JPH0249143A - Detector for liquid mixing ratio of mixed liquid - Google Patents
Detector for liquid mixing ratio of mixed liquidInfo
- Publication number
- JPH0249143A JPH0249143A JP20039488A JP20039488A JPH0249143A JP H0249143 A JPH0249143 A JP H0249143A JP 20039488 A JP20039488 A JP 20039488A JP 20039488 A JP20039488 A JP 20039488A JP H0249143 A JPH0249143 A JP H0249143A
- Authority
- JP
- Japan
- Prior art keywords
- light
- liquid
- receiving element
- wall surface
- transmitting body
- 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
- 239000007788 liquid Substances 0.000 title claims description 40
- 239000000203 mixture Substances 0.000 claims description 14
- 230000003247 decreasing effect Effects 0.000 claims description 3
- 239000000446 fuel Substances 0.000 abstract description 31
- 239000005308 flint glass Substances 0.000 abstract description 14
- 229920002050 silicone resin Polymers 0.000 abstract description 5
- 230000007423 decrease Effects 0.000 abstract description 2
- 239000011521 glass Substances 0.000 abstract description 2
- LFQSCWFLJHTTHZ-UHFFFAOYSA-N Ethanol Chemical compound CCO LFQSCWFLJHTTHZ-UHFFFAOYSA-N 0.000 description 7
- 239000003502 gasoline Substances 0.000 description 7
- 230000003287 optical effect Effects 0.000 description 4
- 230000000694 effects Effects 0.000 description 3
- 238000005516 engineering process Methods 0.000 description 3
- LRHPLDYGYMQRHN-UHFFFAOYSA-N N-Butanol Chemical compound CCCCO LRHPLDYGYMQRHN-UHFFFAOYSA-N 0.000 description 2
- 150000001298 alcohols Chemical class 0.000 description 2
- 238000002347 injection Methods 0.000 description 2
- 239000007924 injection Substances 0.000 description 2
- VNWKTOKETHGBQD-UHFFFAOYSA-N methane Chemical compound C VNWKTOKETHGBQD-UHFFFAOYSA-N 0.000 description 2
- 238000007789 sealing Methods 0.000 description 2
- 239000012780 transparent material Substances 0.000 description 2
- JBRZTFJDHDCESZ-UHFFFAOYSA-N AsGa Chemical compound [As]#[Ga] JBRZTFJDHDCESZ-UHFFFAOYSA-N 0.000 description 1
- 239000002028 Biomass Substances 0.000 description 1
- 229910001218 Gallium arsenide Inorganic materials 0.000 description 1
- BZLVMXJERCGZMT-UHFFFAOYSA-N Methyl tert-butyl ether Chemical compound COC(C)(C)C BZLVMXJERCGZMT-UHFFFAOYSA-N 0.000 description 1
- 230000032683 aging Effects 0.000 description 1
- 239000003034 coal gas Substances 0.000 description 1
- 238000002485 combustion reaction Methods 0.000 description 1
- 239000002131 composite material Substances 0.000 description 1
- 235000012489 doughnuts Nutrition 0.000 description 1
- 239000003822 epoxy resin Substances 0.000 description 1
- 239000002828 fuel tank Substances 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 239000003345 natural gas Substances 0.000 description 1
- 229920000647 polyepoxide Polymers 0.000 description 1
- 229920005989 resin Polymers 0.000 description 1
- 239000011347 resin Substances 0.000 description 1
- 230000035945 sensitivity Effects 0.000 description 1
- 125000006850 spacer group Chemical group 0.000 description 1
Landscapes
- Investigating Or Analysing Materials By Optical Means (AREA)
Abstract
Description
【発明の詳細な説明】
[産業上の利用分野]
本発明は、2種以上の異なる燃料を混合して利用するエ
ンジンの混合燃料比を光学的に検出する検出器に係り、
特にガソリンとアルコールの混合燃料の混合比の検出に
好適な検出器に関する。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a detector that optically detects the mixed fuel ratio of an engine that uses a mixture of two or more different fuels.
In particular, the present invention relates to a detector suitable for detecting the mixing ratio of a mixed fuel of gasoline and alcohol.
[従来の技術]
ガソリン代替燃料として天然ガス、石炭ガス、バイオマ
スより製造されるアルコール燃料をガソリンと混合させ
、既存の内燃機関に利用する試みが各方面で進められて
いる。このアルコール混合ガソリンはそのまま使用する
と、理論空燃比などの違いによりうまく運転できなかっ
たり、NOx、HC,Co等の発生を増加させたりする
ので、混合比を適宜検出して最適な噴射量を決定する必
要がある。[Prior Art] Attempts are being made in various fields to mix alcohol fuel produced from natural gas, coal gas, or biomass with gasoline as an alternative fuel to gasoline and use it in existing internal combustion engines. If this alcohol-mixed gasoline is used as is, it may not operate properly due to differences in the stoichiometric air-fuel ratio, etc., or it may increase the generation of NOx, HC, Co, etc., so the mixture ratio should be detected appropriately to determine the optimal injection amount. There is a need to.
この混合比を検出する技術として、この特許出願人は、
特願昭61−22578号(従来例1)、特願昭62−
43960号〈従来例2)等を提案している。これらの
技術では、ガソリンとアルコールの被測定液体の混合比
を、透光体と被測定液体との境界面での臨界角が変化す
ることを利用し、発光素子から出た光が、前記境界面で
全反射を起こし受光素子に戻ることにより、該受光素子
の入射光量の変化から求めていた。As a technology for detecting this mixing ratio, the patent applicant has
Patent Application No. 1983-22578 (Conventional Example 1), Patent Application No. 1982-
No. 43960 (Conventional Example 2) and the like are proposed. In these technologies, the mixing ratio of gasoline and alcohol to be measured is adjusted by using the fact that the critical angle at the interface between the transparent body and the measured liquid changes, and the light emitted from the light emitting element is It was determined from the change in the amount of light incident on the light receiving element by causing total reflection on the surface and returning to the light receiving element.
[発明が解決しようとする課題] しかるに、従来の技術では、次のような欠点があった。[Problem to be solved by the invention] However, the conventional technology has the following drawbacks.
(I)被測定液体中に気泡が存在した場合、受光素子の
出力値の変化量が非常に大きい(従来例1および2)。(I) When bubbles are present in the liquid to be measured, the amount of change in the output value of the light receiving element is very large (Conventional Examples 1 and 2).
(II)被測定液体の流路中に透光体を突出して配設す
る必要があり、透光体の取付け、シールがやり難い、ま
た、被測定液体が流れている場合は、流れを乱すことに
なり、気泡が発生しやすい(従来例1)。(II) It is necessary to place a transparent body protruding into the flow path of the liquid to be measured, which makes it difficult to attach and seal the transparent body, and if the liquid to be measured is flowing, it may disturb the flow. As a result, bubbles are likely to be generated (Conventional Example 1).
<III)発光素子と受光素子との間隔、受光素子の大
きさなどの寸法精度が要求される(従来例1.2)。<III) Dimensional accuracy is required in terms of the distance between the light emitting element and the light receiving element, the size of the light receiving element, etc. (Conventional Example 1.2).
本発明の目的は、被測定液体に気泡が存在する場合でも
、混合比の測定誤差が少ない、混合液体の液体混合比検
出器の提供にある。SUMMARY OF THE INVENTION An object of the present invention is to provide a liquid mixture ratio detector for a mixed liquid, which has a small error in measuring the mixture ratio even when bubbles are present in the liquid to be measured.
[課題を解決するための手段]
上記課題の達成のため、本発明は、2種以上の液体を混
合してなる被測定液体で溝たされたハウジングの内壁面
と面一的に配された第1の壁面を有する第1の透光体と
、該第1の透光体の他の壁面側に配された発光素子と、
該発光素子から前記第1の透光体への入射角を、設定入
射角以下の光のみに制限する入射角制限手段と、被測定
液体を隔てて前記第1の透光体と対向配置され、且つハ
ウジングの内壁面と面一的に配された第2の壁面を有す
る第2の透光体と、該第2の透光体の他の壁面側に配さ
れた受光素子と、前記第2の透光体の他の壁面側で且つ
、前記発光素子に近い側に配された補償用の受光素子と
を備え、前記透光体の形状と、入射角制限手段、発光素
子、受光素子および補償用の受光素子との取付は位置と
の関係は、(イ)発光素子からの光は、第1の透光体中
を進行し、前記入射角制限手段により設定入射角以下と
なり、前記第1の透光体の第1の壁面と被測定液体との
境界面で屈折し、被測定液体中を進行し、被測定液体と
第2の透光体との境界面で屈折し、前記第2の透光体中
を進行した光が前記受光素子に入射し、該受光素子の出
力は前記被測定液体の屈折率に応じて増減されるように
設定され、(口〉被測定液体の屈折率の全範囲にわたっ
て、前記入射角制限手段により制限された入射光の最大
の入射角の光を受光素子に入射させるように設定され、
(ハ)補償用の受光素子は、屈折光を常に受け、その出
力が一定となるように発光素子の光量の制御を行う構成
を採用した。[Means for Solving the Problems] In order to achieve the above-mentioned problems, the present invention provides a housing that is disposed flush with the inner wall surface of a housing grooved with a liquid to be measured which is a mixture of two or more types of liquids. a first light transmitting body having a first wall surface; a light emitting element disposed on the other wall surface side of the first light transmitting body;
an incident angle limiting means for limiting an incident angle from the light emitting element to the first light transmitting body to only light that is equal to or less than a set incident angle; , a second light transmitting body having a second wall surface disposed flush with the inner wall surface of the housing; a light receiving element disposed on the other wall surface side of the second light transmitting body; a compensating light-receiving element disposed on the other wall surface side of the light-transmitting body of No. 2 and on the side closer to the light-emitting element; The relationship between the mounting position and the compensation light-receiving element is as follows: (a) The light from the light-emitting element travels through the first transparent body, and the incident angle becomes equal to or less than the set incident angle by the incident angle limiting means. It is refracted at the interface between the first wall surface of the first transparent body and the liquid to be measured, travels through the liquid to be measured, is refracted at the boundary between the liquid to be measured and the second transparent body, and the The light traveling through the second transparent body is incident on the light receiving element, and the output of the light receiving element is set to be increased or decreased according to the refractive index of the liquid to be measured. It is set so that light at the maximum incident angle of the incident light limited by the incident angle limiting means is made incident on the light receiving element over the entire range of refractive index,
(c) The compensating light-receiving element always receives refracted light, and the light intensity of the light-emitting element is controlled so that its output is constant.
[作用および発明の効果] 本発明は、つぎの作用および効果を有する。[Action and effect of invention] The present invention has the following functions and effects.
■被測定液体に気泡が存在する場合、該気泡を通った光
は、多くの場合、気泡を通過する範囲の光が、そのまま
受光素子に入射する位置がずれるのみで、受光素子の受
光量に変化は生じない、よって、被測定液体に気泡が存
在する場合でも、混合比の測定誤差が少ない。■If there are bubbles in the liquid to be measured, in most cases, the light that passes through the bubbles will simply shift the position of the light that passes through the bubbles, and the amount of light received by the light-receiving element will change. No change occurs. Therefore, even if bubbles are present in the liquid to be measured, there is little error in measuring the mixing ratio.
■検出器は、ハウジングの内壁面と面一的に配されるの
で、透光体の取付けやすさおよびシール性に優れる。ま
た、被測定液体が流れている場合は、その流れを乱さな
いため気泡が発生し難い。■Since the detector is arranged flush with the inner wall surface of the housing, it is easy to attach the transparent body and has excellent sealing performance. Furthermore, when the liquid to be measured is flowing, bubbles are less likely to occur because the flow is not disturbed.
0発光素子や受光素子の位置や間隔、受光素子の大きさ
などについて精密な寸法を要求されない。0 Precise dimensions are not required for the position and spacing of the light-emitting element and the light-receiving element, the size of the light-receiving element, etc.
[実施例]
つぎに本発明を第1図および第2図に示す一実施例に基
づき説明する。[Example] Next, the present invention will be explained based on an example shown in FIGS. 1 and 2.
本発明の混合液体の液体混合比検出器Aは、第1図に示
すように、フリントガラス1.2をパイプ90の内壁面
91と面一的に配し、壁面11.21をガソリン・アル
コール混合燃料92に晒し、他の壁面12側には、発光
ダイオード3およびマスク4を配し、別の他の端面22
側には、出力用ホトダイオード5および補償用ホトダイ
オード6を配してなる。また、パイプ90は、混合燃料
タンクとプレッシャレギュレータ(いずれも図示せず)
とを連結するパイプである。As shown in FIG. 1, the liquid mixture ratio detector A for mixed liquids of the present invention has a flint glass 1.2 disposed flush with the inner wall surface 91 of the pipe 90, and the wall surface 11.21 is arranged flush with the inner wall surface 91 of the pipe 90. A light emitting diode 3 and a mask 4 are arranged on the other wall surface 12 side exposed to the mixed fuel 92, and another end surface 22 is exposed to the mixed fuel 92.
An output photodiode 5 and a compensation photodiode 6 are arranged on the side. The pipe 90 also connects a mixed fuel tank and a pressure regulator (both not shown).
It is a pipe that connects the
フリントガラス1.2は、円板状の屈折率1゜55の透
光体で、前記パイプ90に貫いて形成された切削孔93
に液密的に固定されている。The flint glass 1.2 is a disc-shaped transparent material with a refractive index of 1°55, and has a cut hole 93 formed through the pipe 90.
is fixed in a liquid-tight manner.
発光ダイオード3は、ガリウム砒素型で赤外光を発光さ
せている。この発光ダイオード3は、透光性のシリコン
樹脂31でモールドされ、前記切削孔93内に、スペー
サ94および蓋板95により固着されている。赤外光3
2は、混合燃料92の屈折率が最大の時は、光路33と
なり、最小の時は、光路34となる。The light emitting diode 3 is of the gallium arsenide type and emits infrared light. The light emitting diode 3 is molded with a transparent silicone resin 31 and is fixed in the cut hole 93 with a spacer 94 and a cover plate 95. Infrared light 3
2 becomes the optical path 33 when the refractive index of the mixed fuel 92 is maximum, and becomes the optical path 34 when it is the minimum.
マスク4は、略ドーナツ状を呈する遮光材で形成され前
記フリントガラス1の他の壁面12とシリコン樹脂31
の内側端との間に周設されている。The mask 4 is formed of a light-shielding material and has a substantially donut shape, and is connected to the other wall surface 12 of the flint glass 1 and the silicone resin 31.
and the inner edge of the inner edge.
また、このマスク4は、混合燃料92が屈折率最小のと
きく第1図中点線で示す光路34の光路より図示上方)
でも前記出力用ホトダイオード5から入射光が端51か
らはみ出さないように制限している。Furthermore, this mask 4 is located above the optical path 34 shown by the dotted line in FIG. 1 when the mixed fuel 92 has the minimum refractive index).
However, the incident light from the output photodiode 5 is restricted so that it does not protrude from the end 51.
出力用ホトダイオード5は、発光ダイオード3から出た
赤外光32がシリコン樹脂31、フリントガラス1中を
進行し、前記マスク4より設定入射角以下となり、前記
フリントガラス1の壁面11と混合燃料92との境界面
で屈折し、混合燃料92中を進行し、混合燃料92とフ
リントガラス2との境界面で屈折し、フリントガラス2
中を進行して入射が行われる。また、出力用ホトダイオ
ード5の出力は前記混合燃料92の屈折率に応じて増減
される。In the output photodiode 5, the infrared light 32 emitted from the light emitting diode 3 travels through the silicone resin 31 and the flint glass 1, becomes less than the set incident angle from the mask 4, and reaches the wall surface 11 of the flint glass 1 and the mixed fuel 92. The mixed fuel 92 is refracted at the interface between the flint glass 2 and the flint glass 2.
Injection is performed by proceeding inside. Further, the output of the output photodiode 5 is increased or decreased depending on the refractive index of the mixed fuel 92.
補償用ホトダイオード6は、赤外光35を常に受け、(
あ)発光ダイオード3や出力用ホトダイオード5の感度
が温度により変化すること、(い)発光ダイオード3か
らの光量が該発光ダイオード3の経時変化やフリントガ
ラス1.2の汚れなどにより減少することを補償するた
めに配設されている。前記(あ)、(い)は、補償用ホ
トダイオード6の出力が一定となるように発光ダイオー
ド3の通電量の制御を行って補償される。また混合燃料
92の屈折率が約−4X 10−’/’Cで変化するこ
との補償は発光ダイオード3の電圧降下の温度特性を利
用することにより成される。The compensation photodiode 6 always receives infrared light 35 and (
A) The sensitivity of the light emitting diode 3 and the output photodiode 5 changes depending on the temperature, and (b) The amount of light from the light emitting diode 3 decreases due to aging of the light emitting diode 3, dirt on the flint glass 1.2, etc. It is arranged to compensate. The above (a) and (b) are compensated by controlling the amount of current flowing through the light emitting diode 3 so that the output of the compensation photodiode 6 is constant. Further, compensation for the fact that the refractive index of the mixed fuel 92 changes by approximately -4×10-'/'C is achieved by utilizing the temperature characteristics of the voltage drop of the light emitting diode 3.
本実施例の混合液体の液体混合比検出器Aは、つぎの作
用および効果を有する。The liquid mixture ratio detector A of the present embodiment has the following functions and effects.
■第2図に示すように混合燃料92中に気泡96が存在
する場合、多くの場合、気泡96を通過する範囲の光(
例えば赤外光32)が、そのまま出力用のホトダイオー
ド5に入射する位置がずれる(光路36となる)のみで
、出力用ホトダイオード5の出力の変化は極小である。■When air bubbles 96 exist in the mixed fuel 92 as shown in FIG.
For example, the change in the output of the output photodiode 5 is minimal, simply by shifting the position where the infrared light 32) directly enters the output photodiode 5 (to form an optical path 36).
よって、混合燃料92に気泡96が存在する場合でも、
混合比の測定誤差が少ない。Therefore, even if there are bubbles 96 in the mixed fuel 92,
There is little error in measuring the mixing ratio.
■検出器Aは、パイプ90の内壁面91と面一的に配さ
れるので、フリントガラス1.2の取付けやすさおよび
シール性に優れる。また、混合燃料92の流れを乱さな
いため気泡96が発生し難い。(2) Since the detector A is arranged flush with the inner wall surface 91 of the pipe 90, it is easy to attach the flint glass 1.2 and has excellent sealing performance. Furthermore, since the flow of the mixed fuel 92 is not disturbed, bubbles 96 are less likely to occur.
■屈折率により混合燃料92の混合比を検出しているの
で各素子の位置や間隔、大きさなどについて精密な寸法
を要求されない。(2) Since the mixture ratio of the mixed fuel 92 is detected by the refractive index, precise dimensions such as the position, spacing, and size of each element are not required.
本発明は、上記実施例以外に次の実施態様を含む。The present invention includes the following embodiments in addition to the above embodiments.
a、ハウジングの内壁面と面一的に配するとは、多少、
第1、第2の透光体がハウジングの内壁面とずれている
場合を含む。a. Placing it flush with the inner wall surface of the housing means that
This includes a case where the first and second light-transmitting bodies are misaligned with the inner wall surface of the housing.
b、2種以上の液体とは、混合比が変化する液体が任意
の2種であり、燃料以外の液体であっても良く、流れの
方向性は自由であり、また、静止状態であっても良い。b. Two or more types of liquids are any two types of liquids whose mixing ratio changes, may be liquids other than fuel, have free direction of flow, and are in a stationary state. Also good.
C1上記実施例で使用する混合燃料92は、エタノール
、MTBE、ブタノール、その他高級アルコールを含む
複合アルコールと、ガソリンとの混合液体、上記アルコ
ール類と、軽油との混合液体であっても良い。C1 The mixed fuel 92 used in the above embodiment may be a liquid mixture of gasoline and a composite alcohol containing ethanol, MTBE, butanol, or other higher alcohols, or a liquid mixture of the above alcohols and light oil.
60発光素子、受光素子が使用する光は、単光色が望ま
しく、波長は特に限定されない。The light used by the 60 light-emitting element and the light-receiving element is preferably of a single color, and the wavelength is not particularly limited.
e、シリコン樹脂は透光体であれば良く、例えばエポキ
シ樹脂などでも良い。e. The silicone resin may be any transparent material, such as epoxy resin.
f、透光体は、フリントガラスのようなガラスだけでは
なく、被測定液体に冒されなければ透明な樹脂でも良い
。f. The light transmitting body is not limited to glass such as flint glass, but may also be a transparent resin as long as it is not affected by the liquid to be measured.
第1図は本発明の混合液体の液体混合比検出器の一実施
例を示し、混合燃料が流れるパイプ内に貫いて配設され
た状態を示す断面図、第2図は、その実施例において混
合燃料中に気泡が存在する場合の検出器の作動を説明す
るための断面図である。
図中 1・・・フリントガラス(第1の透光体)2・・
・フリントガラス(第2の透光体) 3・・・発光ダイ
オード(発光素子) 4・・・マスク(入射角制限手段
) 5・・・出力用のホトダイオード(受光素子) 6
・・・補償用のホトダイオード(補償用の受光素子)1
1・・・壁面(第1の壁面) 12.22・・・他の壁
面 21・・・壁面(第2の壁面> 90・・・パイ
プ(ハウジング)91・・・内壁面 92・・・ガソリ
ン・アルコール混合燃料 A・・・混合液体の液体混合
比検出器FIG. 1 shows an embodiment of the liquid mixture ratio detector for mixed liquid of the present invention, and is a cross-sectional view showing the state in which it is installed through a pipe through which mixed fuel flows, and FIG. FIG. 3 is a cross-sectional view for explaining the operation of the detector when bubbles are present in the mixed fuel. In the figure 1...Flint glass (first transparent body) 2...
・Flint glass (second transparent body) 3... Light emitting diode (light emitting element) 4... Mask (incident angle limiting means) 5... Photodiode for output (light receiving element) 6
...Compensation photodiode (compensation light receiving element) 1
1...Wall surface (first wall surface) 12.22...Other wall surface 21...Wall surface (second wall surface>90...Pipe (housing) 91...Inner wall surface 92...Gasoline・Alcohol mixed fuel A...Liquid mixture ratio detector for mixed liquid
Claims (1)
れたハウジングの内壁面と面一的に配された第1の壁面
を有する第1の透光体と、 該第1の透光体の他の壁面側に配された発光素子と、 該発光素子から前記第1の透光体への入射角を、設定入
射角以下の光のみに制限する入射角制限手段と、 被測定液体を隔てて前記第1の透光体と対向配置され、
且つハウジングの内壁面と面一的に配された第2の壁面
を有する第2の透光体と、 該第2の透光体の他の壁面側に配された受光素子と、 前記第2の透光体の他の壁面側で且つ、前記発光素子に
近い側に配された補償用の受光素子とを備え、 前記透光体の形状と、入射角制限手段、発光素子、受光
素子および補償用の受光素子との取付け位置との関係は
、 (イ)発光素子からの光は、第1の透光体中を進行し、
前記入射角制限手段により設定入射角以下となり、前記
第1の透光体の第1の壁面と被測定液体との境界面で屈
折し、被測定液体中を進行し、被測定液体と第2の透光
体との境界面で屈折し、前記第2の透光体中を進行した
光が前記受光素子に入射し、該受光素子の出力は前記被
測定液体の屈折率に応じて増減されるように設定され、
(ロ)被測定液体の屈折率の全範囲にわたって、前記入
射角制限手段により制限された入射光の最大の入射角の
光を受光素子に入射させるように設定され、 (ハ)補償用の受光素子は、屈折光を常に受け、その出
力が一定となるように発光素子の光量の制御を行う混合
液体の液体混合比検出器。[Scope of Claims] 1) A first light-transmitting body having a first wall surface disposed flush with an inner wall surface of a housing filled with a liquid to be measured which is a mixture of two or more types of liquids; , a light emitting element disposed on the other wall side of the first light transmitting body, and an incident angle that limits the incident angle from the light emitting element to the first light transmitting body to only light that is equal to or less than a set incident angle. a restricting means, disposed facing the first transparent body across the liquid to be measured,
and a second light transmitting body having a second wall surface disposed flush with the inner wall surface of the housing; a light receiving element disposed on the other wall surface side of the second light transmitting body; and a compensating light-receiving element disposed on the other wall side of the light-transmitting body and on the side closer to the light-emitting element, and the shape of the light-transmitting body, the incident angle limiting means, the light-emitting element, the light-receiving element, and The relationship between the mounting position and the compensation light-receiving element is as follows: (a) The light from the light-emitting element travels through the first transparent body,
The incident angle becomes equal to or less than the set angle by the incident angle limiting means, is refracted at the interface between the first wall surface of the first light-transmitting body and the liquid to be measured, and travels through the liquid to be measured. The light that is refracted at the interface with the second light-transmitting body and travels through the second light-transmitting body enters the light-receiving element, and the output of the light-receiving element is increased or decreased according to the refractive index of the liquid to be measured. is set to
(b) It is set so that light with the maximum angle of incidence of the incident light limited by the incident angle limiting means is made incident on the light receiving element over the entire range of the refractive index of the liquid to be measured, and (c) Light reception for compensation The element is a liquid mixture ratio detector for a mixed liquid that constantly receives refracted light and controls the amount of light from the light emitting element so that its output remains constant.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP20039488A JPH0249143A (en) | 1988-08-11 | 1988-08-11 | Detector for liquid mixing ratio of mixed liquid |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP20039488A JPH0249143A (en) | 1988-08-11 | 1988-08-11 | Detector for liquid mixing ratio of mixed liquid |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH0249143A true JPH0249143A (en) | 1990-02-19 |
Family
ID=16423593
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP20039488A Pending JPH0249143A (en) | 1988-08-11 | 1988-08-11 | Detector for liquid mixing ratio of mixed liquid |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH0249143A (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2007171182A (en) * | 2005-12-22 | 2007-07-05 | Palo Alto Research Center Inc | Supplying light to the channel or its components |
US9638637B2 (en) | 2007-01-26 | 2017-05-02 | Palo Alto Research Center Incorporated | Method and system implementing spatially modulated excitation or emission for particle characterization with enhanced sensitivity |
-
1988
- 1988-08-11 JP JP20039488A patent/JPH0249143A/en active Pending
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2007171182A (en) * | 2005-12-22 | 2007-07-05 | Palo Alto Research Center Inc | Supplying light to the channel or its components |
US9638637B2 (en) | 2007-01-26 | 2017-05-02 | Palo Alto Research Center Incorporated | Method and system implementing spatially modulated excitation or emission for particle characterization with enhanced sensitivity |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
KR910004217B1 (en) | Alcohol content detection device | |
JPS62192633A (en) | Mixing ratio sensor for alcohol mixed fuel | |
KR940002500B1 (en) | Apparatus for detecting alcohol concentration | |
EP0370807B1 (en) | A liquid mixture ratio detector device | |
US4895444A (en) | Detector device for mixing ratio for gasoline and alcohol or the like | |
JPH0249143A (en) | Detector for liquid mixing ratio of mixed liquid | |
JPH04169839A (en) | Alcohol-content detecting apparatus | |
JPH0249144A (en) | Detector for liquid mixing ratio of mixed liquid | |
JPH0526992Y2 (en) | ||
JPH01263536A (en) | Apparatus of detecting content ratio of alcohol | |
JPH02107948A (en) | Liquid mixing ratio detector for mixed liquid | |
JPH0222540A (en) | Detector for liquid mixing ratio of liquid mixture | |
JPH02141645A (en) | Detector of mixing ratio of mixed liquid | |
JPH0282138A (en) | Liquid mixing ratio detector for mixed liquid | |
JPH0222538A (en) | Device for detecting mixing ratio in liquid mixture | |
JPS62276438A (en) | Mixing ratio sensor for alcohol mixed fuel | |
JPH0452679Y2 (en) | ||
JPS62127646A (en) | Sensor for gasoline-alcohol mixture ratio | |
JPH0440343A (en) | Alcohol content detecting device | |
JPS62127645A (en) | Sensor for gasoline-alcohol mixture ratio | |
JPH0298654A (en) | Detector for mixing rate of liquid mixture | |
JPH0534283A (en) | Liquid property detecting apparatus | |
JPH01262442A (en) | Alcohol content detector | |
JPH03233347A (en) | Detector for alcohol content | |
JPS63210645A (en) | Mixing ratio detector for fluid such as gasoline-alcohol |