JPH0244213A - Liquid level sensor - Google Patents
Liquid level sensorInfo
- Publication number
- JPH0244213A JPH0244213A JP19413688A JP19413688A JPH0244213A JP H0244213 A JPH0244213 A JP H0244213A JP 19413688 A JP19413688 A JP 19413688A JP 19413688 A JP19413688 A JP 19413688A JP H0244213 A JPH0244213 A JP H0244213A
- Authority
- JP
- Japan
- Prior art keywords
- prism
- light
- emitting element
- liquid level
- light emitting
- 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 abstract description 15
- 239000000126 substance Substances 0.000 claims description 4
- 229920005668 polycarbonate resin Polymers 0.000 abstract description 5
- 239000004431 polycarbonate resin Substances 0.000 abstract description 5
- 238000001514 detection method Methods 0.000 abstract description 4
- 230000035945 sensitivity Effects 0.000 abstract description 4
- XUIMIQQOPSSXEZ-UHFFFAOYSA-N Silicon Chemical compound [Si] XUIMIQQOPSSXEZ-UHFFFAOYSA-N 0.000 abstract 2
- 229920005989 resin Polymers 0.000 abstract 2
- 239000011347 resin Substances 0.000 abstract 2
- 229910052710 silicon Inorganic materials 0.000 abstract 2
- 239000010703 silicon Substances 0.000 abstract 2
- 238000012856 packing Methods 0.000 abstract 1
- 239000012780 transparent material Substances 0.000 abstract 1
- 229920002050 silicone resin Polymers 0.000 description 7
- 230000007423 decrease Effects 0.000 description 5
- 239000000463 material Substances 0.000 description 3
- WABPQHHGFIMREM-UHFFFAOYSA-N lead(0) Chemical compound [Pb] WABPQHHGFIMREM-UHFFFAOYSA-N 0.000 description 1
Landscapes
- Measurement Of Levels Of Liquids Or Fluent Solid Materials (AREA)
Abstract
Description
【発明の詳細な説明】
産業上の利用分野
零発′明はプリズムの裏面に発光素子と受光素子とを並
置し、前記プリズムの外面が空気に触れているときは発
光素子から発せられた光がプリズムの他の2面に反射し
て受光素子で受光され、プリズムの外面が液体に触れて
いるときは発光素子から発せられた光がプリズムの外へ
屈折して出ていって受光素子で受光されないことにより
、液面がプリズムの外面に達したか否かを検出するよう
にした液面センサに関する。[Detailed description of the invention] The zero invention in the industrial application field is that a light emitting element and a light receiving element are arranged side by side on the back surface of a prism, and when the outer surface of the prism is in contact with air, the light emitted from the light emitting element is is reflected by the other two surfaces of the prism and received by the light receiving element, and when the outer surface of the prism is in contact with the liquid, the light emitted from the light emitting element is refracted out of the prism and is received by the light receiving element. The present invention relates to a liquid level sensor that detects whether the liquid level has reached the outer surface of a prism by not receiving light.
従来の技術及び発明が解決しようとする間麗点従来、こ
の種の液面センサにおいては、発光素子と受光素子をプ
リズムの裏面にできるだけ接近するように配置している
が完全に密着させることは困難であっである程度の隙間
が生ずる。Conventionally, in this type of liquid level sensor, the light-emitting element and the light-receiving element are arranged as close as possible to the back surface of the prism, but they cannot be brought into complete contact with each other. It is difficult to do this, and some gaps are created.
一方、フレネルの法則によれば、屈折率Naの物質から
屈折率Ngの物質に光を垂直に入射させた場合の反射率
Rは次式で表される。On the other hand, according to Fresnel's law, the reflectance R when light is perpendicularly incident on a substance with a refractive index of Ng from a substance with a refractive index of Na is expressed by the following equation.
n= (Ng−Na)/(Ng+Na)”ここで、プリ
ズムの材質をポリカーボネート樹脂とすると、その屈折
率N、は1.586であり、空気の屈折率Naは1.0
であるから、反射率は0.0513となり、約5%がプ
リズムで反射されて受光率が低下して感度が低下する欠
点があった。n= (Ng-Na)/(Ng+Na)" Here, if the material of the prism is polycarbonate resin, its refractive index N is 1.586, and the refractive index Na of air is 1.0.
Therefore, the reflectance was 0.0513, and about 5% of the light was reflected by the prism, resulting in a decrease in the light receiving rate and a decrease in sensitivity.
問題点を解決するための手段
本発明はこのような問題点を解決するための手段として
、プリズムと発光素子の間の空間に屈折率がプリズムに
近い透明な物質を充填した構成とした。Means for Solving the Problems As a means for solving these problems, the present invention adopts a structure in which the space between the prism and the light emitting element is filled with a transparent substance whose refractive index is close to that of the prism.
発明の作用及び効果
本発明は上記構成になり、萌記フレネルの式においてN
a#Ngとなるから反射率Rが減少し、受光素子の受光
率が向上し、発光素子の消費電流を減して耐久性を向上
し得るとともに、発光素子の傾きにより受光徂が減少し
てもこれを補うことができ、さらに、充填する物質とし
てシリコン樹脂等の固化物を用いることにより発光素子
をケース内にしっかりと固定することができる効果があ
る。Functions and Effects of the Invention The present invention has the above configuration, and in the Moeki Fresnel equation, N
a#Ng, the reflectance R decreases, the light-receiving rate of the light-receiving element improves, the current consumption of the light-emitting element decreases, and the durability improves, and the light-receiving area decreases due to the inclination of the light-emitting element. Furthermore, by using a solidified material such as silicone resin as the filling material, it is possible to firmly fix the light emitting element within the case.
実施例 以下、本発明の一実施例を添付図面に基いて説明する。Example An embodiment of the present invention will be described below with reference to the accompanying drawings.
図においてlは透明なポリカーボネイト樹脂からなる円
筒形のケースであって、下端に頂角90°の円錐形をな
すプリズム2が一体に形成されている。ケースlの底部
には第2図に拡大して示すように、発光素子3と受光素
子4を並置したフォトカブラ5がプリズム2の裏面との
間に小間隙を空けて装置され、画素子3.4のリード線
6はケースlの上部に装置された図示しない信号処理回
路に接続されており、フォトカブラ5とプリズム2の間
の間隙にはシリコン樹脂7が充填されて固化している。In the figure, l is a cylindrical case made of transparent polycarbonate resin, and a conical prism 2 with an apex angle of 90° is integrally formed at the lower end. At the bottom of the case l, as shown in an enlarged view in FIG. The lead wire 6 of .4 is connected to a signal processing circuit (not shown) installed in the upper part of the case l, and the gap between the photocoupler 5 and the prism 2 is filled with silicone resin 7 and solidified.
本実施例においては、プリズム2が空気に触れていると
きは、発光素子3から発せられた光がシリコン樹脂7を
通過し、プリズム2の2点1、bで反射して再びシリコ
ン樹脂7を通り、受光素子4で受光されて信号処理回路
に液面不検知信号が人力され、プリズム2が液体に触れ
ているときは、第2図に鎖線で示すように、発光素子3
から発せられた光がプリズムの点aにおいて屈折して外
へ出ることにより受光素子4に受光されないことにより
液面検知信号が発せられるのであるが、発光素子3から
発せられた光がシリコン樹脂7からプリズム2に垂直に
入る際の反射率は、ポリカーボネイト樹脂の屈折率は1
.586、シリコン樹脂7の屈折率は1.4であるから
前述のフレネルの式によりR= 0.00388と極め
て小さく、略Oに近いため、発光素子3から発せられた
光の略総てが受光素子4で受光されて著しい高感度を得
ることができる。In this embodiment, when the prism 2 is in contact with the air, the light emitted from the light emitting element 3 passes through the silicone resin 7, is reflected at two points 1 and b of the prism 2, and returns to the silicone resin 7. As shown in FIG. 2, when the light is received by the light receiving element 4 and a liquid level non-detection signal is inputted to the signal processing circuit, and the prism 2 is in contact with the liquid, the light emitting element 3 is detected as shown by the chain line in FIG.
The light emitted from the light emitting element 3 is refracted at point a of the prism and goes out, and is not received by the light receiving element 4, so that a liquid level detection signal is generated. The reflectance when entering the prism 2 perpendicularly from the polycarbonate resin is 1.
.. 586, the refractive index of the silicone resin 7 is 1.4, so according to the Fresnel equation mentioned above, R = 0.00388, which is extremely small and close to O, so almost all of the light emitted from the light emitting element 3 is received. The light is received by the element 4 and extremely high sensitivity can be obtained.
また、シリコン樹脂7はフォトカブラ5をケースl内に
安定して固定する利点がある。Furthermore, the silicone resin 7 has the advantage of stably fixing the photocoupler 5 inside the case l.
第1図は本発明の一実施例の一部切欠斜視図、第2図は
、その要部の拡大断面図である。
!二ケース 2ニブリズム 3:発光素子 4:受光素
子 7:シリコン樹脂
第1面FIG. 1 is a partially cutaway perspective view of an embodiment of the present invention, and FIG. 2 is an enlarged sectional view of the main part thereof. ! 2 cases 2 Nibrism 3: Light emitting element 4: Light receiving element 7: Silicone resin first surface
Claims (1)
もに、該プリズムの裏面に空間を空けて発光素子と受光
素子を並置し、前記プリズムの外面が空気に触れている
ときは前記発光素子から発せられた光が前記プリズムの
他の2面で反射して受光素子で受光され、前記プリズム
の外面が液体に触れているときは前記発光素子から発せ
られた光が前記プリズムの外へ屈折して出ていつて前記
受光素子で受光されないことにより液面がプリズムの外
面に達したか否かを検出するようにした液面センサであ
つて、前記プリズムと前記発光素子の間の前記空間に屈
折率が前記プリズムに近い透明な物質を充填したことを
特徴とする液面センサA prism is integrally fixed to the tip of a cylindrical case, and a light emitting element and a light receiving element are arranged side by side with a space left on the back side of the prism, and when the outer surface of the prism is in contact with air, the light emitting element is removed from the prism. The emitted light is reflected by the other two surfaces of the prism and received by the light receiving element, and when the outer surface of the prism is in contact with the liquid, the light emitted from the light emitting element is refracted out of the prism. The liquid level sensor detects whether or not the liquid level has reached the outer surface of the prism by emitting light and not being received by the light receiving element, the liquid level sensor detecting whether or not the liquid level has reached the outer surface of the prism. A liquid level sensor characterized in that it is filled with a transparent substance whose ratio is similar to that of the prism.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP19413688A JPH0244213A (en) | 1988-08-03 | 1988-08-03 | Liquid level sensor |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP19413688A JPH0244213A (en) | 1988-08-03 | 1988-08-03 | Liquid level sensor |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH0244213A true JPH0244213A (en) | 1990-02-14 |
Family
ID=16319507
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP19413688A Pending JPH0244213A (en) | 1988-08-03 | 1988-08-03 | Liquid level sensor |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0244213A (en) |
-
1988
- 1988-08-03 JP JP19413688A patent/JPH0244213A/en active Pending
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