JPH06103200B2 - Flowmeter - Google Patents

Flowmeter

Info

Publication number
JPH06103200B2
JPH06103200B2 JP2276708A JP27670890A JPH06103200B2 JP H06103200 B2 JPH06103200 B2 JP H06103200B2 JP 2276708 A JP2276708 A JP 2276708A JP 27670890 A JP27670890 A JP 27670890A JP H06103200 B2 JPH06103200 B2 JP H06103200B2
Authority
JP
Japan
Prior art keywords
phase
flow
liquid phase
gas phase
liquid
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 - Fee Related
Application number
JP2276708A
Other languages
Japanese (ja)
Other versions
JPH04151520A (en
Inventor
守 永瀬
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.)
TLV Co Ltd
Original Assignee
TLV 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 TLV Co Ltd filed Critical TLV Co Ltd
Priority to JP2276708A priority Critical patent/JPH06103200B2/en
Publication of JPH04151520A publication Critical patent/JPH04151520A/en
Publication of JPH06103200B2 publication Critical patent/JPH06103200B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Description

【発明の詳細な説明】 <産業上の利用分野> 本発明は、例えば蒸気のような気相と復水のような液相
とが、層を成して流れている管体に於て、気相と液相の
各流量を測定する流量計に関する。
DETAILED DESCRIPTION OF THE INVENTION <Industrial field of application> The present invention relates to a tubular body in which a vapor phase such as steam and a liquid phase such as condensate flow in layers. The present invention relates to a flow meter that measures each flow rate of a gas phase and a liquid phase.

<従来の技術> 一般に、蒸気と復水とは同じ管体を流れるが、これらの
蒸気と復水の両方の流量を測定する必要に迫られること
がある。この様な場合、従来では第2図に示すように、
蒸気と復水とが流れる配管1の中途に蒸気専用の配管2
と、復水専用の配管3とを設け、配管2に蒸気用の流量
計4を配置すると共に、配管3に復水用の流量計5を配
置して、両方の流量を測定するようにしていた。
<Prior Art> Generally, steam and condensate flow through the same pipe, but sometimes it is necessary to measure the flow rates of both steam and condensate. In such a case, as shown in FIG.
Pipe 2 for steam only in the middle of pipe 1 through which steam and condensate flow
And a pipe 3 dedicated to condensate, a flow meter 4 for steam is arranged in the pipe 2, and a flow meter 5 for condensate is arranged in the pipe 3 to measure both flow rates. It was

<発明が解決しようとする課題> しかし、この様な技術では蒸気と復水とに専用の配管
2、3が必要であり、第2図に示していないが蒸気と復
水を分離するためのセパレーター等の装置が必要で、装
置全体が大型になるという問題があった。
<Problems to be Solved by the Invention> However, in such a technique, dedicated pipes 2 and 3 are required for steam and condensate, and although not shown in FIG. Since a device such as a separator is required, there is a problem that the entire device becomes large.

この発明は気相と液相とが分離することなく、気相と液
相の各流量を測定できるようにすることである。
The present invention is to be able to measure each flow rate of a gas phase and a liquid phase without separating the gas phase and the liquid phase.

<課題を解決するための手段> 上記の技術的課題を解決するために講じた本発明の技術
的手段は、気相と液相とが層を成して流れる管体と、こ
の管体に垂直に配置された電極である渦発生体と、この
渦発生体で発生した振動を検出する振動センサと、この
振動センサからの信号のうち気相による振動信号のみを
透過せしめる気相フィルタ及び液相による振動信号のみ
を透過せしめる液相フィルタと、この透過せしめられた
夫々の信号から気相と液相の各流速を演算する手段と、
上記渦発生体と管体との間の電気的信号から液位を演算
する手段と、この液位と上記気相および液相の夫々の流
速とに基づいて気相と液相の各流量を演算する手段とか
らなる流量計にある。
<Means for Solving the Problems> The technical means of the present invention taken to solve the above technical problems is a tubular body in which a gas phase and a liquid phase flow in layers, and A vortex generator that is a vertically arranged electrode, a vibration sensor that detects the vibration generated by this vortex generator, and a gas-phase filter and liquid that allow only the vibration signal due to the gas phase to pass through among the signals from this vibration sensor. A liquid phase filter that allows only the vibration signal due to the phase to pass, and a means for calculating each flow velocity of the gas phase and the liquid phase from the respective transmitted signals.
Means for calculating the liquid level from the electric signal between the vortex generator and the pipe, and the respective flow rates of the gas phase and the liquid phase based on the liquid level and the respective flow velocities of the gas phase and the liquid phase. It is in a flowmeter consisting of means for calculating.

<作用> 上記の技術的手段の作用は下記の通りである。<Operation> The operation of the above technical means is as follows.

流れの中に置かれた渦発生体の下流側には規則的にカル
マン渦が発生し、その発生数(周波数f)と流速uには
下記(1)式の関係がある。従って、下記(2)式のよ
うに、この流速uに通過断面積Sを乗じることにより、
流量Qを求めることができる。
Karman vortices are regularly generated on the downstream side of the vortex generator placed in the flow, and the number of occurrences (frequency f) and the flow velocity u have the relationship of the following formula (1). Therefore, by multiplying the flow velocity u by the passage cross-sectional area S as in the following equation (2),
The flow rate Q can be obtained.

f=st・(u/d) ……(1) Q=S・u ……(2) ここで、stはストローハル数、uは流体の渦発生体を通
過する時の流速、dは渦発生体の幅(円柱の場合は直
径)である。
f = st ・ (u / d) ・ ・ ・ (1) Q = S ・ u ・ ・ ・ (2) where st is the Strouhal number, u is the velocity of the fluid passing through the vortex generator, and d is the vortex. It is the width of the generator (the diameter in the case of a cylinder).

本発明の流量計によれば、渦発生体により発生した気相
と液相の合成渦周波数の中から、気相、液相の各渦周波
数を抽出し、上記(1)式により気相、液相の各流速を
演算する。また、電極と管体との間の抵抗や容量の変化
として液位を検出することにより、管体内を流れる気
相、液相の各通過断面積を求めることができる。このよ
うにして求められた流速と段面積とから気相、液相の各
流量を演算して求めることができる。
According to the flow meter of the present invention, the vortex frequencies of the gas phase and the liquid phase are extracted from the combined vortex frequencies of the gas phase and the liquid phase generated by the vortex generator, and the gas phase is calculated by the equation (1). Calculate each flow rate of the liquid phase. Further, by detecting the liquid level as a change in resistance or capacitance between the electrode and the tube, it is possible to obtain the cross-sectional areas of passage of the gas phase and the liquid phase flowing in the tube. Each flow rate of the gas phase and the liquid phase can be calculated and calculated from the flow velocity and the step area thus obtained.

<実施例> 本発明の具体例を示す実施例を説明する。(第1図参
照)。
<Example> An example showing a specific example of the present invention will be described. (See FIG. 1).

10は管体でその内部には気相12が流速u1で、液相14が流
速u2でそれぞれ図の左から右へ流れている。管体10の内
部中心に管体10と垂直に渦発生体16を配置し、管体10の
外側からボルト18で固定する。渦発生体16は、有底の円
筒形状で上端にフランジを形成したセラミック製の外筒
20と、その内部に圧入した電極棒22とからなる。
Reference numeral 10 denotes a tubular body in which a gas phase 12 flows at a flow rate u1 and a liquid phase 14 flows at a flow rate u2 from left to right in the figure. A vortex generator (16) is arranged at the center of the inside of the tube (10) perpendicularly to the tube (10) and fixed from the outside of the tube (10) with a bolt (18). The vortex generator 16 is a ceramic outer cylinder having a bottomed cylindrical shape and a flange formed at the upper end.
It is composed of 20 and an electrode rod 22 press-fitted therein.

電極棒22と管体10は夫々導線を介して演算器24に接続さ
れ、演算器24で静電容量の変化から液位を演算し、気相
12と液相14の夫々の通過断面積を演算する。
The electrode rod 22 and the tubular body 10 are connected to a calculator 24 via conductors, respectively, and the calculator 24 calculates the liquid level from the change in electrostatic capacity, and the vapor phase is calculated.
Calculate the cross-sectional area of passage of each of 12 and the liquid phase 14.

電極棒22の上面に振動センサ26を取り付ける。振動セン
サ26からの信号は導線を介して増幅器28に連結される。
参照番号30は断熱部材、32はカバーである。
The vibration sensor 26 is attached to the upper surface of the electrode rod 22. The signal from vibration sensor 26 is coupled to amplifier 28 via a conductor.
Reference numeral 30 is a heat insulating member, and 32 is a cover.

管体10内を流れる気相流12と液相流14は渦発生体16の両
側で剥離して渦に巻込み、渦発生体16の下流側に振動的
な後流を生じる。この後流はカルマン渦の放出周波数f
で振動し下流に行くに従い粘性により減衰し、定常流に
戻る。この振動数fは気相流と液相流によって発生する
振動が合成されたものでり、振動センサ26で検出され
る。
The gas-phase flow 12 and the liquid-phase flow 14 that flow in the tube body 10 separate on both sides of the vortex generator 16 and are entrained in the vortex, and generate an oscillating wake downstream of the vortex generator 16. This wake is the emission frequency f of the Karman vortex.
It vibrates at and attenuates due to viscosity as it goes downstream, returning to a steady flow. The frequency f is a combination of vibrations generated by the gas-phase flow and the liquid-phase flow, and is detected by the vibration sensor 26.

振動センサ26で検出された振動信号は増幅器28で増幅さ
れ、気相フィルタ34及び液相フィルタ36へ流れる。ここ
で、気相に於ける渦周波数と流速の関係と、液相に於け
る渦周波数と流速の関係を予め判明させておき、前記気
相、及び液相フィルタ34、36でハード的に周波数分析す
る。つまり、それぞれの相に発生し得る渦周波数の範囲
のみを残し、他の渦周波数域を除去するのである。前記
気相、及び液相フィルタ34、36で出力された渦信号をカ
ウンタ38でそれぞれカウントし、演算器24で前記(1)
式に基づいて気相流速u1、及び液相流速u2を計算する。
The vibration signal detected by the vibration sensor 26 is amplified by the amplifier 28 and flows to the gas phase filter 34 and the liquid phase filter 36. Here, the relationship between the vortex frequency and the flow velocity in the gas phase and the relationship between the vortex frequency and the flow velocity in the liquid phase are known in advance. analyse. That is, only the range of the vortex frequency that can occur in each phase is left and the other vortex frequency regions are removed. The counter 38 counts the vortex signals output from the gas phase and liquid phase filters 34 and 36, respectively, and the calculator 24 calculates the vortex signals (1).
The gas phase flow rate u1 and the liquid phase flow rate u2 are calculated based on the equations.

そして、更に演算器24に於て前記(2)式に基づいて各
相の流速と断面積とから各相の流量を演算する。
Then, the calculator 24 further calculates the flow rate of each phase from the flow velocity and the cross-sectional area of each phase based on the equation (2).

<発明の効果> 特開昭51−99561号公報に開示の流量計は、気相と液相
の流速を同一と仮定して各流量を求めるものであるの
で、気相と液相の流速が異なると正確な流量を求めるこ
とができない。本発明では、気相と液相の各流速を演算
するので、各流量を正確に求めることができる。
<Effects of the Invention> Since the flowmeter disclosed in Japanese Patent Laid-Open No. 51-99561 determines each flow rate assuming that the flow rates of the gas phase and the liquid phase are the same, the flow rates of the gas phase and the liquid phase are If they are different, an accurate flow rate cannot be obtained. In the present invention, since the respective flow velocities of the gas phase and the liquid phase are calculated, each flow rate can be accurately obtained.

従って、本発明の流量計を例えば蒸気使用装置とスチー
ムトラップとの間の特にスチームトラップに近い側に設
けると、蒸気使用装置での蒸気使用量(復水の発生量)
及びスチームトラップでの蒸気漏洩量を正確に計測でき
る。また、蒸気使用装置の入口側に設けると、蒸気の使
用量及び復水の混入量を正確に計測できる。
Therefore, if the flow meter of the present invention is provided, for example, between the steam using device and the steam trap, particularly on the side close to the steam trap, the amount of steam used in the device using steam (amount of condensed water)
Also, the amount of steam leak in the steam trap can be accurately measured. Further, if it is provided on the inlet side of the steam using device, the amount of steam used and the amount of condensate mixed in can be accurately measured.

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

第1図はこの発明による流量計の一実施例の概略構成
図、第2図は従来の流量計の配管図である。 10:管体、12:気相 14:液相、16:渦発生体 20:外筒、22:電極棒 24:演算器、34:気相フィルタ 36:液相フィルタ
FIG. 1 is a schematic configuration diagram of an embodiment of a flow meter according to the present invention, and FIG. 2 is a piping diagram of a conventional flow meter. 10: Tube, 12: Gas phase 14: Liquid phase, 16: Vortex generator 20: Outer cylinder, 22: Electrode rod 24: Calculator, 34: Gas phase filter 36: Liquid phase filter

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】気相と液相とが層を成して流れる管体と、
この管体に垂直に配置された電極である渦発生体と、こ
の渦発生体で発生した振動を検出する振動センサと、こ
の振動センサからの信号のうち気相による振動信号のみ
を透過せしめる気相フィルタ及び液相による振動信号の
みを透過せしめる液相フィルタと、この透過せしめられ
た夫々の信号から気相と液相の各流速を演算する手段
と、上記渦発生体と管体との間の電気的信号から液位を
演算する手段と、この液位と上記気相および液相の夫々
の流速とに基づいて気相と液相の各流量を演算する手段
とからなる流量計。
1. A tube body in which a gas phase and a liquid phase flow in layers,
A vortex generator that is an electrode that is arranged perpendicularly to this tube, a vibration sensor that detects the vibration generated by this vortex generator, and a Between the vortex generator and the tubular body, a liquid phase filter for transmitting only the vibration signal due to the phase filter and the liquid phase, a means for calculating the respective flow velocities of the gas phase and the liquid phase from the respective transmitted signals. A flow meter comprising means for calculating the liquid level from the electric signal of 1. and means for calculating the respective flow rates of the gas phase and the liquid phase based on the liquid level and the flow rates of the gas phase and the liquid phase.
JP2276708A 1990-10-15 1990-10-15 Flowmeter Expired - Fee Related JPH06103200B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2276708A JPH06103200B2 (en) 1990-10-15 1990-10-15 Flowmeter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2276708A JPH06103200B2 (en) 1990-10-15 1990-10-15 Flowmeter

Publications (2)

Publication Number Publication Date
JPH04151520A JPH04151520A (en) 1992-05-25
JPH06103200B2 true JPH06103200B2 (en) 1994-12-14

Family

ID=17573222

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2276708A Expired - Fee Related JPH06103200B2 (en) 1990-10-15 1990-10-15 Flowmeter

Country Status (1)

Country Link
JP (1) JPH06103200B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE102012220505B4 (en) * 2012-11-09 2016-10-20 Gestra Ag Monitoring a steam trap

Family Cites Families (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5529064Y2 (en) * 1974-07-29 1980-07-11
JPS5199561A (en) * 1975-02-27 1976-09-02 Mitsubishi Heavy Ind Ltd KANRONAINIOKERUKIEKI 2 SORYUNORYURYOKE ISOKUSOCHI

Also Published As

Publication number Publication date
JPH04151520A (en) 1992-05-25

Similar Documents

Publication Publication Date Title
CN102348959B (en) Vortex flow measuring device for monitoring and/or measuring distributed particle and/or droplet flow
CN100383493C (en) Method for measuring the mass flow of a fluid flowing in a pipe
JPH0933309A (en) Coriolis mass flowmeter having at least one measuring tube
CN108680208A (en) A kind of hot type flux of vortex street metering device, flowmeter and its flow-measuring method
EP0970351A1 (en) Capacitive vortex mass flow sensor
CA1099952A (en) Vortex shedding flowmeter assembly
JPH06103200B2 (en) Flowmeter
CN112654842A (en) Non-invasive sensor for vortex flowmeter
GB2148003A (en) Measurement of flowrate
JPH0585025B2 (en)
JP2001194193A (en) Flow meter
RU2071595C1 (en) Vortex flowmeter
JP2863967B2 (en) Wetness measuring device
JP3611004B2 (en) Vortex flow meter
JPS61253423A (en) Vortex flowmeter
JPS62198716A (en) Vortex flow meter
JP3528436B2 (en) Ultrasonic flow meter and current meter
JP3500516B2 (en) Vortex flow meter
JPH0748053B2 (en) Liquid flow meter
JPH0626815Y2 (en) Vortex flowmeter
RU2118797C1 (en) Flowmeter with fluidal radiation
JPH059724B2 (en)
KR0133625Y1 (en) Vibratory flowmeter
JPS62163929A (en) Mass flow meter
JPH06288806A (en) Vibration measuring device

Legal Events

Date Code Title Description
R250 Receipt of annual fees

Free format text: JAPANESE INTERMEDIATE CODE: R250

R250 Receipt of annual fees

Free format text: JAPANESE INTERMEDIATE CODE: R250

LAPS Cancellation because of no payment of annual fees