JPH0421808B2 - - Google Patents

Info

Publication number
JPH0421808B2
JPH0421808B2 JP57084824A JP8482482A JPH0421808B2 JP H0421808 B2 JPH0421808 B2 JP H0421808B2 JP 57084824 A JP57084824 A JP 57084824A JP 8482482 A JP8482482 A JP 8482482A JP H0421808 B2 JPH0421808 B2 JP H0421808B2
Authority
JP
Japan
Prior art keywords
signal
doppler shift
shift frequency
reflected
proportional
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
JP57084824A
Other languages
Japanese (ja)
Other versions
JPS58202829A (en
Inventor
Koji Saito
Masao Fukunaga
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.)
Hitachi Ltd
Original Assignee
Hitachi 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 Hitachi Ltd filed Critical Hitachi Ltd
Priority to JP57084824A priority Critical patent/JPS58202829A/en
Publication of JPS58202829A publication Critical patent/JPS58202829A/en
Publication of JPH0421808B2 publication Critical patent/JPH0421808B2/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
    • G01F1/663Measuring 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 by measuring Doppler frequency shift

Landscapes

  • Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Fluid Mechanics (AREA)
  • General Physics & Mathematics (AREA)
  • Measuring Volume Flow (AREA)
  • Manipulation Of Pulses (AREA)
  • Measurement Of Velocity Or Position Using Acoustic Or Ultrasonic Waves (AREA)

Description

【発明の詳細な説明】 本発明は、ドツプラーシフト周波数を検出して
流体の流量を測定する超音波ドツプラー流量計に
関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an ultrasonic Doppler flowmeter that measures fluid flow rate by detecting Doppler shift frequency.

従来の超音波ドツプラー流量計においては、一
般に、信号処理手段内に比較器を設け、ドツプラ
ーシフト周波数と雑音信号とを弁別していた。そ
の際、比較器の基準値となるべき信号は、正負の
定電圧を分圧抵抗で分圧することにより、固定値
に設定されていた。
In conventional ultrasonic Doppler flowmeters, a comparator is generally provided within the signal processing means to discriminate between the Doppler shift frequency and the noise signal. At that time, the signal that should serve as the reference value of the comparator was set to a fixed value by dividing positive and negative constant voltages using voltage dividing resistors.

そのため受信信号が著しく変化し、それに伴い
上記比較器の入力信号が著しく変化した場合に
は、雑音波分を有効的に除去できなかつたり、計
数誤りを生じていた。
Therefore, if the received signal changes significantly and the input signal of the comparator changes accordingly, the noise wave component cannot be effectively removed or a counting error occurs.

つまり入力信号が基準値に比べて著しく大きく
なつた場合には、入力信号に重畳した雑音をも計
数してしまい正の誤差を、逆に著しく小さくなつ
た場合には、信号が基準値以下に隠れてしまい検
出されず負の誤差を、それぞれ生じていた。
In other words, if the input signal becomes significantly larger than the reference value, the noise superimposed on the input signal will also be counted, resulting in a positive error; if the input signal becomes significantly smaller, the signal will fall below the reference value. Each of them was hidden and undetected, resulting in a negative error.

また前述の原因の他に、送受信子の特性の劣
化、高低周波増幅器の利得の経時的変化によつて
も、このような計数誤りを生じていた。
In addition to the above-mentioned causes, such counting errors also occur due to deterioration of the characteristics of the transmitter/receiver and changes over time in the gain of the high/low frequency amplifier.

本発明は、上記従来装置の欠点を解消するため
になされたものであり、上記種々の原因による受
信信号の変動に対して安定で、高精度な超音波ド
ツプラー流量計を提供することを目的とする。
The present invention has been made to eliminate the drawbacks of the conventional devices described above, and an object thereof is to provide a highly accurate ultrasonic Doppler flowmeter that is stable against fluctuations in received signals due to the various causes described above. do.

この目的を達成するための本発明の特徴は、流
体からのドツプラーシフト周波数成分の反射信号
と後述の基準信号とを比較して、前記ドツプラー
シフト周波数に比例した信号を出力する比較手段
(以下「コンパレータ」という)を設けると共に、
前記基準信号を、前記コンパレータ出力の極性と
前記反射信号の信号の大きさとに応じて設定する
ことにより、前記ドツプラーシフト周波数検出用
のコンパレータに反射信号の大きさに応じたヒス
テリシス機能を持たせたところにある。
A feature of the present invention for achieving this object is a comparison means (1) that compares a reflected signal of a Doppler shift frequency component from a fluid with a reference signal (to be described later) and outputs a signal proportional to the Doppler shift frequency. In addition to providing a "comparator" (hereinafter referred to as a "comparator"),
By setting the reference signal according to the polarity of the comparator output and the signal magnitude of the reflected signal, the comparator for detecting the Doppler shift frequency is provided with a hysteresis function according to the magnitude of the reflected signal. It's somewhere.

以下、図面を用いて本発明の一実施例を説明す
る。第1図にその全体構成を示す。
An embodiment of the present invention will be described below with reference to the drawings. Figure 1 shows its overall configuration.

送信部102からの電気信号は、送信子104
で超音波に変換され、送信波として被測定流体に
向けて送信される。流体中の散乱体106により
反射された超音波は、送信波ともども受信子10
8で受信される高周波増幅器202、包絡線検波
器204を経てドツプラーシフト周波数を含んだ
信号だけが取り出される。この信号は、フイルタ
ー206によつて検波ノイズ等のノイズ成分を除
去された後、低周波増幅器208によつて増幅さ
れ、ゼロクスロコンパレータ302の入力信号と
なる。
The electrical signal from the transmitter 102 is sent to the transmitter 104
The ultrasonic wave is converted into an ultrasonic wave and sent as a transmission wave toward the fluid to be measured. The ultrasonic waves reflected by the scatterer 106 in the fluid reach the receiver 10 together with the transmitted waves.
Only the signal containing the Doppler shift frequency is extracted through a high frequency amplifier 202 and an envelope detector 204. After noise components such as detection noise are removed from this signal by a filter 206 , it is amplified by a low frequency amplifier 208 and becomes an input signal to a zerox cross comparator 302 .

この入力信号は、直接コンパレータ302に入
力される信号と、全波整流器304に入力される
信号とに分かれる。全波整流された信号は、さら
に平均値検出器306によりドツプラーシフト周
波数成分の反射信号の大きさに比例した信号に整
形され、ヒステリシス制御器308へ入力され
る。このヒステリシス制御器308は、コンパレ
ータ302の他方の入力端子(+)へ印加する基
準値を設定するものであり、前記コンパレータ3
02の出力極性であつて、前記平均値検出器30
6の大きさに応じてその基準値を設定することに
より、コンパレータ302にヒステリシス機能を
持たせている。
This input signal is divided into a signal directly input to the comparator 302 and a signal input to the full-wave rectifier 304. The full-wave rectified signal is further shaped by an average value detector 306 into a signal proportional to the magnitude of the reflected signal of the Doppler shift frequency component, and is input to a hysteresis controller 308 . This hysteresis controller 308 sets a reference value to be applied to the other input terminal (+) of the comparator 302.
02 output polarity, and the average value detector 30
By setting the reference value according to the magnitude of 6, the comparator 302 is provided with a hysteresis function.

上記コンパレータ302の出力がドツプラーシ
フト周波数に比例することから、このコンパレー
タ302の出力信号に応じて被測定流体の流量を
算出する。すなわち、上記コンパレータ302か
らのドツプラーシフト周波数は、周波数・電圧変
換器402によつて直流電圧に変換される。この
直流電圧が流速に比例していることから、断面積
補正部404で流速と断面積の積をとる演算を行
い、流量出力5を得る。
Since the output of the comparator 302 is proportional to the Doppler shift frequency, the flow rate of the fluid to be measured is calculated according to the output signal of the comparator 302. That is, the Doppler shift frequency from the comparator 302 is converted into a DC voltage by the frequency/voltage converter 402. Since this DC voltage is proportional to the flow velocity, the cross-sectional area correction unit 404 performs a calculation to calculate the product of the flow velocity and the cross-sectional area to obtain the flow rate output 5.

次に第1図各点aからfまでの波形を第2図a
〜fにそれぞれ示す。
Next, the waveforms from each point a to f in Figure 1 are shown in Figure 2 a.
- f respectively.

第2図aは高周波増幅器202で増幅されたド
ツプラーシフト周波数を含んだ受信信号波形で、
コンパレータ302に入力されるまでに検波され
て同図bのドツプラーシフト信号波形になる。同
図c,dはそれぞれ全波整流器304、平均値検
出器306の出力波形であり、ドツプラーシフト
信号の大きさに比例した信号に整形される。同図
eは、ヒステリシス制御器308の出力である基
準信号eを示す。この基準信号eは、同図fに示
すコンパレータ302の出力fと平均値検出器3
06の出力dに基づき、出力fの極性でもつて出
力dの大きさを持つ値に設定される。したがつ
て、コンパレータ302は、この基準値eと前記
ドツプラーシフト信号bとを比較し、ドツプラー
シフト信号bが前記基準信号eを越える期間、同
図fの出力を発生する。この出力fが前述のよう
にヒステリシス制御器308へ入力されてヒステ
リシスループを構成する一方、この出力fがドツ
プラーシフト周波数に比例した信号となる。
FIG. 2a shows the received signal waveform including the Doppler shift frequency amplified by the high frequency amplifier 202.
Before being input to the comparator 302, the signal is detected and becomes the Doppler shift signal waveform shown in FIG. The waveforms c and d in the figure are the output waveforms of the full-wave rectifier 304 and the average value detector 306, respectively, and are shaped into signals proportional to the magnitude of the Doppler shift signal. Figure e shows the reference signal e that is the output of the hysteresis controller 308. This reference signal e is combined with the output f of the comparator 302 shown in the figure f and the average value detector 3.
Based on the output d of 06, the polarity of the output f is set to a value having the magnitude of the output d. Therefore, the comparator 302 compares the reference value e with the Doppler shift signal b, and generates the output f in the figure during a period in which the Doppler shift signal b exceeds the reference signal e. This output f is input to the hysteresis controller 308 to form a hysteresis loop as described above, while this output f becomes a signal proportional to the Doppler shift frequency.

このようにドツプラーシフト信号が小さくなつ
た場合には、その基準信号eの大きさも小さくな
つてヒステリシスが小さくなるため、計数誤りを
生じることが無い。また、入力信号が大きくなつ
た場合には、ヒステリシスも大きくなり零付近に
重畳した雑音が有効に除去される。
When the Doppler shift signal becomes small in this way, the magnitude of the reference signal e also becomes small and the hysteresis becomes small, so that no counting error occurs. Furthermore, when the input signal becomes large, the hysteresis also becomes large, and noise superimposed near zero can be effectively removed.

以上のごとく本発明によれば、ヒステリシス付
きコンパレータのヒステリシスが、常に入力信号
の大きさに追従しているので、散乱体の濃度変
化、送受信子の特性の劣化、高低周波増幅器の利
得の経時的変化、及び導管壁と検出器の音響的結
合度の変動などの原因で、入力信号の強度が著し
く変化することがあつても、常に入力信号とヒス
テリシスの比率が等しいために高精度で安定なド
ツプラーシフト周波数の計数が行える効果があ
る。
As described above, according to the present invention, the hysteresis of the comparator with hysteresis always follows the magnitude of the input signal, so that changes in the concentration of scatterers, deterioration of the characteristics of the transmitter and receiver, and the change in the gain of the high and low frequency amplifier over time Even if the input signal strength changes significantly due to changes in the acoustic coupling between the conduit wall and the detector, the ratio of the input signal to the hysteresis is always the same, ensuring high accuracy and stability. This has the effect of being able to count Doppler shift frequencies.

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

第1図は本発明の一実施例の全体構成を示す
図、第2図は第1図の各点の信号波形を示す図で
ある。 102……送信部、104……送信子、106
……散乱体等、108……受信子、202……高
周波増幅器、204……包絡線検波器、206…
…フイルター、208……低周波増幅器、302
……ゼロクロスコンパレータ、304……全波整
流器、306……平均値検出器、308……ヒス
テリシス制御器、402……周波数/電圧変換
器、404……断面積補正部、5……流量出力。
FIG. 1 is a diagram showing the overall configuration of an embodiment of the present invention, and FIG. 2 is a diagram showing signal waveforms at each point in FIG. 1. 102... Transmitter, 104... Transmitter, 106
...Scatterer, etc., 108...Receiver, 202...High frequency amplifier, 204...Envelope detector, 206...
... Filter, 208 ... Low frequency amplifier, 302
. . . Zero cross comparator, 304 . . . Full wave rectifier, 306 .

Claims (1)

【特許請求の範囲】 1 流路を流れる被測定流体に一定周波数の超音
波を送信する送信手段と、 該流体によるドツプラーシフト周波数を含む反
射波及び前記送信手段からの送信波を受信する超
音波受信手段と、 前記受信手段出力を包絡線検波し前記ドツプラ
ーシフト周波数成分の反射信号を取り出す包絡線
検波手段と、 該手段からの反射信号と後述の基準信号とを比
較し、前記ドツプラーシフト周波数に比例した信
号を出力する比較手段と、 前記反射信号の信号の大きさに比例した信号を
出力する手段と、 前記比較手段が出力している極性であつて、前
記反射信号の大きさに比例した値を持つ信号を前
記基準信号として出力するヒステリシス制御手段
と、 前記比較手段からのドツプラーシフト周波数に
比例した信号に応じて前記被測定流体の流量を算
出する手段とを備えたことを特徴とする超音波ド
ツプラー流量計。
[Scope of Claims] 1. A transmitting means for transmitting ultrasonic waves of a constant frequency to a fluid to be measured flowing through a flow path, and an ultrasonic wave receiving means for receiving reflected waves including a Doppler shift frequency by the fluid and transmitted waves from the transmitting means. sound wave receiving means; envelope detection means for envelope-detecting the output of the receiving means and extracting a reflected signal of the Doppler shift frequency component; comparing the reflected signal from the means with a reference signal to be described later; a comparison means for outputting a signal proportional to the shift frequency; a means for outputting a signal proportional to the magnitude of the reflected signal; and a polarity outputted by the comparison means, the magnitude of the reflected signal hysteresis control means for outputting a signal having a value proportional to the reference signal as the reference signal; and means for calculating the flow rate of the fluid to be measured in accordance with the signal proportional to the Doppler shift frequency from the comparison means. Ultrasonic Doppler flowmeter featuring
JP57084824A 1982-05-21 1982-05-21 Ultrasonic wave doppler flowmeter Granted JPS58202829A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP57084824A JPS58202829A (en) 1982-05-21 1982-05-21 Ultrasonic wave doppler flowmeter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP57084824A JPS58202829A (en) 1982-05-21 1982-05-21 Ultrasonic wave doppler flowmeter

Publications (2)

Publication Number Publication Date
JPS58202829A JPS58202829A (en) 1983-11-26
JPH0421808B2 true JPH0421808B2 (en) 1992-04-14

Family

ID=13841496

Family Applications (1)

Application Number Title Priority Date Filing Date
JP57084824A Granted JPS58202829A (en) 1982-05-21 1982-05-21 Ultrasonic wave doppler flowmeter

Country Status (1)

Country Link
JP (1) JPS58202829A (en)

Also Published As

Publication number Publication date
JPS58202829A (en) 1983-11-26

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