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JPH0345783B2 - - Google Patents
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JPH0345783B2 - - Google Patents

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Publication number
JPH0345783B2
JPH0345783B2 JP59064215A JP6421584A JPH0345783B2 JP H0345783 B2 JPH0345783 B2 JP H0345783B2 JP 59064215 A JP59064215 A JP 59064215A JP 6421584 A JP6421584 A JP 6421584A JP H0345783 B2 JPH0345783 B2 JP H0345783B2
Authority
JP
Japan
Prior art keywords
coating layer
optical waveguide
substrate
refractive index
oil
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.)
Expired - Lifetime
Application number
JP59064215A
Other languages
Japanese (ja)
Other versions
JPS60209144A (en
Inventor
Tetsuya Yamazaki
Hiroshi Wada
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.)
Nippon Sheet Glass Co Ltd
Original Assignee
Nippon Sheet Glass 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 Nippon Sheet Glass Co Ltd filed Critical Nippon Sheet Glass Co Ltd
Priority to JP59064215A priority Critical patent/JPS60209144A/en
Publication of JPS60209144A publication Critical patent/JPS60209144A/en
Publication of JPH0345783B2 publication Critical patent/JPH0345783B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N21/00Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
    • G01N21/17Systems in which incident light is modified in accordance with the properties of the material investigated
    • G01N21/41Refractivity; Phase-affecting properties, e.g. optical path length
    • G01N21/43Refractivity; Phase-affecting properties, e.g. optical path length by measuring critical angle
    • G01N21/431Dip refractometers, e.g. using optical fibres

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)
  • Geophysics And Detection Of Objects (AREA)

Description

【発明の詳細な説明】 本発明は、油等の液体を光学的に感知する液体
感知器に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a liquid sensor that optically senses liquid such as oil.

最近、石油備蓄基地や石油化学プラント等で油
漏れ事故が多発しており、この様な事故を早期に
発見する為の法的規制等によつて、信頼度の高い
感知器が必要とされている。
Recently, oil leak accidents have been occurring frequently at oil storage bases, petrochemical plants, etc., and highly reliable detectors are required due to legal regulations to detect such accidents early. There is.

第1図及び第2図は、この様な感知器の1つの
従来例であるポリマクラツド光フアイバを示して
いる。このポリマクラツド光フアイバ1は、石英
から成るコア2と屈折率が石英よりも小さなシリ
コン樹脂等のポリマ(高分子材料)から成るクラ
ツド3とを有している。
1 and 2 illustrate one conventional example of such a sensor, a polymer clad optical fiber. This polymer-clad optical fiber 1 has a core 2 made of quartz and a cladding 3 made of a polymer (polymer material) such as silicone resin having a refractive index smaller than that of quartz.

油漏れが発生していない状態、つまり光フアイ
バ1に油が付着していない状態では、光フアイバ
1の一端からこの光フアイバ1内へ入射した光i1
は、第1図に示す様に、コア2とクラツド3との
界面で全反射を繰り返しながら、低損失で他端ま
で伝播する。
When there is no oil leakage, that is, when no oil is attached to the optical fiber 1, the light i 1 that enters the optical fiber 1 from one end of the optical fiber 1
As shown in FIG. 1, the light propagates to the other end with low loss while repeating total reflection at the interface between the core 2 and the cladding 3.

ところが、屈折率の大きな油が光フアイバ1に
付着してクラツド3内へ浸潤すると、クラツド3
の屈折率が高くなる。この結果、光フアイバ1内
へ入射した光i1の中には、第2図に示す様に、コ
ア2とクラツド3との界面で全反射せずに屈折
し、コア2外へ出て行く光が生じる。
However, when oil with a high refractive index adheres to the optical fiber 1 and infiltrates into the cladding 3, the cladding 3
The refractive index of As a result, some of the light i 1 that has entered the optical fiber 1 is refracted without being totally reflected at the interface between the core 2 and the cladding 3 and exits the core 2, as shown in Figure 2. Light arises.

この為に、光フアイバ1中に全反射しながら伝
播する光の量が、油の浸潤前に比べて減少する。
従つて、光フアイバ1の一端には光源を、また他
端には受光器を夫々配置して、伝播光量の変化を
監視すれば、油漏れを感知することができる。
For this reason, the amount of light that propagates into the optical fiber 1 while being totally reflected is reduced compared to before being infiltrated with oil.
Therefore, by arranging a light source at one end of the optical fiber 1 and a light receiver at the other end and monitoring changes in the amount of propagated light, oil leakage can be detected.

ところで、光フアイバ1の径は非常に小さいの
で、油漏れが発生した場所に光フアイバ1が正確
に位置していなければ、この油漏れを感知するこ
とができない。つまり、光フアイバ1では油漏れ
を言わば線状にしか感知することができない為
に、油漏れを見逃す確率が高くて、信頼度の高い
感知器とは成り得ない。
By the way, since the diameter of the optical fiber 1 is very small, the oil leak cannot be detected unless the optical fiber 1 is precisely positioned at the location where the oil leak occurs. In other words, since the optical fiber 1 can only detect oil leaks linearly, there is a high probability that oil leaks will be missed, and it cannot be a highly reliable sensor.

本発明は、この様な問題点に鑑み、広い範囲に
亘つて液体を感知することができる液体感知器を
提供することを目的としている。
In view of these problems, it is an object of the present invention to provide a liquid sensor that can sense liquid over a wide range.

以下、本発明の一実施例を第3図〜第5図を参
照しながら説明する。
An embodiment of the present invention will be described below with reference to FIGS. 3 to 5.

第3図及び第4図は、本発明の一実施例を示す
夫々斜視図及び縦断面図である。屈折率がn1であ
る透光性の基板11中には、n1よりも大きな屈折
率n2を有する光導波路12が形成されている。
3 and 4 are a perspective view and a longitudinal sectional view, respectively, showing an embodiment of the present invention. An optical waveguide 12 having a refractive index n 2 larger than n 1 is formed in a transparent substrate 11 having a refractive index n 1 .

光導波路12は、その入射端12Aと出射端1
2Bとの間で2本の分岐路12Cに分岐してい
る。入射端12Aと出射端12Bとの近傍の光導
波路12は基板11中に完全に埋め込まれている
が、分岐路12Cは基板11の表面11Aに露出
している露出部12Dをその略全長に亘つて有し
ている。
The optical waveguide 12 has an input end 12A and an output end 1.
2B, it branches into two branch paths 12C. The optical waveguide 12 near the input end 12A and the output end 12B is completely embedded in the substrate 11, but the branch path 12C covers almost the entire length of the exposed portion 12D exposed on the surface 11A of the substrate 11. I have it.

露出部12Dとこの露出部12Dに連なつてい
る表面11Aとは、共に被覆層13によつて覆わ
れている。被覆層13は、n1及びn2の何れよりも
小さな屈折率n3を有し且つ液体の浸潤が可能な材
質、例えばシリコン樹脂から成つている。
The exposed portion 12D and the surface 11A connected to the exposed portion 12D are both covered with a coating layer 13. The covering layer 13 is made of a material that has a refractive index n 3 smaller than either n 1 or n 2 and can be infiltrated with liquid, such as silicone resin.

基板11、光導波路12及び被覆層13の夫々
の屈折率n1,n2,n3は、上述の様にn2>n1>n3
なる様に選定されている。この為に、光導波路1
2中を伝播可能な光は、光導波路12と基板11
との界面に於ける臨界角θ1によつて決定される。
The refractive indices n 1 , n 2 , n 3 of the substrate 11, the optical waveguide 12, and the coating layer 13 are selected so that n 2 >n 1 >n 3 as described above. For this purpose, the optical waveguide 1
2, the light that can propagate through the optical waveguide 12 and the substrate 11
It is determined by the critical angle θ 1 at the interface with

もし、屈折率の大きな油等が被覆層13に付着
してこの被覆層13内へ浸潤することによつて、
n3がn1よりも大きくなると、夫々の屈折率間の関
係はn2>n3>n1となる。従つて、この場合に光導
波路12中を伝播可能な光は、上述の臨界角θ1
はなく光導波路12と被覆層13との界面に於け
る臨界角θ2によつて決定される。
If oil or the like with a high refractive index adheres to the coating layer 13 and infiltrates into the coating layer 13,
When n 3 becomes larger than n 1 , the relationship between the respective refractive indices becomes n 2 > n 3 > n 1 . Therefore, in this case, the light that can propagate through the optical waveguide 12 is determined by the critical angle θ 2 at the interface between the optical waveguide 12 and the coating layer 13 rather than the critical angle θ 1 described above.

ところが、θ2はθ1よりも大きいので、全反射の
割合が減少して伝播光量も減少し、油漏れを感知
することができる。しかも、被覆層13は露出部
12Dのみならずこの露出部12Dに連なつてい
る表面11Aをも覆つており、露出部12D以外
の部分で被覆層13に付着した油が露出部12D
の部分にまで浸潤可能であり、更にまた光導波路
12が2本の分岐路12Cに分岐しているので、
光導波路12の径よりもはるかに広い範囲に亘つ
て面状に油漏れを感知することができる。
However, since θ 2 is larger than θ 1 , the total reflection rate decreases and the amount of propagated light also decreases, making it possible to detect oil leakage. Moreover, the coating layer 13 covers not only the exposed portion 12D but also the surface 11A connected to the exposed portion 12D, and the oil adhering to the coating layer 13 in areas other than the exposed portion 12D may be transferred to the exposed portion 12D.
Furthermore, since the optical waveguide 12 is branched into two branch paths 12C,
Oil leakage can be detected in a planar manner over a much wider range than the diameter of the optical waveguide 12.

従つて、この為には、露出部12Dの径の少な
くとも1.5倍以上の巾で、被覆層13が露出部1
2Dを覆つていることが望ましい。
Therefore, for this purpose, the coating layer 13 must be formed on the exposed portion 12D with a width that is at least 1.5 times the diameter of the exposed portion 12D.
It is desirable to cover 2D.

なお、基板12の材質として石英ガラス或いは
プラスチツクを夫々用いた場合は、光フアイバ等
の製作に利用されている火炎加水分解法、或いは
光重合法等の周知の技術を夫々利用することによ
つて、光導波路12を形成することができる。こ
の光導波路12の軸心に垂直な断面に於ける屈折
率分布は、均一であつてもよいし勾配を有してい
てもよい。
In addition, when quartz glass or plastic is used as the material of the substrate 12, it is possible to use well-known techniques such as flame hydrolysis or photopolymerization, which are used in the production of optical fibers, respectively. , the optical waveguide 12 can be formed. The refractive index distribution in a cross section perpendicular to the axis of the optical waveguide 12 may be uniform or may have a slope.

そして、以上の様な構成を有する感知器14の
光導波路12の入射端12Aと出射端12Bとに
は、夫々入力用及び出力用の光フアイバ15が接
続されている。
Optical fibers 15 for input and output are connected to the input end 12A and output end 12B of the optical waveguide 12 of the sensor 14 having the above-described configuration, respectively.

具体例 1 基板11を石英ガラスで構成し、被覆層13を
シリコン樹脂で構成すると、上記の夫々の屈折率
はn1=1.456、n2=1.47、n3=1.405であり、臨界
角はθ1=82.1゜、θ2=72.9゜である。
Specific Example 1 When the substrate 11 is made of quartz glass and the coating layer 13 is made of silicone resin, the above respective refractive indices are n 1 = 1.456, n 2 = 1.47, and n 3 = 1.405, and the critical angle is θ. 1 = 82.1°, θ 2 = 72.9°.

そして、1.47の屈折率を有する油が被覆層13
に浸潤すると、この被覆層13の屈折率n3が1.46
まで増大して、θ2=83.3゜となる。この結果、θ2
θ1となつて全反射の割合が減少し、伝播光量が減
少して油漏れを感知することができる。
Then, oil having a refractive index of 1.47 is applied to the coating layer 13.
When infiltrated into the coating layer 13, the refractive index n 3 of this coating layer 13 becomes 1.46.
It increases to θ 2 =83.3°. As a result, θ 2 >
θ 1 , the rate of total reflection decreases, the amount of propagated light decreases, and oil leakage can be detected.

この具体例1の様に基板11を石英ガラスで構
成すれば、光フアイバ15として伝送損失の少な
いガラス光フアイバを使用しても、この光フアイ
バ15と基板11とを融着等によつて容易に接続
することができる。従つて、油漏れ事故が発生し
た場合、油が浸潤して再使用できなくなつた感知
器14のみを容易に取り替えることができる。
If the substrate 11 is made of quartz glass as in this specific example 1, even if a glass optical fiber with low transmission loss is used as the optical fiber 15, the optical fiber 15 and the substrate 11 can be easily bonded together by fusing or the like. can be connected to. Therefore, in the event of an oil leakage accident, only the sensor 14 that has become infiltrated with oil and cannot be reused can be easily replaced.

具体例 2 基板11をプラスチツクで構成し、被覆層13
をシリコン樹脂で構成すると、上記の夫々の屈折
率はn1=1.44、n2=1.48、n3=1.405であり、臨界
角はθ1=76.6゜、θ2=71.7゜である。
Specific example 2 The substrate 11 is made of plastic, and the coating layer 13
When made of silicone resin, the respective refractive indexes mentioned above are n 1 =1.44, n 2 =1.48, and n 3 =1.405, and the critical angles are θ 1 =76.6° and θ 2 =71.7°.

そして、1.458の屈折率を有する油が被覆層1
3に浸潤すると、この被覆層13の屈折率n3
1.451まで増大して、θ2=78.6゜となる。この結果、
θ2>θ1となつて全反射の割合が減少し、伝播光量
が減少して油漏れを感知することができる。
Then, oil with a refractive index of 1.458 is applied to the coating layer 1.
3, the refractive index n 3 of this coating layer 13 becomes
It increases to 1.451 and becomes θ 2 =78.6°. As a result,
When θ 21 , the rate of total reflection decreases, the amount of propagated light decreases, and oil leakage can be detected.

第5図は、感知器14を適用して実際に油漏れ
を感知する為の装置を示している。まず、油タン
ク21の油漏れが発生しそうな個所に感知器14
を配置し、これらの感知器14を光フアイバ15
によつて直列若しくは並列に接続しておく。光フ
アイバ15へは光源22からの光を入射させ、こ
の光フアイバ15から射出される光を光検出器2
3で検出する。そして、光検出器23からの電気
信号を、増巾器24及び比較器25を介して警報
器26へ導く。
FIG. 5 shows a device for actually detecting oil leakage using the sensor 14. First, a sensor 14 is installed at a location in the oil tank 21 where oil leakage is likely to occur.
and connect these sensors 14 with optical fibers 15.
Connect in series or in parallel depending on the Light from a light source 22 is input into the optical fiber 15, and the light emitted from the optical fiber 15 is detected by a photodetector 2.
Detect with 3. Then, the electrical signal from the photodetector 23 is guided to the alarm 26 via the amplifier 24 and the comparator 25.

なお、光フアイバコネクタの接続損失や光フア
イバの伝送損失の測定に利用されている後方散乱
法を併用すれば、単に油漏れを感知するのみでは
なく、油漏れの個所をも知ることができる。
If the backscattering method, which is used to measure the connection loss of optical fiber connectors and the transmission loss of optical fibers, is also used, it is possible to not only detect oil leaks but also to know the location of oil leaks.

以上の説明では油のみの感知について述べた
が、被覆層13に浸潤してこの被覆層13の屈折
率を増大させる液体であれば油に限られることな
く感知することができる。
Although the above description deals with sensing only oil, any liquid that infiltrates the coating layer 13 and increases the refractive index of the coating layer 13 can be detected without being limited to oil.

上述の様に、本発明による液体感知器では、光
導波路の露出部以外の基板表面をも被覆層によつ
て覆う様にしているので、露出部以外の部分で液
体が被覆層に浸潤しても、この液体が露出部の部
分にまで浸潤可能であり、広い範囲に亘つて液体
を感知することができる。
As described above, in the liquid sensor according to the present invention, since the surface of the substrate other than the exposed portion of the optical waveguide is also covered with the coating layer, there is no possibility that the liquid will infiltrate into the coating layer in the portion other than the exposed portion. However, this liquid can infiltrate even the exposed parts, and the liquid can be sensed over a wide range.

しかも、光導波路を複数の分岐路に分けて夫々
の分岐路に露出部を設ける様にしているので、更
に広い範囲に亘つて液体を感知することができ
る。
Furthermore, since the optical waveguide is divided into a plurality of branch paths and each branch path is provided with an exposed portion, liquid can be sensed over a wider range.

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

第1図及び第2図は本発明の一従来例を示す概
略的な側断面図である。第3図及び第4図は本発
明の一実施例を示す夫々概略的な斜視図及び縦断
面図、第5図は第3図及び第4図に示した一実施
例の適用装置を示す概略図である。 なお図面に用いられた符号において、11…基
板、11A…表面、12…光導波路、12A…入
射端、12B…出射端、12C…分岐路、12D
…露出部、13…被覆層、14…感知器である。
1 and 2 are schematic side sectional views showing a conventional example of the present invention. 3 and 4 are schematic perspective views and vertical sectional views, respectively, showing one embodiment of the present invention, and FIG. 5 is a schematic diagram showing an application device of the embodiment shown in FIGS. 3 and 4. It is a diagram. In addition, in the symbols used in the drawings, 11...substrate, 11A...surface, 12...optical waveguide, 12A...incident end, 12B...outgoing end, 12C...branch path, 12D
...Exposed portion, 13...Coating layer, 14...Sensor.

Claims (1)

【特許請求の範囲】[Claims] 1 透光性の基板と、入射端から出射端へ至る複
数の分岐路を有する様に前記基板中に形成されて
いる光導波路と、前記複数の分岐路の夫々が前記
基板の表面に露出する様にこれらの分岐路の夫々
に設けられている露出部と、前記光導波路の屈折
率よりも小さな屈折率を有すると共に液体の浸潤
が可能であり且つ前記露出部よりも広い面積でこ
れらの露出部を覆う様に前記基板の表面に配され
ている被覆層とを夫々具備し、前記液体の浸潤に
よる前記被覆層の屈折率の増大に伴い前記光導波
路中を前記複数の分岐路の夫々を経由して前記入
射端から前記出射端へ伝播する光の量が減少する
ことによつて前記液体を感知する様にした液体感
知器。
1. A transparent substrate, an optical waveguide formed in the substrate so as to have a plurality of branch paths extending from an input end to an output end, and each of the plurality of branch paths being exposed on the surface of the substrate. exposed portions provided in each of these branch paths, and having a refractive index smaller than the refractive index of the optical waveguide, allowing infiltration of liquid, and having an area larger than the exposed portion. a coating layer disposed on the surface of the substrate so as to cover a portion of the optical waveguide, and as the refractive index of the coating layer increases due to the liquid infiltration, each of the plurality of branch paths A liquid sensor configured to sense the liquid by reducing the amount of light propagating from the input end to the output end.
JP59064215A 1984-03-31 1984-03-31 Liquid sensor Granted JPS60209144A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP59064215A JPS60209144A (en) 1984-03-31 1984-03-31 Liquid sensor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP59064215A JPS60209144A (en) 1984-03-31 1984-03-31 Liquid sensor

Publications (2)

Publication Number Publication Date
JPS60209144A JPS60209144A (en) 1985-10-21
JPH0345783B2 true JPH0345783B2 (en) 1991-07-12

Family

ID=13251639

Family Applications (1)

Application Number Title Priority Date Filing Date
JP59064215A Granted JPS60209144A (en) 1984-03-31 1984-03-31 Liquid sensor

Country Status (1)

Country Link
JP (1) JPS60209144A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5209275A (en) * 1987-07-09 1993-05-11 Junkosha Co., Ltd. Liquid dispensing apparatus and method by sensing the type of liquid vapors in the receiver

Also Published As

Publication number Publication date
JPS60209144A (en) 1985-10-21

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