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JPH038695B2 - - Google Patents
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JPH038695B2 - - Google Patents

Info

Publication number
JPH038695B2
JPH038695B2 JP58148928A JP14892883A JPH038695B2 JP H038695 B2 JPH038695 B2 JP H038695B2 JP 58148928 A JP58148928 A JP 58148928A JP 14892883 A JP14892883 A JP 14892883A JP H038695 B2 JPH038695 B2 JP H038695B2
Authority
JP
Japan
Prior art keywords
vortex
hollow body
pressure introduction
introduction hole
flow
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
JP58148928A
Other languages
Japanese (ja)
Other versions
JPS6040914A (en
Inventor
Katsuo Misumi
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.)
OBARA KIKI KOGYO KK
Original Assignee
OBARA KIKI KOGYO 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 OBARA KIKI KOGYO KK filed Critical OBARA KIKI KOGYO KK
Priority to JP58148928A priority Critical patent/JPS6040914A/en
Priority to US06/637,924 priority patent/US4683760A/en
Priority to DE8484109373T priority patent/DE3476449D1/en
Priority to EP84109373A priority patent/EP0137945B1/en
Priority to CA000461004A priority patent/CA1228752A/en
Priority to KR1019840004876A priority patent/KR890004447B1/en
Publication of JPS6040914A publication Critical patent/JPS6040914A/en
Publication of JPH038695B2 publication Critical patent/JPH038695B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01FMEASURING VOLUME, VOLUME FLOW, MASS FLOW OR LIQUID LEVEL; METERING BY VOLUME
    • G01F1/00Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow
    • G01F1/05Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow by using mechanical effects
    • G01F1/20Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow by using mechanical effects by detection of dynamic effects of the flow
    • G01F1/32Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow by using mechanical effects by detection of dynamic effects of the flow using swirl flowmeters
    • G01F1/325Means for detecting quantities used as proxy variables for swirl
    • G01F1/3282Means for detecting quantities used as proxy variables for swirl for detecting variations in infrasonic, sonic or ultrasonic waves, due to modulation by passing through the swirling fluid

Landscapes

  • Physics & Mathematics (AREA)
  • Fluid Mechanics (AREA)
  • General Physics & Mathematics (AREA)

Description

【発明の詳細な説明】 技術分野 本発明は、流体中に配設された渦発生体により
発生されるカルマン渦を利用した渦流量計に関す
る。
TECHNICAL FIELD The present invention relates to a vortex flowmeter that utilizes a Karman vortex generated by a vortex generator disposed in a fluid.

従来技術 周知のように、流体中に柱状の渦発生体を挿入
すると、該渦発生体の両側面で流れが剥離し、該
渦発生体の下流側に交互に規則的な渦すなわちカ
ルマン渦を発生する。このカルマン渦の発生数
は、流体又は流量に比例しているところから、こ
のカルマン渦の数を計数することにより、流量を
計測することができる。而して、従来は、このカ
ルマン渦を計数するために、該カルマン渦を横切
つて超音波を送受信し、該超音波の周波数変調或
いは位相変調を検出するようにしていたが、超音
波は拡散するので受信々号レベルが小さく、更に
渦近傍流れが乱れているため、これとの干渉によ
りS/Nが低下し、これが計測誤差をもたらすこ
とがあつた。
PRIOR ART As is well known, when a columnar vortex generator is inserted into a fluid, the flow separates on both sides of the vortex generator, and regular vortices, that is, Karman vortices are alternately generated on the downstream side of the vortex generator. Occur. Since the number of Karman vortices generated is proportional to the fluid or flow rate, the flow rate can be measured by counting the number of Karman vortices. Conventionally, in order to count these Karman vortices, ultrasonic waves were transmitted and received across the Karman vortices and the frequency modulation or phase modulation of the ultrasonic waves was detected. Due to the diffusion, the received signal level is low, and since the flow near the vortex is disturbed, interference with this causes a reduction in S/N, which sometimes causes measurement errors.

目的 本発明は、上述のごとき実情に鑑みてなされた
もので、渦変動差圧による流れを整流し、超音波
の拡散をなくし外乱の影響を受けることなく、正
確にカルマン渦を計測し得るようにした渦流量計
に関する。
Purpose The present invention was made in view of the above-mentioned circumstances, and aims to rectify the flow due to eddy fluctuation differential pressure, eliminate the diffusion of ultrasonic waves, and accurately measure Karman vortices without being affected by disturbances. Regarding the vortex flow meter.

構 成 第1図は、本発明による渦流量計の一実施例を
説明するための要部断面構成図、第2図は、第1
図の−線断面図で、図中、1は被測定流体が
流れている流路管、2は周知の渦発生体、3a,
3bは該渦発生体によつて発生されたカルマン
渦、4は本発明によつて設けられた中空体で、該
中空体4は前記渦発生体2の下流側に該渦発生体
2と交差する方向に配設された中空体である。而
して、本発明においては、前記中空体4は流路管
1の管体壁に設けられた孔Aを貫通して配設さ
れ、該流路管1の外部において孔Bが設けられて
いる。従つて本発明によると、渦発生体2によつ
て発生されたカルマン渦による被測定流体の圧力
変動は孔A及びBを通して中空体4内に導入さ
れ、該中空体内の圧力変動又は該圧力変動による
流体変動が例えば超音波発信器5及び超音波受信
器6によつて検出され、それによつて、被測定流
体の流速又は流量が計測される。
Configuration FIG. 1 is a cross-sectional configuration diagram of main parts for explaining one embodiment of a vortex flowmeter according to the present invention, and FIG.
This is a sectional view taken along the - line in the figure. In the figure, 1 is a flow pipe through which the fluid to be measured flows, 2 is a well-known vortex generator, 3a,
3b is a Karman vortex generated by the vortex generator, 4 is a hollow body provided according to the present invention, and the hollow body 4 intersects with the vortex generator 2 on the downstream side of the vortex generator 2. It is a hollow body arranged in the direction of According to the present invention, the hollow body 4 is disposed to pass through the hole A provided in the wall of the flow pipe 1, and the hole B is provided outside the flow pipe 1. There is. Therefore, according to the present invention, the pressure fluctuation of the fluid to be measured due to the Karman vortex generated by the vortex generator 2 is introduced into the hollow body 4 through the holes A and B, and the pressure fluctuation within the hollow body or the pressure fluctuation is introduced into the hollow body 4 through the holes A and B. Fluid fluctuations caused by this are detected by, for example, the ultrasonic transmitter 5 and the ultrasonic receiver 6, and thereby the flow velocity or flow rate of the fluid to be measured is measured.

上述のように、本発明によると、被測定流体流
路を形成する管体の管壁に渦圧導入孔Aを設ける
とともに、管壁の外側において中空体4に渦圧導
入孔Bを設けるようにしたので、流路管1内で発
生されるノイズの影響を受けにくく、渦変動圧に
よる流れも整流されるので、検出波形の質がよ
く、また、渦圧導入孔Bを大きくすることができ
るので、流路管1内におけるダスト等の影響を受
けにくく、従つて、渦圧を効果的に検出すること
ができる。また、圧力導入孔Bを第2図に示すよ
うに流路管1に対して垂直にすることができるの
で、流路管内の水分、ダスト等に対して有効であ
り、更には、孔Aと孔Bが直交しているので、外
乱超音波に対して有効である等の利点を有する。
As described above, according to the present invention, the vortex pressure introduction hole A is provided in the tube wall of the tube forming the fluid flow path to be measured, and the vortex pressure introduction hole B is provided in the hollow body 4 on the outside of the tube wall. , it is less susceptible to the influence of noise generated within the flow path pipe 1, and the flow due to eddy fluctuation pressure is rectified, so the quality of the detected waveform is good and the eddy pressure introduction hole B can be made larger. Therefore, it is less susceptible to the influence of dust, etc. in the flow path pipe 1, and therefore, the vortex pressure can be detected effectively. In addition, since the pressure introduction hole B can be made perpendicular to the flow path pipe 1 as shown in FIG. 2, it is effective against moisture, dust, etc. in the flow path pipe. Since the holes B are orthogonal, it has advantages such as being effective against disturbance ultrasonic waves.

第3図は、渦圧導入孔Aを中空体4の貫通孔と
別にしたもので、このようにしても、第1図及び
第2図に示した実施例と同様の作用効果を奏する
ことは容易に理解できよう。
In FIG. 3, the vortex pressure introduction hole A is separated from the through hole of the hollow body 4. Even with this arrangement, the same effect as the embodiment shown in FIGS. 1 and 2 can be achieved. It's easy to understand.

第4図は、渦圧導入孔Bの近傍の部材の表面に
吸音材7を設け、外乱超音波が中空体内に侵入し
て検出信号に悪影響をしないようにしたものあ
る。
In FIG. 4, a sound absorbing material 7 is provided on the surface of the member near the vortex pressure introduction hole B to prevent disturbance ultrasonic waves from entering the hollow body and having an adverse effect on the detection signal.

また本発明の実施例として、渦圧導入孔Aの近
傍、例えば第4図の吸音材7の位置、即ち、渦圧
導入孔Bの中間位にフイルタを着脱自在に嵌挿す
るもので、被測定流体中に混入している塵埃が中
空体4内に侵入し、該中空体4内の流れが乱れた
り閉鎖したりするのを防ぐ為のもので、フイルタ
としては多孔質金属で圧力損失の小さい性状のも
のが望ましい。
Further, as an embodiment of the present invention, a filter is removably inserted in the vicinity of the vortex pressure introduction hole A, for example, at the position of the sound absorbing material 7 in FIG. This is to prevent dust mixed in the measured fluid from entering the hollow body 4 and disrupting or blocking the flow within the hollow body 4.The filter is a porous metal filter that reduces pressure loss. Small properties are desirable.

効 果 以上の説明から明らかなように、本発明による
と、外乱の影響を受けず、かつ、被測定流体中に
混入されている塵埃によつて渦圧導入孔が閉塞さ
れる心配のない渦流量計を提供することができ
る。
Effects As is clear from the above explanation, according to the present invention, the vortex is not affected by disturbances and there is no fear that the vortex pressure introduction hole will be blocked by dust mixed in the fluid to be measured. A flow meter can be provided.

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

第1図は、本発明による渦流量計の一実施例を
説明するための要部断面構成図、第2図は、第1
図の−線断面図、第3図は、渦圧導入孔A位
置を変更した図、第4図は、吸音材を装着した構
成図である。 1……流路管、2……渦発生体、3a,3b…
…カルマン渦、4……中空体、5……超音波送信
器、6……超音波受信器、7……吸音材、A,B
……渦圧導入孔。
FIG. 1 is a cross-sectional configuration diagram of main parts for explaining one embodiment of a vortex flowmeter according to the present invention, and FIG.
3 is a cross-sectional view taken along the line 3, FIG. 3 is a diagram with the position of the vortex pressure introduction hole A changed, and FIG. 4 is a configuration diagram in which a sound absorbing material is installed. 1... Channel pipe, 2... Vortex generator, 3a, 3b...
...Karman vortex, 4...Hollow body, 5...Ultrasonic transmitter, 6...Ultrasonic receiver, 7...Sound absorbing material, A, B
...Vortex pressure introduction hole.

Claims (1)

【特許請求の範囲】 1 流路の管体内に流れに対向して配設された渦
発生体と、該渦発生体の後流側に前記渦発生体と
交差する方向に前記管体壁を貫通し、該管体壁外
部に渦による変動圧力を導入する渦圧導入孔を有
する中空体と、該中空体近傍の管体壁を穿孔し、
前記中空体の渦圧導入孔に連通する他の渦圧導入
孔と、前記中空体両端部に対向配設した超音波送
受信器とからなり、渦信号を、中空体内において
前記変動圧力により流れる流体変動の超音波の伝
播速度の変化から求めることを特徴とする渦流量
計。 2 前記中空体の各々の渦圧導入口間に多孔質体
を着脱自在に嵌挿したことを特徴とする特許請求
の範囲第1項に記載の渦流量計。 3 前記中空体に穿設した渦圧導入孔を流路管に
対して垂直方向としたことを特徴とする特許請求
の範囲第1項又は第2項に記載の渦流量計。
[Scope of Claims] 1. A vortex generator disposed in a tube of a flow path to face the flow, and a wall of the tube in a direction intersecting the vortex generator on the trailing side of the vortex generator. a hollow body having a vortex pressure introduction hole that penetrates through and introduces fluctuating pressure due to the vortex to the outside of the tube wall; and a hole in the tube wall near the hollow body;
It consists of another vortex pressure introduction hole communicating with the vortex pressure introduction hole of the hollow body, and an ultrasonic transmitter/receiver arranged oppositely at both ends of the hollow body, and transmits a vortex signal to the fluid flowing in the hollow body due to the fluctuating pressure. A vortex flow meter characterized by determining fluctuations from changes in the propagation velocity of ultrasonic waves. 2. The vortex flowmeter according to claim 1, wherein a porous body is removably inserted between the vortex pressure introduction ports of each of the hollow bodies. 3. The vortex flow meter according to claim 1 or 2, characterized in that the vortex pressure introduction hole bored in the hollow body is oriented perpendicularly to the flow pipe.
JP58148928A 1983-08-15 1983-08-15 Vortex flowmeter Granted JPS6040914A (en)

Priority Applications (6)

Application Number Priority Date Filing Date Title
JP58148928A JPS6040914A (en) 1983-08-15 1983-08-15 Vortex flowmeter
US06/637,924 US4683760A (en) 1983-08-15 1984-08-06 Vortex flow meter
DE8484109373T DE3476449D1 (en) 1983-08-15 1984-08-07 VORTEX FLOW METER
EP84109373A EP0137945B1 (en) 1983-08-15 1984-08-07 Vortex flow meter
CA000461004A CA1228752A (en) 1983-08-15 1984-08-14 Vortex flow meter
KR1019840004876A KR890004447B1 (en) 1983-08-15 1984-08-14 Vortex Flowmeter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP58148928A JPS6040914A (en) 1983-08-15 1983-08-15 Vortex flowmeter

Publications (2)

Publication Number Publication Date
JPS6040914A JPS6040914A (en) 1985-03-04
JPH038695B2 true JPH038695B2 (en) 1991-02-06

Family

ID=15463794

Family Applications (1)

Application Number Title Priority Date Filing Date
JP58148928A Granted JPS6040914A (en) 1983-08-15 1983-08-15 Vortex flowmeter

Country Status (1)

Country Link
JP (1) JPS6040914A (en)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS62177414A (en) * 1986-01-31 1987-08-04 Oval Eng Co Ltd Vortex flow meter
JPS62214321A (en) * 1986-03-17 1987-09-21 Oval Eng Co Ltd Vortex flowmeter
US6435036B1 (en) 2000-07-17 2002-08-20 Matsushita Electric Industrial Co., Ltd. Vortex flow meter

Family Cites Families (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5368272A (en) * 1976-11-30 1978-06-17 Nissan Motor Flow meter for von k*arman*s vortex street
JPS562886A (en) * 1979-06-19 1981-01-13 Ebara Infilco Co Ltd Neutralization of acidic water containing iron ion
JPS5826620U (en) * 1981-08-12 1983-02-21 オ−バル機器工業株式会社 vortex flow meter

Also Published As

Publication number Publication date
JPS6040914A (en) 1985-03-04

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