JPS62214321A - Vortex flowmeter - Google Patents

Vortex flowmeter

Info

Publication number
JPS62214321A
JPS62214321A JP61058975A JP5897586A JPS62214321A JP S62214321 A JPS62214321 A JP S62214321A JP 61058975 A JP61058975 A JP 61058975A JP 5897586 A JP5897586 A JP 5897586A JP S62214321 A JPS62214321 A JP S62214321A
Authority
JP
Japan
Prior art keywords
vortex
vortex generating
tubular body
flow
flow path
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
JP61058975A
Other languages
Japanese (ja)
Other versions
JPH0460535B2 (en
Inventor
Katsuo Misumi
勝夫 三角
Koji Atsumi
浩司 渥美
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 Engineering Co Ltd
Original Assignee
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 Engineering Co Ltd filed Critical Oval Engineering Co Ltd
Priority to JP61058975A priority Critical patent/JPS62214321A/en
Priority to US07/024,294 priority patent/US4838092A/en
Priority to CA000532031A priority patent/CA1306120C/en
Priority to DE3750965T priority patent/DE3750965T2/en
Priority to EP87103713A priority patent/EP0240772B1/en
Priority to KR1019870002350A priority patent/KR920004100B1/en
Publication of JPS62214321A publication Critical patent/JPS62214321A/en
Priority to US07/283,656 priority patent/US4891989A/en
Priority to US07/398,197 priority patent/US4977781A/en
Publication of JPH0460535B2 publication Critical patent/JPH0460535B2/ja
Granted legal-status Critical Current

Links

Abstract

PURPOSE:To obtain a flowmeter which has superior linearity over a wide flow rate range by arranging a tubular body having pressure intakes where pressure variation due to a vortex is admitted on the downstream side of a vortex generating body so that the tubular body crosses a flow. CONSTITUTION:The vortex generating device 2 arranged opposite the flow in a flow passage 1 is constituted by arranging successively an upstream-side vortex generating element 2a in an isosceles triangle shape, a T-shaped downstream-side vortex generating element 2b which has a little bit lower vortex frequency than it, and a flat plate 2c which is arranged between them at specific intervals. The tubular body 3 is supported penetrating the wall of the flow passage 1 on the downstream side of the vortex generating body 2 while crossing it. The tubular body 3 has both end surfaces closed and a tube body 32 having plural pressure intakes 33 is fixed communicating it at right angles. Then, variation pressure is admitted into the pressure intakes 33 to cause fluid displacement, which is detected as an ultrasonic modulated wave. A vortex with superior linearity is obtained by interference due to a difference in vortex frequency between the elements 2a and 2b.

Description

【発明の詳細な説明】 狡亙分互 本発明は、渦流量計においてS/Nの優れた渦信号を検
出するための構造に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a structure for detecting a vortex signal with excellent S/N in a vortex flowmeter.

災米技豊 本出願人は、特願昭58−60333号において、第3
図にしめすように、渦発生体2の後方に該渦発生体2と
交叉する方向に管状体3を配設するとともに、この管状
体3の軸方向に所定の間隔を置いて少くとも1対の圧力
適圧孔31が穿孔されている渦流量計について提案した
。この流量計は、変動圧力を管状体3内に印加して流体
変動を生せしめ、この流体変動を比較的小さい流通面積
の管状体3内に導入することにより、流体が整流される
ことに着目したものである。このようにすると管状体の
ない場合に比して、流路向流れに含まれる乱流渦までも
検出してしまうようなことがなくなり、検出信号内に混
入する雑音成分が少なくなりS/Nの優れた検出信号を
得ることができた。既に発生した渦信号の検出について
は叙上の如き方法により改善されるが、渦発生体に関し
ても、特公昭55−40804号公報に示されるごとく
、流れ方向Aに対して鋭角の二等辺三角形状体を設け、
この発生体の後方に順次所望の間隔をおいて夫々独立し
た平板を配設することにより渦に増幅効果を与え、強い
安定した渦を発生することができた。
The applicant of the present application, in Japanese Patent Application No. 58-60333,
As shown in the figure, a tubular body 3 is disposed behind the vortex generating body 2 in a direction crossing the vortex generating body 2, and at least one pair of tubular bodies 3 is arranged at a predetermined interval in the axial direction of the tubular body 3. We have proposed a vortex flow meter in which a pressure adjustment hole 31 is bored. This flowmeter focuses on the fact that the fluid is rectified by applying a fluctuating pressure inside the tubular body 3 to cause fluid fluctuations, and introducing this fluid fluctuation into the tubular body 3, which has a relatively small flow area. This is what I did. In this way, compared to the case without a tubular body, even turbulent vortices included in the flow in the direction of the flow path will not be detected, and noise components mixed in the detection signal will be reduced, resulting in a lower S/N ratio. We were able to obtain an excellent detection signal. Detection of already generated vortex signals can be improved by the method described above, but the vortex generator also has an isosceles triangular shape with an acute angle to the flow direction A, as shown in Japanese Patent Publication No. 55-40804. Set up your body,
By sequentially arranging independent flat plates behind this generator at desired intervals, it was possible to amplify the vortex and generate a strong and stable vortex.

従迷111旧」悪 しかしながら、叙上の従来技術によると、強い安定した
渦を発生する手段と、これから発生された渦をS/Nの
優れた検出手段とにより、従来にない安定した渦流量計
を具現することができたが、より広範囲な流量を計測す
るためには、渦信号をより強力に得るとともにストロ−
ハル数も前記に対応して広範囲で一定した値を保持する
必要があつた。また、前記特公昭55−40804号公
報においては小流域においてプラスの器差特性をもつの
で、安定な渦発生体でありながらより広範囲の計測を要
求される流量計に対しては不満足な面があった。
However, according to the conventional technology described above, by means of generating a strong and stable vortex and means of detecting the generated vortex with an excellent S/N ratio, it is possible to achieve an unprecedented stable vortex flow rate. However, in order to measure the flow rate over a wider range, it is necessary to obtain a stronger vortex signal and a stroke meter.
Corresponding to the above, it was also necessary to maintain a constant value over a wide range of hull numbers. Furthermore, in the above-mentioned Japanese Patent Publication No. 55-40804, it has a positive instrumental error characteristic in a small flow area, so although it is a stable vortex generator, it is unsatisfactory for flowmeters that are required to measure a wider range. there were.

山 点を °するための手段 本発明は、叙上の問題点に対してなされたもので、渦検
出手段における従来技術の圧力導入孔31が管状体3の
軸方向に配列していたことに対し、渦発生体から発生す
る渦は3次元的には渦柱として渦発生体から剥離される
ことに着目して有効な圧力変動を導入するように渦柱方
向に圧力導入孔を配設するとともに、渦発生体に固有の
特性を改善して広範囲流量に対して直線性の優れた流量
計を得るために、渦発生体を構成する渦発生素子が単独
にもつ渦周波数比に着目をすることにより従来技術の問
題点を解決したものである。
The present invention has been made to solve the above-mentioned problems, and has an advantage in that the pressure introduction holes 31 of the prior art in the vortex detection means are arranged in the axial direction of the tubular body 3. On the other hand, focusing on the fact that the vortex generated from the vortex generator is separated from the vortex generator as a vortex column three-dimensionally, pressure introduction holes are arranged in the direction of the vortex column to introduce effective pressure fluctuations. At the same time, in order to improve the unique characteristics of the vortex generator and obtain a flowmeter with excellent linearity over a wide range of flow rates, we focused on the vortex frequency ratio of the individual vortex generating elements that make up the vortex generator. This solves the problems of the prior art.

某−生一里 第1図は、本発明の詳細な説明するための図で1図中、
第3図に示した従来技術と同一の構造のものには同一の
符号が付しである。渦発生体2は上流側渦発生素子であ
る二等辺三角形状の渦発生素子2aと、下流側に配設さ
れた丁字形の渦発生素子2bと、これらの中間に配設さ
れた平板2cとが、代表長さdが対面する形で順次と配
置されて構成されている。このように配設された渦発生
体2の後流に渦による圧力変動を導入する管状体3が該
渦発生体2と交叉するように流路壁1を貫通して支持さ
れている。第1図(C)は、管状体3の詳細をしめすも
ので、管状体3に1対の管体32が直交して連通して固
着されている。尚、管体の端面は閉鎖されており、複数
の圧力導入孔33が直管壁土に開口している。変動圧力
は1対の圧力導入孔33に導入され、それに従った流体
変位が矢標の如く生ずる。この流体変位を超音波変調信
号として検出する場合は流体中に含まれる超音波の外乱
が侵入するのを防ぐ目的で不織布等の吸音材34を管体
32の内壁に貼付する。第1図(D)は、その斜示図を
しめすもので、切欠35は導圧孔33を閉鎖しないため
に設けられている。一方、渦発生体2は渦発生素子2a
の渦周波数に対して渦発生素子2bの渦周波数比が0.
7〜0.9になる形状が与えられている。平板2cはこ
の間に併置され、各々はtx+ tel t。
Figure 1 is a diagram for explaining the present invention in detail, and in Figure 1,
Components having the same structure as the prior art shown in FIG. 3 are given the same reference numerals. The vortex generating element 2 includes an isosceles triangular vortex generating element 2a which is an upstream vortex generating element, a T-shaped vortex generating element 2b disposed on the downstream side, and a flat plate 2c disposed in the middle thereof. are sequentially arranged so that the representative lengths d face each other. A tubular body 3 that introduces pressure fluctuations due to the vortex into the wake of the vortex generator 2 arranged in this manner is supported so as to penetrate through the channel wall 1 so as to intersect with the vortex generator 2 . FIG. 1(C) shows details of the tubular body 3, in which a pair of tubular bodies 32 are fixed to the tubular body 3 in communication with each other orthogonally. Note that the end face of the pipe body is closed, and a plurality of pressure introduction holes 33 are opened to the wall soil of the straight pipe. The fluctuating pressure is introduced into a pair of pressure introduction holes 33, and a corresponding fluid displacement occurs as indicated by the arrow. When detecting this fluid displacement as an ultrasonic modulation signal, a sound absorbing material 34 such as a nonwoven fabric is attached to the inner wall of the tube body 32 in order to prevent disturbance of ultrasonic waves contained in the fluid from entering. FIG. 1(D) shows a perspective view thereof, and the notch 35 is provided so as not to close the pressure guiding hole 33. On the other hand, the vortex generator 2 is a vortex generator 2a.
The vortex frequency ratio of the vortex generating element 2b to the vortex frequency of 0.
7 to 0.9 is given. The plates 2c are juxtaposed between them, each with tx+tel t.

の間隙が与えられ、t工〜t、=0.1d〜0.4dに
選択される。このように構成された第1図の渦流量計は
、渦発生素子間における渦周波数の相異による干渉によ
り、直線性の優れた渦が得られる。
A gap of t to t is given and selected to be 0.1 d to 0.4 d. The vortex flowmeter of FIG. 1 configured in this way can obtain vortices with excellent linearity due to interference due to differences in vortex frequencies between the vortex generating elements.

即ち、下流側の渦発生素子2bの渦発生周波数は低いの
で渦の循環は強く、高レイノルズ数域を支配し、低レイ
ノルズ数で発生する渦周波数の差が渦発生素子2a、2
b間の間隙に生ずる渦発生素子2aの渦との干渉により
、低レイノルズ数域の渦周波数を規制するものである。
That is, since the vortex generation frequency of the vortex generation element 2b on the downstream side is low, the vortex circulation is strong and dominates the high Reynolds number region, and the difference in vortex frequency generated at a low Reynolds number is the difference between the vortex generation elements 2a and 2.
The vortex frequency in the low Reynolds number region is regulated by interference with the vortex of the vortex generating element 2a generated in the gap between b.

上に述べた渦発生体から剥離する渦は渦発生体の軸に平
行した渦柱として流下するので圧力変動もこれに従った
傾向をもってあられれるので、導入差圧も大きく、且つ
平均化される。
The vortex that separates from the vortex generator described above flows down as a vortex column parallel to the axis of the vortex generator, so pressure fluctuations tend to follow this, so the introduced pressure difference is also large and averaged out. .

尚、平板2Cは渦発生素子2aで発生した渦を間隙t工
t t3間に導入し、成長させる増幅効果をもたらすた
めのものである。渦発生体は第1図(A)にしめした構
成以外にも三角柱と梯形、平板を組合わせて第2図(A
)、(B)、(C)の構成とし、これに前記条件を付加
することにより有効である。
The flat plate 2C is used to introduce the vortex generated by the vortex generating element 2a between the gaps tt and tt3, thereby producing an amplifying effect of growing the vortex. In addition to the configuration shown in Figure 1 (A), the vortex generator can be constructed by combining a triangular prism, a trapezoid, and a flat plate as shown in Figure 2 (A).
), (B), and (C), and it is effective by adding the above conditions to these configurations.

麦−一釆 以上に述べたように1本発明によると、渦発生周波数は
広範囲に且つて流量と比例する直線性の優れた。更には
、安定した渦信号が得られ、一方。
As described above, according to the present invention, the vortex generation frequency has a wide range and has excellent linearity that is proportional to the flow rate. Furthermore, a stable eddy signal is obtained, while.

渦検出においても更に強い変動差圧が得られるため1両
者を含めて、流量計測範囲の極めて広い渦流量計が得ら
れる。
Even in vortex detection, a stronger fluctuating differential pressure can be obtained, so that a vortex flow meter with an extremely wide flow rate measurement range can be obtained, including both methods.

【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を説明するための図で
、(A)図は側断面図、(B)図は(A)図のB−B線
断面図、(C)図は管状体の詳細図。 (D)図は不織布の詳細図、第2図は、渦発生体の他の
実施例を示す断面図、第3図は、従来の渦流量計の例を
示す図である。 1・・・流路、2・・・渦発生体、3・・・管状体、4
・・・超音波発振器、5・・・超音波受信器、32・・
・管体、33・・・圧力導入孔、34・・・不織布。 特許出願人  オーバル機器工業株式会社wJ  j 
 図 (B)2 (C)           (D) 第2 (A)(B) 第3 (C) 図 (B)
FIG. 1 is a diagram for explaining the vortex flowmeter according to the present invention, in which (A) is a side sectional view, (B) is a sectional view taken along the line B-B in (A), and (C) is a sectional view taken along the line B-B of (A). Detailed view of the tubular body. (D) is a detailed view of the nonwoven fabric, FIG. 2 is a sectional view showing another embodiment of the vortex generator, and FIG. 3 is a view showing an example of a conventional vortex flowmeter. 1... Channel, 2... Vortex generator, 3... Tubular body, 4
... Ultrasonic oscillator, 5... Ultrasonic receiver, 32...
- Pipe body, 33...Pressure introduction hole, 34...Nonwoven fabric. Patent applicant Oval Equipment Industry Co., Ltd. wJ j
Figure (B) 2 (C) (D) 2nd (A) (B) 3rd (C) Figure (B)

Claims (8)

【特許請求の範囲】[Claims] (1)、流路内に流れに対向して配設される渦発生体の
後方に該渦発生体と交叉するごとく上記流路壁を貫通し
て支持される管状体と直交して連通する一対の管体を固
設し、該管体には圧力導入孔が穿孔されており、該圧力
導入孔より導入される渦変動圧により上記管状体内に流
通する流体変位を検出することを特徴とする渦流量計。
(1) At the rear of the vortex generator disposed in the flow path facing the flow, it communicates orthogonally with a tubular body supported by passing through the flow path wall so as to intersect with the vortex generator. A pair of tubular bodies are fixedly installed, a pressure introduction hole is perforated in the tubular bodies, and the displacement of the fluid flowing inside the tubular body is detected by the vortex fluctuating pressure introduced from the pressure introduction hole. vortex flow meter.
(2)、上記渦発生体は、断面形状が流路軸上に頂点を
もつ二等辺三角形状およびT字形状の渦発生素子が所定
間隔を隔てて配設さ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) A patent characterized in that the above-mentioned vortex generating body is characterized in that vortex generating elements each having an isosceles triangular or T-shaped cross-sectional shape with an apex on the flow path axis are arranged at predetermined intervals. A vortex flowmeter according to claim (1).
(3)、上記渦発生体は、断面形状が流路軸上に頂点を
もつ二等辺三角形状、平板状およびT字形状の渦発生素
子が所定間隔を隔てて順次配設され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。
(3) The above-mentioned vortex generating body is characterized in that vortex generating elements each having an isosceles triangular cross-sectional shape, a flat plate shape, and a T-shaped cross-sectional shape with the apex on the flow path axis are sequentially arranged at predetermined intervals. A vortex flowmeter according to claim (1).
(4)、上記渦発生体は、断面形状が流路軸上に頂点を
もつ二等辺三角形状および梯形状の渦発生素子が所定間
隔を隔てて配設され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。
(4) The above-mentioned vortex generating body is characterized in that vortex generating elements each having an isosceles triangular or ladder-shaped cross-sectional shape with an apex on the flow path axis are arranged at predetermined intervals. A vortex flowmeter according to scope (1).
(5)、上記渦発生体は、断面形状が流路軸上に頂点を
もつ二等辺三角形状、平板状および梯形状の渦発生素子
が所定間隔を隔てて順次配設され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。
(5) The above-mentioned vortex generating body is characterized in that vortex generating elements each having a cross-sectional shape having an isosceles triangular shape, a flat plate shape, and a ladder shape with an apex on the flow path axis are sequentially arranged at a predetermined interval. A vortex flowmeter according to claim (1).
(6)、上記渦発生体は、上流側に配設される二等辺三
角形状渦発生素子と下流側に配設されるT字形状又は梯
形状の渦発生素子との渦周波数比を前者を基準として0
.7〜0.9としたことを特徴とする特許請求の範囲第
(2)項乃至第(5)項のいずれか1項に記載の渦流量
計。
(6) The vortex generating body has a vortex frequency ratio of an isosceles triangular vortex generating element disposed on the upstream side and a T-shaped or ladder-shaped vortex generating element disposed on the downstream side. 0 as a standard
.. 7 to 0.9. The vortex flowmeter according to any one of claims (2) to (5).
(7)、流体変位を管状体両端に配設された超音波発振
器および受信器間における変動流の超音波変調信号とし
て検出することを特徴とする特許請求の範囲第(1)項
乃至第(6)項のいずれか1項に記載の渦流量計。
(7) The fluid displacement is detected as an ultrasonic modulation signal of a fluctuating flow between an ultrasonic oscillator and a receiver disposed at both ends of the tubular body. 6) The vortex flow meter according to any one of paragraphs.
(8)、管状体と直交して連通する一対の管体内壁に不
織布等の吸音材を内装した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
渦流量計。
(8) Any one of claims (1) to (7), characterized in that a sound-absorbing material such as a nonwoven fabric is provided inside the inner walls of a pair of tubes that communicate orthogonally with the tubular body. Vortex flowmeter as described in section.
JP61058975A 1986-03-15 1986-03-17 Vortex flowmeter Granted JPS62214321A (en)

Priority Applications (8)

Application Number Priority Date Filing Date Title
JP61058975A JPS62214321A (en) 1986-03-17 1986-03-17 Vortex flowmeter
US07/024,294 US4838092A (en) 1986-03-15 1987-03-10 Vortex flow meter
CA000532031A CA1306120C (en) 1986-03-15 1987-03-13 Vortex flow meter
DE3750965T DE3750965T2 (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
JP61058975A JPS62214321A (en) 1986-03-17 1986-03-17 Vortex flowmeter

Publications (2)

Publication Number Publication Date
JPS62214321A true JPS62214321A (en) 1987-09-21
JPH0460535B2 JPH0460535B2 (en) 1992-09-28

Family

ID=13099848

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61058975A Granted JPS62214321A (en) 1986-03-15 1986-03-17 Vortex flowmeter

Country Status (1)

Country Link
JP (1) JPS62214321A (en)

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS58144712A (en) * 1981-12-10 1983-08-29 アイ・テイ・テイ・インダストリ−ズ・インコ−ポレ−テツド Eddy flowmeter
JPS6040914A (en) * 1983-08-15 1985-03-04 Oval Eng Co Ltd Vortex flowmeter

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS58144712A (en) * 1981-12-10 1983-08-29 アイ・テイ・テイ・インダストリ−ズ・インコ−ポレ−テツド Eddy flowmeter
JPS6040914A (en) * 1983-08-15 1985-03-04 Oval Eng Co Ltd Vortex flowmeter

Also Published As

Publication number Publication date
JPH0460535B2 (en) 1992-09-28

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