JPS59187222A - Vortex flow-meter - Google Patents

Vortex flow-meter

Info

Publication number
JPS59187222A
JPS59187222A JP58060333A JP6033383A JPS59187222A JP S59187222 A JPS59187222 A JP S59187222A JP 58060333 A JP58060333 A JP 58060333A JP 6033383 A JP6033383 A JP 6033383A JP S59187222 A JPS59187222 A JP S59187222A
Authority
JP
Japan
Prior art keywords
hollow body
vortex
hole
karman
holes
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.)
Granted
Application number
JP58060333A
Other languages
Japanese (ja)
Other versions
JPH059724B2 (en
Inventor
Katsuo Misumi
勝夫 三角
Masahiro Kanayama
金山 昌弘
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.)
Oval Kiki Kogyo KK
Oval Engineering Co Ltd
Original Assignee
Oval Kiki Kogyo KK
Oval Engineering 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 Oval Kiki Kogyo KK, Oval Engineering Co Ltd filed Critical Oval Kiki Kogyo KK
Priority to JP58060333A priority Critical patent/JPS59187222A/en
Publication of JPS59187222A publication Critical patent/JPS59187222A/en
Publication of JPH059724B2 publication Critical patent/JPH059724B2/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
    • G01F1/3259Means for detecting quantities used as proxy variables for swirl for detecting fluid pressure oscillations

Landscapes

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

Abstract

PURPOSE:To measure Karman vortex accurately without being influenced by external noise by a method wherein a hollow body is provided to the downstream side of a vortex producing body at a right angle with the vortex producing body and a pair of holes are provided to the hollow body along the axial direction at a prescribed interval. CONSTITUTION:A hollow body 4 is provided to the downstream side of a vortex producing body 2 at a right angle with the vortex producing body 2. A pair of holes 4a, 4b are provided to the hollow body 4 along the axial direction at a prescribed interval. When a Karman vortex 3a is produced at the left side, the pressure at the side of the hole 4a is reduced and, when the Karman vortex 3b is produced at the right side, the pressure at the side of the hole 4b is reduced. Because these pressure changes are produced alternately, the number of the produced Karman vortexes can be measured by measuring the pressure change with a pressure sensitive element or the like. Therefore, transmitting and receiving of a ultrasonic wave and the like across the Karman vortex are not necessary so that the number of the Karman vortexes is accurately measured without being influenced by external noise.

Description

【発明の詳細な説明】 皮亙芳■ 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Wc tlに関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a vortex flow Wc tl that utilizes a Karman vortex generated by a vortex generator disposed in a fluid.

疋、LL苅 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が発生する。
LL.KariAs 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 generated alternately on the downstream side of the vortex generator.

このカルマン渦の発生数は、流体の流速又は流量に比例
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
横切っ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、外部からの雑
音等によって被測定流体の流れに乱れが生じ、これが3
1測誤差の一因ともなっていた。
Since the number of Karman vortices generated is proportional to the flow velocity or flow rate of the fluid, 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. Disturbances occur in the flow of the fluid to be measured due to
This was also a cause of measurement error.

比−一一旬 本発明は、L述のごとき実情に鑑みてなされたもので、
外部雑音等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新規構成の渦流量計に関する。
The present invention was made in view of the actual situation as described in L.
This invention relates to a vortex flow meter with a new configuration that allows accurate measurement of Karman vortices without being affected by external noise.

乳−−] 第1図は、本発明による渦流量計の一実施例を説明する
ための要部構成図で(A)図は(B)図のA−A線断面
図、(B)図は(A)図のB−B線断面図で、図中、l
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2によって発生されたカルマ
ン渦、4は本発明によって設けられた中空体て、該中空
体4は前記渦発生体2の下流側に該渦発生体2と直角に
交る方向に配設され、かつ、軸方向に所定の間隔をもっ
て少なくとも1対の孔4 a ’+ 4 bを41して
いる。而して、周知のように、カルマン渦3aが発生し
た時は、孔4a側の圧力が下り、カルマン渦3bが発生
した時は、孔4b側の圧力が下るか、この圧力変化は、
孔4a、4bを通して中空体4内の流体にも及び、該中
空体4内の流体に矢印方向に△Pの圧力差を交互に発生
させる。従って、この中空体4内における流体の移動、
圧力差等を任意所望の手段例えば超音波、レーザ光、感
圧素子等を用いて計測すれば、力、ルマン渦の発生数を
計測することができる・ 第2図は、上記中空体の変形例を示す断面図で、(A)
図は前記孔4a、4bを中空体4の下流側に設けた例、
CB)図は前記中空体4の下流側を流線形にし、もって
、該中空体4によってカルマン渦が発生するのを防止す
るようにした例(該中空体4によって発生されるカルマ
ン渦が該中空体4に設けられた孔4a、4bを通して該
中空体4内の流体に影響する恐れがある)、(C)図は
前記流線形中空体4の下流側に孔4a 、 4bを設け
た例、(D)図は円筒形中空体4の下流側に該中空体4
と平行に仕切板5を設け、中空体4によってカルマン渦
ができるのを防止するようにした例、(E)図は前記仕
切板を設けた中空体において、該中空体4の下流側に孔
4a 、4bを設けた例、(F)図は前記中空体4の上
流側に防塵板6を設け、孔4a、4bが塵埃等によって
詰まったり、鎖孔4a、4bを通して中空体4内に塵埃
が入るのを防止するようにした例で、この防塵板6は中
空体4の一ヒ流側全長に亘って設けても、或いは、孔4
a、4bの」二流側にのみ設けてもよい。なお、本発明
はよる渦流量計は、液体、気体のいずれに対しても適用
可能であるが、気体、特に、高温ノ左気等の流量を測定
する場合には、第1図(A)に示すように、中空体4に
更に排水孔7を設けておき、該中空体4内に溜まった水
滴を該()1水孔7を通して排出するようにするとよい
。また、以Hに、中空体4に1対の孔4a、4bを設け
た例について説明したが、鎖孔は1対に限定されるもの
ではなく、また、必ずしも対になっていなくてはならな
いものでもないことは容易に理解されよう。
[Milk--] Figure 1 is a main part configuration diagram for explaining one embodiment of a vortex flowmeter according to the present invention, and (A) is a cross-sectional view taken along line A-A in (B), and (B) is is a sectional view taken along the line B-B in figure (A), and in the figure, l
2 is a well-known vortex generator; 3a and 3b are Karman vortices generated by the vortex generator 2; 4 is a hollow body provided according to the present invention; The body 4 is disposed on the downstream side of the vortex generator 2 in a direction perpendicular to the vortex generator 2, and has at least one pair of holes 4a'+4b at a predetermined interval in the axial direction. are doing. As is well known, when the Karman vortex 3a is generated, the pressure on the hole 4a side decreases, and when the Karman vortex 3b is generated, the pressure on the hole 4b side decreases, or this pressure change is
The pressure is also applied to the fluid inside the hollow body 4 through the holes 4a and 4b, and a pressure difference of ΔP is alternately generated in the fluid inside the hollow body 4 in the direction of the arrow. Therefore, the movement of fluid within this hollow body 4,
By measuring the pressure difference using any desired means such as ultrasonic waves, laser light, pressure-sensitive elements, etc., the force and the number of Le Mans vortices generated can be measured. Figure 2 shows the deformation of the hollow body described above. In a cross-sectional view showing an example, (A)
The figure shows an example in which the holes 4a and 4b are provided on the downstream side of the hollow body 4,
Figure CB) shows an example in which the downstream side of the hollow body 4 is streamlined to prevent the generation of Karman vortex by the hollow body 4 (the Karman vortex generated by the hollow body 4 is The fluid inside the hollow body 4 may be affected through the holes 4a and 4b provided in the body 4), (C) is an example in which the holes 4a and 4b are provided on the downstream side of the streamlined hollow body 4. (D) The diagram shows the hollow body 4 on the downstream side of the cylindrical hollow body 4.
An example in which a partition plate 5 is provided in parallel with the hollow body 4 to prevent the formation of Karman vortices. 4a and 4b, in which a dustproof plate 6 is provided on the upstream side of the hollow body 4, and the holes 4a and 4b are clogged with dust, and dust enters the hollow body 4 through the chain holes 4a and 4b. In this example, the dust-proof plate 6 can be provided over the entire length of the flow side of the hollow body 4, or can be provided over the entire length of the hole 4.
It may be provided only on the second-stream side of a and 4b. The vortex flowmeter according to the present invention can be applied to both liquids and gases, but when measuring the flow rate of gases, especially high-temperature air, etc., the vortex flowmeter shown in FIG. As shown in FIG. 1, it is preferable that a drainage hole 7 is further provided in the hollow body 4 so that the water droplets accumulated in the hollow body 4 can be discharged through the water hole 7. In addition, although an example in which a pair of holes 4a and 4b are provided in the hollow body 4 has been described below, the number of chain holes is not limited to one pair, and they do not necessarily have to form a pair. It is easy to understand that this is nothing.

第3図は、本発明の他の実施例を示す要部拡大構成図で
、この実施例は、図示のように、中空体4の孔4a 、
4bをギ0う防塵板6a、6bを中空体4と一体的に設
けたもので、このようにすると、中空体4の穴4a、4
bの方向を上流側、下流側のいずれの方向に向けても鎖
孔4a、4bを通して中空体4内に塵埃等が混入するよ
うなことはない。その際、防塵板の開口部を図示のよう
に渦側に開口しておくと、該渦に基づく圧力変化を効果
的に中空体4内に導くことができる。
FIG. 3 is an enlarged configuration diagram of main parts showing another embodiment of the present invention. In this embodiment, as shown, the holes 4a of the hollow body 4,
The dustproof plates 6a and 6b that cover the holes 4b are provided integrally with the hollow body 4.
No matter which direction b is directed, upstream or downstream, no dust or the like will enter the hollow body 4 through the chain holes 4a, 4b. At that time, if the opening of the dustproof plate is opened toward the vortex side as shown in the figure, pressure changes caused by the vortex can be effectively guided into the hollow body 4.

軌−一一盟 以トの説明から明らかなように、本発明によると、カル
マン渦の計測を、外乱の影響を受けない中空体内で行う
よにしたので、精度よく行うことができる。
As is clear from the above description, according to the present invention, since the Karman vortex is measured in a hollow body that is not affected by disturbances, it can be performed with high accuracy.

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

第1図は、本発明による渦流量計の要部構成図で、(A
)図は(B)図のA、−A線断面図、CB)図は(A)
図のB−B線断面図、第2図(A)〜(F)は、それぞ
れ本発明の実施に使用し得る中空体の変形例を示す図、
第3図は、本発明の一実施例を示す要部拡大構成図であ
る。 1・・・流路管、2・・・渦発生体、3a、3b・・・
カルマン渦、4・・・中空体、4a、4b・・・孔、5
・・・仕切板、6.6a、6b・・・防塵板、7・・・
刊本孔。 特許出願人  オーバル機器工業株式会社第  l  
図 CA1     (B。 第2図 (A)     tFl 第3図
FIG. 1 is a block diagram of the main parts of the vortex flow meter according to the present invention, (A
) The figure is (B) A, -A cross-sectional view of the figure, CB) The figure is (A)
The cross-sectional view taken along the line B-B in the figure and FIGS. 2 (A) to (F) are views showing modified examples of the hollow body that can be used to implement the present invention, respectively.
FIG. 3 is an enlarged configuration diagram of main parts showing an embodiment of the present invention. 1... Channel pipe, 2... Vortex generator, 3a, 3b...
Karman vortex, 4... hollow body, 4a, 4b... hole, 5
...Partition plate, 6.6a, 6b...Dustproof plate, 7...
Published by Honkou. Patent applicant Oval Equipment Industry Co., Ltd. No. 1
Figure CA1 (B. Figure 2 (A) tFl Figure 3

Claims (7)

【特許請求の範囲】[Claims] (1)、被測定流体中に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配設され
た中空体と、該中空体の軸方向に所定の間隔を置いて設
けられた少なくとも1対の孔を有し、該中空体内におけ
る流体の圧力変動を検出するようにしたことを特徴とす
る渦流量計。
(1) A vortex generator disposed in the fluid to be measured, a hollow body disposed on the downstream side of the vortex generator in a direction intersecting the vortex generator, and an axial direction of the hollow body. 1. A vortex flowmeter comprising at least one pair of holes provided at a predetermined interval in the hollow body, the vortex flowmeter being configured to detect pressure fluctuations of fluid within the hollow body.
(2)、前記孔が前記中空体の1−流側の面に設けられ
ている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。
(2) The vortex flowmeter according to claim (1), wherein the hole is provided on the 1-stream side surface of the hollow body.
(3) 、 niJ記孔が前記中空体の下流側の面に設
けられていることを特徴とする特許請求の範囲第(+)
項に記載の渦流量計。
(3) Claim No. (+) characterized in that niJ holes are provided on the downstream surface of the hollow body.
Vortex flowmeter as described in Section.
(4)、前記中空体の下流側が流線形に形成されている
ことを特徴とする特許請求の範囲第(1)項乃¥第(3
) fAのいずれか1項に記載の渦流量計。
(4) The downstream side of the hollow body is formed in a streamlined shape.
) The vortex flowmeter according to any one of fA.
(5)、前記中空体の下流側に該中÷体と平行に仕切り
板か設けられていることを特徴とする特許請求の範囲第
(1)項乃至第(3)項のいずれか1項に記載の渦流量
計。
(5) Any one of claims (1) to (3), characterized in that a partition plate is provided on the downstream side of the hollow body in parallel with the hollow body. Vortex flowmeter as described in.
(6)、前記中空体の上流側に、前記孔に塵埃が入るの
を防止するための防塵板を有することを特徴とする特許
請求の範囲第(1)項乃至第(5)項のいずれか1項に
記載の渦流量計。
(6) A dustproof plate is provided on the upstream side of the hollow body to prevent dust from entering the hole. The vortex flow meter according to item 1.
(7)、前記中空体の孔の北側に該中空体と一体的に該
孔に塵埃か入るのを防止する防塵板を設けたことを特徴
とする特許請求の範囲fB(1)項乃至第(5)項のい
ずれか1項に記載の渦流量目。 (e) 、 「1ij記中空体に排水孔を有することを
特徴とする特許請求の範囲第(1)項乃至第(7)項の
いずれか1項に記載の渦がL箪ハ1゜
(7) Claims fB (1) to (1) above characterized in that a dustproof plate is provided on the north side of the hole of the hollow body to prevent dust from entering the hole integrally with the hollow body. (5) The eddy flow item described in any one of the items. (e) The vortex according to any one of claims (1) to (7), characterized in that the hollow body has a drainage hole,
JP58060333A 1983-04-06 1983-04-06 Vortex flow-meter Granted JPS59187222A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP58060333A JPS59187222A (en) 1983-04-06 1983-04-06 Vortex flow-meter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP58060333A JPS59187222A (en) 1983-04-06 1983-04-06 Vortex flow-meter

Publications (2)

Publication Number Publication Date
JPS59187222A true JPS59187222A (en) 1984-10-24
JPH059724B2 JPH059724B2 (en) 1993-02-05

Family

ID=13139133

Family Applications (1)

Application Number Title Priority Date Filing Date
JP58060333A Granted JPS59187222A (en) 1983-04-06 1983-04-06 Vortex flow-meter

Country Status (1)

Country Link
JP (1) JPS59187222A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS62150630U (en) * 1986-03-16 1987-09-24
EP0240772A2 (en) * 1986-03-15 1987-10-14 Oval Engineering Co., Ltd. A vortex flow meter

Citations (1)

* 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

Patent Citations (1)

* 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

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0240772A2 (en) * 1986-03-15 1987-10-14 Oval Engineering Co., Ltd. A vortex flow meter
US4838092A (en) * 1986-03-15 1989-06-13 Oval Engineering Co., Ltd. Vortex flow meter
JPS62150630U (en) * 1986-03-16 1987-09-24

Also Published As

Publication number Publication date
JPH059724B2 (en) 1993-02-05

Similar Documents

Publication Publication Date Title
US3732731A (en) Bluff body flowmeter with internal sensor
US4976155A (en) Fluidic flowmeter
US8136413B2 (en) Bi-directional oscillating jet flowmeter
GB2161941A (en) Mass flow meter
US4030355A (en) Obstacle assembly for vortex type flowmeter
US4683760A (en) Vortex flow meter
CA1325734C (en) Trapped-vortex pair flowmeter
US4457181A (en) Narrow profile vortex shedding body
JPS59187222A (en) Vortex flow-meter
CZ290693A3 (en) Liquid oscillator
US4995269A (en) Vortex flowmeter having an asymmetric center body
JPH0456246B2 (en)
GB1598581A (en) Flowmeters
JPS6040914A (en) Vortex flowmeter
CA3051107A1 (en) Insert vortex flowmeter element
JPS60327A (en) Vortex flow meter
JP4675503B2 (en) Ultrasonic vortex flowmeter
JPH01178820A (en) Karman vortex flowmeter
JPS6143205Y2 (en)
SU1746223A1 (en) Vortex-type flowmeter
JP2577705Y2 (en) Vortex flow meter
JPS59107208A (en) Vortex street flowmeter
JPS61280521A (en) Flowmeter
JPH0450725A (en) Vortex flowmeter
JP2001141535A (en) Flowmeter