JPH0620972Y2 - Vortex flowmeter - Google Patents

Vortex flowmeter

Info

Publication number
JPH0620972Y2
JPH0620972Y2 JP1986178079U JP17807986U JPH0620972Y2 JP H0620972 Y2 JPH0620972 Y2 JP H0620972Y2 JP 1986178079 U JP1986178079 U JP 1986178079U JP 17807986 U JP17807986 U JP 17807986U JP H0620972 Y2 JPH0620972 Y2 JP H0620972Y2
Authority
JP
Japan
Prior art keywords
vortex
flow
generating element
flat plate
vortex generating
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 - Lifetime
Application number
JP1986178079U
Other languages
Japanese (ja)
Other versions
JPS6383618U (en
Inventor
勝夫 三角
浩司 渥美
Original Assignee
オ−バル機器工業株式会社
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 オ−バル機器工業株式会社 filed Critical オ−バル機器工業株式会社
Priority to JP1986178079U priority Critical patent/JPH0620972Y2/en
Priority to US07/024,294 priority patent/US4838092A/en
Priority to EP87103713A priority patent/EP0240772B1/en
Priority to DE3750965T priority patent/DE3750965T2/en
Priority to CA000532031A priority patent/CA1306120C/en
Priority to KR1019870002350A priority patent/KR920004100B1/en
Publication of JPS6383618U publication Critical patent/JPS6383618U/ja
Priority to US07/283,656 priority patent/US4891989A/en
Priority to US07/398,197 priority patent/US4977781A/en
Application granted granted Critical
Publication of JPH0620972Y2 publication Critical patent/JPH0620972Y2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Description

【考案の詳細な説明】 技術分野 本考案は、渦流量計における渦発生体の構造に関する。TECHNICAL FIELD The present invention relates to a structure of a vortex generator in a vortex flowmeter.

従来技術 本出願人は特公昭55−40804号公報において流体
の流れ方向に対して渦発生素子を設け、この渦発生素子
の後方に所望の厚さを有するカルマン渦発生素子板を一
体的に設け、さらにこのカルマン渦発生素子板の後方に
少なくとも1若しくは2以上の前記と同様のカルマン渦
発生素子板を所望の間隔においてかつそれぞれ独立して
配設するカルマン渦形成装置を提案した。上記の渦発生
素子は流れ軸上に頂点をもつ鋭角な二等辺三角形状をし
た断面形状をしており、ここで発生した渦を後部に配設
された1若しくは2以上のカルマン渦発生素子板(以
下、単に平板と呼ぶ)により渦を最適な強さに発達さ
せ、最終段の平板より渦を剥離させるものである。この
ようにしてカルマン渦発生素子で発生した渦は充分強い
渦として発達させることができるので安定した渦発生体
を得ることができた。
2. Description of the Related Art The applicant of the present application discloses, in Japanese Patent Publication No. 55-40804, a vortex generating element provided in the direction of fluid flow, and a Karman vortex generating element plate having a desired thickness is integrally provided behind the vortex generating element. Furthermore, there has been proposed a Karman vortex forming device in which at least one or more Karman vortex generating element plates similar to those described above are arranged behind the Karman vortex generating element plate at desired intervals and independently of each other. The above-mentioned vortex generating element has a cross-sectional shape of an isosceles triangle having an apex on the flow axis, and one or more Karman vortex generating element plates provided at the rear of the vortex generated here. (Hereinafter, simply referred to as a flat plate), the vortex is developed to have an optimum strength, and the vortex is separated from the final flat plate. In this way, the vortex generated by the Karman vortex generating element can be developed as a sufficiently strong vortex, so that a stable vortex generator can be obtained.

従来技術の問題点 叙上の従来技術においては渦発生体の後流側に平板を併
置することにより渦の増幅効果があるため、適当な平板
の数を選択することにより最終段の平板から剥離する場
合、それまでに充分に発達した渦が生成されているので
剥離に要する時間も短くなり周波数の極めて安定した渦
が生成される特徴があるが、低レイノルズ数域で渦流量
計の器差はプラスに暫増する特性を持つという問題点が
あった。
Problems of the prior art In the above prior art, since the vortex amplification effect is obtained by arranging flat plates on the wake side of the vortex generator, separation from the final flat plate by selecting an appropriate number of flat plates. In this case, the fully developed vortex has been generated so far, so the time required for separation is shortened and the vortex with extremely stable frequency is generated. Had a problem that it had a positively increasing characteristic.

問題点解決のための手段 上記問題点に対し、本出願人は、渦発生体が流路内に配
設された状態において、渦発生体を構成する渦発生素子
が単独に配設されたときの上流側渦発生体と下流側渦発
生素子とから、各々発生する渦の渦周波数比が所定の比
率であるとき器差のレイノルズ数特性、特に、低レイノ
ルズ数域で改善されることを着目した。例えば、複数の
渦発生素子からなる渦発生体として、上記の流れ軸上に
頂点をもつ鋭角な二等辺三角状の渦発生素子と、この渦
発生素子の後流側に1又は2以上の平板からなる渦発生
素子で構成された場合では、上流側の二等辺三角状の渦
発生素子の断面形状が底面の長さをd,高さを0.6dと
し、最終段の平板の流れに面した方向の長さをd、該平
板の厚さを0.2〜0.3dとし、前記渦発生素子間の間隔を
0.1〜0.9dとした場合に、上流側の渦発生素子から単独
に発生する渦周波数に対して最終段の平板から単独に発
生する渦の渦周波数の比率が0.7〜0.9であり、このとき
平坦なレイノルズ数器差特性になることが確かめられ
た。更に、上記周波数比を充たす渦発生素子の形状を試
験した結果、上流側渦発生素子の断面形状が上流側に円
弧を有する弓形、下流側渦発生素子の断面形状を流れに
面した方向の長さが前記弓形の弦に平行で長さが弦の長
さに等しい略等しい底辺を有し下流側に突出する辺を有
するT字形をした場合、広い流量範囲に亘って一定の器
差特性をもつ渦流量計が実現できた。
Means for Solving the Problems To solve the above problems, the present applicant has proposed that when the vortex generating element forming the vortex generator is arranged independently in a state where the vortex generator is arranged in the flow path. Focusing on the Reynolds number characteristic of the instrumental error, especially in the low Reynolds number region, when the vortex frequency ratio of each vortex generated from the upstream side vortex generator and the downstream side vortex generator is a predetermined ratio. did. For example, as a vortex generator including a plurality of vortex generators, an acute-angled isosceles triangular vortex generator having an apex on the above-mentioned flow axis and one or more flat plates on the downstream side of the vortex generator. In the case of the vortex generating element consisting of, the cross section of the upstream isosceles triangular vortex generating element has a bottom length of d and a height of 0.6d, and faces the flow of the flat plate at the final stage. The length in the direction is d, the thickness of the flat plate is 0.2 to 0.3d, and the space between the vortex generating elements is
When 0.1 to 0.9d is set, the ratio of the vortex frequency of the vortex independently generated from the final flat plate to the vortex frequency independently generated from the upstream vortex generating element is 0.7 to 0.9. It was confirmed that the Reynolds number instrumental error characteristic was obtained. Furthermore, as a result of testing the shape of the vortex generating element that satisfies the above frequency ratio, the cross-sectional shape of the upstream vortex generating element is arcuate with an arc on the upstream side, and the length in the direction facing the flow of the cross-sectional shape of the downstream vortex generating element. In the case of a T-shape having a base parallel to the chord of the bow and having a length substantially equal to the length of the chord and a side projecting to the downstream side, a constant instrumental error characteristic is obtained over a wide flow range. A vortex flowmeter with a gyro was realized.

実施例 第1図は、本考案による渦流量計の側断面図、第2図は
平断面図で、流路1内に渦発生素子2a,2bが流れ方
向Qに垂直に対向して平行に配設されている。渦発生体
2aは流れた面した弧をもつ弓形で、図においては直径
の半円をしている。2bはT字形で、底部はd
幅をもち、前記渦発生素子2aの弦と平行している。各
々の渦発生素子2a,2bの間には幅dの平板2cが
等間隔で配設されている。渦発生素子2a,2bと平板
2cの幅d,d,dは各々等しい幅dとすること
が好ましく、間隔tは0.1〜0.9dの値である。渦信号は
渦検出器(図示せず)により電気信号に変換され、プリ
アンプ3で整形増幅されて信号処理される。平板は渦増
幅作用を与えるものであるが、従来技術における三角柱
と平板とを組合せた前記従来の渦発生体では低流領域に
おいて器差が上昇する特性をもっていた。渦周波数はス
トローハル数に比例するがストローハル数は渦強度が強
い程小さくなり、従って、渦周波数は渦強度の逆関数と
なる。平板を組合せた場合は渦の増幅作用により渦強度
を増すが先端の三角柱の単独での渦強度は低い。これら
を組合せた渦発生体では各々の渦特性が相互に影響し、
しかも流速との関連において組合せの特性が生ずるの
で、前述のごとき従来技術では低流領域において先端の
三角柱の影響が大きく、これが低流領域での器差上昇特
性となったものである。本出願人は前に述べたごとく、
下流側と上流側との渦発生素子のもつ渦周波数比を0.7
〜0.9とすることを提案したが、本考案においては第3
図及び第4図に示すごとく流路1内に流れQに垂直に対
向して弦長dの弓形の渦発生素子(第3図)と、幅d
のT字形の渦発生素子(第4図)との渦周波数比が前
記の範囲内にあり、幅d=d=dとし、この中央位
置に幅d=dの平板を配置し、この間隔tを0.1〜1.9
dとしたとき、小流から大流領域までの広い流量範囲で
平坦な流量、器差特性をもつことが確認された。また、
これらの特性は安定しており、強い渦信号を発信してい
る。
Embodiment FIG. 1 is a side sectional view of a vortex flowmeter according to the present invention, and FIG. 2 is a plan sectional view, in which a vortex generating element 2a, 2b in a flow path 1 is vertically opposed to and parallel to a flow direction Q. It is arranged. The vortex generator 2a has an arcuate shape with a flow-facing arc, and has a semicircle with a diameter d 1 in the figure. 2b is T-shaped, and the bottom has a width of d 2 and is parallel to the chord of the vortex generating element 2a. Flat plates 2c having a width d 2 are arranged at equal intervals between the vortex generating elements 2a and 2b. The widths d 1 , d 2 , d 3 of the vortex generating elements 2a, 2b and the flat plate 2c are preferably equal to each other, and the interval t is a value of 0.1 to 0.9d. The vortex signal is converted into an electric signal by a vortex detector (not shown), shaped and amplified by the preamplifier 3, and processed. Although the flat plate provides a vortex amplification effect, the conventional vortex generator combining the triangular prism and the flat plate in the prior art has a characteristic that the instrumental error increases in the low flow region. The vortex frequency is proportional to the Strouhal number, but the Strouhal number becomes smaller as the vortex strength becomes stronger. Therefore, the vortex frequency becomes an inverse function of the vortex strength. When flat plates are combined, the vortex strength increases due to the vortex amplification effect, but the vortex strength of the triangular prism at the tip is low. In a vortex generator that combines these, each vortex characteristic affects each other,
In addition, since a combination of characteristics is generated in relation to the flow velocity, in the prior art as described above, the influence of the triangular prism at the tip is large in the low flow region, which is the device difference increasing characteristic in the low flow region. The Applicant, as stated earlier,
Set the vortex frequency ratio of the vortex generators on the downstream side and the upstream side to 0.7.
It was proposed to set the value to ~ 0.9, but in the present invention, the third
As shown in FIGS. 4 and 5, an arcuate vortex generating element (FIG. 3) having a chord length d 1 facing the flow Q in the channel 1 and having a width d
Vortex frequency ratio of the vortex generating elements 2 of T-shaped (FIG. 4) is in the range described above, the width d 1 = d 2 = d, the flat plate of width d 3 = d disposed in the central position , This interval t is 0.1 to 1.9
It was confirmed that when d is set, the flow rate is flat and the instrumental error characteristic is wide in a wide flow range from a small flow area to a large flow area. Also,
These properties are stable and emit strong eddy signals.

効果 上記のように、本考案によると広い流量範囲、即ち、広
いレイノルズ数域で器差の小さい高精度のしかも安定し
た渦流量計を実現できた。
Effect As described above, according to the present invention, a highly accurate and stable vortex flowmeter with a small instrumental error can be realized in a wide flow range, that is, a wide Reynolds number range.

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

第1図及び第2図は本考案における渦流量計の側断面図
および平断面図、第3図及び第4図は本考案の説明に用
いるもので、渦発生素子2a,2bが流路に単独に配設
された場合を示す図である。 1……流路,2a……弓形の渦発生素子,2b……T字
形の渦発生素子,2c……平板。
FIGS. 1 and 2 are side and plan sectional views of the vortex flowmeter according to the present invention, and FIGS. 3 and 4 are used for explaining the present invention. The vortex generating elements 2a and 2b are used as flow paths. It is a figure which shows the case where it is arrange | positioned independently. 1 ... Channel, 2a ... Bow-shaped vortex generating element, 2b ... T-shaped vortex generating element, 2c ... Flat plate.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] 【請求項1】流路内に流れに対向して配設される渦発生
体を流れに面した幅が等しい複数の渦発生素子で構成
し、該渦発生素子の断面形状を上流より順次と、流れに
面した弧をもつ弓形、平板、および該平板と平行した底
部をもつT形とし、前記各々の渦発生素子を所定間隔を
もって配設したことを特徴とする渦流量計。
1. A vortex generator disposed in a flow path so as to face a flow is composed of a plurality of vortex generators having the same width facing the flow, and the cross-sectional shape of the vortex generator is sequentially arranged from upstream. A vortex flowmeter, wherein the vortex flowmeter has a bow shape having an arc facing the flow, a flat plate, and a T shape having a bottom portion parallel to the flat plate, and the vortex generating elements are arranged at predetermined intervals.
JP1986178079U 1986-03-15 1986-11-19 Vortex flowmeter Expired - Lifetime JPH0620972Y2 (en)

Priority Applications (8)

Application Number Priority Date Filing Date Title
JP1986178079U JPH0620972Y2 (en) 1986-11-19 1986-11-19 Vortex flowmeter
US07/024,294 US4838092A (en) 1986-03-15 1987-03-10 Vortex flow meter
DE3750965T DE3750965T2 (en) 1986-03-15 1987-03-13 Vortex flow meter.
CA000532031A CA1306120C (en) 1986-03-15 1987-03-13 Vortex flow meter
EP87103713A EP0240772B1 (en) 1986-03-15 1987-03-13 A vortex flow meter
KR1019870002350A KR920004100B1 (en) 1986-03-15 1987-03-16 The eddy water meter
US07/283,656 US4891989A (en) 1986-03-15 1988-12-13 Vortex flow meter
US07/398,197 US4977781A (en) 1986-03-15 1989-08-24 Vortex flow meter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1986178079U JPH0620972Y2 (en) 1986-11-19 1986-11-19 Vortex flowmeter

Publications (2)

Publication Number Publication Date
JPS6383618U JPS6383618U (en) 1988-06-01
JPH0620972Y2 true JPH0620972Y2 (en) 1994-06-01

Family

ID=31119878

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1986178079U Expired - Lifetime JPH0620972Y2 (en) 1986-03-15 1986-11-19 Vortex flowmeter

Country Status (1)

Country Link
JP (1) JPH0620972Y2 (en)

Family Cites Families (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5438513A (en) * 1977-09-02 1979-03-23 Hitachi Ltd Controller for ac thyristor motor
JPS561119U (en) * 1979-06-18 1981-01-08
JPS61164115A (en) * 1985-01-17 1986-07-24 Nippon Denso Co Ltd Karman's vortex street type air flow rate measuring instrument

Also Published As

Publication number Publication date
JPS6383618U (en) 1988-06-01

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