JPH02307018A - Vortex flowmeter - Google Patents

Vortex flowmeter

Info

Publication number
JPH02307018A
JPH02307018A JP12933789A JP12933789A JPH02307018A JP H02307018 A JPH02307018 A JP H02307018A JP 12933789 A JP12933789 A JP 12933789A JP 12933789 A JP12933789 A JP 12933789A JP H02307018 A JPH02307018 A JP H02307018A
Authority
JP
Japan
Prior art keywords
vortex
turbulence
conduit
column
fluid
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
JP12933789A
Other languages
Japanese (ja)
Other versions
JP2527237B2 (en
Inventor
Yoshihiko Tanimura
嘉彦 谷村
Hisato Ishiguro
石黒 久人
Yasuo Tada
多田 靖夫
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
Mitsubishi Motors Corp
Original Assignee
Mitsubishi Electric Corp
Mitsubishi Motors 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, Mitsubishi Motors Corp filed Critical Mitsubishi Electric Corp
Priority to JP1129337A priority Critical patent/JP2527237B2/en
Priority to AU55825/90A priority patent/AU621755B2/en
Priority to DE4016673A priority patent/DE4016673A1/en
Priority to US07/527,506 priority patent/US5052229A/en
Publication of JPH02307018A publication Critical patent/JPH02307018A/en
Priority to KR2019930025563U priority patent/KR940000704Y1/en
Application granted granted Critical
Publication of JP2527237B2 publication Critical patent/JP2527237B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Abstract

PURPOSE:To enable stable vortex generation and to obtain an inexpensive, high- accuracy vortex flowmeter by molding a turbulence generation body, which is provided on the entrance surface side of a straightener on the center axis of a vortex generation body in parallel to it, and a fixation member in one body. CONSTITUTION:The vortex generation column 3 arranged in a conduit 1 consists of an upstream-side vortex generation column 31 and a downstream-side vortex generation column 32. The honeycomb-shaped straightener 4 fitted to the opening part of the conduit 1 on the fluid entrance side has the fixation member 5b supported on the opening flange of the conduit 2 with rivets 6. The turbulence generation body 5a arranged on the entrance surface side of the straightener 4 on the center axis of the vortex generation column 3 in parallel to it is molded integrally with the fixation member 5b. Thus, the turbulence generation body 5a is provided on the upstream side of the vortex generation column 3, so a turbulence is generated in part of fluid and Karman vortexes which are generated on the downstream side of the vortex generation column 3 as a result are stabilized to obtain the vortexes with small fluctuations. Further, the turbulence generation body 5a is molded integrally with the fixation member 5b for supporting the straightener 4, so the number of parts is decreased and the manufacture and assembly are facilitated.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 この発明は車両等の内燃機関に用いられ、特に流れの乱
れの大きい流体を測定するための渦流量針に関するもの
である。
DETAILED DESCRIPTION OF THE INVENTION [Industrial Application Field] The present invention relates to a vortex flow needle used in internal combustion engines such as vehicles, and particularly for measuring fluids whose flow is highly turbulent.

〔従来の技術〕[Conventional technology]

車両等の内燃機関に渦流量計が用いられる場合は、例え
ば特開昭5El−21517号公報や特公昭62−26
686号公報に開示されているように、必らず機関のエ
アクリーナの下流側に取付けられる。このような構成に
おいては、流体の流れの安定性が低いため低流量から高
流量まで精度よく計測できないという問題があった。こ
のため、例えば特開昭61−134620号公報では渦
発生柱の上流側に流体の一部に乱れを発生させる乱流発
生体を配置し、渦の発生の安定性向上を計ることが促案
されている。
When a vortex flow meter is used in an internal combustion engine such as a vehicle, for example, Japanese Patent Application Laid-Open No. 5 El-21517 and Japanese Patent Publication No. 62-26
As disclosed in Japanese Patent No. 686, it is always installed downstream of the air cleaner of the engine. In such a configuration, there is a problem in that the stability of the fluid flow is low, so that accurate measurement from low flow rates to high flow rates cannot be performed. For this reason, for example, Japanese Patent Application Laid-Open No. 61-134620 recommends placing a turbulence generator that generates turbulence in a part of the fluid upstream of the vortex generating column to improve the stability of vortex generation. has been done.

〔発明が解決しようとする課題〕[Problem to be solved by the invention]

しかしながら、上記による方法では例えば特開昭57−
67863号公報に記述しであるように乱流発生体は渦
発生柱によって決まるべき渦周波数、すなわち流量特性
を補正できるほどの強い影響を有しているため、乱流発
生体が発生する渦が柱状でかつ、周期的ないわゆるカル
マン渦になりやすい場合、渦発生体で流量特性に与える
影響が大きいので、乱流発生体の形状寸法や配置精度を
蔽しく要求されていた。
However, in the above method, for example,
As described in Publication No. 67863, turbulence generators have a strong enough influence to correct the vortex frequency, that is, the flow rate characteristics that should be determined by the vortex generation column, so the vortices generated by the turbulence generators If the vortex tends to form a columnar and periodic Karman vortex, the vortex generator has a large influence on the flow characteristics, so the shape and placement accuracy of the turbulence generator must be carefully selected.

ごの発明は上記のような課題を解消するためになされた
もので、安定した渦発生が得られると共に、安価で高精
度な渦流量計を得ることを目的とする。
This invention was made in order to solve the above-mentioned problems, and aims to obtain a vortex flowmeter that can stably generate vortices and is inexpensive and highly accurate.

〔課題を解決するための手段〕[Means to solve the problem]

この発明に係る渦流量計は、被測定流体の流れる導管を
有し、この導管内にカルマン渦を発生させる渦発生柱と
、上記導管の入口側にハニカム状あるいは網目状の整流
器と、この整流器を上記導管の入口開口部に支持する固
定部材とを備えた渦流量計において、上記整流器の入口
面側に上記渦発生柱の中心軸線上でかつ、これと平行に
被測定流体の流れを阻害する乱流発生体を設け、この乱
流発生体と上記固定部材とを一体成形したことを特徴と
する。
The vortex flowmeter according to the present invention has a conduit through which a fluid to be measured flows, a vortex generating column that generates a Karman vortex in the conduit, a honeycomb-shaped or mesh-shaped rectifier on the inlet side of the conduit, and the rectifier. and a fixing member that supports the inlet opening of the conduit, the flow of the fluid to be measured is obstructed on the inlet surface side of the rectifier on and parallel to the central axis of the vortex generating column. The present invention is characterized in that a turbulence generator is provided, and the turbulence generator and the fixing member are integrally molded.

〔作 用) この発明においては、渦発生柱の上流側に乱流発生体を
設けたことで、流体の一部に乱流を発生させ、これによ
って渦発生柱の下流に生じるカルマン渦を安定化し、揺
らぎの少ない渦を得ることができる。
[Function] In this invention, by providing a turbulence generator upstream of the vortex generating column, turbulence is generated in a part of the fluid, thereby stabilizing the Karman vortex generated downstream of the vortex generating column. It is possible to obtain a vortex with little fluctuation.

〔実施例〕〔Example〕

以下、この発明の一実施例を図について説明する。第1
図はこの発明による渦流量計の横断平面図、第2図は渦
流量計を流体入口側より見た正面図、第3図は第1図の
11線断面図を示す。各図において、渦流量計は全体を
符号1で示し、2は被測定流体の流れる導管である。3
は導管l内に配置した渦発生柱で、上流側渦発生柱31
と下流側渦発生柱32から構成されている。4は上記導
管lの流体入口側の開口部に取付けたハニカム形状の整
流器で、この整流器4は固定部材5bをリベット6で導
管2の開口フランジ2aに支持しである。5aは上記整
流器4の入口面側で上記渦発生柱3の中心軸線上に位置
しかつ、これと平行に配置した乱流発生体であり、この
乱流発生体5aは上記固定部材5bと一体的に成形され
ている。
An embodiment of the present invention will be described below with reference to the drawings. 1st
2 is a cross-sectional plan view of a vortex flowmeter according to the present invention, FIG. 2 is a front view of the vortex flowmeter viewed from the fluid inlet side, and FIG. 3 is a sectional view taken along line 11 in FIG. 1. In each figure, the vortex flow meter is designated as a whole by the reference numeral 1, and 2 is a conduit through which the fluid to be measured flows. 3
is a vortex generation column placed inside the conduit l, and the upstream vortex generation column 31
and a downstream vortex generating column 32. Reference numeral 4 denotes a honeycomb-shaped rectifier attached to the opening on the fluid inlet side of the conduit 1. The rectifier 4 has a fixing member 5b supported by a rivet 6 on the opening flange 2a of the conduit 2. Reference numeral 5a denotes a turbulence generator located on the central axis of the vortex generating column 3 on the inlet side of the rectifier 4 and arranged parallel thereto, and the turbulence generator 5a is integrated with the fixing member 5b. It is shaped like this.

次に動作について説明する。第1図において、流体がF
1〜F、で示す流れを存していると、主導管l内の渦発
生柱3の直上流の流体はf 7.  r zl。
Next, the operation will be explained. In Figure 1, the fluid is F
1 to F, the fluid immediately upstream of the vortex generating column 3 in the main pipe l is f7. r zl.

Ext、Isに示す流れとなり、渦発生柱3の後流にカ
ルマン渦Vが発゛生ずる。ここで、乱流発生体5aがな
い1合は破線で示す流体rtが流体r。
The flow becomes as shown in Ext and Is, and a Karman vortex V is generated in the wake of the vortex generating column 3. Here, if there is no turbulence generator 5a, the fluid rt shown by the broken line is the fluid r.

f、と平行に生じることになるが、乱流発生体5aが存
在すると流体Fつは乱流発生体5aの直後より乱れが発
生する。そして、流体’ 11+  f 12で囲まれ
る領域巳は乱流域である。
If the turbulence generator 5a is present, turbulence will occur in the fluid F immediately after the turbulence generator 5a. The region surrounded by the fluid '11+f12 is a turbulent region.

渦発生柱3に衝突する流体に乱れがあるとカルマン渦が
発生しやすいことは周知のことである。
It is well known that Karman vortices are likely to occur when there is turbulence in the fluid colliding with the vortex generating column 3.

ここで、上記した乱流域Eの乱流杖態を説明する。Here, the turbulent flow state of the above-mentioned turbulent region E will be explained.

乱流発生体5aの後流の渦は流れに対して直角断面では
勇往状となる。また渦はいわゆるカルマン渦である。し
かし、乱流発生体5aの直後の整流器4によって直角断
面方向に流れが分断されるため、第4図に示すVtgに
示す流速分布にて明らかなように溝柱はくずされる。し
たがって乱流域E内は流れに平行面および直角面のいず
れの方向にも乱れることになる。このため、乱流発生体
5aの発生する乱流が渦発生柱3のカルマン渦発生のト
リガ的要素となるのみで、渦発生柱3のカルマン渦発生
周期に大きく拘わることがない、したがって、乱流発生
体5aの幅寸法dが多少変化しても渦発生柱3によって
決定されるカルマン渦発生周期を乱すことがないため、
乱流発生体5aの寸法精度を高める必要はなくなる。
The vortices downstream of the turbulent flow generator 5a have a turbulent shape in a cross section perpendicular to the flow. Moreover, the vortex is a so-called Karman vortex. However, since the flow is divided in the perpendicular cross-sectional direction by the rectifier 4 immediately after the turbulent flow generator 5a, the groove column is collapsed as is clear from the flow velocity distribution shown by Vtg shown in FIG. Therefore, within the turbulent region E, turbulence occurs in both directions parallel to and perpendicular to the flow. Therefore, the turbulent flow generated by the turbulence generating body 5a only serves as a triggering factor for the generation of Karman vortices in the vortex generating column 3, and does not greatly affect the Karman vortex generation period of the vortex generating column 3. Even if the width dimension d of the flow generator 5a changes slightly, the Karman vortex generation period determined by the vortex generation column 3 is not disturbed.
There is no need to improve the dimensional accuracy of the turbulent flow generator 5a.

ここで、第4図に乱流発生体5aの寸法dと渦発生柱3
の寸法りによるカルマン渦の発生周期の安定性すなわち
、渦の揺らぎ率を示す、この図から実線はこの発明によ
るd/Dと揺らぎ重度化を示し、破線は従来装置による
揺らぎ率を示す。
Here, the dimension d of the turbulence generating body 5a and the vortex generating column 3 are shown in FIG.
In this figure, the solid line shows d/D and fluctuation severity according to the present invention, and the broken line shows the fluctuation rate according to the conventional device.

第5図(al〜(句は上記乱流発生体5aの種々の断面
形状を示す、これについては(a)図に示すように流体
の流れに対し矩形であるのが最も流体に乱れが生じやす
いが、逆に流体の圧力損失が大きいため、(ロ)〜(d
)図に示すように乱流発生体5aの上流面にそれぞれの
形状の凸状部を形成するようにした方が圧力損失が小さ
くできて好ましい。
Figure 5 (al~) shows various cross-sectional shapes of the turbulence generating body 5a, as shown in Figure (a), a rectangular shape is most likely to cause turbulence in the fluid. However, since the pressure loss of the fluid is large, (b) ~ (d
) As shown in the figure, it is preferable to form convex portions of respective shapes on the upstream surface of the turbulent flow generating body 5a because the pressure loss can be reduced.

また、上記したように乱流発生体5aと整流器4を支持
する固定部材5bとを一体成形することで、乱流発生体
5aの支持部材は不要となり、その分、組立て工数も削
減と共に、乱流発生体5aとして特別な部材を用意する
こともない。
Furthermore, as described above, by integrally molding the turbulence generator 5a and the fixing member 5b that supports the rectifier 4, the support member for the turbulence generator 5a is not required, and the number of assembly steps is reduced accordingly. There is no need to prepare a special member as the flow generator 5a.

なお、実施例では整流器4.7はハニカム形状のものを
使用した例について説明したが、その他、網目状の整流
器であっても上記同様の作用が得られる。
In the embodiment, an example in which a honeycomb-shaped rectifier 4.7 is used has been described, but the same effect as described above can be obtained even if a mesh-shaped rectifier is used.

〔発明の効果〕〔Effect of the invention〕

以上説明したようにこの発明によれば、導管内に配!し
た渦発生柱の上流で整流器の入口面側に乱流発生体を配
置したので、流量特性が乱流発生体の寸法精度によって
大きく影響を受けることなく、しかも、渦発生柱の上流
の流れに乱れがあっても渦の揺らぎの少ない高精度で安
価な渦流量計となる。また、上流乱流発生体は整流器を
支持するための固定部材と一体成形したことで、部品点
数が削減できると共に、製作および組立が容昌となる。
As explained above, according to the present invention, the Since the turbulence generator is placed on the inlet side of the rectifier upstream of the vortex generating column, the flow characteristics are not significantly affected by the dimensional accuracy of the turbulence generator, and moreover, The result is a highly accurate and inexpensive vortex flowmeter that exhibits little vortex fluctuation even when there is turbulence. Furthermore, since the upstream turbulence generator is integrally molded with the fixing member for supporting the rectifier, the number of parts can be reduced and manufacturing and assembly can be simplified.

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

第1図はこの発明の一実施例による渦流量計の横断平面
図、第2図は渦流量計を流体の入口側より見た正面図、
第3図第1図の11線断面図、第4図は渦の13らぎ率
の特性図、第5図(a)〜(d)は乱流発生体の横断面
形状の種々の例を示す断面図である。 2・・・導管、3・・・渦発生柱、4・・・整流器、5
a・・・乱流発生体、5b・・・固定部材。 なお、図中同一符号は同−又は相当部分を示す。
FIG. 1 is a cross-sectional plan view of a vortex flowmeter according to an embodiment of the present invention, FIG. 2 is a front view of the vortex flowmeter seen from the fluid inlet side,
Figure 3 is a sectional view taken along the line 11 in Figure 1, Figure 4 is a characteristic diagram of the 13 lag factor of the vortex, and Figures 5 (a) to (d) are various examples of the cross-sectional shape of the turbulence generator. FIG. 2... Conduit, 3... Vortex generating column, 4... Rectifier, 5
a... Turbulent flow generator, 5b... Fixing member. Note that the same reference numerals in the figures indicate the same or equivalent parts.

Claims (1)

【特許請求の範囲】[Claims] 被測定流体の流れる導管を有し、この導管内にカルマン
渦を発生させる渦発生柱と、上記導管の入口側にハニカ
ム状あるいは綱目状の整流器と、この整流器を上記導管
の入口開口部に支持する固定部材とを備えた渦流量計に
おいて、上記整流器の入口面側に上記渦発生柱の中心軸
線上でかつ、これと平行に被測定流体の流れを阻害する
乱流発生体を設け、この乱流発生体と上記固定部材とを
一体成形したことを特徴とする渦流量計。
It has a conduit through which the fluid to be measured flows, a vortex generation column that generates a Karman vortex in the conduit, a honeycomb-shaped or wire-shaped rectifier on the inlet side of the conduit, and this rectifier supported at the inlet opening of the conduit. In the vortex flowmeter, a turbulence generator is provided on the inlet surface side of the rectifier on the central axis of the vortex generating column and parallel to the central axis to obstruct the flow of the fluid to be measured. A vortex flowmeter characterized in that a turbulent flow generator and the fixing member are integrally molded.
JP1129337A 1989-05-23 1989-05-23 Vortex flowmeter Expired - Lifetime JP2527237B2 (en)

Priority Applications (5)

Application Number Priority Date Filing Date Title
JP1129337A JP2527237B2 (en) 1989-05-23 1989-05-23 Vortex flowmeter
AU55825/90A AU621755B2 (en) 1989-05-23 1990-05-22 Vortex flowmeter
DE4016673A DE4016673A1 (en) 1989-05-23 1990-05-23 Vortex flow measuring device
US07/527,506 US5052229A (en) 1989-05-23 1990-05-23 Vortex flowmeter
KR2019930025563U KR940000704Y1 (en) 1989-05-23 1993-11-30 Turbulence flow meter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1129337A JP2527237B2 (en) 1989-05-23 1989-05-23 Vortex flowmeter

Publications (2)

Publication Number Publication Date
JPH02307018A true JPH02307018A (en) 1990-12-20
JP2527237B2 JP2527237B2 (en) 1996-08-21

Family

ID=15007113

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1129337A Expired - Lifetime JP2527237B2 (en) 1989-05-23 1989-05-23 Vortex flowmeter

Country Status (1)

Country Link
JP (1) JP2527237B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2002243515A (en) * 2001-02-14 2002-08-28 Ricoh Co Ltd Flow velocity measuring device

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5181154A (en) * 1975-01-10 1976-07-15 Yokogawa Electric Works Ltd RYUSOKUSOKUTEISOCHI
JPS61134620A (en) * 1984-12-05 1986-06-21 Nippon Denso Co Ltd Flow rate measuring device of karman's vortex street type
JPS63180819A (en) * 1987-01-22 1988-07-25 Nippon Denso Co Ltd Air flowmeter having straightening lattice

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5181154A (en) * 1975-01-10 1976-07-15 Yokogawa Electric Works Ltd RYUSOKUSOKUTEISOCHI
JPS61134620A (en) * 1984-12-05 1986-06-21 Nippon Denso Co Ltd Flow rate measuring device of karman's vortex street type
JPS63180819A (en) * 1987-01-22 1988-07-25 Nippon Denso Co Ltd Air flowmeter having straightening lattice

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2002243515A (en) * 2001-02-14 2002-08-28 Ricoh Co Ltd Flow velocity measuring device

Also Published As

Publication number Publication date
JP2527237B2 (en) 1996-08-21

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