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JP4172091B2 - Ultrasonic vortex flowmeter - Google Patents
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JP4172091B2 - Ultrasonic vortex flowmeter - Google Patents

Ultrasonic vortex flowmeter Download PDF

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JP4172091B2
JP4172091B2 JP14496299A JP14496299A JP4172091B2 JP 4172091 B2 JP4172091 B2 JP 4172091B2 JP 14496299 A JP14496299 A JP 14496299A JP 14496299 A JP14496299 A JP 14496299A JP 4172091 B2 JP4172091 B2 JP 4172091B2
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internal space
ultrasonic
hole
vortex
tube
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JP2000337936A (en
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博史 吉倉
耕一 田代
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トキコテクノ株式会社
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Description

【0001】
【発明の属する技術分野】
本発明は、流体の流量を計測する超音波渦流量計に関する。
【0002】
【従来の技術】
従来の超音波渦流量計を、図3に基づき説明する。
【0003】
従来の超音波渦流量計51においては、被測定流体であるガスが流れる管52内に、管52の中心を通って管52の直径方向と軸方向が平行となる略3角柱形状の渦発生体53が設けられ、この渦発生体53は、三角形の底辺に当たる側面が被測定流体の上流方向に向けられ、その内部に当該渦発生体53の両端部に開口した内部空間54が形成されている。
【0004】
また、渦発生体53の周壁部には該内部空間54と管2内とを連通する孔55,55が、渦発生体53の三角形の両辺に当たる側面に互いに渦発生体53の軸方向にずれて、一つずつ穿設されている。
【0005】
前記内部空間54の一側の開口部には超音波を内部空間54に向けて送信する送信器56a,56bが設けられ、前記内部空間54の他側の開口部には前記送信器56が送信した超音波を受信して超音波信号として出力する受信器57a,57bが設けられている。
【0006】
送信器56a,56bの入力端子は、送信器56a,56bへ所定の周波数の発振信号を出力することで該発振信号の周波数の超音波を送信させる発振回路58の出力端子に接続されており、また、受信器57a,57bの出力端子は超音波信号(受信した超音波信号を電気信号化したもの)を増幅する増幅回路59a,59bの入力端子に接続されている。
【0007】
また、発振回路58の出力端子は位相比較回路60a,60bの一の入力端子にも接続されており、位相比較回路60a,60bの他の入力端子は、前記増幅回路59a,59bに接続されている。
【0008】
位相比較回路60a,60bは、発振回路58の発振信号と増幅回路59a,59bからの増幅された超音波信号との位相を比較し、その位相差信号(超音波信号の発振信号に対する位相の遅進の変化を示す信号)を出力する。
【0009】
位相比較回路60a,60bの出力端子を、図示しない増幅・波形整形回路の入力端子に接続し、増幅・波形整形回路で、アナログ信号である位相差信号を増幅しパルス化し、さらに、図示しない演算回路で、パルス化された位相差信号の周波数から管52内の流量を演算し図示しない表示器や制御装置に出力するように接続する。この場合には、位相比較回路60a,60bからの出力それぞれに対応して2つの流量値が求められるため、平均をとるなどして出力する。
【0010】
または、図示しない位相差比較回路の入力端子に前記増幅回路59a,59bそれぞれの出力端子を接続し、該図示しない位相差比較回路の出力端子を図示しない増幅・波形整形回路の入力端子に接続し、増幅・波形整形回路で、アナログ信号である位相差信号を増幅しパルス化し、さらに、図示しない演算回路で、パルス化された位相差信号の周波数から管52内の流量を演算し図示しない表示器や制御装置に出力するように接続してもよい。この場合には、求められる流量値は1つである。
【0011】
上記流量計51において、前記管52内を被測定流体が流れると、前記渦発生体53により該渦発生体53の下流には渦発生体53断面の三角形の両辺に当たる側面に交番にカルマン渦が発生する。
【0012】
渦発生体53断面の三角形の両辺に当たる側面のうち一の側面側にカルマン渦が発生すると、一の側面には負圧が生じ、該一の側面の孔55から内部空間54内の被測定流体が流出するため、他の側面の孔55から被測定流体が流入し、内部空間54内に他の側面の孔55から一の側面の孔55へ被測定流体の流れが生じる。
【0013】
同様に渦発生体53の他の側面側にカルマン渦が発生すると、内部空間54内に一の側面の孔55から他の側面の孔55へ被測定流体の流れが生じる。
【0014】
このカルマン渦によって内部空間54内に生じる被測定流体の流れは、前記送信器56aから前記受信器57aへ送信される超音波及び前記送信器56bから前記受信器57bへ送信される超音波の伝播方向と略同方向または逆方向となるため、超音波の伝播方向と同方向の被測定流体の流れが生じているときには超音波の位相が進み、超音波の伝播方向と逆方向の被測定流体の流れが生じているときには超音波の位相が遅れる。
【0015】
この超音波の位相遅進の周波数はカルマン渦の発生周波数と同期しており、カルマン渦の発生周波数は、管52内の流速に比例するので、超音波の位相遅進の周波数を計測することで管52内の被測定流体の流量を演算することができる。
【0016】
【発明が解決しようとする課題】
上記従来の超音波渦流量計は、ノイズ等をキャンセルする目的で受信信号同士を比較するため、超音波送信器と超音波受信器とを2対設けている。
【0017】
このような構成において、各対の超音波の伝播方向が略同方向(逆向き)にあるため、それぞれの超音波が打ち消しあったり強めあったりするなど互いに干渉してしまい、良好な流量計測が阻害されるおそれがある。
【0018】
【課題を解決するための手段】
上記問題を解決するために、請求項1の発明は、被測定流体が流れる管と、該管に設けられて下流側にカルマン渦を発生させる渦発生体と、該渦発生体内に設けられた内部空間と、渦発生体の前記管内壁と対抗する一側面に穿設され、前記内部空間と前記管の内部とを連通させる第1の孔と、渦発生体の前記一側面に対抗する側面に穿設され、前記内部空間と前記管の内部とを連通させる第2の孔と、前記内部空間内に設けられ、基端が当該内部空間の一端に位置し、先端が当該内部空間の他端側に向けて前記第1の孔と第2の孔とを結ぶ線よりも突出することにより、当該内部空間の一端側を前記渦発生体の一側面側と他側面側との2つに仕切る仕切りと、前記内部空間のうちの他端側に設けられ、当該内部空間の一端に超音波を送信する送信器と、前記仕切りにより仕切られた一端側にそれぞれ設けられ、前記送信器から送信された超音波を受信する2つの受信器と、前記2つの受信器により受信される超音波から前記管に流れる被測定流体の流量を求める流量計測手段と、を備えたことを特徴とする。
【0019】
これにより、2つの受信手段で受信される超音波が、異なる伝播経路をとるため、互いに干渉することを防止できる。
【0020】
【発明の実施の形態】
本発明の実施の形態を図1を用いて説明する。
【0021】
図1の超音波渦流量計1Aは、被測定流体である被測定流体であるガスが流れる管2内に、管2の中心を通って管2の直径方向と軸方向が平行となる略3角柱形状の渦発生体3が設けられ、この渦発生体3は、三角形の底辺に当たる側面が被測定流体の上流方向に向けて設けられている。
【0022】
該渦発生体3内部には、当該渦発生体3の軸方向に沿って形成された内部空間4が設けられており、また、渦発生体3断面の三角形の両辺に当たる側面の管2中央付近には、内部空間4と管2内とを連通する孔5a,5bがそれぞれ穿設されている。
【0023】
該内部空間4内には、基端が当該内部空間4の一端側の開口部4aに位置し、先端が内部空間4の他端側の開口部4bに向けて前記孔5aと孔5bとを結ぶ線よりも突出する仕切り4cが設けられており、該仕切り4cによって、内部空間4の一端側は孔5a側の空間4dと孔5b側の空間4eとに仕切られている。
【0024】
前記内部空間4の他端側の開口部4bには超音波を前記仕切り4cによって仕切られた一端側の開口部4aa,4abそれぞれに向けて送信する送信器6が、前記内部空間4の開口部4aa,4abには前記送信器6が送信した超音波を受信して超音波信号として出力する受信器7a,7bが設けられている。
【0025】
送信器6の入力端子は、送信器6へ所定の周波数の発振信号を出力することで該発振信号の周波数の超音波を送信させる発振回路8の出力端子に接続されており、また、受信器7a,7bの出力端子は、超音波信号(受信した超音波信号を電気信号化したもの)を増幅する増幅回路9a,9bの入力端子に接続されている。
【0026】
該増幅回路9a,9bの出力端子は、位相比較回路10の各入力端子に接続されており、該位相比較回路10は、増幅回路9a,9bからの増幅された超音波信号の位相を比較し、その位相差信号(2つの超音波信号の位相の遅進の変化を示す信号)を出力する。
【0027】
位相比較回路10の出力端子は、増幅・波形整形回路11の入力端子に接続され、該増幅・波形整形回路10の出力端子は、演算回路12の入力端子に接続されている。増幅・波形整形回路10は、アナログ信号である位相差信号を増幅しパルス化して渦信号として出力する。演算回路12は、パルス化された位相差信号の周波数から管2内の流量を演算し流量信号を出力する。演算回路12の出力端子は、演算した流量を表示する表示回路13及び外部装置に流量信号を出力する出力回路14に接続されている。
【0028】
次に、上記のように構成した超音波渦流量計1Aの動作を説明する。
【0029】
前記管2内を被測定流体が流れると、前記渦発生体3により該渦発生体3の下流には渦発生体3断面の三角形の両辺に当たる側面から下流に交番にカルマン渦が発生する。
【0030】
渦発生体3断面の三角形の両辺に当たる側面のうち一の側面(図中X側面)側にカルマン渦が発生すると、X側面には負圧が生じ、該X側面の孔5aから内部空間4の空間4d内にある被測定流体が流出するため、他の側面(図中Y側面)の孔5bから内部空間4の空間4e内に被測定流体が流入し、内部空間4内に孔5bから仕切り4cの先端付近を経由して孔5aへ図中点線で示したように略V字状の被測定流体の流れが生じる。
【0031】
同様に渦発生体3のY側面側にカルマン渦が発生すると、内部空間4内に孔5aから仕切り4cの先端付近を経由して孔5bへ図中点線で示したように略V字状の被測定流体の流れが生じる。
【0032】
このとき、仕切り4cの先端が孔5aと孔5bとを結ぶ線よりも突出していない場合には被測定流体の流れが孔5aから孔5bへ直線的に生じてしまい、前記のように略V字状とはならなくなってしまうが、本実施の形態では、仕切り4cの先端は孔5aと孔5bとを結ぶ線よりも突出しているため、カルマン渦によって内部空間4内に生じる被測定流体の流れは略V字状となり、前記送信器6から前記受信器7a,7bへ送信される超音波の伝播経路(図中一点鎖線で示した部分)付近において伝播方向と略同方向または逆方向となる。
【0033】
このため、超音波の伝播方向と同方向の被測定流体の流れが生じているときには超音波の位相が進み、超音波の伝播方向と逆方向の被測定流体の流れが生じているときには超音波の位相が遅れる。例えば、孔5aから孔5bへ被測定流体の流れが生じるときには、受信器7aで受信される超音波の位相は遅れ、受信器7bで受信される超音波の位相は進む。また、同様に、孔5bから孔5aへ被測定流体の流れが生じるときには、受信器7aで受信される超音波の位相は進み、受信器7bで受信される超音波の位相は遅れる。
【0034】
このように、2つの受信器7a,7bで受信される超音波の位相が一方は進み、一方は遅れるように構成しているため、位相比較回路10でそれぞれの超音波の差分をとった場合には、位相の遅進のみが差として残り、超音波成分やノイズ成分はキャンセルされてしまう。そして、この超音波の位相遅進の周波数はカルマン渦の発生周波数と同期しており、カルマン渦の発生周波数は、管2内の流速に比例することに基づいて、管2内の被測定流体の流量を演算することができる。
【0035】
上記のように、本実施の形態の超音波渦流量計1Aにおいては、内部空間4を空間4dと空間4eとに仕切る仕切り4cを設けることで受信器7aが受信する超音波の受信経路と受信器7bが受信する超音波の伝播経路とが異なるようにしたため、受信器7aが受信する超音波と受信器7bが受信する超音波とが互いに干渉を起こして流量計測に影響を及ぼすことを防止できる。
【0036】
また、本実施の形態の超音波渦流量計1Aは、内部空間4を略V状とし被測定流体の流れを取り込む孔5a,5bを空間4d,4eに穿設して内部空間4内の被測定流体の流れを略V字状とすることで位相の遅れと進みを受ける超音波の伝播方向を略同方向とすることができるため、送信器6が1つで済み、部品数の低減が図れる。
【0037】
また、本実施の形態の超音波渦流量計1Aは、管2内で流速の最も高い管2の中心付近に孔5a,5bを穿設しているため、カルマン渦のエネルギーが大きく内部空間4内に生じる被測定流体の流れのエネルギーが大きくなり、S/N比を向上させることができる。
【0038】
なお、本実施の形態の超音波渦流量計1Aでは、内部空間4が一端側の開口部4aから他端側の開口部4bへ向けて断面積が逓減しそれに伴って仕切り4cの断面積も逓減するよう構成したが、図2に示す超音波渦流量計1Bのように内部空間4の断面積が一端側の開口部4aと他端側の開口部4bと変わらないようにしまた仕切り4cも断面積一定の板状となるよう構成しても同様の効果が図れる。
【0039】
なお、仕切り4cの先端を送信器6と平行な平面状とするとそこで送信器6から送信された超音波が反射して定在波が生じて流量計測に悪影響を及ぼすおそれがあるため、実施の形態の超音波流量計1Aのように先端を尖らせたり、変形例の超音波流量計1Bのように先端を丸めたりするほうが望ましい。
【0040】
【発明の効果】
上記のように、本発明の超音波渦流量計は、内部空間を2つに仕切る仕切りを設けることで一の受信器が受信する超音波の受信経路と他の受信器が受信する超音波の伝播経路とが異なるようにしたため、一の受信器が受信する超音波と他の受信器が受信する超音波とが互いに干渉を起こして流量計測に影響を及ぼすことを防止できる。
【0041】
また、本発明の超音波渦流量計は、第1の孔と第2の孔とを渦発生体と管との接合部付近に設けることなく内部空間内で被測定流体の流れによって超音波が変調を受ける距離を大きくすることができ、したがって、流量測定に誤差が生じさせることなくS/N比を向上させることができる。
【図面の簡単な説明】
【図1】 本発明の実施の形態の超音波渦流量計1Aを示す概略図である。
【図2】 本発明の実施の形態の変形例の超音波渦流量計1Bを示す概略図である。
【図3】 従来の超音波渦流量計を示す概略図である。
【符号の説明】
1A 実施の形態の超音波渦流量計
1B 実施の形態の変形例の超音波渦流量計
2 管
3 渦発生体
4 内部空間
4a 内部空間4の一端側の開口部
4b 内部空間4の他端側の開口部
4c 仕切り
4d 仕切り4cによって仕切られた一方の空間
4e 仕切り4cによって仕切られた他方の空間
5a 孔
5b 孔
6 送信器
7a 受信器
7b 受信器
8 発振回路
9a 増幅回路
9b 増幅回路
10 位相比較回路
11 増幅・波形整形回路
12 演算回路
13 表示回路
14 出力回路
51 従来の超音波渦流量計
52 管
53 渦発生体
54 内部空間
55 孔
56 送信器
57 受信器
58 発振回路
59 増幅回路
60 位相比較回路
61 増幅・波形整形回路
62 演算回路
[0001]
BACKGROUND OF THE INVENTION
The present invention relates to an ultrasonic vortex flowmeter that measures the flow rate of a fluid.
[0002]
[Prior art]
A conventional ultrasonic vortex flowmeter will be described with reference to FIG.
[0003]
In the conventional ultrasonic vortex flowmeter 51, a substantially triangular prism-shaped vortex is generated in a pipe 52 through which a gas as a fluid to be measured flows, and the diameter direction and the axial direction of the pipe 52 are parallel to each other through the center of the pipe 52. The vortex generator 53 has a side face corresponding to the base of the triangle directed in the upstream direction of the fluid to be measured, and an internal space 54 opened at both ends of the vortex generator 53 is formed therein. Yes.
[0004]
Further, holes 55, 55 communicating the inner space 54 and the inside of the pipe 2 are formed in the peripheral wall portion of the vortex generator 53 so as to be displaced from each other in the axial direction of the vortex generator 53 on the side surfaces corresponding to both sides of the triangle. One by one.
[0005]
Transmitters 56 a and 56 b that transmit ultrasonic waves toward the internal space 54 are provided in an opening on one side of the internal space 54, and the transmitter 56 transmits in an opening on the other side of the internal space 54. Receivers 57a and 57b that receive the ultrasonic waves and output them as ultrasonic signals are provided.
[0006]
The input terminals of the transmitters 56a and 56b are connected to the output terminal of an oscillation circuit 58 that transmits an ultrasonic signal having a frequency of the oscillation signal by outputting an oscillation signal having a predetermined frequency to the transmitters 56a and 56b. The output terminals of the receivers 57a and 57b are connected to input terminals of amplification circuits 59a and 59b that amplify the ultrasonic signals (the electric signals obtained from the received ultrasonic signals).
[0007]
The output terminal of the oscillation circuit 58 is also connected to one input terminal of the phase comparison circuits 60a and 60b, and the other input terminal of the phase comparison circuits 60a and 60b is connected to the amplification circuits 59a and 59b. Yes.
[0008]
The phase comparison circuits 60a and 60b compare the phases of the oscillation signal of the oscillation circuit 58 and the amplified ultrasonic signals from the amplification circuits 59a and 59b, and the phase difference signal (the phase delay of the ultrasonic signal relative to the oscillation signal). Output a signal indicating a change in decimal).
[0009]
The output terminals of the phase comparison circuits 60a and 60b are connected to the input terminals of an amplification / waveform shaping circuit (not shown), and the amplification / waveform shaping circuit amplifies and pulsates the phase difference signal, which is an analog signal, and further performs an operation (not shown) The circuit is connected so as to calculate the flow rate in the tube 52 from the frequency of the pulsed phase difference signal and output it to a display or control device (not shown). In this case, since two flow rate values are obtained corresponding to the outputs from the phase comparison circuits 60a and 60b, they are output by taking an average or the like.
[0010]
Alternatively, the output terminals of the amplifier circuits 59a and 59b are connected to the input terminal of a phase difference comparison circuit (not shown), and the output terminal of the phase difference comparison circuit (not shown) is connected to the input terminal of an amplification / waveform shaping circuit (not shown). The phase difference signal, which is an analog signal, is amplified and pulsed by the amplification / waveform shaping circuit, and the flow rate in the tube 52 is calculated from the frequency of the pulsed phase difference signal by the calculation circuit (not shown) and displayed (not shown). You may connect so that it may output to a device or a control device. In this case, the required flow rate value is one.
[0011]
In the flow meter 51, when a fluid to be measured flows in the pipe 52, Karman vortices are alternately formed on the side surfaces corresponding to both sides of the triangle of the vortex generator 53 in the downstream of the vortex generator 53 by the vortex generator 53. appear.
[0012]
When a Karman vortex is generated on one side of the side surfaces corresponding to both sides of the triangle of the cross section of the vortex generator 53, negative pressure is generated on one side, and the fluid to be measured in the internal space 54 from the hole 55 on the one side. Flows out from the hole 55 on the other side surface, and the fluid to be measured flows into the internal space 54 from the hole 55 on the other side surface to the hole 55 on the one side surface.
[0013]
Similarly, when a Karman vortex is generated on the other side surface of the vortex generator 53, a fluid to be measured flows from the hole 55 on one side surface to the hole 55 on the other side surface in the internal space 54.
[0014]
The flow of the fluid to be measured generated in the internal space 54 by the Karman vortex propagates the ultrasonic wave transmitted from the transmitter 56a to the receiver 57a and the ultrasonic wave transmitted from the transmitter 56b to the receiver 57b. The direction of the ultrasonic wave advances when the flow of the measured fluid in the same direction as the propagation direction of the ultrasonic wave is generated, and the measured fluid in the direction opposite to the propagation direction of the ultrasonic wave. When the flow of is occurring, the phase of the ultrasonic wave is delayed.
[0015]
The ultrasonic phase delay frequency is synchronized with the Karman vortex generation frequency. Since the Karman vortex generation frequency is proportional to the flow velocity in the tube 52, the ultrasonic phase delay frequency is measured. Thus, the flow rate of the fluid to be measured in the pipe 52 can be calculated.
[0016]
[Problems to be solved by the invention]
The conventional ultrasonic vortex flowmeter has two pairs of ultrasonic transmitters and ultrasonic receivers for comparing received signals for the purpose of canceling noise or the like.
[0017]
In such a configuration, since the propagation direction of each pair of ultrasonic waves is substantially the same direction (reverse direction), the respective ultrasonic waves may interfere with each other such as canceling or strengthening, and good flow measurement is possible. May be disturbed.
[0018]
[Means for Solving the Problems]
In order to solve the above problem, the invention of claim 1 is provided with a pipe through which a fluid to be measured flows, a vortex generator that is provided in the pipe and generates a Karman vortex downstream, and is provided in the vortex generator. A first hole that is perforated on an inner space and one side surface of the vortex generator facing the inner wall of the tube, communicates the inner space with the inside of the tube, and a side surface that opposes the one side surface of the vortex generator. A second hole that communicates between the internal space and the inside of the pipe, and is provided in the internal space. A proximal end is located at one end of the internal space, and a distal end is located in the other end of the internal space. By projecting from the line connecting the first hole and the second hole toward the end side, one end side of the internal space is divided into two sides, one side and the other side of the vortex generator. A partition and a partition provided on the other end side of the internal space, and transmit ultrasonic waves to one end of the internal space. A receiver, two receivers each provided on one end side partitioned by the partition, and receiving ultrasonic waves transmitted from the transmitter; and ultrasonic waves received by the two receivers from the two receivers to the tube. And a flow rate measuring means for obtaining a flow rate of the fluid to be measured.
[0019]
Thereby, since the ultrasonic waves received by the two receiving means take different propagation paths, they can be prevented from interfering with each other.
[0020]
DETAILED DESCRIPTION OF THE INVENTION
An embodiment of the present invention will be described with reference to FIG.
[0021]
The ultrasonic vortex flowmeter 1A shown in FIG. 1 passes through the center of the tube 2 in the tube 2 through which the gas to be measured, which is the fluid to be measured, flows, and the diameter direction of the tube 2 is substantially parallel to the axial direction. A prismatic vortex generator 3 is provided, and the vortex generator 3 has a side face corresponding to the base of the triangle facing the upstream direction of the fluid to be measured.
[0022]
Inside the vortex generator 3, an internal space 4 formed along the axial direction of the vortex generator 3 is provided, and in the vicinity of the center of the tube 2 on the side surface corresponding to both sides of the triangle of the vortex generator 3 cross section Are provided with holes 5a and 5b communicating with the internal space 4 and the inside of the pipe 2, respectively.
[0023]
In the internal space 4, the base end is located in the opening 4 a on one end side of the internal space 4, and the tip 5 a and the hole 5 b are directed toward the opening 4 b on the other end side of the internal space 4. A partition 4c protruding from the connecting line is provided, and the partition 4c partitions one end side of the internal space 4 into a space 4d on the hole 5a side and a space 4e on the hole 5b side.
[0024]
A transmitter 6 that transmits ultrasonic waves to the openings 4aa and 4ab on one end side partitioned by the partition 4c is provided in the opening 4b on the other end side of the internal space 4. 4aa and 4ab are provided with receivers 7a and 7b for receiving the ultrasonic waves transmitted from the transmitter 6 and outputting them as ultrasonic signals.
[0025]
An input terminal of the transmitter 6 is connected to an output terminal of an oscillation circuit 8 that transmits an ultrasonic wave having a frequency of the oscillation signal by outputting an oscillation signal having a predetermined frequency to the transmitter 6. The output terminals 7a and 7b are connected to input terminals of amplification circuits 9a and 9b that amplify the ultrasonic signals (the electric signals obtained from the received ultrasonic signals).
[0026]
The output terminals of the amplification circuits 9a and 9b are connected to the input terminals of the phase comparison circuit 10, and the phase comparison circuit 10 compares the phases of the amplified ultrasonic signals from the amplification circuits 9a and 9b. The phase difference signal (a signal indicating a change in the phase delay of the two ultrasonic signals) is output.
[0027]
The output terminal of the phase comparison circuit 10 is connected to the input terminal of the amplification / waveform shaping circuit 11, and the output terminal of the amplification / waveform shaping circuit 10 is connected to the input terminal of the arithmetic circuit 12. The amplification / waveform shaping circuit 10 amplifies the phase difference signal, which is an analog signal, turns it into a pulse, and outputs it as a vortex signal. The arithmetic circuit 12 calculates the flow rate in the tube 2 from the frequency of the pulsed phase difference signal and outputs a flow rate signal. The output terminal of the arithmetic circuit 12 is connected to a display circuit 13 that displays the calculated flow rate and an output circuit 14 that outputs a flow rate signal to an external device.
[0028]
Next, the operation of the ultrasonic vortex flowmeter 1A configured as described above will be described.
[0029]
When the fluid to be measured flows through the pipe 2, Karman vortices are generated by the vortex generator 3 alternately downstream from the side surfaces corresponding to both sides of the triangle of the vortex generator 3 in the downstream of the vortex generator 3.
[0030]
When a Karman vortex is generated on one side (X side in the figure) of the side surfaces corresponding to both sides of the triangle of the cross section of the vortex generator 3, negative pressure is generated on the X side and Since the fluid to be measured in the space 4d flows out, the fluid to be measured flows into the space 4e of the internal space 4 from the hole 5b on the other side surface (Y side surface in the figure), and is partitioned from the hole 5b into the internal space 4. As shown by the dotted line in the figure, a substantially V-shaped fluid to be measured flows to the hole 5a via the vicinity of the tip of 4c.
[0031]
Similarly, when a Karman vortex is generated on the Y side surface of the vortex generator 3, a substantially V-shape is formed in the internal space 4 from the hole 5a through the vicinity of the tip of the partition 4c to the hole 5b as shown by a dotted line in the figure. A flow of the fluid to be measured is generated.
[0032]
At this time, if the tip of the partition 4c does not protrude beyond the line connecting the hole 5a and the hole 5b, the flow of the fluid to be measured is generated linearly from the hole 5a to the hole 5b. In this embodiment, the tip of the partition 4c protrudes beyond the line connecting the hole 5a and the hole 5b, so that the fluid to be measured generated in the internal space 4 by the Karman vortex is not used. The flow is substantially V-shaped, and in the vicinity of the propagation path of ultrasonic waves transmitted from the transmitter 6 to the receivers 7a and 7b (the portion indicated by the one-dot chain line in the figure), the direction is substantially the same as or opposite to the propagation direction. Become.
[0033]
Therefore, the phase of the ultrasonic wave advances when the flow of the fluid under measurement in the same direction as the propagation direction of the ultrasonic wave is generated, and the ultrasonic wave occurs when the flow of the fluid under measurement in the direction opposite to the propagation direction of the ultrasonic wave occurs. The phase of is delayed. For example, when the fluid to be measured flows from the hole 5a to the hole 5b, the phase of the ultrasonic wave received by the receiver 7a is delayed, and the phase of the ultrasonic wave received by the receiver 7b is advanced. Similarly, when a fluid to be measured flows from the hole 5b to the hole 5a, the phase of the ultrasonic wave received by the receiver 7a is advanced, and the phase of the ultrasonic wave received by the receiver 7b is delayed.
[0034]
As described above, since the phases of the ultrasonic waves received by the two receivers 7a and 7b are configured so that one of them is advanced and the other is delayed, the difference between the respective ultrasonic waves is obtained by the phase comparison circuit 10. Therefore, only the phase delay remains as a difference, and the ultrasonic component and the noise component are canceled. The phase delay frequency of this ultrasonic wave is synchronized with the Karman vortex generation frequency, and based on the fact that the Karman vortex generation frequency is proportional to the flow velocity in the tube 2, the fluid to be measured in the tube 2. Can be calculated.
[0035]
As described above, in the ultrasonic vortex flowmeter 1A of the present embodiment, the reception path and reception of the ultrasonic wave received by the receiver 7a by providing the partition 4c that partitions the internal space 4 into the space 4d and the space 4e. Since the propagation path of the ultrasonic wave received by the receiver 7b is different, the ultrasonic wave received by the receiver 7a and the ultrasonic wave received by the receiver 7b are prevented from interfering with each other and affecting flow measurement. it can.
[0036]
Further, the ultrasonic vortex flowmeter 1A of the present embodiment has an internal space 4 that is substantially V-shaped, and holes 5a and 5b that take in the flow of the fluid to be measured are formed in the spaces 4d and 4e. By making the flow of the measurement fluid substantially V-shaped, the propagation direction of the ultrasonic wave receiving the phase lag and advance can be made substantially the same direction, so only one transmitter 6 is required, and the number of parts can be reduced. I can plan.
[0037]
Further, since the ultrasonic vortex flowmeter 1A of the present embodiment has holes 5a and 5b in the vicinity of the center of the pipe 2 having the highest flow velocity in the pipe 2, the energy of the Karman vortex is large and the internal space 4 The energy of the flow of the fluid to be measured generated inside increases, and the S / N ratio can be improved.
[0038]
In the ultrasonic vortex flowmeter 1A of the present embodiment, the cross-sectional area of the internal space 4 gradually decreases from the opening 4a on one end side to the opening 4b on the other end side, and accordingly, the cross-sectional area of the partition 4c is also reduced. Although configured so as to decrease, the cross-sectional area of the internal space 4 does not change between the opening 4a on one end side and the opening 4b on the other end side as in the ultrasonic vortex flowmeter 1B shown in FIG. The same effect can be achieved even if the plate is configured to have a constant cross-sectional area.
[0039]
Note that if the tip of the partition 4c has a planar shape parallel to the transmitter 6, the ultrasonic wave transmitted from the transmitter 6 may be reflected to generate a standing wave, which may adversely affect flow measurement. It is preferable to sharpen the tip as in the ultrasonic flow meter 1A of the form, or to round the tip as in the ultrasonic flow meter 1B in the modification.
[0040]
【The invention's effect】
As described above, the ultrasonic vortex flowmeter of the present invention is provided with a partition that divides the internal space into two, so that the ultrasonic reception path that one receiver receives and the ultrasonic wave that the other receiver receives. Since the propagation paths are different from each other, it is possible to prevent the ultrasonic wave received by one receiver and the ultrasonic wave received by another receiver from interfering with each other and affecting flow measurement.
[0041]
Further, the ultrasonic vortex flowmeter of the present invention does not provide the first hole and the second hole near the junction between the vortex generator and the tube, and the ultrasonic wave is generated by the flow of the fluid to be measured in the internal space. The distance subjected to the modulation can be increased, and therefore the S / N ratio can be improved without causing an error in the flow rate measurement.
[Brief description of the drawings]
FIG. 1 is a schematic diagram showing an ultrasonic vortex flowmeter 1A according to an embodiment of the present invention.
FIG. 2 is a schematic view showing an ultrasonic vortex flowmeter 1B according to a modification of the embodiment of the present invention.
FIG. 3 is a schematic view showing a conventional ultrasonic vortex flowmeter.
[Explanation of symbols]
1A Ultrasonic Vortex Flowmeter 1B Embodiment Ultrasonic Vortex Flowmeter 2 Modification Example Embodiment Tube 3 Vortex Generator 4 Internal Space 4a Opening 4b on One End Side of Internal Space 4 Other End Side of Internal Space 4 Opening 4c partition 4d one space 4e partitioned by partition 4c other space 5a partitioned by partition 4c hole 5b hole 6 transmitter 7a receiver 7b receiver 8 oscillator circuit 9a amplifier circuit 9b amplifier circuit 10 phase comparison Circuit 11 Amplification / waveform shaping circuit 12 Arithmetic circuit 13 Display circuit 14 Output circuit 51 Conventional ultrasonic vortex flowmeter 52 Tube 53 Vortex generator 54 Internal space 55 Hole 56 Transmitter 57 Receiver 58 Oscillation circuit 59 Amplification circuit 60 Phase comparison Circuit 61 Amplification / waveform shaping circuit 62 Arithmetic circuit

Claims (1)

被測定流体が流れる管と、
該管に設けられて下流側にカルマン渦を発生させる渦発生体と、
該渦発生体内に設けられた内部空間と、
渦発生体の前記管内壁と対抗する一側面に穿設され、前記内部空間と前記管の内部とを連通させる第1の孔と、
渦発生体の前記一側面に対抗する側面に穿設され、前記内部空間と前記管の内部とを連通させる第2の孔と、
前記内部空間内に設けられ、基端が当該内部空間の一端に位置し、先端が当該内部空間の他端側に向けて前記第1の孔と第2の孔とを結ぶ線よりも突出することにより、当該内部空間の一端側を前記渦発生体の一側面側と他側面側との2つに仕切る仕切りと、
前記内部空間のうちの他端側に設けられ、当該内部空間の一端に超音波を送信する送信器と、
前記仕切りにより仕切られた一端側にそれぞれ設けられ、前記送信器から送信された超音波を受信する2つの受信器と、
前記2つの受信器により受信される超音波から前記管に流れる被測定流体の流量を求める流量計測手段と、
を備えたことを特徴とする超音波渦流量計。
A tube through which the fluid to be measured flows;
A vortex generator that is provided in the tube and generates a Karman vortex downstream;
An internal space provided in the vortex generator;
A first hole that is formed in one side of the vortex generator facing the inner wall of the tube and that communicates the internal space with the inside of the tube;
A second hole that is drilled in a side surface that opposes the one side surface of the vortex generator and communicates the internal space with the inside of the tube;
Provided in the internal space, the base end is located at one end of the internal space, and the tip protrudes from the line connecting the first hole and the second hole toward the other end of the internal space. A partition for partitioning one end side of the internal space into two of one side and the other side of the vortex generator;
A transmitter that is provided on the other end side of the internal space and transmits ultrasonic waves to one end of the internal space;
Two receivers each provided on one end side partitioned by the partition and receiving ultrasonic waves transmitted from the transmitter;
Flow rate measuring means for obtaining a flow rate of the fluid to be measured flowing from the ultrasonic waves received by the two receivers to the tube;
An ultrasonic vortex flowmeter characterized by comprising:
JP14496299A 1999-05-25 1999-05-25 Ultrasonic vortex flowmeter Expired - Fee Related JP4172091B2 (en)

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AU2011202538B2 (en) * 2004-11-12 2012-06-07 Garrett Thermal Systems Limited Method and apparatus for determining flow
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