JPS59132313A - Krmn vortex flow speed meter - Google Patents
Krmn vortex flow speed meterInfo
- Publication number
- JPS59132313A JPS59132313A JP700183A JP700183A JPS59132313A JP S59132313 A JPS59132313 A JP S59132313A JP 700183 A JP700183 A JP 700183A JP 700183 A JP700183 A JP 700183A JP S59132313 A JPS59132313 A JP S59132313A
- Authority
- JP
- Japan
- Prior art keywords
- krmn
- karman vortex
- vortex
- flow speed
- measurement
- 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.)
- Pending
Links
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01F—MEASURING VOLUME, VOLUME FLOW, MASS FLOW OR LIQUID LEVEL; METERING BY VOLUME
- G01F1/00—Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow
- G01F1/05—Measuring 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
- G01F1/20—Measuring 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
- G01F1/32—Measuring 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
- G01F1/3209—Measuring 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 using Karman vortices
Landscapes
- Physics & Mathematics (AREA)
- Fluid Mechanics (AREA)
- General Physics & Mathematics (AREA)
Abstract
Description
【発明の詳細な説明】
本発明は、カルマン渦流速計の改良に関するものである
。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to improvements in Karman vortex current meters.
気体の流速計として、第1図に示すようなJIS規格の
L字型ピトー管、或は、第2図に示すようなASII規
格の特殊ピトー管(ウェスタン型ともいう)が一般に使
用されている。As a gas flowmeter, a JIS standard L-shaped pitot tube as shown in Figure 1 or an ASII standard special pitot tube (also called a Western type) as shown in Figure 2 is generally used. .
しかし、これらのピトー管はいずれも気体の単相流用の
流速計として開発されたものであり。However, all of these pitot tubes were developed as flow meters for single-phase gas flow.
固気、又は、気液の二相流の計測においては。For measurement of two-phase flow of solid gas or gas/liquid.
粉粒体、又は、液滴などが測圧孔に入って目詰りし、測
定不能になる欠点がある。このため。There is a drawback that powder, granules, liquid droplets, etc. enter the pressure measurement hole and clog it, making measurement impossible. For this reason.
ピトー管を二相流計測に使用するときは、空気や蒸気釡
測圧孔に流し頻繁にパージする必要があり計測時間が長
時間に及ぶ。また、高濃度領域では、ピトー管は瞬時に
目詰りしてしまい。When using a pitot tube for two-phase flow measurement, it is necessary to pour air or steam into the pressure measurement hole and purge it frequently, resulting in a long measurement time. Additionally, in high concentration areas, pitot tubes can become clogged instantly.
計測不能となる大きな欠点がある。It has a major drawback that it cannot be measured.
一方、流体流速の計測には、カルマン渦流速計も多用さ
れている。Cれは流体流れ中にカルマン渦発生体を配設
し9発生したカルマン渦の周波数から流速を求めるもの
である。この流速計ではいわゆる測圧孔が無いので、そ
のり詰りという問題がないが、カルマン渦発生体に粉体
や液体が付着し、やはり不具合となる。On the other hand, Karman vortex current meters are also frequently used to measure fluid flow velocity. C-cure is a method in which a Karman vortex generator is placed in a fluid flow, and the flow velocity is determined from the frequency of the Karman vortex generated. Since this current meter does not have a so-called pressure measuring hole, there is no problem of clogging of the hole, but powder or liquid may adhere to the Karman vortex generating body, which also causes problems.
つまり、カルマン渦発生体の工、ジ付近に粉体等が付着
すると、気体のはく離条件が不安定になり、安定的にカ
ルマン渦が発生せず計測誤差となる。In other words, if powder or the like adheres to the vicinity of the Karman vortex generator, the gas separation conditions become unstable, and the Karman vortex is not stably generated, resulting in measurement errors.
本発明は、これらの欠点を排除するものであって、流体
流れ中に配設されカルマン渦を発生させる柱状のカルマ
ン渦発生体と、同発生体で発生したカルマン渦の周波数
を測定する手段とからなるカルマン渦流速計において、
カルマン渦発生体をその軸芯と直交する方向に振動させ
る手段を具備したことを特徴とし、その目的とするとこ
ろは、カルマン渦の発生を安定させ流速計測に誤差の生
じないカルマン渦流速計を提供するものである。The present invention eliminates these drawbacks, and includes a columnar Karman vortex generator disposed in a fluid flow that generates a Karman vortex, and a means for measuring the frequency of the Karman vortex generated by the same generator. In the Karman vortex current meter consisting of
It is characterized by being equipped with a means for vibrating the Karman vortex generator in a direction perpendicular to its axis, and its purpose is to stabilize the generation of Karman vortices and create a Karman vortex current meter that does not cause errors in flow velocity measurement. This is what we provide.
以下9本発明を第3図および第4図に示す一実施例の流
速計について説明する。The present invention will be described below with respect to an embodiment of a current meter shown in FIGS. 3 and 4.
1はカルマン渦発生体であって、第4図に示すように断
面5角形を有する柱状をなし、磁性部材なりなる。この
カルマン渦発生体lは支持棒4の先端に金具2により取
り付けられており。Reference numeral 1 denotes a Karman vortex generator, which has a columnar shape with a pentagonal cross section as shown in FIG. 4, and is made of a magnetic member. This Karman vortex generator 1 is attached to the tip of a support rod 4 with a metal fitting 2.
流れと軸芯とが直交するように配置される。また、カル
マン渦発生体lの軸方向+5は貫通孔1人が形成され、
一方、流れ下流側に向けて開孔IBが貫通孔IAと連通
ずるように設けられている。It is arranged so that the flow and the axis are perpendicular to each other. In addition, one through hole is formed in the axial direction +5 of the Karman vortex generator l,
On the other hand, an opening IB is provided toward the downstream side so as to communicate with the through hole IA.
3は金具2内に埋設された電磁石であって7リード線5
を介して制御器6に結線されていて。3 is an electromagnet buried in the metal fitting 2, and 7 lead wires 5
It is connected to the controller 6 via.
カルマン渦発生体1をその軸芯と直交する向きに任意の
振動数で振動させるものである。The Karman vortex generator 1 is made to vibrate at an arbitrary frequency in a direction perpendicular to its axis.
8は熱線式センサであって、カルマン渦発生体1の貫通
孔IA内であって開孔IBに近接して配設されており、
公知の手段によりカルマン渦の周波数を計測するCとが
できる。8 is a hot wire type sensor, which is disposed within the through hole IA of the Karman vortex generator 1 and close to the opening IB;
The frequency of the Karman vortex can be measured using known means.
なお、10は流れ中の気体の流線、11は粒体の流線で
ある。Note that 10 is a streamline of gas in the flow, and 11 is a streamline of particles.
さて、流体がカルマン渦発生体lに当たると。Now, when the fluid hits the Karman vortex generator l.
その後流にカルマン渦が発生する。その周波数をセンサ
8で検出し1次式により流速を求める。A Karman vortex is generated in its wake. The frequency is detected by the sensor 8 and the flow velocity is determined by a linear equation.
V = ar、’st
ここそ、■:気体流速〔m/s〕
d:カルマン渦発生体の幅(m)
Stニスドローハル数〔定数〕
f二側波数(1/、)
粉体の量が増し、粉体流量と気体流量との比が大きくな
ってくると、カルマン渦発生体lの角部lCの付近に粉
体が付着し、気体流線1oのはく離が不安定になる。V = ar,'st Kokoso, ■: Gas flow velocity [m/s] d: Width of Karman vortex generator (m) Stnis-Drawhal number [constant] f second side wave number (1/,) The amount of powder increases When the ratio of the powder flow rate to the gas flow rate becomes large, the powder adheres to the vicinity of the corner 1C of the Karman vortex generator 1, and the separation of the gas streamline 1o becomes unstable.
この時制御器6を作動させ、電磁石3を、適当な周波数
で交番に励磁させ、カルマン渦発生体1をその軸芯と、
つまり、流れと直交する向きに振動させる。カルマン渦
発生体1の角部10表面と粉体との間に空間が生じるた
め、角部ICにおける気体流線10のはく離条件が安定
し。At this time, the controller 6 is activated to alternately excite the electromagnet 3 at an appropriate frequency, and the Karman vortex generator 1 is aligned with its axis.
In other words, it vibrates in a direction perpendicular to the flow. Since a space is created between the surface of the corner 10 of the Karman vortex generator 1 and the powder, the separation conditions of the gas streamline 10 at the corner IC are stabilized.
カルマン渦が安定的に発生するようになる。Karman vortex will be generated stably.
また、カルマン渦の強度が弱い場合電磁石3の加振周波
数を制御して、カルマン渦の周波数と共振させると、カ
ルマン渦の強度が増し、カルマン渦の周波数の計測精度
が向上することになる、
このように2本実施例の流速計によれば。Furthermore, when the strength of the Karman vortex is weak, if the excitation frequency of the electromagnet 3 is controlled to resonate with the frequency of the Karman vortex, the strength of the Karman vortex will increase, and the measurement accuracy of the frequency of the Karman vortex will improve. As described above, according to the current velocity meters of the two embodiments.
(1) カルマン渦発生体1を電磁石3により振動さ
せたことによって、カルマン渦発生体1の角部IC付近
に粉体、又は、液滴が付着しなくなり、このため混相流
の高濃度領域においても、カルマン渦が発生しやすくな
り、気体パージをしないで、連続的に気体流速を計測で
きる。したがって、計測時間が従来法より大幅に短縮で
きる。(1) By vibrating the Karman vortex generator 1 with the electromagnet 3, powder or droplets do not adhere to the vicinity of the corner IC of the Karman vortex generator 1, and therefore in the high concentration region of multiphase flow. Also, Karman vortices are more likely to occur, and the gas flow velocity can be measured continuously without gas purge. Therefore, the measurement time can be significantly reduced compared to the conventional method.
(2) カルマン渦発生体lの加振周波数を制御し。(2) Control the excitation frequency of the Karman vortex generator l.
カルマン渦周波数と共振させるようにしたことによりカ
ルマン渦による圧力変動が大きくなり、渦周波数の検出
が容易になるので、気体流速の計測精度が向上する。By making it resonate with the Karman vortex frequency, pressure fluctuations due to the Karman vortex become larger, and the vortex frequency becomes easier to detect, thereby improving the measurement accuracy of the gas flow velocity.
などの効果を得ることができる。You can obtain effects such as
第1図および第2図はピトー管の例示図、第3図は本発
明の一実施例を示す流速計の図、第4図は第3図のIV
−IV断面図である。
1:カルマン渦発生体、3:電磁石、8:センサFigures 1 and 2 are illustrations of a pitot tube, Figure 3 is a diagram of a current meter showing an embodiment of the present invention, and Figure 4 is an IV of Figure 3.
-IV sectional view. 1: Karman vortex generator, 3: electromagnet, 8: sensor
Claims (1)
ルマン渦発生体と、同発生体で発生したカルマン渦の周
波数を測定する手段とからなるカルマン渦流速計におい
て、カルマン渦発生体をその軸芯と直交する方向に振動
させる手段を具備したことを特徴とするカルマン渦流速
計。In a Karman vortex velocimeter, which consists of a columnar Karman vortex generator that is placed in a fluid flow and generates a Karman vortex, and a means for measuring the frequency of the Karman vortex generated by the generator, the Karman vortex generator is connected to the axis of the Karman vortex generator. A Karman vortex current meter characterized by comprising a means for vibrating in a direction perpendicular to the core.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP700183A JPS59132313A (en) | 1983-01-19 | 1983-01-19 | Krmn vortex flow speed meter |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP700183A JPS59132313A (en) | 1983-01-19 | 1983-01-19 | Krmn vortex flow speed meter |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS59132313A true JPS59132313A (en) | 1984-07-30 |
Family
ID=11653850
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP700183A Pending JPS59132313A (en) | 1983-01-19 | 1983-01-19 | Krmn vortex flow speed meter |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS59132313A (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS61253423A (en) * | 1985-05-01 | 1986-11-11 | Hajime Onoda | Vortex flowmeter |
JPS62198716A (en) * | 1986-02-27 | 1987-09-02 | Hajime Onoda | Vortex flow meter |
-
1983
- 1983-01-19 JP JP700183A patent/JPS59132313A/en active Pending
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS61253423A (en) * | 1985-05-01 | 1986-11-11 | Hajime Onoda | Vortex flowmeter |
JPS62198716A (en) * | 1986-02-27 | 1987-09-02 | Hajime Onoda | Vortex flow meter |
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