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JPS5834765B2 - Karman vortex current meter - Google Patents
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JPS5834765B2 - Karman vortex current meter - Google Patents

Karman vortex current meter

Info

Publication number
JPS5834765B2
JPS5834765B2 JP53014768A JP1476878A JPS5834765B2 JP S5834765 B2 JPS5834765 B2 JP S5834765B2 JP 53014768 A JP53014768 A JP 53014768A JP 1476878 A JP1476878 A JP 1476878A JP S5834765 B2 JPS5834765 B2 JP S5834765B2
Authority
JP
Japan
Prior art keywords
vortex
fluid
karman
measured
column
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
Application number
JP53014768A
Other languages
Japanese (ja)
Other versions
JPS54107362A (en
Inventor
久嗣 伊藤
嘉明 浅山
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric Corp
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 Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP53014768A priority Critical patent/JPS5834765B2/en
Publication of JPS54107362A publication Critical patent/JPS54107362A/en
Publication of JPS5834765B2 publication Critical patent/JPS5834765B2/en
Expired legal-status Critical Current

Links

Description

【発明の詳細な説明】 この発明は導管内を流れる測定流体中に渦発生柱を設け
、その下流に発生したカルマン渦の数(発生渦周波数)
を超音波で検出して流速または流量を測定するカルマン
渦流速計に関するものでその目的は低流速における微弱
な渦をも容易に検出できる方法を提供するものである。
[Detailed Description of the Invention] This invention provides a vortex generation column in the measurement fluid flowing in a conduit, and the number of Karman vortices (occurrence vortex frequency) generated downstream of the vortex generation column.
This paper relates to a Karman vortex current meter that measures flow velocity or flow rate by detecting it using ultrasonic waves, and its purpose is to provide a method that can easily detect even weak vortices at low flow speeds.

導管内に渦発生柱を設け、その下流に発生したカルマン
渦の発生周波数を超音波で検出して管内を流れる流体の
流速または流量をIjllJfflする方法は実開昭5
1−24154で提案されている。
A method of installing a vortex generation column in a conduit and detecting the generation frequency of the Karman vortex generated downstream of the column using ultrasonic waves to determine the flow velocity or flow rate of the fluid flowing in the tube was developed in 1973.
1-24154.

この方法でカルマン渦を検出する場合、超音波発信器か
ら発信された超音波は流体中を伝播しカルマン渦で変調
され受信器で受信される。
When detecting the Karman vortex using this method, the ultrasound transmitted from the ultrasound transmitter propagates through the fluid, is modulated by the Karman vortex, and is received by the receiver.

しかし流体の流速が低い場合はカルマン渦は弱くしたが
って伝播する超音波が受ける変調の度合も小さい。
However, when the flow velocity of the fluid is low, the Karman vortex is weak and the degree of modulation received by the propagating ultrasonic waves is also small.

このために低流速でのカルマン渦の検出は困難である。For this reason, it is difficult to detect Karman vortices at low flow speeds.

この発明は流体中を伝播する超音波がカルマン渦の発生
数に比例して変調される度合を増大し、低流速(3rT
l/s以下程度)以下力ルマン渦の検出を容易にするた
めに渦発生体の左右を流れる流体間に温度差をもたせた
りあるいは一方の流体中に異質流体を混入して左右流体
間に状態変化を与えることにより、左右両流体により発
生するカルマン渦間で超音波の伝播速度に変化を与える
ようにしたものである。
This invention increases the degree to which ultrasonic waves propagating in a fluid is modulated in proportion to the number of Karman vortices, and
In order to facilitate the detection of Le Mans vortices, a temperature difference is created between the fluids flowing on the left and right sides of the vortex generating body, or a different fluid is mixed into one fluid to create a state between the left and right fluids. By applying a change, the propagation speed of the ultrasonic wave is changed between the Karman vortices generated by both the left and right fluids.

以下、図に示す実施例について説明する。The embodiment shown in the figures will be described below.

図中1は測定流体を流すための導管、2は前記測定流体
の流れと略直角に設けられた渦発生柱、3,4は該渦発
生柱2により発生するカルマン渦、5は超音波発信器、
6は発振装置、7は超音波受信器、8は受信装置であり
、前記超音波発信器5、発振装置6、超音波受信器7、
および受信装置8により超音波渦検出装置が構成されて
いる。
In the figure, 1 is a conduit for flowing the measurement fluid, 2 is a vortex generation column installed approximately perpendicular to the flow of the measurement fluid, 3 and 4 are Karman vortices generated by the vortex generation column 2, and 5 is an ultrasonic wave generator. vessel,
6 is an oscillating device, 7 is an ultrasonic receiver, 8 is a receiving device, the ultrasonic transmitter 5, the oscillating device 6, the ultrasonic receiver 7,
The receiving device 8 constitutes an ultrasonic vortex detection device.

9は前記渦発生柱2の上流に且つ、前記渦発生柱2に沿
って配置され前記測定流体の流れをA、B12つの流れ
に分割する仕切板、10はこの仕切板によって分割され
た流れの一方Bを加熱すべく設けられた電熱器、11は
バッテリーである。
9 is a partition plate arranged upstream of the vortex generating column 2 and along the vortex generating column 2 to divide the flow of the measurement fluid into two flows A and B; 10 is a partition plate of the flow divided by this partition plate; On the other hand, an electric heater 11 provided to heat B is a battery.

以上の構成において導管1内を測定流体(例えば空気)
が矢印の方向に流れると渦発生柱2によりカルマン渦3
,4が発生する。
In the above configuration, the inside of the conduit 1 is filled with a measuring fluid (for example, air).
flows in the direction of the arrow, Karman vortex 3 is created by vortex generation column 2
, 4 occurs.

超音波発信器5は発振装置6により駆動され超音波を受
信器7に送信する。
The ultrasonic transmitter 5 is driven by an oscillation device 6 and transmits ultrasonic waves to a receiver 7.

この時、前記演児流体中を伝播する間に超音波は前記カ
ルマン渦により変調され受信器7は変調された超音波を
受信する。
At this time, the ultrasonic waves are modulated by the Karman vortices while propagating through the performer fluid, and the receiver 7 receives the modulated ultrasonic waves.

そして受信装置8により前記カルマン渦の発生周波数を
検知する。
Then, the receiving device 8 detects the frequency at which the Karman vortex occurs.

前記測定流体の流速が低い場合(例えば3rrV/s以
下)は前記カルマン渦は弱く、シたがって伝播する前記
超音波が受ける変調の度合が小さくなりカルマン渦の検
出が不可能となる。
When the flow velocity of the measurement fluid is low (for example, 3 rrV/s or less), the Karman vortex is weak, and therefore the degree of modulation received by the propagating ultrasonic wave becomes small, making it impossible to detect the Karman vortex.

このような時、電熱器10によりB側の測定流体を加熱
し、春巻のカルマン渦3と左巻のカルマン渦4の間に温
度差をもたせると、前記超音波の伝播速度が前記カルマ
ン渦3中を伝播する時と前記カルマン渦4中を伝播する
時で著しく異なるようになる。
In such a case, when the measurement fluid on the B side is heated by the electric heater 10 to create a temperature difference between the spring roll Karman vortex 3 and the left-handed Karman vortex 4, the propagation speed of the ultrasonic wave increases 3 and the Karman vortex 4 are significantly different from each other.

すなわち交互に発生する前記カルマン渦3と4の発生頻
度に比例して前記伝播する超音波は変調されることにな
る。
That is, the propagating ultrasonic waves are modulated in proportion to the frequency of occurrence of the Karman vortices 3 and 4 that occur alternately.

測定流体が空気の場合、図に示すように発信器5側の流
れBを加熱しAの流れより数℃高い温度にすると、前記
伝播する超音波はカルマン渦による変調とカルマン渦3
と4の温度差による伝播速度の差による変調が加えられ
だものとなり低流速における弱いカルマン渦をも容易に
検出できるようになる。
When the fluid to be measured is air, if the flow B on the transmitter 5 side is heated to a temperature several degrees higher than the flow A as shown in the figure, the propagating ultrasonic wave will be modulated by the Karman vortex and the Karman vortex 3.
The modulation caused by the difference in propagation velocity due to the temperature difference between

以上のようにこの発明は超音波の伝播速度がカルマン渦
3とカルマン渦4との間で異なるようにしたものであり
、前記AとBの何れかの流れを加熱または冷却してもよ
く、また片方の流れに音速の異なる異質流体を混入して
も同じ効果が得られる、例えば測定流体が空気の場合、
発信器5側の流れBに水蒸気を混入させるかあるいは受
信器T側の流れAにガソリン蒸気を混入させることによ
り伝播する超音波の変離を増大することができ低流速に
おける微弱なカルマン渦をも検出することができる。
As described above, in this invention, the propagation speed of the ultrasonic wave is made different between the Karman vortex 3 and the Karman vortex 4, and either of the flows A and B may be heated or cooled. The same effect can also be obtained by mixing a different fluid with a different sound speed into one of the flows. For example, if the fluid to be measured is air,
By mixing water vapor into the flow B on the transmitter 5 side or gasoline vapor into the flow A on the receiver T side, the displacement of the propagating ultrasonic waves can be increased and the weak Karman vortices at low flow speeds can be increased. can also be detected.

この異質流体の混入手段としては例えば通常の気化器の
原理を利用して構成することも容易である。
The means for mixing this foreign fluid can be easily constructed using, for example, the principle of a normal vaporizer.

以上のようにこの発明は導管1の内部に配置された渦発
生柱2とこの渦発生柱2の上流側で該過発生柱の両側の
被測定流体間に温度差をもたせ、あるいは前記渦発生柱
の両側の各被測定流体の一方に被測定流体以外の異質流
体を混入して、渦発生柱の両側の各被測定流体間に雰囲
気(状態)変化を与えることにより低流速におけるカル
マン渦の発生頻度を容易に検出するようにしたものであ
り低流速においても検出能力の優れたカルマン渦流速計
を得ることができtも
As described above, the present invention provides a temperature difference between the vortex generating column 2 disposed inside the conduit 1 and the measured fluid on both sides of the vortex generating column 2 on the upstream side of the vortex generating column 2, or By mixing a different fluid other than the fluid to be measured into one of the fluids to be measured on both sides of the column and changing the atmosphere (state) between the fluids to be measured on both sides of the vortex generating column, Karman vortices can be generated at low flow speeds. It is designed to easily detect the frequency of occurrence, and it is possible to obtain a Karman vortex current meter with excellent detection ability even at low flow speeds.

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

図はこの発明の一実施例を示す構成図である。 図中1は導管、2は渦発生柱、3,4はカルマン渦、5
は超音波発信器、1は超音波受信器、9は仕切板、10
は電熱器である。
The figure is a configuration diagram showing an embodiment of the present invention. In the figure, 1 is a conduit, 2 is a vortex generation column, 3 and 4 are Karman vortices, and 5
is an ultrasonic transmitter, 1 is an ultrasonic receiver, 9 is a partition plate, 10
is an electric heater.

Claims (1)

【特許請求の範囲】 1 導管の内部に被測定流体の流れに略直交して配設さ
れた渦発生柱、この発生柱の下流側に発生するカルマン
渦の数を検出する超音波渦検出装置、及び上記渦発生柱
の上流側で該渦発生柱の両側の被測定流体間に温度差を
与える手段を備えて成るカルマン渦流速計0 2 温度差を与える手段は、被測定流体を部分的に加熱
又は冷却する加熱器又は冷却器によって構成されている
特許請求の範囲第1項記載のカルマン渦流速計。 3 温度差を与える手段は、渦発生柱の上流側で該渦発
生柱に沿って被測定流体を2分割する仕切板と、該2分
割された被測定流体の一方を加熱又は冷却する手段を含
んで構成されている特許請求の範囲第1項記載のカルマ
ン渦流速計。 4 導管の内部に被測定流体の流れに略直交して配設さ
れた渦発生柱、この渦発生柱の下流側に発生するカルマ
ン渦の数を検出する超音波検出器、上記渦発生柱の上流
側で該渦発生柱に沿って被測定流体を2分割する仕切板
、及び上記仕切板によって2分割された被測定流体の一
方に異質流体を混入させる手段を備えたカルマン渦流速
計。
[Scope of Claims] 1. A vortex generation column disposed inside a conduit substantially perpendicular to the flow of the fluid to be measured, and an ultrasonic vortex detection device that detects the number of Karman vortices generated downstream of this generation column. , and means for applying a temperature difference between the measured fluids on both sides of the vortex generating column on the upstream side of the vortex generating column. The Karman vortex current meter according to claim 1, which comprises a heater or a cooler for heating or cooling. 3. The means for providing a temperature difference includes a partition plate that divides the fluid to be measured into two along the vortex generating column on the upstream side of the vortex generating column, and a means for heating or cooling one of the two divided fluids to be measured. A Karman vortex current meter according to claim 1, comprising: 4. A vortex generating column disposed inside the conduit substantially perpendicular to the flow of the fluid to be measured, an ultrasonic detector for detecting the number of Karman vortices generated on the downstream side of this vortex generating column, and a A Karman vortex current meter comprising: a partition plate that divides a fluid to be measured into two along the vortex generation column on the upstream side; and means for mixing a foreign fluid into one of the fluids to be measured divided into two by the partition plate.
JP53014768A 1978-02-09 1978-02-09 Karman vortex current meter Expired JPS5834765B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP53014768A JPS5834765B2 (en) 1978-02-09 1978-02-09 Karman vortex current meter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP53014768A JPS5834765B2 (en) 1978-02-09 1978-02-09 Karman vortex current meter

Publications (2)

Publication Number Publication Date
JPS54107362A JPS54107362A (en) 1979-08-23
JPS5834765B2 true JPS5834765B2 (en) 1983-07-28

Family

ID=11870235

Family Applications (1)

Application Number Title Priority Date Filing Date
JP53014768A Expired JPS5834765B2 (en) 1978-02-09 1978-02-09 Karman vortex current meter

Country Status (1)

Country Link
JP (1) JPS5834765B2 (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5936258U (en) * 1982-08-28 1984-03-07 ソニー株式会社 Hybrid IC terminal structure
JPH03201471A (en) * 1989-12-28 1991-09-03 Mitsubishi Electric Corp Package structure of semiconductor device

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5697830A (en) * 1979-12-29 1981-08-06 Mitsubishi Electric Corp Karman vortex flow meter
JPS56103368A (en) * 1980-01-22 1981-08-18 Mitsubishi Electric Corp Karman's vortex street current meter
JPS59197825A (en) * 1983-04-26 1984-11-09 Mitsubishi Motors Corp Detector of intake quantity of engine

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5936258U (en) * 1982-08-28 1984-03-07 ソニー株式会社 Hybrid IC terminal structure
JPH03201471A (en) * 1989-12-28 1991-09-03 Mitsubishi Electric Corp Package structure of semiconductor device

Also Published As

Publication number Publication date
JPS54107362A (en) 1979-08-23

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