JPH0361892B2 - - Google Patents

Info

Publication number
JPH0361892B2
JPH0361892B2 JP8881483A JP8881483A JPH0361892B2 JP H0361892 B2 JPH0361892 B2 JP H0361892B2 JP 8881483 A JP8881483 A JP 8881483A JP 8881483 A JP8881483 A JP 8881483A JP H0361892 B2 JPH0361892 B2 JP H0361892B2
Authority
JP
Japan
Prior art keywords
ultrasonic
time
flow path
transmitter
level
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
Application number
JP8881483A
Other languages
Japanese (ja)
Other versions
JPS59214714A (en
Inventor
Masaki Takamoto
Akinori Yokota
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.)
National Institute of Advanced Industrial Science and Technology AIST
Original Assignee
Agency of Industrial Science and Technology
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 Agency of Industrial Science and Technology filed Critical Agency of Industrial Science and Technology
Priority to JP8881483A priority Critical patent/JPS59214714A/en
Publication of JPS59214714A publication Critical patent/JPS59214714A/en
Publication of JPH0361892B2 publication Critical patent/JPH0361892B2/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
    • G01F1/66Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow by measuring frequency, phase shift or propagation time of electromagnetic or other waves, e.g. using ultrasonic flowmeters
    • G01F1/667Arrangements of transducers for ultrasonic flowmeters; Circuits for operating ultrasonic flowmeters

Landscapes

  • Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Fluid Mechanics (AREA)
  • General Physics & Mathematics (AREA)
  • Measuring Volume Flow (AREA)

Description

【発明の詳細な説明】 本発明は、超音波流量計、特に、流路を形成す
る管路壁に対して一定の取付角度をもつて対向し
て配設された超音波送受波器を有し、該送受波器
間の超音波伝播時間から流速又は流量を求める超
音波流量計に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an ultrasonic flowmeter, particularly an ultrasonic transducer that is disposed facing a pipe wall forming a flow path at a fixed angle. The present invention relates to an ultrasonic flowmeter that determines the flow velocity or flow rate from the ultrasonic propagation time between the transducer and the transducer.

超音波を利用して流速、流量を測定する所謂超
音波流量計は周知であり、上下水道、水力発電所
等において実際に使用されている。
2. Description of the Related Art So-called ultrasonic flowmeters that measure flow velocity and flow rate using ultrasonic waves are well known and are actually used in water supply and sewage systems, hydroelectric power plants, and the like.

この超音波流量計の側定原理は、流れている流
体中における音波の伝播速度が流れの方向に伝わ
るときは流速だけ見掛け上速くなり、逆の方向に
はそれだけおそくなることを応用したもので、管
内流速をv、静止流体中の音速をcとし、距離L
だけへだたる2点に送受波器をおいた場合、上流
側A点から発射された超音波が下流側B点に達す
る時間t1がt1=L/(c+v)であり、下流側B
点から発射された超音波が上流側A点に達する時
間t2がt2=L(c−v)であり、c≫vであるこ
とから、 t2−t1=2Lv/c2 を求め、この時間差t2−t1を求めることにより流
速vを求めるものである。
The principle of lateral determination of this ultrasonic flowmeter is based on the fact that when the propagation speed of sound waves in a flowing fluid is propagated in the direction of the flow, the flow velocity becomes apparently faster, and in the opposite direction, it becomes slower. , the flow velocity in the pipe is v, the sound velocity in the stationary fluid is c, and the distance L
When a transducer is placed at two points that are separated by a
Since the time t 2 for the ultrasonic wave emitted from the point to reach the upstream point A is t 2 = L(c-v) and c≫v, calculate t 2 - t 1 = 2Lv/c 2 , the flow velocity v is determined by determining this time difference t 2 −t 1 .

而して、上記時間差t2−t1は非常に短いもので
あり、この時間差を正確に求めることは非常に困
難であつた。即ち従来の方式においては送受波器
は1対となつており、それぞれ固有振動数をもつ
た振動体でもある。従つて送波器に対して発振信
号が印加されたとしても定常状態に到るまでには
時間遅れを伴なう。
Therefore, the above-mentioned time difference t 2 −t 1 is very short, and it is very difficult to accurately determine this time difference. That is, in the conventional system, the transducers are a pair, each of which is a vibrating body with its own natural frequency. Therefore, even if an oscillation signal is applied to the transmitter, there is a time delay until the steady state is reached.

しかるに媒質内における超音波は距離に対して
指数関数的に減衰するので、送受信器間の距離が
大きくのる大口径の流量計においては受波器側の
音圧は極めて低くなる。加えて音圧−電圧の変換
効率を加味すると数10デシベル以上もの電圧値と
なり、従つて、上記送波器の信号を受波器で受波
した受信信号は極めて小さい。また、送波器の時
間遅れと同様に受波器にも時間遅れがあるため受
信信号はゆるやかに増大し、t1,t2を算出する信
号の検出レベルが不安定となる。
However, since ultrasonic waves in a medium attenuate exponentially with distance, in a large-diameter flowmeter where the distance between the transmitter and receiver is large, the sound pressure on the receiver side becomes extremely low. In addition, when the sound pressure-voltage conversion efficiency is taken into consideration, the voltage value becomes several tens of decibels or more, and therefore, the received signal obtained by receiving the signal from the transmitter by the receiver is extremely small. Furthermore, since there is a time delay in the receiver as well as a time delay in the transmitter, the received signal increases slowly, and the detection level of the signal used to calculate t 1 and t 2 becomes unstable.

本発明は、上述のごとき実情に鑑みてなされた
もので、特に、超音波流量計における超音波の伝
播時間を正確に求め得るようにし、もつて、測定
精度の向上を図つたものである。
The present invention has been made in view of the above-mentioned circumstances, and is particularly intended to accurately determine the propagation time of ultrasonic waves in an ultrasonic flowmeter, thereby improving measurement accuracy.

第1図及び第2図は、本発明の測定原理を説明
するための信号波系図で、第1図は超音波送波器
より発射される超音波の信号波形図、第2図は、
超音波受波器により受波される超音波の信号波形
図で、図示例の場合、超音波送受波器を2対有
し、送波器側において発射された第1図aに示す
超音波は受波器側において第2図aに示すような
波形の超音波として受波され、一方、送波器側に
おいて発射された第1図bに示す超音波は受波器
側において第2図bに示すような波形の超音波と
して受波される。而して、送波器側より発射され
る2つの超音波(第1図a及びb)は、立上り位
相及び振幅が同一で、かつ、周波数が異なつてい
る。なお、第1図cには、第1図a及びbに示し
た超音波を加算した場合の波形を示す。上述のよ
うにして送波器側により発射された超音波は被測
定流体中を伝播して受波器側に達するが、各受波
器の出力信号波形は該受波器の立上り時に時間遅
れ等によつてそれぞれ第2図a及びbのようにな
り、これら両信号を加え合わせると第2図cに示
すようになり、受信開始より所定時間経過後に特
異レベルPに達するが、この特異レベルPが現わ
れる時間は、常に、受信開始より一定時間後であ
る。従つて、送波器側において超音波を発射する
時刻から前記特異レベルが現われる時刻までの時
間を測れば、超音波が被測定流体中を伝播する時
間を測ることができ、前記特異レベルが顕著に現
われるので、被測定流体中における超音波伝播時
間を正確に求めることができる。
Figures 1 and 2 are signal wave diagrams for explaining the measurement principle of the present invention. Figure 1 is a signal waveform diagram of the ultrasound emitted from the ultrasound transmitter, and Figure 2 is
This is a signal waveform diagram of ultrasonic waves received by an ultrasonic receiver. In the illustrated example, there are two pairs of ultrasonic transducers, and the ultrasonic wave shown in FIG. 1a is emitted from the transmitter side. is received by the receiver as an ultrasonic wave with a waveform as shown in Fig. 2a, while the ultrasonic wave shown in Fig. 1b emitted from the transmitter side is received by the receiver as an ultrasonic wave with a waveform as shown in Fig. 2a. It is received as an ultrasonic wave with a waveform as shown in b. Thus, the two ultrasonic waves (FIG. 1 a and b) emitted from the transmitter side have the same rising phase and amplitude, but different frequencies. Note that FIG. 1c shows a waveform when the ultrasonic waves shown in FIGS. 1a and 1b are added. The ultrasonic waves emitted by the transmitter as described above propagate through the fluid to be measured and reach the receiver, but the output signal waveform of each receiver has a time delay at the rise of the receiver. etc., as shown in Figure 2 a and b, respectively, and when these two signals are added together, the result is as shown in Figure 2 c, which reaches a singular level P after a predetermined time has elapsed from the start of reception, but this singular level The time when P appears is always a certain period of time after the start of reception. Therefore, by measuring the time from the time when the ultrasonic wave is emitted on the transmitter side to the time when the singular level appears, it is possible to measure the time that the ultrasonic wave propagates in the fluid to be measured, and it is possible to measure the time during which the ultrasonic wave propagates through the fluid to be measured. Therefore, the ultrasonic propagation time in the fluid to be measured can be accurately determined.

第3図は、上述のごとき測定原理に基づいて構
成した本発明による超音波流量計の一実施例を示
す図で、図中、1はトリガ回路、2及び3は発振
器、4及び5は超音波送波器、6及び7は超音波
受波器、8及び9は増幅器、10は加算器、11
は波形整形回路、12はフリツプフロツプ回路、
13はクロツクパルス発生器、14はゲート回
路、15はカウンター、20は流路管で、該流路
管20の管壁には、図示のように、流路に対して
一定の取り付け角度をもつて2対の超音波送受波
器4,6及び5,7が対向して配設されており、
例えば、送波器4からは第1図aに示した超音波
信号が発射され、送波器5からは第1図bに示し
た超音波信号が発射され、送波器4よりの超音波
は受波器6により、また、送波器5よりの超音波
は受波器7によりそれぞれ受信されるようになつ
ている。而して、本発明においては、超音波送波
器4と受波器6との間の距離L1と超音波送波器
5と受波器7との間の距離L2は全く等しくなる
ようにこれら2対の超音波送受波器が配設され、
両超音波器4及び5からは、第1図a及びbに示
したような立上り位相及び振幅が等しく、かつ、
周波数の異なる超音波が発射されるが、これら両
超音波の立上り位相は、トリガ回路1によつて両
発振器2及び3を同時に起動することによつて同
一位相に保たれている。トリガ回路1は上述のよ
うにして発振器2及び3を同時起動するととも
に、SRフリツプフロツプ回路12をオンしてゲ
ート回路14を開き、クロツクパルス発生回路1
3からクロツクパルスをカウンター15にて計数
し始める。一方、前述のごとくして超音波送波器
4及び5より発射された超音波は、それぞれ超音
波受波器6及び7によつて受波され、加算器10
によつて加算され、第2図cに示したような信号
に変換される。この加算器10の出力信号中には
第2図cにPにて示したような特異レベル点が現
われるので、この特異レベル点Pを波形整形回路
11によつて検出してフリツプフロツプ回路12
をオフすれば、カウンター15は超音波送信から
前記特異レベル発生までの時間を計測したことに
なる。而して、受信から特異レベル発生までの時
間tは前述のように一定であるので、該カウンタ
ー15の計数値より被測定流体中における超音波
の伝播時間を求めることができる。なお、以上に
説明した実施例は、被測定流体の一方向の流れに
対してのみ測定するようにしたものであるが、本
発明は、上記実施例に限定されるものではなく、
例えば、上記実施例を更に改良してシングアラウ
ンド方式の超音波流量計を構成することも可能
で、その場合には、波形整形回路11の出力信号
によつて、超音波送受波器を切り換えるとともに
(すなわち、発振器2及び3の出力を受波器6及
び7に入力して該受波器6及び7を送波器とする
とともに、送波器4及び5を受波器とし、該受波
器4及び5の出力をそれぞれ増幅器8及び9に入
力する)、トリガ回路1を起動するようにすれば、
被測定流体の順方向及び逆方向の流れに対して交
互に測定することができる。
FIG. 3 is a diagram showing an embodiment of an ultrasonic flowmeter according to the present invention constructed based on the measurement principle as described above. In the figure, 1 is a trigger circuit, 2 and 3 are oscillators, and 4 and 5 are ultrasonic flowmeters. Sonic wave transmitter, 6 and 7 are ultrasonic wave receivers, 8 and 9 are amplifiers, 10 is an adder, 11
12 is a waveform shaping circuit, 12 is a flip-flop circuit,
13 is a clock pulse generator, 14 is a gate circuit, 15 is a counter, and 20 is a flow path tube.As shown in the figure, the flow path tube 20 has a wall having a fixed angle with respect to the flow path. Two pairs of ultrasonic transducers 4, 6 and 5, 7 are arranged facing each other,
For example, the ultrasonic signal shown in FIG. 1a is emitted from the transmitter 4, the ultrasonic signal shown in FIG. 1b is emitted from the transmitter 5, and the ultrasonic signal shown in FIG. The ultrasonic wave from the wave transmitter 5 is received by the wave receiver 6, and the ultrasonic wave from the wave transmitter 5 is received by the wave receiver 7. Therefore, in the present invention, the distance L 1 between the ultrasonic transmitter 4 and the receiver 6 and the distance L 2 between the ultrasonic transmitter 5 and the receiver 7 are completely equal. These two pairs of ultrasonic transducers are arranged as follows.
Both ultrasonicators 4 and 5 have the same rising phase and amplitude as shown in FIGS. 1a and 1b, and
Ultrasonic waves having different frequencies are emitted, but the rising phases of both ultrasonic waves are kept in the same phase by activating both oscillators 2 and 3 simultaneously by the trigger circuit 1. The trigger circuit 1 simultaneously activates the oscillators 2 and 3 as described above, turns on the SR flip-flop circuit 12, opens the gate circuit 14, and activates the clock pulse generation circuit 1.
3, the counter 15 starts counting clock pulses. On the other hand, the ultrasonic waves emitted from the ultrasonic transmitters 4 and 5 as described above are received by the ultrasonic receivers 6 and 7, respectively, and the adder 10
The signals are added by , and converted into a signal as shown in FIG. 2c. In the output signal of the adder 10, a singular level point as shown by P in FIG.
If it is turned off, the counter 15 will have measured the time from ultrasonic transmission to generation of the singular level. Since the time t from reception to generation of the singular level is constant as described above, the propagation time of the ultrasonic wave in the fluid to be measured can be determined from the count value of the counter 15. In addition, although the embodiment described above measures only the flow of the fluid to be measured in one direction, the present invention is not limited to the above embodiment.
For example, it is possible to further improve the above embodiment to configure a single-around type ultrasonic flowmeter. In that case, the output signal of the waveform shaping circuit 11 can be used to switch the ultrasonic transducer and (In other words, the outputs of the oscillators 2 and 3 are input to the receivers 6 and 7, and the receivers 6 and 7 are used as transmitters, and the transmitters 4 and 5 are used as receivers, and the receivers 6 and 7 are used as transmitters. The outputs of the amplifiers 4 and 5 are input to the amplifiers 8 and 9 respectively), and the trigger circuit 1 is activated.
Measurements can be taken alternately for forward and reverse flows of the fluid to be measured.

以上の説明から明らかなように、本発明による
と、簡単な構成で、しかも、測定精度の高い超音
波流量計を提供することができる。
As is clear from the above description, according to the present invention, it is possible to provide an ultrasonic flowmeter with a simple configuration and high measurement accuracy.

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

第1図及び第2図は、本発明の動作原理を説明
するための信号波形図で、第1図は、送波超音波
の波形図、第2図は、受波超音波の波形図、第3
図は、本発明の一実施例を示す構成図である。 1……トリガ回路、2,3……バースト発振
器、4,5……超音波送波(受波)器、6,7…
…超音波受波(送波)器、8,9……増幅器、1
0……加算器、11……波形整形回路、12……
SRフリツプフロツプ回路、13……クロツクパ
ルス発生回路、14……ゲート回路、15……カ
ウンター。
1 and 2 are signal waveform diagrams for explaining the operating principle of the present invention, FIG. 1 is a waveform diagram of transmitted ultrasound waves, FIG. 2 is a waveform diagram of received ultrasound waves, Third
The figure is a configuration diagram showing an embodiment of the present invention. 1... Trigger circuit, 2, 3... Burst oscillator, 4, 5... Ultrasonic wave transmitter (receiver) device, 6, 7...
...Ultrasonic wave receiver (transmitter), 8, 9...Amplifier, 1
0... Adder, 11... Waveform shaping circuit, 12...
SR flip-flop circuit, 13... clock pulse generation circuit, 14... gate circuit, 15... counter.

Claims (1)

【特許請求の範囲】 1 流路を形成する管路壁に流路に対して一定の
取付角度をもつて対向して配設された超音波送受
波器を有し、該送受波器間を伝播する超音波の伝
播時間から流量を測定する超音波流量計におい
て、前記超音波送受波器を複数対同一の超音波伝
播距離をもつて配設し、前記各送波器は同一立上
り位相、同一レベルでかつ周波数の異なる超音波
を発射し、前記受波器側において各受波器の検出
信号を加算し、その加算値が所定レベルに達した
時刻を検出し、前記立上り時間より前記所定レベ
ルに達するまでの時間により前記流路内を流れる
流体の流量を測定するようにしたことを特徴とす
る超音波流量計。 2 流路を形成する管路壁に流路に対し一定の取
付角度で対向して配設された超音波送受波器を有
し、該送受波器間で超音波のバースト信号を送信
し、この受信々号にもとづいて送信することによ
つて流れの順方向と逆方向における超音波の伝播
時間差から流量を求める超音波流量計において、
上記超音波送受波器を複数対配設し、これら送受
波器の超音波伝播距離および信号レベルを一定と
して、かつ、それぞれの送波器には同一位相で異
なる周波数の超音波信号を印加し、受波されたビ
ート信号により送信するようにしたことを特徴と
する超音波流量計。
[Claims] 1. An ultrasonic transducer is provided on a pipe wall that forms a flow path and is disposed facing the flow path at a fixed angle, and a In an ultrasonic flowmeter that measures a flow rate from the propagation time of a propagating ultrasonic wave, a plurality of the ultrasonic transducers are arranged with the same ultrasonic propagation distance, and each of the transmitters has the same rising phase, Ultrasonic waves of the same level and different frequencies are emitted, the detection signals of each receiver are added on the receiver side, the time when the added value reaches a predetermined level is detected, and the predetermined value is determined from the rise time. An ultrasonic flowmeter characterized in that the flow rate of the fluid flowing in the flow path is measured based on the time it takes to reach a level. 2. An ultrasonic transducer is disposed on a pipe wall forming a flow path facing the flow path at a fixed angle, and an ultrasonic burst signal is transmitted between the transducer and the ultrasonic wave transmitter. In an ultrasonic flowmeter that calculates the flow rate from the difference in propagation time of ultrasonic waves in the forward and reverse directions of the flow by transmitting based on these received signals,
A plurality of pairs of the above-mentioned ultrasonic transducers are arranged, the ultrasonic propagation distance and signal level of these transducers are kept constant, and ultrasonic signals of different frequencies with the same phase are applied to each transmitter. An ultrasonic flowmeter characterized in that the ultrasonic flowmeter transmits data using a received beat signal.
JP8881483A 1983-05-20 1983-05-20 Ultrasonic wave flowmeter Granted JPS59214714A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP8881483A JPS59214714A (en) 1983-05-20 1983-05-20 Ultrasonic wave flowmeter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP8881483A JPS59214714A (en) 1983-05-20 1983-05-20 Ultrasonic wave flowmeter

Publications (2)

Publication Number Publication Date
JPS59214714A JPS59214714A (en) 1984-12-04
JPH0361892B2 true JPH0361892B2 (en) 1991-09-24

Family

ID=13953367

Family Applications (1)

Application Number Title Priority Date Filing Date
JP8881483A Granted JPS59214714A (en) 1983-05-20 1983-05-20 Ultrasonic wave flowmeter

Country Status (1)

Country Link
JP (1) JPS59214714A (en)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4727314A (en) * 1982-12-23 1988-02-23 The United States Of America As Represented By The Secretary Of The Air Force Transient detector apparatus
JP6987554B2 (en) * 2017-07-18 2022-01-05 株式会社東京精密 Non-destructive inspection equipment and its method
DE102018132055B4 (en) 2018-12-13 2022-08-25 Endress + Hauser Flowtec Ag Ultrasonic transducer assembly of a clamp-on ultrasonic flowmeter, and a clamp-on ultrasonic flowmeter and methods for commissioning the clamp-on ultrasonic flowmeter

Also Published As

Publication number Publication date
JPS59214714A (en) 1984-12-04

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