JPH0367579B2 - - Google Patents

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Publication number
JPH0367579B2
JPH0367579B2 JP61211060A JP21106086A JPH0367579B2 JP H0367579 B2 JPH0367579 B2 JP H0367579B2 JP 61211060 A JP61211060 A JP 61211060A JP 21106086 A JP21106086 A JP 21106086A JP H0367579 B2 JPH0367579 B2 JP H0367579B2
Authority
JP
Japan
Prior art keywords
liquid level
light
optical fiber
optical
amount
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
JP61211060A
Other languages
Japanese (ja)
Other versions
JPS6365321A (en
Inventor
Hajime Hatsutori
Takashi Takeo
Koji Shibata
Atsushi Okamoto
Kazuyuki Nishama
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.)
NAGOYASHI
TSUCHA KK
Original Assignee
NAGOYASHI
TSUCHA KK
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 NAGOYASHI, TSUCHA KK filed Critical NAGOYASHI
Priority to JP21106086A priority Critical patent/JPS6365321A/en
Publication of JPS6365321A publication Critical patent/JPS6365321A/en
Publication of JPH0367579B2 publication Critical patent/JPH0367579B2/ja
Granted legal-status Critical Current

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  • Measurement Of Levels Of Liquids Or Fluent Solid Materials (AREA)

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は光伝送路内を伝搬する光が気相と液相
の屈折率差に対応して漏洩する性質を利用した光
学式液面レベルセンサに関する。
Detailed Description of the Invention (Industrial Application Field) The present invention is an optical liquid level leveling system that utilizes the property that light propagating in an optical transmission line leaks in response to the difference in refractive index between the gas phase and the liquid phase. Regarding sensors.

(従来の技術) 近年、産業計測分野における液面計測において
光フアイバなどの光伝送路を用いた計測センサが
種々提案されている。例えば、光フアイバのクラ
ツド部の一部を剥離してコア部を露出させ、光フ
アイバ中の光透過量の変化により液体の有無もし
くは液面を検出するセンサ、もしくは特開昭58−
18126号公報には入射光を伝送する第1の光路と
反射光を伝送する第2の光路を光フアイバで形成
し、前記光路の開放端となる光フアイバの一端に
プリズムを付設した液面センサなどが開示されて
いる。
(Prior Art) In recent years, various measurement sensors using optical transmission paths such as optical fibers have been proposed for liquid level measurement in the industrial measurement field. For example, a sensor that detects the presence or absence of liquid or the liquid level by peeling off a part of the cladding part of an optical fiber to expose the core part and detecting the presence or absence of liquid or the liquid level based on changes in the amount of light transmitted through the optical fiber, or
Publication No. 18126 discloses a liquid level sensor in which a first optical path for transmitting incident light and a second optical path for transmitting reflected light are formed by optical fibers, and a prism is attached to one end of the optical fiber that becomes the open end of the optical fiber. etc. are disclosed.

(発明が解決しようとする問題点) 上記従来の液面計測センサの前者においては、
光フアイバのクラツド剥離部が、後者においては
プリズムの部分がセンサとして機能している。こ
のため液面レベルの測定領域はポイントであり、
1個のセンサで連続した液面レベルの変化を測定
することは不可能であつた。仮に連続した液面レ
ベルの変化を測定するためには、同様のセンサを
多数並べる必要があり、コストが高く分解能も不
十分であるという問題があつた。
(Problems to be solved by the invention) In the former of the above conventional liquid level measurement sensors,
The optical fiber cladding section, in the latter case the prism section, functions as a sensor. For this reason, the measurement area of the liquid level is a point;
It has been impossible to measure continuous changes in liquid level with one sensor. In order to measure continuous changes in liquid level, it would be necessary to line up a large number of similar sensors, resulting in high cost and insufficient resolution.

そこで本発明は、1本の光伝送路をある曲率半
径で曲げることにより、連続した液面レベルの変
化を測定可能とした簡易で安価な光伝送路を用い
た光学的液面レベルセンサを提供することを解決
すべき技術的課題とするものである。
Therefore, the present invention provides an optical liquid level sensor using a simple and inexpensive optical transmission line that can measure continuous changes in liquid level by bending one optical transmission line with a certain radius of curvature. This is a technical problem to be solved.

(問題点を解決するための手段) 上記課題解決のための技術的手段は、光フアイ
バの途中部分を液面レベル変化範囲に配置したう
え、前記光フアイバの一端部から入射された所定
光量の光が他端部において受光されたときの受光
量に基づいて液面のレベルを検出する光学式液面
レベルセンサにおいて、前記光フアイバの途中部
分を、巻き中心軸方向が前記液面レベル変化方向
に一致するように複数回巻きの単層コイル状に形
成したうえ、液面が低い場合の光の漏洩を抑制す
る一方、液面が高い場合の光の漏洩量を増加させ
ることによつて前記液面レベルの変化に対応して
前記受光量が直線的に変化するように前記コイル
状部の巻きピツチ、あるいは巻き直径を次第に変
化させた構成にすることである。
(Means for solving the problem) The technical means for solving the above problem is to arrange the middle part of the optical fiber in the liquid level change range, and to reduce the amount of light incident from one end of the optical fiber to a predetermined amount of light. In an optical liquid level sensor that detects the liquid level based on the amount of light received at the other end, a middle part of the optical fiber is wound so that the central axis direction is the liquid level change direction. In addition to forming the coil into a single-layer coil with multiple turns to match the above, it suppresses light leakage when the liquid level is low, while increasing the amount of light leakage when the liquid level is high. The present invention is to adopt a structure in which the winding pitch or winding diameter of the coiled portion is gradually changed so that the amount of light received changes linearly in response to changes in the liquid level.

(作用,原理) 次に、本発明の光学的液面レベルセンサにおけ
る液面計測の原理を第1図〜第3図に従つて説明
する。
(Operation, Principle) Next, the principle of liquid level measurement in the optical liquid level sensor of the present invention will be explained with reference to FIGS. 1 to 3.

最初に第1図を参照し屈折率nfを有する光伝送
路1の空気2中での光3の伝搬を考える。光伝送
路1と空気2との境界面に対して角度θで光3が
入射した場合、入射角θに対して光3の伝搬角は
θa=sin-1(na/nf)(但しnaは空気の屈折率)で
与えられる。すなわち入射角θがθa<θ≦90゜の
範囲では光3は左右の境界面で全反射を繰り返
し、光伝送路1内を伝搬していく。
First, with reference to FIG. 1, consider the propagation of light 3 in air 2 through optical transmission line 1 having a refractive index nf. When light 3 is incident on the interface between optical transmission line 1 and air 2 at an angle θ, the propagation angle of light 3 with respect to the incident angle θ is θa = sin -1 (na/nf) (however, na is refractive index of air). That is, when the incident angle θ is in the range θa<θ≦90°, the light 3 is repeatedly totally reflected at the left and right interfaces and propagates within the optical transmission path 1.

次に第2図に示すように、上記光伝送路1の一
部が屈折率nlを有する液相4と接している場合を
考える。液相4では光3の伝搬角はθl=sin-1
(nl/nf)で与えられ、入射角θがθl<θ≦90゜の
範囲では光3は減衰することなく伝搬していく。
しかし入射角θがθa<θ<θlの範囲の光3は放射
モードとなり急速に減衰していく。換言すれば、
光伝送路1のある範囲が液に浸されることによ
り、放射モードとなつた光3が漏洩光6として漏
洩してしまえば、あとは液面レベル5によらず一
定光量が伝搬する。このため所望の高さにわたる
液面レベル5の変化を、透過光強度により測定す
ることはできない。
Next, as shown in FIG. 2, consider a case where a part of the optical transmission line 1 is in contact with a liquid phase 4 having a refractive index nl. In liquid phase 4, the propagation angle of light 3 is θl=sin -1
It is given by (nl/nf), and the light 3 propagates without attenuation in the range where the incident angle θ is θl<θ≦90°.
However, the light 3 whose incident angle θ is in the range θa<θ<θl becomes a radiation mode and rapidly attenuates. In other words,
Once a certain range of the optical transmission path 1 is immersed in the liquid and the light 3 in the radiation mode leaks out as leaked light 6, a constant amount of light is propagated irrespective of the liquid level 5. Therefore, it is not possible to measure changes in the liquid level 5 over a desired height using transmitted light intensity.

次に第3図に示すように、前記光伝送路1を半
径Rで曲げた場合を考える。光伝送路1の直線部
より無反射で伝搬してきた光7は、光伝送路1の
R部の外側面で反射される。同様に液相4中を反
射しながら伝搬してきた光8も、光伝送路1の外
側及び内側R部で反射され伝搬していく。このと
き光伝送路1が半径Rで曲がつているために、伝
搬光の反射角度が変化する。このため反射角が
θa<θ<θlの範囲に変換されたものは新たに液相
放射モードとなり、液面レベル5の上昇に伴い、
透過光量が減少することになる。
Next, consider a case where the optical transmission line 1 is bent with a radius R as shown in FIG. The light 7 propagating without reflection from the straight portion of the optical transmission line 1 is reflected at the outer surface of the R portion of the optical transmission line 1. Similarly, the light 8 that has propagated while being reflected in the liquid phase 4 is also reflected at the outer and inner R portions of the optical transmission line 1 and propagates. At this time, since the optical transmission line 1 is curved with a radius R, the reflection angle of the propagating light changes. Therefore, the reflection angle converted to the range θa < θ < θl becomes a new liquid phase radiation mode, and as the liquid level 5 rises,
The amount of transmitted light will decrease.

この原理を応用して光伝送路1を大きな半径か
ら徐々に小さな半径となるように曲げることによ
り液面レベル5に応じて透過光量を減少させるこ
とが可能となり、この透過光量を計測することに
より液面レベル5を連続的に測定することができ
る。
By applying this principle and bending the optical transmission line 1 from a large radius to a gradually smaller radius, it is possible to reduce the amount of transmitted light according to the liquid level 5, and by measuring this amount of transmitted light. The liquid level 5 can be measured continuously.

(実施例) 次に本発明による光伝送路を用いた光学式液面
レベルセンサの実施例を図面に従つて説明する。
(Example) Next, an example of an optical liquid level sensor using an optical transmission line according to the present invention will be described with reference to the drawings.

第4図a,bは光フアイバ13を円柱14に巻
き付け、連続的に任意の曲率半径を持たせること
により形成した液面レベルセンサである。この液
面レベルセンサは図示していない発光ダイオード
などの光源からの光を光フアイバ13の一端11
より入射し、光フアイバ13を透過した光を受光
するための例えばフオトトランジスタを光フアイ
バ13の他端12側に設けたものである。第4図
aは光フアイバ13の巻きピツチを一定にした液
面レベルセンサである。この液面レベルセンサの
出力は、第5図aのような特性を有し、液面レベ
ルセンサの下部が、液相に浸つているときの光の
漏洩量が多く、液面レベルが上部に達するに従い
透過光量変化は少なくなる。そこで、第4図bに
示すように光フアイバの巻きピツチを始めは大き
くそして上になるに従つて徐々に小さくしていく
ことにより、液面が低い場合の光の急激な漏洩を
防ぎ、液面が高い場合の光の漏洩量を増加させ、
全体として第5図bのようなリニアな出力特性が
得られる。
4a and 4b show a liquid level sensor formed by winding an optical fiber 13 around a cylinder 14 and continuously giving it an arbitrary radius of curvature. This liquid level sensor transmits light from a light source such as a light emitting diode (not shown) to one end 11 of an optical fiber 13.
For example, a phototransistor is provided on the other end 12 side of the optical fiber 13 to receive light that has entered the optical fiber 13 and has passed through the optical fiber 13. FIG. 4a shows a liquid level sensor in which the winding pitch of the optical fiber 13 is constant. The output of this liquid level sensor has the characteristics shown in Figure 5a, where the lower part of the liquid level sensor leaks a large amount of light when immersed in the liquid phase, and the liquid level is higher than the upper part. The change in the amount of transmitted light decreases as it reaches this point. Therefore, as shown in Figure 4b, by making the winding pitch of the optical fiber large at the beginning and gradually decreasing it towards the top, we can prevent the sudden leakage of light when the liquid level is low and Increases the amount of light leakage when the surface is high,
As a whole, a linear output characteristic as shown in FIG. 5b is obtained.

また、光フアイバ13を巻く支柱の形状を第6
図に示すような上方になるに従つて徐々に曲率半
径が小さくなる形状の支柱14a,14bとする
ことによつてもリニアな出力特性が得られる。第
6図a及びcは円錐状の支柱14aの平面図及び
正面図であり、第6図b及びdは四角柱状の支柱
14bの平面図及び正面図である。
In addition, the shape of the support around which the optical fiber 13 is wound is changed to the sixth shape.
Linear output characteristics can also be obtained by forming the pillars 14a and 14b in a shape in which the radius of curvature gradually decreases toward the top as shown in the figure. FIGS. 6a and 6c are a plan view and a front view of the conical support 14a, and FIGS. 6b and d are a plan view and a front view of the quadrangular pillar 14b.

第6図bは四角柱のコーナーにRを持たせ、そ
の曲率半径を上にいくに従い小さくしたものであ
る。この支柱に巻かれた光フアイバは直線部とR
部を持つことになる。このように直線部とR部を
組合せてセンサ部を構成することにより光の漏洩
量を制御しやすく、より広範囲の液面計測ができ
る。
In Fig. 6b, the corners of a rectangular prism are rounded, and the radius of curvature decreases as it goes upward. The optical fiber wound around this support is connected to the straight part and R
will have a department. By configuring the sensor section by combining the straight section and the R section in this way, the amount of light leakage can be easily controlled and the liquid level can be measured over a wider range.

第7図は光フアイバ13を蛇行状にくねらせ連
続的に任意の曲率半径を持たせた液面レベルセン
サであり、並列に並べた支柱14に沿つて光フア
イバ13を蛇行状にくねらせている。
FIG. 7 shows a liquid level sensor in which an optical fiber 13 is twisted in a meandering manner to continuously give an arbitrary radius of curvature. There is.

また、光フアイバとしてプラスチツクフアイバ
を用いる場合は、これを円柱14に巻いて熱変形
させた後、支柱14を取り除いてもよい。尚、支
柱14は1本の棒でなく何本もの細い棒で構成し
てもよい。このことにより、光フアイバの液切れ
がよくなり、応答時間が短かくなる。しかし自動
車のガソリン液面レベル測定用としては、一般に
応答時間が遅い方が良いのでこの必要はない。
Further, when a plastic fiber is used as the optical fiber, the support 14 may be removed after being wound around the cylinder 14 and thermally deformed. Incidentally, the support 14 may be composed of several thin rods instead of one rod. This improves the drainage of the optical fiber and shortens the response time. However, this is not necessary for measuring the level of gasoline in an automobile, as it is generally better to have a slower response time.

第8図は、光学的に透明な誘電体基板10上
に、任意の曲率半径で曲げたリツジ形光伝送路9
を形成した液面レベルセンサである。発光ダイオ
ードなどの光源からの光をリツジ形光伝送路9の
一端11より入射し、透過光を受光する例えばフ
オトトランジスタをリツジ形光伝送路9の他端側
12に設けるものである。また、リツジ形光伝送
路9の曲率半径は、タンク底面で大きく、上にい
くに従つて徐々に小さくしていく。このことによ
り液面が低い位置での光の漏洩量を少なくし、液
面レベルに対してリニアな出力特性が得られる。
この光の漏洩量はリツジ形光伝送路9の曲率半
径,巾,屈折率及び被測定液体の屈折率によつて
決まる。
FIG. 8 shows a ridge-shaped optical transmission line 9 bent at an arbitrary radius of curvature on an optically transparent dielectric substrate 10.
This is a liquid level sensor with a Light from a light source such as a light emitting diode is incident on one end 11 of the rigid optical transmission line 9, and a phototransistor, for example, for receiving transmitted light is provided at the other end 12 of the rigid optical transmission line 9. Further, the radius of curvature of the rod-shaped optical transmission line 9 is large at the bottom of the tank, and gradually decreases as it goes upward. This reduces the amount of light leakage at locations where the liquid level is low, and provides output characteristics that are linear with respect to the liquid level.
The amount of light leakage is determined by the radius of curvature, width, and refractive index of the ridge-shaped optical transmission line 9 and the refractive index of the liquid to be measured.

また第8図のリツジ形光伝送路9(屈折率nf)
に屈折率nc(nc<nf)の光学的に透明な材質によ
りクラツド層を設けると、クラツド層の作用によ
り、光伝送路より大きな屈折率を持つ液相に対し
ても液面レベルの連続した変化を測定できる。
Also, the rigid optical transmission line 9 (refractive index nf) in Fig. 8
When a cladding layer is provided with an optically transparent material with a refractive index nc (nc<nf) on Changes can be measured.

(発明の効果) 以上のように本発明によれば、光フアイバの途
中部分を液面レベル変化範囲に配置したうえ、前
記光フアイバの一端部から入射された所定光量の
光が他端部において受光されたときの受光量に基
づいて液面のレベルを検出する光学式液面レベル
センサにおいて、前記光フアイバの途中部分を、
巻き中心軸方向が前記液面レベル変化方向に一致
するように複数回巻きの単層コイル状に形成した
うえ、液面が低い場合の光の漏洩を抑制する一
方、液面が高い場合の光の漏洩量を増加させるよ
うに前記コイル状部の巻きピツチ、あるいは巻き
直径を次第に変化させる構成にしたため、簡単な
構成で安価に前記液面レベルを直線的に検出する
ことができるという効果がある。
(Effects of the Invention) As described above, according to the present invention, the middle part of the optical fiber is disposed in the liquid level change range, and a predetermined amount of light incident from one end of the optical fiber is transmitted to the other end. In an optical liquid level sensor that detects the liquid level based on the amount of light received when the light is received, the intermediate part of the optical fiber is
The coil is formed into a single-layer coil with multiple turns so that the direction of the winding center axis coincides with the direction of the liquid level change, and it suppresses light leakage when the liquid level is low, while suppressing light leakage when the liquid level is high. Since the winding pitch or the winding diameter of the coiled portion is configured to be gradually changed so as to increase the amount of leakage, the liquid level can be detected linearly at low cost with a simple configuration. .

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

第1図は光伝送路の光の伝搬特性を示す原理説
明図、第2図は光伝送路の1部が液相と接してい
るときの光の伝搬特性を示す原理説明図、第3図
は半径Rで曲げた光伝送路の1部を液相に浸した
ときの光の伝搬特性を示す原理説明図である。以
下図面は実施例に係り、第4図aは光フアイバを
円柱面にピツチ一定で巻いた液面レベルセンサの
外観図、第4図bは光フアイバを円柱面にピツチ
を徐々に変化させて巻いた液面レベルセンサの外
観図、第5図aは第4図aに示した液面レベルセ
ンサの出力特性図、第5図bは第4図bに示した
液面レベルセンサの出力特性図、第6図aは液面
レベルセンサにリニアな出力特性を持たせるため
の円錐形支柱の平面図、第6図cは第6図aの正
面図、第6図bは四角柱状支柱の平面図、第6図
dは第6図bの正面図である。第7図は光フアイ
バを蛇行状に形成した液面レベルセンサの外観
図、第8図aは基板上に形成されたリツジ形光伝
送路を備えた液面レベルセンサの外観図、第8図
bは第8図aのA−A′矢視断面図である。 9…リツジ形光伝送路、10…基板、11…光
入射位置、12…フオトトランジスタ取付位置、
13…光フアイバ、14…円柱、14a…円錐形
支柱、14b…四角柱状支柱。
Fig. 1 is a principle explanatory diagram showing the light propagation characteristics of an optical transmission line, Fig. 2 is a principle explanatory diagram showing the light propagation characteristics when a part of the optical transmission line is in contact with a liquid phase, and Fig. 3 1 is a principle explanatory diagram showing light propagation characteristics when a part of an optical transmission line bent with a radius R is immersed in a liquid phase. The following drawings relate to embodiments: Fig. 4a is an external view of a liquid level sensor in which an optical fiber is wound on a cylindrical surface with a constant pitch, and Fig. 4b is an external view of a liquid level sensor in which an optical fiber is wound on a cylindrical surface with a gradually changing pitch. An external view of the rolled liquid level sensor, Fig. 5a shows the output characteristics of the liquid level sensor shown in Fig. 4a, and Fig. 5b shows the output characteristics of the liquid level sensor shown in Fig. 4b. Figure 6a is a plan view of a conical column for providing linear output characteristics to the liquid level sensor, Figure 6c is a front view of Figure 6a, and Figure 6b is a square columnar column. The plan view, FIG. 6d, is a front view of FIG. 6b. Fig. 7 is an external view of a liquid level sensor with optical fibers formed in a meandering shape, Fig. 8a is an external view of a liquid level sensor with a ridge-shaped optical transmission path formed on a substrate, Fig. 8 b is a sectional view taken along the line A-A' in FIG. 8a. 9...Rigid optical transmission line, 10...Substrate, 11...Light incident position, 12...Phototransistor mounting position,
13... Optical fiber, 14... Cylindrical column, 14a... Conical support, 14b... Square columnar support.

Claims (1)

【特許請求の範囲】 1 光フアイバの一端から入射された所定光量の
光が気相と液相の屈折率差に応じて漏洩したあと
の受光光量に基づいて液面レベルを検出する光学
式液面レベルセンサにおいて、 前記受光光量が液面レベルの変化に対してリニ
アに変化するように巻きピツチを次第に変化させ
る形状に前記光フアイバを円柱状、もしくは円筒
状の巻芯に単層コイル状に巻いたことを特徴とす
る光学式液面レベルセンサ。 2 光フアイバの一端から入射された所定光量の
光が気相と液相の屈折率差に応じて漏洩したあと
の受光光量に基づいて液面レベルを検出する光学
式液面レベルセンサにおいて、 前記受光光量が液面レベルの変化に対してリニ
アに変化するように前記光フアイバを円錐状、も
しくは角錐状の巻芯に単層コイル状に巻いたこと
を特徴とする光学式液面レベルセンサ。
[Claims] 1. An optical liquid that detects the liquid level based on the amount of light received after a predetermined amount of light incident from one end of an optical fiber leaks according to the refractive index difference between the gas phase and the liquid phase. In the surface level sensor, the optical fiber is wound in a cylindrical shape or in a single-layer coil around a cylindrical core in a shape that gradually changes the winding pitch so that the amount of received light changes linearly with changes in the liquid level. An optical liquid level sensor characterized by a coiled surface. 2. In an optical liquid level sensor that detects the liquid level based on the amount of light received after a predetermined amount of light incident from one end of an optical fiber leaks according to the refractive index difference between the gas phase and the liquid phase, the above-mentioned An optical liquid level sensor characterized in that the optical fiber is wound in a single-layer coil around a conical or pyramidal core so that the amount of received light changes linearly with changes in the liquid level.
JP21106086A 1986-09-08 1986-09-08 Optical liquid level sensor Granted JPS6365321A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP21106086A JPS6365321A (en) 1986-09-08 1986-09-08 Optical liquid level sensor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP21106086A JPS6365321A (en) 1986-09-08 1986-09-08 Optical liquid level sensor

Publications (2)

Publication Number Publication Date
JPS6365321A JPS6365321A (en) 1988-03-23
JPH0367579B2 true JPH0367579B2 (en) 1991-10-23

Family

ID=16599732

Family Applications (1)

Application Number Title Priority Date Filing Date
JP21106086A Granted JPS6365321A (en) 1986-09-08 1986-09-08 Optical liquid level sensor

Country Status (1)

Country Link
JP (1) JPS6365321A (en)

Families Citing this family (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
ES2294950B1 (en) * 2006-09-28 2009-02-01 Universidad De Cantabria OPTICAL FIBER SENSOR SYSTEM FOR LIQUID LEVEL MEASUREMENT IN TANKS.
ES2339205B1 (en) * 2008-02-13 2011-03-11 Universidad Carlos Iii De Madrid ULTRALIGEROS FUEL LEVEL MEASUREMENT SYSTEM.
CN105444839B (en) * 2015-11-18 2019-09-20 中北大学 Plastic optical fiber liquid level sensor and measurement method based on optical time domain reflectometry
GB2576773A (en) 2018-08-31 2020-03-04 Advanced Fibreoptic Eng Ltd Fluid level sensing device and method

Family Cites Families (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5199049A (en) * 1975-02-10 1976-09-01 Shiro Okamura
JPS55134321A (en) * 1979-04-06 1980-10-20 Toshiba Corp Liquid level detector
JPS55134322A (en) * 1979-04-06 1980-10-20 Toshiba Corp Liquid level detector
SE7903175L (en) * 1979-04-10 1980-10-11 Asea Ab FIBEROPTICAL METDON
DE3144541C2 (en) * 1981-11-10 1984-05-24 Wolfram 8501 Allersberg Henning Rod-like device for detecting the level of liquids in containers, channels or the like.

Also Published As

Publication number Publication date
JPS6365321A (en) 1988-03-23

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