JPH073296Y2 - Vortex detector and vortex detector - Google Patents

Vortex detector and vortex detector

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Publication number
JPH073296Y2
JPH073296Y2 JP1989025732U JP2573289U JPH073296Y2 JP H073296 Y2 JPH073296 Y2 JP H073296Y2 JP 1989025732 U JP1989025732 U JP 1989025732U JP 2573289 U JP2573289 U JP 2573289U JP H073296 Y2 JPH073296 Y2 JP H073296Y2
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JP
Japan
Prior art keywords
vortex
light
optical
thin plate
plate
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.)
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JP1989025732U
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Japanese (ja)
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JPH02118225U (en
Inventor
宏 山本
Original Assignee
オーバル機器工業株式会社
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Description

【考案の詳細な説明】 技術分野 本考案は、光弾性効果を応用した渦検出素子及び該渦検
出素子を利用した渦検出器に関するものである。
Description: TECHNICAL FIELD The present invention relates to a vortex detecting element to which a photoelastic effect is applied and a vortex detector using the vortex detecting element.

従来技術 流体流内に渦発生体を配設するカルマン渦が発生し、該
カルマン渦の単位時間当りの発生数は流速に比例するこ
とを利用した渦流量計は知られている。該渦流量計にお
いて発生した渦を検出する検出手段には、従来、多くの
方式が提案され実用されている。その一つに、渦放出に
伴って生ずる変動圧力を検出する方法がある。この変動
圧力は受圧要素の変動圧力により変化するひずみ量の変
化として電気信号に変換しているが、受圧要素には圧電
素子、静電容量がある。これらの受圧要素からなる検出
器は出力インピーダンスが高く電磁的なノイズを受け易
いという問題がある。これに対して光検出器は電磁ノイ
ズを受けることがないので最近では光検出方式が注目さ
れている。光検出方式のなかには例えば光反射方式があ
る。これは渦発生体に穿設した凹部底面に光反射板を渦
発生体軸に直交して埋設し該光反射板に向けて軸芯から
光を照射する。一方、渦発生体には渦発生に伴って繰返
し曲げ応力が作用するので、渦発生体は静止軸まわりに
振動し、該振動は凹部底面の前記光反射板を対称軸まわ
りに回転変動し、これに従って投射光は軸まわりに振動
する。この振動は渦変動周波数に等しいので、前記光反
射板からの反射光を光強度に変換することにより渦検出
するものである。また、光検出方式の他の方式として光
弾性を利用したものがある。渦発生体軸に平行して光フ
ァイバを埋設し、渦発生体の曲げ変動に伴って該光ファ
イバに作用する応力変動による光強度の変化として渦を
検出するものである。
2. Description of the Related Art A vortex flowmeter is known in which a Karman vortex in which a vortex generator is arranged is generated in a fluid flow, and the number of Karman vortices generated per unit time is proportional to a flow velocity. As a detection means for detecting a vortex generated in the vortex flowmeter, many methods have been proposed and put into practical use. As one of them, there is a method of detecting a fluctuating pressure generated due to vortex shedding. This fluctuating pressure is converted into an electric signal as a change in strain amount that changes according to the fluctuating pressure of the pressure receiving element, and the pressure receiving element includes a piezoelectric element and an electrostatic capacitance. The detector composed of these pressure receiving elements has a problem that it has a high output impedance and is susceptible to electromagnetic noise. On the other hand, since the photodetector does not receive electromagnetic noise, the photodetection method has recently attracted attention. Among the light detection methods is, for example, the light reflection method. In this, a light reflection plate is embedded in the bottom surface of the recess formed in the vortex generator so as to be orthogonal to the axis of the vortex generator, and light is emitted from the axis toward the light reflection plate. On the other hand, since the bending stress is repeatedly applied to the vortex generator as the vortex is generated, the vortex generator vibrates around the stationary axis, and the vibration causes the light reflection plate on the bottom surface of the recess to rotate and rotate about the symmetry axis. According to this, the projected light vibrates around the axis. Since this vibration is equal to the vortex fluctuation frequency, the vortex is detected by converting the reflected light from the light reflection plate into light intensity. Further, as another method of the light detection method, there is one using photoelasticity. An optical fiber is embedded parallel to the axis of the vortex generator, and the vortex is detected as a change in light intensity due to a stress variation acting on the optical fiber due to a bending variation of the vortex generator.

従来技術の問題点 上述した従来の渦流量計の光検出方式においては、光反
射方式のものは光感度を増すためには必要な光路長を選
ばなければならないが、光路長を増大することは外部振
動の影響を受け易く、雑音が発生しやすくなる。更に温
度変化、特に露点以下に温度が低下すると結露して反射
能を著しく損い検出不能となるという問題点があり、ま
た、光弾性方式のものは光ファイバの光量が小さく、ま
た感度も小さい。感度向上のためには光路長を長くする
必要があり、小形の渦流量計に適用することは困難であ
るという問題点がある。
Problems of the Prior Art In the above-described conventional vortex flowmeter photodetection method, the light reflection type must select the required optical path length in order to increase the photosensitivity, but it is not possible to increase the optical path length. It is easily affected by external vibration and noise is likely to occur. Furthermore, there is a problem that when the temperature changes, especially when the temperature drops below the dew point, dew condensation occurs and the reflectivity is significantly impaired, making detection impossible. In addition, the photoelastic type has a small amount of light in the optical fiber and also has low sensitivity. . In order to improve the sensitivity, it is necessary to increase the optical path length, which is a problem that it is difficult to apply to a small vortex flowmeter.

問題点解決のための手段 本考案は、結露等の問題点のある光反射方式によらず光
弾性方式において高感度でS/Nの優れた渦検出素子を提
供することを目的とするもので、渦検出素子を、渦変動
圧力に応動し、変動圧力を該変動圧力に比例した光学量
の変化として検知し、該光学量の変化から渦を検知する
検出素子を具備した渦流量計において、検出素子を光導
体薄板と、該光導体薄板の面に平行した直線上の両側端
に僅かに隔てて対向固着した光導通可能な光導体ファイ
バと、前記光導体薄板と光導体ファイバとを外部光を遮
断し、一体的に囲繞する光不良導で可撓性の遮光膜とか
ら構成した渦検出素子とするものである。
Means for Solving Problems The present invention is intended to provide a vortex detection element having high sensitivity and excellent S / N in a photoelastic method regardless of a light reflection method having a problem such as dew condensation. A vortex flowmeter provided with a detection element that responds to the vortex fluctuation pressure, detects the fluctuation pressure as a change in an optical amount proportional to the fluctuation pressure, and detects a vortex from the change in the optical amount. A light-conducting thin plate, a light-conducting optical fiber having a light-conducting thin plate and a light-conducting fiber that are fixed to each other at opposite ends on a straight line parallel to the surface of the light-conducting thin plate at a slight distance from each other. The eddy detection element is composed of a light-shielding film which is light-shielding and which surrounds and is integrally surrounded by a light-defective conductor.

実施例 第1図は、本考案の渦検出素子の概要説明図であり、
(a)図は要部光弾性の光導通路の構成を示す斜視図、
(b)図は(c)図のX-X線断面図、(c)図は平面図
を示す。図において、1は渦変動圧力を受圧し、光量の
変化として光検出する光導体の極めて薄い、例えば0.2m
m程度のガラス板またはアクリル板である。図示のもの
は矩形であるが、この形に限られたものではなく円形で
もよく光弾性を受ける光導体薄板であればよい。図示の
矩形板では光導入、導出の部を各々の矩形の端面11、12
としている。21、22は光導体ファイバで、これらは複数
本のガラス光ファイバ又は樹脂光ファイバ21a〜21n、2
2a〜22nからなり、21の一端は図示しない端部Aは光源
に、また、22の図示しない端部Bは光電変換器に接続さ
れ、それぞれの他端側は複数の光導体ファイバ21a,
21b,…,21nおよび22a,22b,…,22nが光導体薄板1に
対して各々が平行に平面状に配置される。31は保持板で
前記各々の光導体ファイバを平行のまま固着する光導体
ファイバの一種の固定板である。保持板31と光導体薄板
1とを例えば接合光導体にて光導体を持たせた状態で接
合すると、光結合損失を防ぎ、空間内における状態変化
例えば結露等光伝達上の不安定性を防ぐことができる。
しかし、上述の目的が組立の方法等において達せられれ
ばこの接合光導体は必ずしも必要とするものではなく、
図には、接合光導体を具備しない例が示されている。6
は光不良導体で可撓性のある樹脂からなり、(a)図に
示した光検出要部を遮光するように囲繞する可撓性の遮
光膜である。7は保護チューブで光導体ファイバ21、22
を挿通して保護し遮光膜6に接合するものである。51、5
2は光導体薄板1を遮光膜6で囲繞する際、光導体薄膜
1を保護する光導性膜で、光導体薄板1よりも屈折率の
小さい材質が選ばれる。叙上の如く構成された渦検出素
子は、(a)図に示す如く、渦変動圧力ΔPを端面11、1
2が固定されて配設された光導体薄板1に受けると、渦
変動圧力ΔPの作用方向である矢視方向に弾性変形を受
け、光弾性効果により光源A側から検出B側へ向けての
光量が減少する。この光量変化は渦変動によるものであ
るから、光量変化により渦信号として電気信号に変換で
きる。
Example FIG. 1 is a schematic explanatory view of a vortex detection element of the present invention,
(A) The figure is a perspective view showing the structure of the optical path of the main part photoelastic
The figure (b) shows a sectional view taken along line XX of the figure (c), and the figure (c) shows a plan view. In the figure, 1 is an extremely thin optical conductor, for example 0.2 m, which receives vortex fluctuation pressure and detects light as a change in light quantity.
It is a glass plate or acrylic plate of about m. Although the shape shown in the figure is rectangular, the shape is not limited to this, and it may be circular as long as it is a photoconductor thin plate that receives photoelasticity. In the illustrated rectangular plate, the light introduction and derivation parts are the end faces 1 1 and 1 2 of each rectangle.
I am trying. 2 1 and 2 2 are optical conductor fibers, which are a plurality of glass optical fibers or resin optical fibers 2 1a to 2 1n , 2
2a consists to 2 2n, 2 1 of one end the end portion A of the light source (not shown), also of 2 2 not shown end B is connected to the photoelectric converter, each other end a plurality of optical waveguide fibers 2 1a ,
2 1b, ..., 2 1n and 2 2a, 2 2b, ..., 2 2n is that each relative to the optical conductor sheet 1 is arranged in parallel planar. 3 1 is a fixed plate of one of the optical conductor fiber for fixing remain parallel optical waveguide fibers of each said at holding plate. When the holding plate 3 1 and the thin optical conductor plate 1 are joined together, for example, with a joined optical conductor, the optical coupling loss is prevented, and a change in state in space, such as instability in light transmission such as dew condensation, is prevented. be able to.
However, if the above-mentioned object can be achieved by the method of assembly, etc., this junction light guide is not always necessary,
In the figure, an example without a junction light guide is shown. 6
Is a flexible light-shielding film which is a light-defective conductor and is made of a flexible resin, and surrounds the main part of the light detection shown in FIG. 7 is a protective tube, which is a light guide fiber 2 1 , 2 2
Is to be inserted and protected to be bonded to the light shielding film 6. 5 1 , 5
Reference numeral 2 denotes a light-transmitting film that protects the light guide thin film 1 when the light guide thin plate 1 is surrounded by the light shielding film 6, and a material having a smaller refractive index than the light guide thin plate 1 is selected. Vortex sensing element which is constructed as the Jo, (a) as shown in FIG, the end face 1 1, 1 a vortex variable pressure ΔP
When 2 is received by the fixedly arranged photoconductor thin plate 1, it is elastically deformed in the direction of the arrow, which is the direction of action of the vortex fluctuation pressure ΔP, and the photoelastic effect causes a change from the light source A side to the detection B side. The amount of light decreases. Since this change in the light amount is due to the vortex fluctuation, it can be converted into an electrical signal as a vortex signal by the change in the light amount.

第2図は、他の実施例を示すもので、8は偏光子で、保
持板31と光導体薄板1との間に平行して配置され、光源
A側からの光を直線偏光する。9は1/4波長板、10は検
光子で各々順次に光導体薄板1と保持板32との間に平行
して配置され、第1図の実施例と同様、遮光薄膜6で遮
光して光導通路を一体形成するが、図においては省略し
ている。偏光子8により直線偏光した光が光導体薄板1
に入光し、1/4波長板9により円偏光後、検光子10によ
り光検出されるが、光導体薄板1が渦変動圧力ΔPを受
けることにより光回転を生じ1/4波長板9において楕円
偏光となり検光子10の通過光は圧力に応じた光量変化を
受け、第1図に述べた如く渦信号を検出できる。
FIG. 2, shows another embodiment, 8 is a polarizer, arranged in parallel between the holding plate 3 1 and the light conductor sheet 1, linearly polarized light from a light source A side. 9 quarter-wave plate, 10 is arranged in parallel between each successively to the optical conductor sheet 1 and the holding plate 3 2 in the analyzer, as in the embodiment of FIG. 1, is shielded by the light shielding film 6 Although the light guide path is integrally formed with this, it is omitted in the drawing. Light linearly polarized by the polarizer 8 is the light guide thin plate 1
After being incident on the 1/4 wavelength plate 9 and circularly polarized by the 1/4 wavelength plate 9, the light is detected by the analyzer 10. However, when the light guide thin plate 1 receives the vortex fluctuation pressure ΔP, light rotation occurs and It becomes elliptically polarized light, and the light passing through the analyzer 10 undergoes a change in the amount of light according to the pressure, and the vortex signal can be detected as described in FIG.

第3図は、上述の渦検出器を装着した渦流量計の実施例
で、(a)図は(b)図のY-Y矢視平断面図、(b)図
は(a)図の流れ方向QからみたX-X線断面図である。
図において、11は渦流量計の本体で、上流側が拡大し下
流側が平行な流路をなす断面矩形をしている。12は整流
格子で流れを整流する格子状体で、13は渦発生体で代表
として断面三角形状で示している。100は本考案の渦検
出素子で、本体11の下流側で渦発生体13近傍の側面に該
側面と同一な面に配設され、流れを乱すことのないよう
にしている。14は渦検出素子100の後面に空室15を形成
する外筐であり、16は本体11内と等しい静圧を空室15に
与えるための導通路であり、渦発生体13を挟んで本体13
の両側面に配設されている。叙上の渦流量計においては
渦検出素子100は本体11と平行に且つ内壁面から突起し
ないように配設されるので流体を乱すことがなくS/Nの
優れた検出ができる。両側面の渦検出素子100は紙面に
同一方向の渦変動圧力を受けるので、各々の渦信号は同
期して倍加される。
FIG. 3 shows an embodiment of the vortex flowmeter equipped with the above-mentioned vortex detector. (A) is a horizontal sectional view taken along the line YY in (b), and (b) is a flow direction in (a). It is the XX sectional view seen from Q.
In the figure, reference numeral 11 is a main body of the vortex flowmeter, which has a rectangular cross section in which the upstream side is enlarged and the downstream side is a parallel flow path. Reference numeral 12 is a grid-like body that rectifies the flow by a rectifying grid, and 13 is a vortex generator, which is shown as a typical triangular section. Reference numeral 100 denotes a vortex detecting element of the present invention, which is disposed on the side surface near the vortex generator 13 on the downstream side of the main body 11 and on the same surface as the side surface so as not to disturb the flow. Reference numeral 14 is an outer casing that forms an empty chamber 15 on the rear surface of the vortex detection element 100, and 16 is a conduction path for applying a static pressure equal to that in the main body 11 to the empty chamber 15, with the main body sandwiching the vortex generator 13. 13
Are disposed on both side surfaces of. In the above vortex flowmeter, the vortex detection element 100 is arranged parallel to the main body 11 and so as not to project from the inner wall surface, so that excellent S / N can be detected without disturbing the fluid. Since the vortex detection elements 100 on both sides receive vortex fluctuation pressure in the same direction on the paper surface, each vortex signal is synchronously doubled.

第4図は流管が円形の場合の実施例で、20は円管、21は
渦発生体、24は渦発生体21中央部に渦検出素子100を収
納する空室で22、23は該空室24と渦発生体21側面とを連
通する圧力導入孔で渦検出素子100に渦変動圧力ΔPを
作用させるもので、渦検出素子100は1個でよく、空室2
4を設けることによる積分効果によって微小な変動圧を
除きS/Nを向上させることができる。
FIG. 4 shows an embodiment in which the flow tube is circular, 20 is a circular tube, 21 is a vortex generator, 24 is a vacant chamber for accommodating the vortex detecting element 100 in the central portion of the vortex generator 21, and 22 and 23 are The vortex fluctuation pressure ΔP is applied to the vortex detection element 100 by the pressure introduction hole that connects the vacancy chamber 24 and the side surface of the vortex generator 21. Only one vortex detection element 100 is required.
The S / N can be improved by removing the minute fluctuating pressure by the integration effect of providing 4.

効果 叙上の如く、本考案の渦検出素子によれば、光検出によ
る渦信号変換であるため渦流量計近傍で受ける電磁ノイ
ズもなく、また、光検出方式においても光反射を応用し
た光てこではなく直接受圧するので外部振動の影響も受
けずS/Nの優れた渦信号を得ることができる。しかも従
来技術の如く微細な光ファイバを利用した光弾性ではな
く線上に配置された光導体ファイバからの光となり、面
として受圧するため光量も多くなるので、渦信号は格段
に大きくなり、安定した光渦信号が安価に得られる。
Effect As described above, according to the vortex detector of the present invention, since the vortex signal conversion is performed by light detection, there is no electromagnetic noise received near the vortex flowmeter, and the optical lever that applies light reflection is used in the light detection method. Instead of directly receiving pressure, it is possible to obtain an excellent S / N vortex signal without being affected by external vibration. Moreover, the light is not from the photoelasticity using the fine optical fiber as in the prior art, but from the optical conductor fiber arranged on the line, and the amount of light is increased because it receives pressure as a surface, so the vortex signal becomes significantly large and stable. The optical vortex signal can be obtained at low cost.

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

第1図は、本考案の渦検出素子で、(a)図は要部斜視
図、(b)図は(c)図のX-X矢視断面図、(c)図は
平面図、第2図は、他の実施例、第3図、第4図は、各
々本考案の渦検出素子を装着した渦流量計を示す図であ
る。 1……光導体薄板、21,22……光導体ファイバ、31,32
…保持板、6……遮光膜、8……偏光子、9……1/4波
長板、10……検光子。
FIG. 1 is a vortex detection element of the present invention, in which (a) is a perspective view of essential parts, (b) is a sectional view taken along the line XX of (c), (c) is a plan view, and FIG. FIG. 3 shows another embodiment, and FIGS. 3 and 4 are views showing a vortex flowmeter equipped with the vortex detecting element of the present invention. 1 ... Light guide thin plate, 2 1 , 2 2 ...... Light guide fiber, 3 1 , 3 2
... Holding plate, 6 ... Shading film, 8 ... Polarizer, 9 ... Quarter wave plate, 10 ... Analyzer.

Claims (4)

【実用新案登録請求の範囲】[Scope of utility model registration request] 【請求項1】渦による変動圧力を、該変動圧力に比例し
た光学量の変化として検知し、該光学量の変化から渦を
検出する渦流量計の検出素子において、面と直角方向に
前記変動圧力を受圧する光導体薄板と、該光導体薄板の
面に平行した両側端面に対向して配設された光導体ファ
イバと、非透光性の可撓材で前記光導体薄板と光導体フ
ァイバとを一体に囲繞する遮光膜とからなることを特徴
とする渦検出素子。
1. A detecting element of a vortex flowmeter for detecting a fluctuating pressure due to a vortex as a change in an optical amount proportional to the fluctuating pressure and detecting a vortex from the change in the optical amount, wherein the fluctuating direction is perpendicular to a plane. An optical conductor thin plate for receiving pressure, an optical conductor fiber arranged opposite to both end faces parallel to the surface of the optical conductor thin plate, the optical conductor thin plate and the optical conductor fiber made of a non-translucent flexible material. And a light-shielding film that integrally surrounds the vortex detection element.
【請求項2】前記光導体ファイバと光導体薄板との間
に、入光側には偏光板と、出光側には1/4波長板を各々
配設したことを特徴とする請求項1に記載の渦検出素
子。
2. A polarizing plate on the light-incident side and a quarter-wave plate on the light-exiting side are provided between the optical conductor fiber and the thin optical conductor plate, respectively. The eddy detection element described.
【請求項3】渦発生体と、該渦発生体を軸対称に配設し
た矩形断面の流管とからなる渦流量計本体において、面
と直角方向に前記変動圧力を受圧する光導体薄板と、該
光導体薄板の面に平行した両側端面に対向して配設され
た光導体ファイバと、非透光性の可撓材で前記光導体薄
板と光導体ファイバとを一体に囲繞する遮光膜とからな
る渦検出素子を有し、前記渦発生体近傍の前記流管の管
壁に、渦検出素子を前記管壁と同一面に配設し、該渦検
出素子の他の面に前記流管に連通する空室を配設したこ
とを特徴とする渦検出器。
3. A vortex flowmeter body comprising a vortex generator and a flow tube having a rectangular cross section in which the vortex generator is arranged in axial symmetry, and a thin optical conductor plate for receiving the fluctuating pressure in a direction perpendicular to a plane. A light-shielding film that integrally surrounds the light-conducting thin plate and the light-conducting fiber with a non-light-transmitting flexible material, the light-conducting fibers being disposed so as to face both end surfaces parallel to the surface of the light-conducting thin plate. And a vortex detecting element disposed on the same surface as the tube wall on the tube wall of the flow tube near the vortex generator, and the vortex detecting element is formed on the other surface of the vortex detecting element. A vortex detector characterized in that an empty chamber communicating with the pipe is provided.
【請求項4】面と直角方向に前記変動圧力を受圧する光
導体薄板と、該光導体薄板の面に平行した両側端面に対
向して配設された光導体ファイバと、非透光性の可撓材
で前記光導体薄板と光導体ファイバとを一体に囲繞する
遮光膜とからなる渦検出素子を有し、流れと直角な方向
に渦発生体を貫通した貫通孔内に、該貫通孔を閉止する
前記渦検出素子を該渦検出素子の面と流れ方向と平行に
配設したことを特徴とする渦検出器。
4. A light guide thin plate for receiving the fluctuating pressure in a direction perpendicular to the surface, light guide fibers arranged opposite to both end faces parallel to the face of the light guide thin plate, and a non-translucent material. A through-hole is formed in a through-hole that penetrates the vortex generator in a direction perpendicular to the flow, and has a vortex detecting element formed of a flexible material and a light-shielding film that integrally surrounds the optical-conductor thin plate and the optical-conductor fiber. A vortex detector characterized in that the vortex detecting element for closing the vortex is arranged in parallel to the surface of the vortex detecting element and the flow direction.
JP1989025732U 1989-03-07 1989-03-07 Vortex detector and vortex detector Expired - Lifetime JPH073296Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1989025732U JPH073296Y2 (en) 1989-03-07 1989-03-07 Vortex detector and vortex detector

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1989025732U JPH073296Y2 (en) 1989-03-07 1989-03-07 Vortex detector and vortex detector

Publications (2)

Publication Number Publication Date
JPH02118225U JPH02118225U (en) 1990-09-21
JPH073296Y2 true JPH073296Y2 (en) 1995-01-30

Family

ID=31246725

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1989025732U Expired - Lifetime JPH073296Y2 (en) 1989-03-07 1989-03-07 Vortex detector and vortex detector

Country Status (1)

Country Link
JP (1) JPH073296Y2 (en)

Family Cites Families (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5414565U (en) * 1977-07-01 1979-01-30
JPS601564B2 (en) * 1979-08-30 1985-01-16 横河電機株式会社 transducer
JPS6219937Y2 (en) * 1981-01-20 1987-05-21
JPS59180435A (en) * 1983-03-31 1984-10-13 Fuji Electric Co Ltd Karman vortex flowmeter

Also Published As

Publication number Publication date
JPH02118225U (en) 1990-09-21

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