass, 9,10°11...
...Lens, 12, 13.14...Optical fiber, 15, 16, 17...-Coated chain, 1B.
...Electric circuit section, 19...Light source, 20,
21... Light receiving element. Name of agent: Patent attorney Toshio Nakao and 1 other person11
a1 183 Zukyu 9 4th cause
Claims (1)
バと、上記屈折率分布型レンズから出て測定溶液中を透
過した透過光を第1の受光手段に導びく第2の光ファイ
バと、上記屈折率分布型レンズから出て測定溶液中で散
乱した散乱光を第2の受光手段に導びく第3の光ファイ
バとを具備して々る濁度測定装置。A second light beam that guides the light from the light source to a gradient index lens, and guides the transmitted light that has come out of the gradient index lens and passed through the measurement solution to a first light receiving means. A turbidity measuring device comprising a fiber and a third optical fiber that guides the scattered light emitted from the gradient index lens and scattered in the measurement solution to a second light receiving means.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56204420A JPS58103645A (en) | 1981-12-16 | 1981-12-16 | Measuring apparatus of turbidity |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56204420A JPS58103645A (en) | 1981-12-16 | 1981-12-16 | Measuring apparatus of turbidity |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPS58103645A true JPS58103645A (en) | 1983-06-20 |
Family
ID=16490240
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP56204420A Pending JPS58103645A (en) | 1981-12-16 | 1981-12-16 | Measuring apparatus of turbidity |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS58103645A (en) |
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| FR2583164A1 (en) * | 1985-06-06 | 1986-12-12 | Trapil Transports Petroliers P | METHOD AND DEVICE FOR DETERMINING THE COLOR AND TURBIDITY OF A FLUID |
| JPH02210247A (en) * | 1989-02-10 | 1990-08-21 | Asahi Eng Co Ltd | Measuring instrument for contamination degree of oil |
| CN114002168A (en) * | 2021-08-04 | 2022-02-01 | 河北雄安华清宏远环境科技有限公司 | A method and device for detecting liquid concentration with elimination of turbidity difference |
-
1981
- 1981-12-16 JP JP56204420A patent/JPS58103645A/en active Pending
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| FR2583164A1 (en) * | 1985-06-06 | 1986-12-12 | Trapil Transports Petroliers P | METHOD AND DEVICE FOR DETERMINING THE COLOR AND TURBIDITY OF A FLUID |
| JPH02210247A (en) * | 1989-02-10 | 1990-08-21 | Asahi Eng Co Ltd | Measuring instrument for contamination degree of oil |
| CN114002168A (en) * | 2021-08-04 | 2022-02-01 | 河北雄安华清宏远环境科技有限公司 | A method and device for detecting liquid concentration with elimination of turbidity difference |
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