JPH02218940A - Detector of liquid mixture rate - Google Patents

Detector of liquid mixture rate

Info

Publication number
JPH02218940A
JPH02218940A JP4000889A JP4000889A JPH02218940A JP H02218940 A JPH02218940 A JP H02218940A JP 4000889 A JP4000889 A JP 4000889A JP 4000889 A JP4000889 A JP 4000889A JP H02218940 A JPH02218940 A JP H02218940A
Authority
JP
Japan
Prior art keywords
light
emitting element
incident
liquid
peripheral wall
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
JP4000889A
Other languages
Japanese (ja)
Inventor
Shigeru Miyata
繁 宮田
Kiyotaka Ono
大野 清隆
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.)
Niterra Co Ltd
Original Assignee
NGK Spark Plug Co Ltd
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 NGK Spark Plug Co Ltd filed Critical NGK Spark Plug Co Ltd
Priority to JP4000889A priority Critical patent/JPH02218940A/en
Priority to US07/438,513 priority patent/US4962746A/en
Priority to EP89312161A priority patent/EP0370807B1/en
Priority to DE8989312161T priority patent/DE68901644D1/en
Publication of JPH02218940A publication Critical patent/JPH02218940A/en
Pending legal-status Critical Current

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  • Investigating Or Analysing Materials By Optical Means (AREA)

Abstract

PURPOSE:To compact a light emitting element by making constitution wherein light from the light emitting element is incident to a light transmission body via a filler and it is reflected on a border surface and outgoes from a peripheral wall when its angle is a critical angle determined by the light transmission body and liquid to be measured or larger. CONSTITUTION:Light from a light emitting element 4 which comes against a light path 41 proceeds in silicon gel 3 and is incident in a glass pillar 2 while the incident angle to a border surface 21 is always a critical angle determined by the glass pillar 2 and mixed fuel 510 or larger, and the light is fully reflected on this critical surface 21, proceeds in the glass column 2, outgoes from a peripheral wall 23 and is incident into a compensating diode 6. Light from the light emitting element 4 which comes against a light path 42 proceeds in the gel 3 and is incident into the glass pillar 2, while the incident angle to the border surface 21 is the critical angle determined by the glass pillar 2 and the fuel 510, and it is fully reflected on the border surface 21, outgoes from the peripheral wall 23 into the gel 3 and is incident into an outputting photo diode 5. A range 43 refers to a light receiving area in a current mixture rate of gasoline and alcohol of the fuel 510, and when the mixture rate varies and the critical angle increases, the light path 42 comes close to the light path 41, thereby narrowing the range 43.

Description

【発明の詳細な説明】 [産業上の利用分野] 本発明は、少なくとも2種類の物質を混合してなる被測
定液体の混合比を検出する検出器に係わり、特にガソリ
ンとアルコールと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 for detecting the mixing ratio of a liquid to be measured which is a mixture of at least two types of substances, and particularly relates to a detector for detecting the mixing ratio of a liquid to be measured consisting of a mixture of at least two types of substances, and particularly to a detector that detects the mixing ratio of a liquid to be measured which is a mixture of at least two types of substances. The present invention relates to a detector suitable for detecting.

[従来の技術] 近年、自動車の内燃機関において、ガソリン代用燃料と
して、ガソリン・アルコール混合燃料を用いることが考
えられている。しかし、そのまま使用すると理論空燃比
などの違いにより、スムーズに運転できない。このため
、ガソリンとアルコールとの混合比を検出する検出器が
必要となってくる。従来の技術として例えば、実開昭6
2−121547号公報には、第6図に示すように、混
合燃料110との境界面210を有する三角プリズム2
00を配し、他の二面に発光素子300、受光素子40
0を取付けてなる検出器りが記載されている。
[Prior Art] In recent years, it has been considered to use a gasoline/alcohol mixed fuel as a gasoline substitute fuel in an automobile internal combustion engine. However, if used as is, it will not run smoothly due to differences in the stoichiometric air-fuel ratio, etc. Therefore, a detector is required to detect the mixing ratio of gasoline and alcohol. For example, as a conventional technology,
2-121547, as shown in FIG. 6, a triangular prism 2 having an interface 210 with a mixed fuel 110 is disclosed.
00, and a light emitting element 300 and a light receiving element 40 are arranged on the other two sides.
A detector equipped with 0 is described.

[発明が解決しようとする課題] しかるに、この検出器りはつぎのような欠点がある。■
三角プリズムを使用しているので材料代が高くなる。■
温度補償や発光ダイオードの経時変化の補償が不十分で
あり、精度が悪い。このため、この特許出願人は、つぎ
に述べる検出器Cを特願昭63−295478号で提案
している。
[Problems to be Solved by the Invention] However, this detector has the following drawbacks. ■
Since a triangular prism is used, the material cost is high. ■
Temperature compensation and compensation for changes in light emitting diodes over time are insufficient, resulting in poor accuracy. For this reason, the applicant of this patent proposed the following detector C in Japanese Patent Application No. 63-295478.

第5図に示すように、検出器Cは、ガソリン・メタノー
ル600に境界面710が接する円板状ガラス700を
設置し、該ガラス700の側面の外側に発光ダイオード
810と、ホトダイオード820.830とを対向配置
している。
As shown in FIG. 5, the detector C includes a disk-shaped glass 700 whose interface 710 is in contact with gasoline/methanol 600, and a light-emitting diode 810 and a photodiode 820, 830 on the outside of the side surface of the glass 700. are placed facing each other.

しかし、この検出器Cでもつぎの課題がある。However, this detector C also has the following problem.

(あ)ガラス700の軸方向の厚みが厚くなり、ガラス
700の重量増大を招く。
(A) The thickness of the glass 700 in the axial direction increases, leading to an increase in the weight of the glass 700.

(い)ホトダイオード820へ入射する光の範囲が広い
ので受光面積の大きいものを使用する必要が生じる。
(b) Since the range of light incident on the photodiode 820 is wide, it is necessary to use one with a large light-receiving area.

本発明の目的は、透光体の重量の低減および受光素子の
小型化が図られた液体混合比検出器の提供にある。
An object of the present invention is to provide a liquid mixture ratio detector in which the weight of the light transmitting body is reduced and the light receiving element is miniaturized.

[課題を解決するための手段] 上記目的の達成のため本発明は、つぎの構成を採用した
。
[Means for Solving the Problems] To achieve the above object, the present invention employs the following configuration.

■柱状を呈するとともに、少なくとも2種類の物質を混
合してなる被測定液体に浸される境界面を有する透光体
と、該透光体を保持するホルダと、前記透光体の周壁側
の任意位置に配される発光素子と、前記透光体を挟んで
前記発光素子と対向的に配される少なくとも一つの受光
素子と、前記透光体と、発光素子および受光素子との間
に配される液状またはゲル状の透光性を有する充填材と
からなる液体混合比検出器において、前記発光素子から
発光した光は前記充填材中を進み透光体に入射し、透光
体中を進み、透光体と被測定液体とにより決まる臨界角
以上の場合前記境界面で全反射し、透光体中を進み、前
記周壁または前記境界面と対向する端面から出射するよ
うに、前記柱状透光体の形状および受光素子の取り付け
位置が決められている。
(1) A light-transmitting body having a columnar shape and having a boundary surface immersed in a liquid to be measured made of a mixture of at least two types of substances, a holder for holding the light-transmitting body, and a peripheral wall side of the light-transmitting body; a light emitting element disposed at an arbitrary position, at least one light receiving element disposed opposite to the light emitting element with the light transmitting body in between, and a light receiving element disposed between the light transmitting body and the light emitting element and the light receiving element. In a liquid mixture ratio detector comprising a liquid or gel-like light-transmitting filler, the light emitted from the light-emitting element travels through the filler, enters the light-transmitting body, and enters the light-transmitting body. The columnar light beam travels through the light transmitting body, is totally reflected at the boundary surface when the angle is equal to or greater than a critical angle determined by the light transmitting body and the liquid to be measured, travels through the light transmitting body, and is emitted from the peripheral wall or the end face opposite to the boundary surface. The shape of the transparent body and the mounting position of the light receiving element are determined.

■前記■の構成を有し、かつ、充填材は透光体より屈折
率が小さく、境界面への入射角が、少なくとも透光体と
充填材とにより決まる臨界角以上のものについては、境
界面で反射の後、周壁から出射する。
■If the structure of ■ is mentioned above, and the filler has a smaller refractive index than the transparent material, and the angle of incidence on the boundary surface is at least equal to or greater than the critical angle determined by the transparent material and the filler, the boundary After being reflected by the surface, it is emitted from the surrounding wall.

[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奏する。[Action and effect of invention] The present invention has the following functions and effects.

〈請求項1について〉 発光素子から発光した光は充填材中を進み透光体に入射
し、透光体中を進み、透光体と被測定液体とにより決ま
る臨界角以上の場合前記境界面で全反射し、透光体中を
進み、周壁または境界面と対向する端面から出射するよ
うに、透光体の形状および受光素子の取り付け位置が決
められている。
<Regarding Claim 1> The light emitted from the light-emitting element travels through the filler, enters the light-transmitting body, travels through the light-transmitting body, and when the angle is equal to or greater than a critical angle determined by the light-transmitting body and the liquid to be measured, the light emitted from the boundary surface The shape of the light-transmitting body and the mounting position of the light-receiving element are determined so that the light is totally reflected at the light-transmitting body, travels through the light-transmitting body, and is emitted from the end face facing the peripheral wall or boundary surface.

このため、境界面で全反射した光を全て透光体の周壁側
から充填材中へ出射させる必要はないので透光体の軸方
向の厚みを薄くすることができる。
Therefore, it is not necessary to emit all of the light totally reflected at the boundary surface from the peripheral wall side of the light-transmitting body into the filler, so that the thickness of the light-transmitting body in the axial direction can be reduced.

よって、透光体を軽くする。ことができ、ホルダとの保
持強度が軽くなった分だけ有利となる。
Therefore, the light-transmitting body is made lighter. This is advantageous because the holding strength with the holder is reduced.

く請求項2について〉 ■充填材は透光体より屈折率が小さい。このため第2図
に示すように、透光体の端面から充填材中に出射する際
、光路に示すように曲げられる。よって、被個定液体の
屈折率の増減に伴う受光素子に入射する軸方向の光の広
がりは抑えられ受光素子は受光面積の小さなものが使用
できる。
Regarding Claim 2> (1) The filler has a smaller refractive index than the transparent material. Therefore, as shown in FIG. 2, when the light is emitted from the end face of the transparent body into the filler, the optical path is bent as shown. Therefore, the spread of light incident on the light receiving element in the axial direction due to an increase or decrease in the refractive index of the liquid to be identified is suppressed, and a light receiving element with a small light receiving area can be used.

■境界面への入射角が、少なくとも、透光体と充填材と
により決まる臨界角以上のものについては、境界面で反
射の後、周壁から出射するように規定しているのは、境
界面と対向する端面で反射を起こさないようにするため
である。
■If the incident angle to the boundary surface is at least equal to or greater than the critical angle determined by the transparent material and the filling material, it is specified that the incident light is emitted from the peripheral wall after being reflected at the boundary surface. This is to prevent reflection from occurring at the end face facing the .

[実施例] つぎに、本発明の第1実施例(請求項1および2)を第
1図に基づき説明する。
[Example] Next, a first example (claims 1 and 2) of the present invention will be described based on FIG.

第1図のごとく、ガソリン・アルコール混合比検出器A
は、底部に円形孔11が開けられた金属ホルダと1と、
前記円形孔11内に遊嵌されるガラス柱2と、ホルダ1
内に入れられたシリコンゲル3と、該シリコンゲル中に
配される発光ダイオード4、出力用ホトダイオード5、
補償用ホトダイオード6と、ガラス柱2とホルダ1とを
接合する接着用ガラスリング7とからなる。また、この
検出器Aは、ガソリン・メタノール混合燃料510(屈
折率1.33〜1.43)が流れるパイプ500の穿設
孔520に、Oリング530を介して取付けられている
。
As shown in Figure 1, gasoline/alcohol mixture ratio detector A
1, a metal holder with a circular hole 11 in the bottom;
A glass column 2 loosely fitted into the circular hole 11 and a holder 1
a silicon gel 3 placed inside, a light emitting diode 4 disposed in the silicon gel, an output photodiode 5,
It consists of a compensation photodiode 6 and an adhesive glass ring 7 that joins the glass column 2 and holder 1 together. Further, this detector A is attached via an O-ring 530 to a perforated hole 520 of a pipe 500 through which a gasoline/methanol mixed fuel 510 (refractive index of 1.33 to 1.43) flows.

金属ホルダ1はステンレス鋼で形成されている。The metal holder 1 is made of stainless steel.

また、円形孔11の周面と前記ガラス柱2との間には前
記ガラスリング7用の等幅の環状スペースが設けられて
いる。金属ホルダ1の底面1.2には樹脂円筒13が固
着されている。
Further, an annular space of equal width for the glass ring 7 is provided between the circumferential surface of the circular hole 11 and the glass column 2. A resin cylinder 13 is fixed to the bottom surface 1.2 of the metal holder 1.

ガラス柱2は、直径8mm、長さ2.5mmのフリント
ガラス(M折率1.58)の円柱体である。21は前記
混合燃料510に浸されるとともに全反射が行われる境
界面、22は該境界面21と対向する端面、23はガラ
スリング7の内壁と接する周壁である。
The glass column 2 is a cylindrical body of flint glass (M refractive index 1.58) with a diameter of 8 mm and a length of 2.5 mm. Reference numeral 21 indicates a boundary surface which is immersed in the mixed fuel 510 and undergoes total reflection, 22 is an end surface opposite to the boundary surface 21, and 23 is a peripheral wall in contact with the inner wall of the glass ring 7.

シリコンゲル3は、屈折率1.40で透光性を有する充
填材である。また、このシリコンゲル3は前記樹脂円筒
13の上方開口付近まで金属ホルダ1内に入れられてい
る。
The silicon gel 3 is a filler that has a refractive index of 1.40 and is transparent. Further, this silicone gel 3 is placed in the metal holder 1 up to the vicinity of the upper opening of the resin cylinder 13.

発光ダイオード4は、樹脂円筒13の内壁で、かつ前記
端面22の延長線よりやや下方位置に配されている。
The light emitting diode 4 is arranged on the inner wall of the resin cylinder 13 at a position slightly below the extension line of the end surface 22.

出力用ホトダイオード5は、樹脂円筒13の内壁で、か
つ前記端面22の延長線を跨いで配されている。
The output photodiode 5 is arranged on the inner wall of the resin cylinder 13 and across the extension line of the end surface 22 .

補償用ホトダイオード6は、樹脂円筒13の内壁で、か
つ前記端面22の延長線より下方位置に配されている。
The compensation photodiode 6 is disposed on the inner wall of the resin cylinder 13 and below the extension line of the end surface 22 .

接着用ガラスリング7は、肉厚llnm、高さ1mmの
フリントガラスで形成され、軟化温度が前記ガラス柱2
より低いものである。このガラスリング7は、前記混合
燃料510に浸される境界面21を突出させてガラス柱
2を接着している。
The adhesive glass ring 7 is made of flint glass with a wall thickness of 1 nm and a height of 1 mm, and has a softening temperature equal to that of the glass column 2.
It is lower. This glass ring 7 has a protruding boundary surface 21 immersed in the mixed fuel 510 and adheres to the glass column 2 .

つぎに第2図とともに光路の説明をする。Next, the optical path will be explained with reference to FIG.

発光素子4から発光した光で、光路41にあたる光は、
シリコンゲル3中を進みガラス柱2に入射し、ガラス柱
2中を進み、境界面21への入射角は常にガラス柱2と
混合燃料510とにより決まる臨界角以上であり、この
境界面21で全反射し、ガラス柱2中を進み、周壁23
からシリコンゲル3中へ出射し、シリコンゲル3を進み
補償用ホトダイオード6へ入射する。
The light emitted from the light emitting element 4 and falling on the optical path 41 is
It travels through the silicon gel 3 and enters the glass column 2, and the incident angle at the boundary surface 21 is always greater than or equal to the critical angle determined by the glass column 2 and the mixed fuel 510, and at this boundary surface 21. It is totally reflected, travels through the glass column 2, and reaches the surrounding wall 23.
The light is emitted into the silicon gel 3, travels through the silicon gel 3, and enters the compensation photodiode 6.

発光ダイオード4から発光した光で、光路42にあたる
光は、シリコンゲル3中を進みガラス柱2に入射し、ガ
ラス柱2中を進み境界面21への入射角はちょうどガラ
ス柱2と混合燃料510とにより決まる臨界角であり、
この境界面21で全反射し、ガラス柱2中を進み、周壁
23からシリコンゲル3中へ出射し、シリコンゲル3を
進み出力用ホトダイオード5へ入射する。なお、範囲4
3がガソリン・アルコール混合燃料510のガソリンと
アルコールの現在の混合比における受光面積である。混
合比が変化し、例えば、臨界角が大きくなると光路42
は光路41方向に近づき範囲43は狭くなる。
The light emitted from the light emitting diode 4 and hitting the optical path 42 travels through the silicon gel 3 and enters the glass column 2.The light travels through the glass column 2 and enters the boundary surface 21 at an angle of incidence that is exactly the same as that of the glass column 2 and the mixed fuel 510. is the critical angle determined by
It is totally reflected at this boundary surface 21, travels through the glass column 2, exits from the peripheral wall 23 into the silicon gel 3, travels through the silicon gel 3, and enters the output photodiode 5. In addition, range 4
3 is the light receiving area at the current mixing ratio of gasoline and alcohol of the gasoline/alcohol mixed fuel 510. As the mixing ratio changes, for example the critical angle increases, the optical path 42
approaches the optical path 41 direction, and the range 43 becomes narrower.

つぎに端面22における光の屈折を第3図とともに説明
する。
Next, the refraction of light at the end face 22 will be explained with reference to FIG.

本実施例ではガラス柱2(実線で示す)の屈折率が封入
体であるシリコンゲル3の屈折率より大きくしである。
In this embodiment, the refractive index of the glass column 2 (indicated by a solid line) is greater than the refractive index of the silicon gel 3 which is the enclosure.

このため、発光ダイオード4からの光の光路42は実線
(第3図でθ4〉θ3である)のとおりである。
Therefore, the optical path 42 of the light from the light emitting diode 4 is as shown by a solid line (θ4>θ3 in FIG. 3).

ここで、光路42の光を周壁23からシリコンゲル3中
へ出射させる場合は、ガラス柱2は破線24に示すよう
に大きいものが必要である。この場合の光の進路は破線
に示すように光路44となり、周壁23からシリコンゲ
ル3中への出射は(図示第3図でθ1くθ2である)の
とおりとなる。
Here, if the light on the optical path 42 is to be emitted from the peripheral wall 23 into the silicon gel 3, the glass column 2 needs to be large as shown by the broken line 24. In this case, the path of the light becomes an optical path 44 as shown by the broken line, and the emission from the peripheral wall 23 into the silicon gel 3 is as follows (θ1 and θ2 in FIG. 3).

本実施例のガソリン・アルコール混合比検出器Aはつぎ
の作用および効果を奏する。
The gasoline/alcohol mixture ratio detector A of this embodiment has the following functions and effects.

(ア)光路42の光を周壁23からシリコンゲル3中へ
出射させる場合はガラス柱2は破線24に示すように大
きいものが必要となるが、検出器Aではガラス柱2が実
線で示す大きさのものを用いれば良く、小型化、軽量化
が図れる。
(A) When the light in the optical path 42 is emitted from the peripheral wall 23 into the silicon gel 3, the glass column 2 needs to be large as shown by the broken line 24, but in the detector A, the glass column 2 is large as shown by the solid line. It is sufficient to use one of the same size, and the size and weight can be reduced.

(イ)ガラス柱2の軽量化に伴い、金属ホルダ1との接
合に際し、その接合強度の点で有利となる。
(a) With the reduction in weight of the glass column 2, it becomes advantageous in terms of bonding strength when bonded to the metal holder 1.

(つ)光路42の光を周壁23からシリコンゲル3中へ
出射させる場合の光路42は破ff144となり、出力
用ホトダイオード5への入射が広がる。
(1) When the light in the optical path 42 is emitted from the peripheral wall 23 into the silicon gel 3, the optical path 42 becomes broken ff 144, and the incidence on the output photodiode 5 spreads.

検出器Aでは光路42は実線で示す道筋を通り著しく広
がらない。このため、出力用ホトダイオード5の受光面
積は小さくてすむ。よって、小型のホトダイオードが使
用でき検出器Aのコストは低減される。ここで、シリコ
ンゲル3とガラス柱2との屈折率との差が大きい程この
効果は顕著となる。なお、シリコンゲル3がガラス柱2
の屈折率と同じか、それを越える場合はこの効果は生じ
ない。
In detector A, the optical path 42 follows the path shown by the solid line and does not widen significantly. Therefore, the light receiving area of the output photodiode 5 can be small. Therefore, a small photodiode can be used and the cost of the detector A is reduced. Here, this effect becomes more significant as the difference in refractive index between the silicon gel 3 and the glass column 2 increases. Note that the silicon gel 3 is the glass column 2.
This effect does not occur when the refractive index is equal to or exceeds the refractive index of .

(1)上記の理由により、ガラス柱2は軸方向の長さを
短くできる。このため、温度変化によりガラスリング7
から受ける応力が小さくなるのでガラス柱2の割れが起
き難い。
(1) For the above reasons, the length of the glass column 2 in the axial direction can be shortened. Therefore, due to temperature changes, the glass ring 7
Since the stress received from the glass column 2 is reduced, cracking of the glass column 2 is less likely to occur.

つぎに、本発明の第2実施例(請求項1および2)を第
4図に基づき説明する。
Next, a second embodiment (claims 1 and 2) of the present invention will be described based on FIG.

本実施例の検出器Bでは第4図に示すように、発光ダイ
オード4の発光強度モニタ用の補止用ホトダイオード6
を出力用ホトダイオード5の上方に配置しており、入射
光45は透光体2を通らずにシリコンゲル3中を通って
補償用ホトダイオード6へ入射する。このような配置で
もガソリン・メタノール混合燃料510の混合比の変化
にかかわらず発光ダイオード4の発光強度を監視できる
。
In the detector B of this embodiment, as shown in FIG.
is arranged above the output photodiode 5, and the incident light 45 passes through the silicon gel 3 without passing through the transparent body 2 and enters the compensation photodiode 6. Even with this arrangement, the light emission intensity of the light emitting diode 4 can be monitored regardless of changes in the mixture ratio of the gasoline/methanol mixed fuel 510.

本実施例の検出器Bでは補償用ホトダイオード6への入
射光45が接着用ガラスリング7で邪魔されることがな
い。また、ホトダイオード6の配設位置が混合燃料51
0の混合比による臨界角の影響を受けない。よって、ホ
トダイオード6の位置決めが容易である。
In the detector B of this embodiment, the incident light 45 to the compensation photodiode 6 is not obstructed by the adhesive glass ring 7. Also, the location of the photodiode 6 is the mixed fuel 51.
It is not affected by the critical angle due to a mixing ratio of 0. Therefore, positioning of the photodiode 6 is easy.

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、透光体の屈折率は、透光体の大きさ、発光素子、受
光素子の配置の容易さから見て、被測定液体との臨界角
を45°以上となるように決めることが望ましい。
a. The refractive index of the light-transmitting body should be determined so that the critical angle with the liquid to be measured is 45° or more, considering the size of the light-transmitting body and the ease of arranging the light-emitting element and light-receiving element. .

61発光素子、受光素子の配置は透光体の周壁側であっ
て各々対向していれば良く、境界面と対向する端面より
内方でも外方でも良い。
61 The light-emitting element and the light-receiving element may be disposed on the peripheral wall side of the light-transmitting body so that they are facing each other, and may be placed inside or outside of the end surface facing the boundary surface.

C1被測定液体は、異なる液体どうし、または、固体が
溶けている液体であれば良く、静止していても流動して
いても良い。
The liquid to be measured C1 may be a liquid containing different liquids or a liquid in which a solid is dissolved, and may be stationary or flowing.

d、透光体は、被測定液体に侵されないものであれば良
く、ソーダガラス、パイレックスガラス、ホウケイ酸ガ
ラス等を使用しCも良く、ガラス以外であっても良い。
d. The transparent material may be any material as long as it is not eroded by the liquid to be measured, and soda glass, pyrex glass, borosilicate glass, etc. may be used, and materials other than glass may also be used.

e、透光体は、上記実施例では加工のし易さから円柱体
を使用したが、正多角柱体を使用しても良い。
e. Although a cylindrical body was used as the light-transmitting body in the above embodiment for ease of processing, a regular polygonal column may also be used.

f、透光体を保持するホルダは、上記実施例では金属製
のものを用いたが、セラミック、プラスチックなどを用
いても良く、また、保持方法はその他○リングを介して
行っても良い。
f. The holder for holding the light-transmitting body is made of metal in the above embodiment, but it may also be made of ceramic, plastic, or the like, and the holder may be held using a ring.

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

第1図は本発明にかかる、ガソリン・アルコール混合比
検出器の第1実施例を示す断面図である。 第2図はその検出器における光の光路を示す要部断面図
である。 第3図はその検出器での端面における光の屈折の様子を
示す説明図である。 第4図は本発明にかかる、ガソリン・アルコール混合比
検出器の第2実施例を示す断面図である。 第5図はこの特許出願人が提案した、特願昭63−29
5478号公報記載の検出器の断面図である。 第6図は従来の検出器の断面図である。 図中 1・・・金属ホルダ(ホルダ) 2・・・ガラス
柱(透光体) 3・・・シリコンゲル(充填材) 4・
・・発光ダイオード(発光素子) 5・・・出力用ホト
ダイオード(受光素子) 6・・・補償用ホトダイオー
ド(受光素子)22・・・端面 23・・・周壁 51
0・・・ガソリン・メタノール混合燃料(被測定液体)
A、B・・・ガソリン・アルコール混合比検出器(液体
混合比検出器)
FIG. 1 is a sectional view showing a first embodiment of a gasoline/alcohol mixture ratio detector according to the present invention. FIG. 2 is a sectional view of a main part showing the optical path of light in the detector. FIG. 3 is an explanatory diagram showing how light is refracted at the end face of the detector. FIG. 4 is a sectional view showing a second embodiment of the gasoline/alcohol mixture ratio detector according to the present invention. Figure 5 shows the patent application filed in 1983-29, proposed by this patent applicant.
FIG. 5 is a cross-sectional view of a detector described in Japanese Patent No. 5478. FIG. 6 is a sectional view of a conventional detector. In the figure 1...Metal holder (holder) 2...Glass column (translucent body) 3...Silicon gel (filling material) 4.
...Light emitting diode (light emitting element) 5...Output photodiode (light receiving element) 6...Compensation photodiode (light receiving element) 22...End face 23...Peripheral wall 51
0...Gasoline/methanol mixed fuel (liquid to be measured)
A, B...Gasoline/alcohol mixture ratio detector (liquid mixture ratio detector)

Claims (1)

【特許請求の範囲】 1)柱状を呈するとともに、少なくとも2種類の物質を
混合してなる被測定液体に浸される境界面を有する透光
体と、 該透光体を保持するホルダと、 前記透光体の周壁側の任意位置に配される発光素子と、 前記透光体を挟んで前記発光素子と対向的に配される少
なくとも一つの受光素子と、 前記透光体と、発光素子および受光素子との間に配され
る液状またはゲル状の透光性を有する充填材と からなる液体混合比検出器において、 前記発光素子から発光した光は前記充填材中を進み透光
体に入射し、透光体中を進み、透光体と被測定液体とに
より決まる臨界角以上の場合前記境界面で全反射し、透
光体中を進み、前記周壁または前記境界面と対向する端
面から出射するように、前記柱状透光体の形状および受
光素子の取り付け位置が決められていることを特徴とす
る液体混合比検出器。 2)前記充填材は前記透光体より屈折率が小さく、かつ
、 境界面への入射角が、少なくとも、透光体と充填材とに
より決まる臨界角以上のものについては、境界面で反射
の後、周壁から出射することを特徴とする請求項1記載
の液体混合比検出器。
[Scope of Claims] 1) A light transmitting body having a columnar shape and having a boundary surface that is immersed in a liquid to be measured made of a mixture of at least two types of substances; a holder for holding the light transmitting body; a light-emitting element disposed at any position on the peripheral wall side of the light-transmitting body; at least one light-receiving element disposed opposite to the light-emitting element with the light-transmitting body in between; the light-transmitting body; the light-emitting element; and In a liquid mixture ratio detector consisting of a liquid or gel-like light-transmitting filler placed between a light-receiving element and a light-transmitting element, the light emitted from the light-emitting element travels through the filler and enters the light-transmitting body. The light travels through the transparent body, and when the angle is greater than or equal to the critical angle determined by the transparent body and the liquid to be measured, it is totally reflected at the boundary surface, travels through the transparent body, and exits from the peripheral wall or the end face opposite to the boundary surface. A liquid mixture ratio detector characterized in that the shape of the columnar light transmitting body and the mounting position of the light receiving element are determined so as to emit light. 2) The filler has a lower refractive index than the light transmitting material, and if the incident angle to the boundary surface is at least equal to or greater than the critical angle determined by the light transmitting material and the filler, there is no possibility of reflection at the boundary surface. 2. The liquid mixture ratio detector according to claim 1, wherein the liquid mixture ratio detector emits the liquid from the peripheral wall.
JP4000889A 1988-11-23 1989-02-20 Detector of liquid mixture rate Pending JPH02218940A (en)

Priority Applications (4)

Application Number Priority Date Filing Date Title
JP4000889A JPH02218940A (en) 1989-02-20 1989-02-20 Detector of liquid mixture rate
US07/438,513 US4962746A (en) 1988-11-23 1989-11-17 Mixing liquid ratio detector device
EP89312161A EP0370807B1 (en) 1988-11-23 1989-11-23 A liquid mixture ratio detector device
DE8989312161T DE68901644D1 (en) 1988-11-23 1989-11-23 DEVICE FOR DETERMINING THE MIXING RATIO OF A LIQUID MIXTURE.

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP4000889A JPH02218940A (en) 1989-02-20 1989-02-20 Detector of liquid mixture rate

Publications (1)

Publication Number Publication Date
JPH02218940A true JPH02218940A (en) 1990-08-31

Family

ID=12568880

Family Applications (1)

Application Number Title Priority Date Filing Date
JP4000889A Pending JPH02218940A (en) 1988-11-23 1989-02-20 Detector of liquid mixture rate

Country Status (1)

Country Link
JP (1) JPH02218940A (en)

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