JPS6148843B2 - - Google Patents

Info

Publication number
JPS6148843B2
JPS6148843B2 JP12106280A JP12106280A JPS6148843B2 JP S6148843 B2 JPS6148843 B2 JP S6148843B2 JP 12106280 A JP12106280 A JP 12106280A JP 12106280 A JP12106280 A JP 12106280A JP S6148843 B2 JPS6148843 B2 JP S6148843B2
Authority
JP
Japan
Prior art keywords
circuit
counting
signal
output
reception
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
JP12106280A
Other languages
Japanese (ja)
Other versions
JPS5745413A (en
Inventor
Masao Fukunaga
Hitoshi Kanazawa
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 JP12106280A priority Critical patent/JPS5745413A/en
Publication of JPS5745413A publication Critical patent/JPS5745413A/en
Publication of JPS6148843B2 publication Critical patent/JPS6148843B2/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PLL方式を用いた超音波式流量計に関
し、正常な音波が受信できない状態(以下受波異
常と呼ぶ)が長時間続いてから、正常な音波の受
信状態に復帰した時に再び安定な測定を開始する
ための自動再スタート回路に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an ultrasonic flow meter using a PLL method, and after a state in which normal sound waves cannot be received (hereinafter referred to as reception abnormality) continues for a long time, a state in which normal sound waves are received is restored. This invention relates to an automatic restart circuit for restarting stable measurements when the system returns to normal.

第1図にPLL方式を用いた超音波式流量計の動
作原理図を示す。
Figure 1 shows the operating principle of an ultrasonic flowmeter using the PLL method.

送信回路12で出力された送信信号は一方の送
受信子2により超音波信号に変換され、配管1中
の流体を経て他方の送受信子2に到達し、受信信
号としてスイツチSW2を経た後受信回路3に入
る。
The transmission signal output from the transmission circuit 12 is converted into an ultrasonic signal by one of the transceivers 2, passes through the fluid in the pipe 1, reaches the other transceiver 2, and is sent as a reception signal to the reception circuit 3 after passing through the switch SW2. to go into.

受信回路3では受信信号を増幅し、受信信号が
到達してあらかじめ設定した信号検出レベルに達
すると、ΔT/V変換回路5に検出信号を出力す
る。一方計数回路4は送信回路12からの送信信
号と同期して電圧制御発振器(以下VCOと略
す)8からのパルス信号を計数し、計数回路4が
計数を終了すると計数終了信号を、ΔT/V変換
回路5の他方の入力に出力する。ΔT/V変換回
路5では、両者の時間差に比例した電圧信号を演
算し、SW3を経て積分器6で積分した後VCO8
で電圧に比例した周波数のパルス信号を発生して
前記計数回路4、送信回路12にパルス信号を送
る。
The receiving circuit 3 amplifies the received signal and outputs a detection signal to the ΔT/V conversion circuit 5 when the received signal reaches a preset signal detection level. On the other hand, the counting circuit 4 counts the pulse signals from the voltage controlled oscillator (hereinafter abbreviated as VCO) 8 in synchronization with the transmission signal from the transmitting circuit 12, and when the counting circuit 4 finishes counting, it outputs a counting end signal as ΔT/V It is output to the other input of the conversion circuit 5. The ΔT/V conversion circuit 5 calculates a voltage signal proportional to the time difference between the two, passes through SW3, integrates it with an integrator 6, and then outputs it to VCO8.
A pulse signal having a frequency proportional to the voltage is generated and sent to the counting circuit 4 and the transmitting circuit 12.

今仮に受信回路3からの検出信号のタイミング
が計数回路4からの計数終了信号よりも時間的に
遅い場合を考えると、ΔT/V変換回路5および
積分回路6はVCO8の出力パルス周波数を低く
するように動作するとすれば、VCOの出力パル
ス周波数が低下する結果、計数回路4の計数速度
が遅くなり、計数終了信号の出るタイミングは遅
くなる。このような動作をくりかえすと、遂には
ΔT/V変換回路の2つの入力信号の入るタイミ
ングが一致した時点で系は平衡する。以上はSW
1〜SW4の各スイツチが図示の位置にある場合
(下流側→上流側送信)について述べたが、逆の
場合も同様である。この場合の周波数差変換回路
の出力(Δ)は次式で与えられる。
Now suppose that the timing of the detection signal from the receiving circuit 3 is later than the counting end signal from the counting circuit 4, the ΔT/V conversion circuit 5 and the integrating circuit 6 lower the output pulse frequency of the VCO 8. Assuming that the VCO operates as shown in FIG. By repeating such operations, the system is finally balanced when the input timings of the two input signals of the ΔT/V conversion circuit coincide. The above is SW
Although the case where each switch of SW1 to SW4 is in the illustrated position (downstream side → upstream side transmission) has been described, the same applies to the reverse case. The output (Δ) of the frequency difference conversion circuit in this case is given by the following equation.

Δ=Nsin2θ/D(1+τCcosθ/D)-2
・v……(1) N:Δの増幅率(計数回路の計数値に相当) θ:超音波の水中入射角 D:管の内径 τ:超音波の水中伝播時間以外の伝播時間 C:水中音速 v:流速 (1)式でわかる通り、Δは流速vに比例する。
Δ=Nsin2θ/D(1+τCcosθ/D) -2
・v……(1) N: Amplification factor of Δ (equivalent to the count value of the counting circuit) θ: Incidence angle of ultrasonic wave in water D: Inner diameter of pipe τ: Propagation time other than underwater propagation time of ultrasonic wave C: Underwater Sound velocity v: Flow velocity As can be seen from equation (1), Δ is proportional to the flow velocity v.

従つてΔに比例した信号を取り出せば、流速
vが得られる。これがPLL方式を用いた超音波式
流量計の動作原理である。
Therefore, by extracting a signal proportional to Δ, the flow velocity v can be obtained. This is the operating principle of an ultrasonic flowmeter using the PLL method.

さて、このような超音波式流量計で、音波の送
受信が途切れた場合について考える。例えば気泡
が混入した場合、固形物が混入した場合、水がな
くなつて検出器が空気中にさらされた場合などが
これに該当する。
Now, let's consider a case where the transmission and reception of sound waves is interrupted in such an ultrasonic flowmeter. For example, this may occur if air bubbles get mixed in, if solid objects get mixed in, or if the detector is exposed to the air due to lack of water.

このような場合には受信回路3では受信信号が
到達しないので、検出信号をΔT/V変換回路に
出力することができない。そこで受波異常の信号
を出力して積分回路6の出力をホールドし、
VCO8に発振周波数を一定に保つ。そして流体
の条件が正常になり受信信号が到達するようにな
ると、積分回路6のホールドを解き、再びVCO
8の制御を行う。このようにすれば測定条件が乱
れても出力が不安定になることはない。
In such a case, the reception signal does not reach the reception circuit 3, and therefore the detection signal cannot be output to the ΔT/V conversion circuit. Therefore, a reception abnormality signal is output and the output of the integrating circuit 6 is held.
Keep the oscillation frequency constant in VCO8. Then, when the fluid conditions become normal and the reception signal starts to arrive, the hold of the integrating circuit 6 is released and the VCO is turned on again.
8 control. In this way, even if the measurement conditions are disturbed, the output will not become unstable.

第2図は上記のホールド機能を持つ積分回路の
具体的な一例である。
FIG. 2 shows a specific example of an integrating circuit having the above-mentioned hold function.

ΔT/V変換信号13は抵抗器R1とコンデン
サ16で決まる時定数で積分を行い、基準電源1
7のバイアスを加えてVCO8の入力電圧とな
る。
The ΔT/V conversion signal 13 is integrated with a time constant determined by the resistor R1 and the capacitor 16, and then the reference power supply 1
By adding a bias of 7, it becomes the input voltage of VCO8.

電子スイツチ14は通常はONになつている
が、受波異常信号19が入つた時にはOFFとな
り、積分動作を停止して出力をホールドする。基
準電源17はVCO8の入力に直流バイアスを加
えるためのもので、起動時に積分回路の出力電圧
はゼロとなるが、その場合でもVCOの出力18
が出てPLLループが起動するように動作点を設定
する。
The electronic switch 14 is normally turned on, but when the reception abnormality signal 19 is received, it is turned off, stopping the integral operation and holding the output. The reference power supply 17 is for applying DC bias to the input of the VCO 8, and the output voltage of the integrating circuit becomes zero at startup, but even in that case, the output voltage of the VCO 18
Set the operating point so that the output occurs and the PLL loop starts.

しかし、このような従来回路には次の欠点があ
る。超音波式流量計では測定条件によつて音波の
送受信が妨げられることがあることは既に述べた
が、その状態が数時間以上、場合によつては数日
間以上もの長い間続くことがある。例えば高台に
ある水源池に下から水をポンプで送水する場合の
流量測定がこれに該当する。この場合ポンプは間
欠運転になることが多く、ぱその休止時は数時間
以上になることもある。その場合は一度ぱ静止す
るが、自重によつて徐々に下がり、ついには検出
器取付部の超音波伝播路の水もなくなる結果、正
常な音波の送受信ができない。このように長期間
音波の送受信が妨げられると第2図の積分回路は
その間ホールド状態を続けることになるが、コン
デンサ16のリークと演算増幅器15の入力バイ
アス電流によるドリフトが避けられず、演算増幅
器15の出力が変化する結果、VCOの動作点が
ずれて正常になつても再起動できない。なぜなら
ば、超音波式流量計ではノイズによる誤動作を防
止するために受信ゲートを設定し、その間の信号
しか受信信号と見なさないという信号処理を行う
のが一般的であり、PLL方式ではVCOの出力か
らこのような受信ゲートをつくり出す。従つて
PLLループが起動するためにはVCOの出力にあ
る許容範囲があるが、ドリフトの結果その範囲を
外れるからである。従来、このような場合には電
源を一度切断し、再投入する操作が必要であつ
た。
However, such conventional circuits have the following drawbacks. It has already been mentioned that in ultrasonic flowmeters, the transmission and reception of sound waves may be hindered depending on the measurement conditions, but this condition may continue for a long time, for several hours or more, and in some cases for several days or more. For example, this applies to measuring the flow rate when water is pumped from below to a water source pond located on a hill. In this case, the pump often operates intermittently, and the pump may be inactive for several hours or more. In that case, it will stop once, but it will gradually lower due to its own weight, and eventually there will be no water in the ultrasonic propagation path at the detector mounting part, and normal transmission and reception of sound waves will not be possible. If the transmission and reception of sound waves is prevented for a long period of time in this way, the integrating circuit shown in FIG. As a result of the change in the output of 15, the operating point of the VCO shifts and even if it becomes normal, it cannot be restarted. This is because in order to prevent malfunctions due to noise, ultrasonic flowmeters generally set a reception gate and perform signal processing in which only signals between those gates are considered as received signals.In the PLL method, the VCO output Create a reception gate like this from Accordingly
This is because there is a certain tolerance range for the VCO output in order for the PLL loop to start, but as a result of drift, it falls outside of that range. Conventionally, in such a case, it was necessary to turn off the power and then turn it on again.

本発明は上述のように超音波の送受信が長期間
妨げられた場合でも、従来のように人手によつて
電源を再投入することなく正常に復帰すると同時
に自動的に測定を再開する再スタート機能を提供
することにある。
As mentioned above, the present invention has a restart function that automatically restarts measurement as soon as the system returns to normal even if the transmission and reception of ultrasound is interrupted for a long period of time, without having to manually turn the power back on as in the past. Our goal is to provide the following.

第3図にその例を示す。計数回路20は通常の
動作時は常にリセツトされており受波異常になつ
た時にのみパルス信号入力21を計数して、計数
を終了すると電子スイツチ22を“ON”にす
る。
An example is shown in FIG. The counting circuit 20 is always reset during normal operation, and counts the pulse signal input 21 only when reception becomes abnormal, and when counting is completed, the electronic switch 22 is turned "ON".

これによつてコンデンサ16は短絡されて放電
し、電源投入時と同じ状態にリセツトされる。
As a result, the capacitor 16 is short-circuited and discharged, and is reset to the same state as when the power was turned on.

計数回路20の計数時間を、その間の積分回路
のドリフト量が無視できる値に選べば、受波異常
が長期間続いても積分回路は計数時間で決まる一
定周期毎にリセツトされて、そのドリフトが補正
される。そして測定状態が正常に復帰すると同時
に計数回路20はリセツト状態となり、電子スイ
ツチ22は“OFF”となつて積分回路は通常の
積分動作を行う。即ち流量計としての動作を再開
する。
If the counting time of the counting circuit 20 is selected to a value during which the amount of drift in the integrating circuit can be ignored, even if the reception abnormality continues for a long period of time, the integrating circuit will be reset at regular intervals determined by the counting time, and the drift will be eliminated. Corrected. Then, at the same time as the measurement state returns to normal, the counting circuit 20 enters the reset state, the electronic switch 22 is turned off, and the integrating circuit performs the normal integrating operation. In other words, it resumes operation as a flowmeter.

これらの動作のタイムチヤートを第4図に示
す。
A time chart of these operations is shown in FIG.

なお受波異常でリセツト動作をくりかえしてい
る時にはΔも変化するが、Δ信号を流量に比
例したアナログ信号に変換する出力段にホールド
回路を設けて、受波異常時にはその直前の値をホ
ールドするか、強制的に流量をゼロにするかすれ
ば上記のリセツト動作によるΔの変動は出力に
表れない。またパルス信号入力21には一定周波
数のパルスを出すパルス発生回路を別に設けても
よいし、VCO8の出力信号を用いてもよい。
Note that Δ will also change when the reset operation is repeated due to an abnormal reception, but a hold circuit is provided at the output stage that converts the Δ signal into an analog signal proportional to the flow rate, and the previous value is held when there is an abnormal reception. Alternatively, if the flow rate is forcibly reduced to zero, the fluctuation in Δ caused by the above reset operation will not appear in the output. Further, a pulse generation circuit that generates pulses of a constant frequency may be provided separately for the pulse signal input 21, or the output signal of the VCO 8 may be used.

以上の説明では超音波式満水流量計の場合につ
いて述べたが、開水路流量計の流速測定部に応用
することも可能である。特に開水路流量計では流
速検出器以下に水位が下ることはごく当り前のこ
とであり、本発明の機能を適用すれば低水位→高
水位の切替も自動的に行うことができるので有効
である。
In the above explanation, the case of an ultrasonic full-water flow meter has been described, but it is also possible to apply the present invention to a flow velocity measuring section of an open channel flow meter. Particularly in open channel flowmeters, it is common for the water level to fall below the flow rate detector, and applying the function of the present invention is effective because it can automatically switch from low water level to high water level. .

以上述べたように、本発明によれば、長期間の
受波異常後の手動再スタートの操作が不要になつ
た結果、従来事実上適用が困難であつた特殊な管
路での自動測定が可能になり、その効果は大き
い。
As described above, according to the present invention, it is no longer necessary to manually restart the operation after a long period of abnormal reception, and as a result, automatic measurement in special pipes, which was practically difficult to apply in the past, is now possible. It is now possible, and the effects are great.

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

第1図、第2図は従来技術を説明するための
図、第3図は本発明の具体的な実施例を示す図、
第4図は本発明の内容を説明するための図であ
る。 1……配管、2……送受信子、3……受信回
路、4,20……計数回路、5……ΔT/V変換
回路、6,7……積分回路、8,9……電圧制御
発振器、10……周波数差変換回路、12……送
信回路、14,22……電子スイツチ、15……
演算増幅器、16……コンデンサ、17……基準
電源。
FIG. 1 and FIG. 2 are diagrams for explaining the prior art, and FIG. 3 is a diagram showing a specific embodiment of the present invention.
FIG. 4 is a diagram for explaining the content of the present invention. 1... Piping, 2... Transmitting/receiving element, 3... Receiving circuit, 4, 20... Counting circuit, 5... ΔT/V conversion circuit, 6, 7... Integrating circuit, 8, 9... Voltage controlled oscillator , 10... Frequency difference conversion circuit, 12... Transmission circuit, 14, 22... Electronic switch, 15...
Operational amplifier, 16... capacitor, 17... reference power supply.

Claims (1)

【特許請求の範囲】[Claims] 1 配管に設置され、配管内の被測定流体を伝播
する超音波を送受信する一対の送受信子と、第1
の計数回路と、前記送受信子で受信された受信信
号と第1の計数回路の出力信号との時間差に比例
した電圧を得る変換回路と、この変換回路からの
出力電圧を積分する積分回路と、この積分回路の
出力と基準電圧に対応した周波数のパルス信号を
前記第1の計数回路に出力する電圧制御発振器
と、前記送受信子からの異常信号によつて前記積
分回路への前記変換回路からの入力を阻止する手
段と、前記異常信号によつてパルス信号の計数を
行う第2の計数回路と、この第2の計数回路が所
定の計数時間に達する毎に前記積分回路をリセツ
トする手段とより構成したことを特徴とする超音
波式流量計。
1 A pair of transceivers installed in the piping and transmitting and receiving ultrasonic waves propagating through the fluid to be measured in the piping;
a converting circuit that obtains a voltage proportional to the time difference between the received signal received by the transceiver and the output signal of the first counting circuit; and an integrating circuit that integrates the output voltage from the converting circuit. a voltage controlled oscillator that outputs a pulse signal of a frequency corresponding to the output of the integrating circuit and the reference voltage to the first counting circuit; means for blocking input; a second counting circuit for counting pulse signals according to the abnormal signal; and means for resetting the integrating circuit each time the second counting circuit reaches a predetermined counting time. An ultrasonic flow meter characterized by the following configuration.
JP12106280A 1980-09-03 1980-09-03 Ultrasonic type flowmeter Granted JPS5745413A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP12106280A JPS5745413A (en) 1980-09-03 1980-09-03 Ultrasonic type flowmeter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP12106280A JPS5745413A (en) 1980-09-03 1980-09-03 Ultrasonic type flowmeter

Publications (2)

Publication Number Publication Date
JPS5745413A JPS5745413A (en) 1982-03-15
JPS6148843B2 true JPS6148843B2 (en) 1986-10-27

Family

ID=14801889

Family Applications (1)

Application Number Title Priority Date Filing Date
JP12106280A Granted JPS5745413A (en) 1980-09-03 1980-09-03 Ultrasonic type flowmeter

Country Status (1)

Country Link
JP (1) JPS5745413A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6455180U (en) * 1987-10-02 1989-04-05

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5000039A (en) * 1989-11-21 1991-03-19 Siemens-Bendix Automotive Electronics L.P. Mass air flow integrator

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6455180U (en) * 1987-10-02 1989-04-05

Also Published As

Publication number Publication date
JPS5745413A (en) 1982-03-15

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