JPH0447771B2 - - Google Patents

Info

Publication number
JPH0447771B2
JPH0447771B2 JP57191893A JP19189382A JPH0447771B2 JP H0447771 B2 JPH0447771 B2 JP H0447771B2 JP 57191893 A JP57191893 A JP 57191893A JP 19189382 A JP19189382 A JP 19189382A JP H0447771 B2 JPH0447771 B2 JP H0447771B2
Authority
JP
Japan
Prior art keywords
circuit
transmitting
switching
delay
receiving
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 - Lifetime
Application number
JP57191893A
Other languages
Japanese (ja)
Other versions
JPS5981515A (en
Inventor
Kenichiro Suzuki
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.)
Shimada Rika Kogyo KK
Original Assignee
Shimada Rika Kogyo KK
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 Shimada Rika Kogyo KK filed Critical Shimada Rika Kogyo KK
Priority to JP57191893A priority Critical patent/JPS5981515A/en
Publication of JPS5981515A publication Critical patent/JPS5981515A/en
Publication of JPH0447771B2 publication Critical patent/JPH0447771B2/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)
  • Measurement Of Velocity Or Position Using Acoustic Or Ultrasonic Waves (AREA)
  • Measuring Volume Flow (AREA)

Description

【発明の詳細な説明】 この発明は超音波流量計測装置、詳しくはシン
グアラウンド方式を用いた超音波流量計測装置に
関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an ultrasonic flow rate measuring device, and more particularly to an ultrasonic flow rate measuring device using a sing-around method.

第1図は従来のシングアラウンド方式の超音波
流量計測装置のブロツクダイアグラムであり、流
体6が流れるパイプ5の壁面には取付要素4,7
を介して送受波器3,8が斜めに対向して取付け
られている。そして、この送受波器3,8はそれ
ぞれ切換回路1を介して送信回路2、受信回路9
と接続されており、この切換回路1を切換えるこ
とにより受信モード、送信モードを自由に選択で
きる様になつている。なお、この第1図の場合は
送受波器3が送信モードに、送受波器8が受信モ
ードになつており、この説明においてはこの場合
を順方向系、その逆の場合を逆方向系と称する。
更に受信回路9には逓倍回路11が接続され、逓
倍回路11の出力は差周波数計数回路10に送ら
れる様になつている。
FIG. 1 is a block diagram of a conventional single-around type ultrasonic flow measuring device, in which mounting elements 4, 7 are mounted on the wall of a pipe 5 through which fluid 6 flows.
The transducers 3 and 8 are mounted diagonally opposite each other via the . The transducers 3 and 8 are connected to a transmitting circuit 2 and a receiving circuit 9 via a switching circuit 1, respectively.
By switching this switching circuit 1, the receiving mode and the transmitting mode can be freely selected. In the case of FIG. 1, the transducer 3 is in the transmitting mode and the transducer 8 is in the receiving mode. In this explanation, this case will be referred to as a forward system, and the opposite case will be referred to as a reverse system. to be called.
Furthermore, a multiplier circuit 11 is connected to the receiving circuit 9, and the output of the multiplier circuit 11 is sent to a difference frequency counting circuit 10.

そして、この第1図において切換回路1は順方
向系となつており、この時、切換り直後のトリガ
ー信号により、送信回路2から送信信号が発せら
れ、該送信信号により、送信モードになつている
送受波器3から超音波パルスが発せられ、該超音
波パルスは取付要素4を介してパイプ5内に伝え
られ流体6を伝播して取付要素7を経て受信モー
ドにある送受波器8に到達し、受信回路9へ導入
される。そしてこの受信回路9ではこの流体6中
に伝播した超音波パルスと時間的、レベル的に判
別された信号とにより受信到達した時間に出力パ
ルスが発せられる。そして、この受信回路9の出
力パルスを送信のトリガーパルスとして用いる様
に接続し、送受信のくり返し発振を行う様に構成
している。この場合、受信から次の受信まぜの周
期をシングアラウンド周期、その逆数をシングア
ラウンド周波数と称している。そして、電気回路
系の遅れ時間、パイプ5内及び取付要素4,7内
の伝播時間が超音波の流体6内伝播時間に比して
無視できる程小さい場合には、 順方向系のシングアラウンド周期t1は t1=D/cosθ/C+Vsinθ ……(1) 同様に逆方向系のシングアラウンド周期t2は t2=D/cosθ/C−Vsinθ ……(2) 但し D:パイプの内径 θ:流体に対する超音波パルスの発射角
度 C:音速 となり、 シングアラウンド周波数の差を△fとすれば △f=1/t1−1/t2 ……(3) =C+Vsinθ/D/cosθ−C−Vsinθ/D/cosθ…
…(4) =2Vsinθ/D/cosθ ……(5) =V(2Vsinθ/D/cosθ) ……(6) となり、θ及びDが既知である為、△fを検出す
ることにより流体6の流速が求まる。
In FIG. 1, the switching circuit 1 is a forward system, and at this time, a trigger signal immediately after switching causes the transmitting circuit 2 to generate a transmitting signal, and the transmitting signal causes the transmitter to enter the transmitting mode. An ultrasonic pulse is emitted from the transducer 3 in the receiving mode, which is transmitted through the mounting element 4 into the pipe 5 and propagates through the fluid 6 via the mounting element 7 to the transducer 8 in the receiving mode. The signal reaches the receiving circuit 9 and is introduced into the receiving circuit 9. In the receiving circuit 9, an output pulse is emitted at the time when the ultrasonic pulse propagated into the fluid 6 and the signal determined in terms of time and level are received. The output pulse of this receiving circuit 9 is connected so as to be used as a trigger pulse for transmission, and is configured to perform repeated oscillation of transmission and reception. In this case, the period from one reception to the next reception mix is called a sing-around period, and its reciprocal is called a sing-around frequency. If the delay time of the electric circuit system and the propagation time within the pipe 5 and the attachment elements 4 and 7 are negligibly small compared to the propagation time of the ultrasonic wave within the fluid 6, then the sing-around period of the forward system is t 1 is t 1 = D / cos θ / C + Vsin θ ... (1) Similarly, the sing-around period t 2 of the reverse direction system is t 2 = D / cos θ / C - Vsin θ ... (2) where D: inner diameter of the pipe θ : Launch angle of ultrasonic pulse to fluid C: Speed of sound, and if the difference in sing-around frequency is △f, then △f=1/t 1 -1/t 2 ...(3) =C+Vsinθ/D/cosθ-C −Vsinθ/D/cosθ...
...(4) =2Vsinθ/D/cosθ ...(5) =V(2Vsinθ/D/cosθ) ...(6) Since θ and D are known, by detecting △f, the fluid 6 can be determined. Find the flow velocity.

従つて、差周波数計数回路10の出力は流速、
及び流量に比例することとなる。
Therefore, the output of the difference frequency counting circuit 10 is the flow velocity,
and is proportional to the flow rate.

なお、逓倍回路11は差周波数の検出精度を向
上させる為挿入されており、逓倍数をmとすれば
前記(3)式は △f=m/t1−m/t2 ……(7) =V(2msinθ/D/cosθ) ……(8) となる。
Note that the multiplier circuit 11 is inserted to improve the detection accuracy of the difference frequency, and if the multiplier is m, the above formula (3) is △f=m/t 1 −m/t 2 ...(7) =V(2msinθ/D/cosθ)...(8).

しかしながら、この従来のシングアラウンド方
式の超音波流量検出装置においては流体中の伝播
時間に比較して取付要素内の伝播時間τ2、パイプ
肉厚内の伝播時間τ3が無視できなくなると、この
合計値τ0が直接誤差として測定値に含まれてくる
重大な欠陥があつた。
However, in this conventional single-around type ultrasonic flow rate detection device, the propagation time τ 2 within the mounting element and the propagation time τ 3 within the pipe wall thickness cannot be ignored compared to the propagation time in the fluid. There was a serious defect in which the total value τ 0 was included in the measured value as a direct error.

即ち、 τ0=τ1+τ2+τ3 ……(9) とし、 シングアラウンド周期の順方向をT1 逆方向をT2とすれば T1=t1+τ0 ……(10) T2=t2+τ0 ……(11) となり、前記(3)式にこれを代入すると、 △f=1/T1−1/T2 ……(12) =1/D/cosθ/C+Vsinθ+τ0 −1/D/cosθ/C−Vsinθ+τ0 ……(13) =2Vsinθ・cosθ/D+(c+V)τ0cosθ……(13
′) となり、上式でも明らかな通り、流体中の音速の
項が残り、音速の温度変化による誤差が混入する
欠点である。
That is, if τ 0 = τ 1 + τ 2 + τ 3 ...(9), and the forward direction of the sing-around period is T and the reverse direction is T 2 , then T 1 = t 1 + τ 0 ... (10) T 2 = t 2 + τ 0 ...(11), and by substituting this into the above equation (3), △f=1/T 1 -1/T 2 ...(12) = 1/D/cosθ/C+Vsinθ+τ 0 -1 /D/cosθ/C−Vsinθ+τ 0 …(13) =2Vsinθ・cosθ/D+(c+V)τ 0 cosθ……(13
′), and as is clear from the above equation, the term for the speed of sound in the fluid remains, which has the disadvantage that errors in the speed of sound due to temperature changes are mixed in.

シングアラウンド方式を用いた超音波流量計測
装置においては上述の通りの欠点が存在するが情
報量の豊富さという捨てがたい長所を有してお
り、本発明は上記従来の装置の欠点を除去し、情
報量の豊富さというシングアラウンド方式を用い
た超音波流量計測装置の長所を生かした装置を提
案することを目的とする。以下、第2図以下に示
すこを発明の一実施例に基づいてその構成を説明
する。
Although the ultrasonic flow measuring device using the single-around method has the drawbacks mentioned above, it has the irreplaceable advantage of being rich in information, and the present invention eliminates the drawbacks of the conventional device. The purpose of this study is to propose a device that takes advantage of the advantages of ultrasonic flow measurement devices using the single-around method, such as the abundance of information. Hereinafter, the configuration will be explained based on an embodiment of the invention shown in FIG. 2 and subsequent figures.

第2図はこの発明の一実施例のブロツクダイア
グラムであり、流体6の流れるパイプ5の管壁に
は斜めに対向して一対の送受波器3,7が取付要
素4,4を介して取付けられており、この送受波
器3,7は切換回路1を介して送信回路2、受信
回路9に接続され、切換回路1を切換えることに
より送信、受信を選択的に行える様になつてい
る。なお、これらの康成は第1図に示した従来の
超音波流量計測装置と同じである。
FIG. 2 is a block diagram of an embodiment of the present invention, in which a pair of transducers 3 and 7 are mounted diagonally opposite each other on the wall of a pipe 5 through which a fluid 6 flows, via mounting elements 4 and 4. The transducers 3 and 7 are connected to a transmitting circuit 2 and a receiving circuit 9 via a switching circuit 1, so that transmission and reception can be selectively performed by switching the switching circuit 1. Note that these components are the same as those of the conventional ultrasonic flow rate measuring device shown in FIG.

そして、受信回路9の出力側には遅延回路12
が接続されており、受信された信号を遅延量制御
回路13からの制御信号により遅延させる様にな
つている。更にこの遅延回路12の出力は逓倍回
路11を介して差周波数計数回路10に送られる
様になつている。
A delay circuit 12 is provided on the output side of the receiving circuit 9.
is connected, and the received signal is delayed by a control signal from the delay amount control circuit 13. Furthermore, the output of this delay circuit 12 is sent to a difference frequency counting circuit 10 via a multiplier circuit 11.

なお、前記遅延量制御回路13は切換回路1の
切換に同期し、その切換ごとに遅延量を送信回路
2の送信回数に比例させながら減少させて行く様
になつている。
It should be noted that the delay amount control circuit 13 is configured to be synchronized with the switching of the switching circuit 1, and decrease the delay amount in proportion to the number of transmissions of the transmitting circuit 2 each time the switching circuit 1 switches.

なお、第4図はこの実施例において用いた遅延
回路12、遅延量制御回路の一例を示したもの、
第5図はその各部に発生する信号出力のタイムチ
ヤートであるが、遅延回路、遅延量制御回路はこ
の第4図に示すものに限定されないことはもちろ
んである。
Note that FIG. 4 shows an example of the delay circuit 12 and the delay amount control circuit used in this embodiment.
Although FIG. 5 is a time chart of signal outputs generated in each part, it goes without saying that the delay circuit and delay amount control circuit are not limited to those shown in FIG.

この実施例は上記の通りの構成を有するもので
あり、切換回路1により1対の送受波器3,8の
うち一方が送信モードのときは他方が受信モード
になる様に一定時間毎に交互に送受切換制御を行
いつつ流体6が流れるパイプ5内に超音波パルス
を発射し、受信モードにある送受波器からの微弱
信号を受信回路9によつて増巾、判別し、更にそ
の出力パルスを送信回路2のトリガーとして動作
させ、この受信回路9の出力パルスを遅延回路1
2に送り、ここにおいて遅延量制御回路13から
の制御信号によつて切換回路1の切換タイミング
に同期させ、その切換毎に遅延量を送信回路2の
送信回数に比例させながら減少させて行き、その
遅延回路出力パルスを逓倍回路11によつて逓倍
し、差周波数計数回路10により送受切換の交互
の逓倍回路出力からその時間差を検出し、この時
間差に基づいて流体の流速、流量を求め様とする
ものであり、従来のシングアラウンド方式の流量
計測装置において避けられなかつた取付要素内の
伝播時間τ2、パルス肉厚内の伝播時間τ1、電気回
路中の遅れ時間τ3等に起因する誤差を除去し、正
確な測定結果を得ることができるものである。以
下、その動作を第3図に示すタイムチヤートに基
づいて更に説明する。送信回路2には順方向系に
切換えた直後にセツトトリガー信号が印加され、
シングアラウンドが開発され、波形Bの如く、受
信回路出力パルス列n1,n2,……が発生する。そ
して、この受信回路8の出力パルスは遅延回路1
2で波形Cの如く遅延時間だけシーケンシヤルに
遅れたあと逓倍回路11に入力される。
This embodiment has the configuration as described above, and the switching circuit 1 switches the transducers 3 and 8 alternately at regular intervals so that when one of the transducers 3 and 8 is in the transmission mode, the other is in the reception mode. While performing transmission/reception switching control, an ultrasonic pulse is emitted into the pipe 5 through which the fluid 6 flows, and the weak signal from the transducer in reception mode is amplified and discriminated by the reception circuit 9, and then the output pulse is is operated as a trigger for the transmitting circuit 2, and the output pulse of the receiving circuit 9 is sent to the delay circuit 1.
2, where it is synchronized with the switching timing of the switching circuit 1 by a control signal from the delay amount control circuit 13, and the delay amount is decreased in proportion to the number of transmissions by the transmitting circuit 2 for each switching, The output pulse of the delay circuit is multiplied by the multiplier circuit 11, the time difference is detected from the output of the multiplier circuit for switching between transmission and reception by the difference frequency counting circuit 10, and the flow velocity and flow rate of the fluid are determined based on this time difference. This is due to the propagation time τ 2 within the mounting element, the propagation time τ 1 within the pulse thickness, the delay time τ 3 in the electric circuit, etc., which are unavoidable in conventional single-around flow rate measuring devices. It is possible to remove errors and obtain accurate measurement results. The operation will be further explained below based on the time chart shown in FIG. Immediately after switching to the forward system, a set trigger signal is applied to the transmitting circuit 2,
A sing-around is developed, and as shown in waveform B, a receiving circuit output pulse train n 1 , n 2 , . . . is generated. Then, the output pulse of this receiving circuit 8 is transmitted to the delay circuit 1.
2, the signal is sequentially delayed by a delay time as shown in waveform C and is then input to the multiplier circuit 11.

即ち、 出力パルスn1はi×τ0だけ遅れN1に 出力パルスn2は(i−1)×τ0だけ遅れN2に 〓 出力パルスnjは(i−j)×τだけ遅れNjにな
り、出力パルスの遅れ量はパルス数に比例しτ0
つ少なくなつて行く様になつている。同様に逆方
向系に切換えた場合には p1はi×τ0だけ遅れP1に 〓 pjは(i−j)×τだけ遅れPjになる。
That is, the output pulse n 1 is delayed by i × τ 0 to N 1 The output pulse n 2 is delayed by (i-1) × τ 0 to N 2 〓 The output pulse nj is delayed by (i-j) × τ to N j The delay amount of the output pulse is proportional to the number of pulses and decreases by τ 0 . Similarly, when switching to the reverse direction system, p1 lags P1 by i×τ 0 , and pj lags Pj by (i−j)×τ.

順方向のシングアラウンド周期は前軌10式で示す
如く、t1+τ0であり、遅延回路12を経て逓倍回
路へ印加されるパルスの周期T1′は T1′=T1−τ0となる これを(10)式に代入しT1′=t1となる。同様に逆
方向のそれはt2+τ0であり、遅延回路12を径て
逓倍回路へ印加されるパルスの周期T2′は T2′=T2−τ0となる これを(11)式に代入しT2′=t2となる。そして、
逓倍回路11を経由した差周波数計数回路出力は △f′=m/T1′−m/T2′ =V(2msinθ/D/cosθ) となるが、これは前記(8)式と同じであり、(9)式に
示す遅延量が消去されていることが明らかであ
る。
The singaround period in the forward direction is t 1 + τ 0 , as shown in equation 10, and the period T 1 ′ of the pulse applied to the multiplier circuit via the delay circuit 12 is T 1 ′=T 1 − τ 0. Substituting this into equation (10), we get T 1 ′=t 1 . Similarly, in the opposite direction, it is t 2 + τ 0 , and the period T 2 ′ of the pulse applied to the multiplier circuit via the delay circuit 12 is T 2 ′ = T 2 − τ 0. This can be expressed as equation (11). Assign T 2 ′=t 2 . and,
The output of the difference frequency counting circuit via the multiplier circuit 11 is △f'=m/ T1' -m/ T2 '=V(2msinθ/D/cosθ), which is the same as equation (8) above. It is clear that the delay amount shown in equation (9) has been eliminated.

即ち、本発明の装置においては差周波数計数回
路出力には測定誤差発生の原因となる各遅延量は
全く含まれないこととなる。
That is, in the apparatus of the present invention, the output of the difference frequency counting circuit does not include any amount of delay that causes measurement errors.

なお、当然ながら本装置は (i−j)τ0+α≧0 (i−j)τ0+β≧0 の領域において動作させるものであることは明ら
かである。
Incidentally, it is obvious that the present device is operated in the range of (i-j) τ 0 +α≧0 (i-j) τ 0 +β≧0.

この発明は上記の通りの動作を行うものであ
り、情報量の豊富さというシングアラウンド方式
の利点をそこなうことなく、簡単な構成により取
付要素内の伝播時間、パイプ肉厚内の伝播時間、
電気回路の遅れ時間等の遅延時間、音速の温度依
存性による誤差等を消去し、正確に流体の流速、
流量を測定することができるすぐれた効果を有す
るものである。
This invention operates as described above, and uses a simple configuration to calculate the propagation time within the mounting element, the propagation time within the pipe wall thickness,
It eliminates delays such as electrical circuit delays and errors due to the temperature dependence of sound speed, and accurately determines the fluid flow velocity.
It has an excellent effect of being able to measure the flow rate.

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

第1図は従来のシングアラウンド方式を用いた
超音波流量計測装置のブロツクダイアグラム、第
2図はこの発明の一実施例のブロツクダイアグラ
ム、第3図はそのタイムチヤート、第4図はこの
発明の要部のブロツクダイアグラム、第5図はそ
のタイムチヤートである。 尚、図中1は切換回路、2は送信回路、3は受
波器、4は取付要素、5はパイプ、6は流体、7
は取付要素、8は受波器、9は受信回路、10は
差周波数計数回路、11は逓倍回路、12は遅延
回路、13は遅延量制御回路を夫々示す。
Fig. 1 is a block diagram of an ultrasonic flow rate measuring device using the conventional sing-around method, Fig. 2 is a block diagram of an embodiment of the present invention, Fig. 3 is a time chart thereof, and Fig. 4 is a block diagram of an ultrasonic flow rate measuring device using the conventional sing-around method. A block diagram of the main parts and a time chart are shown in Figure 5. In the figure, 1 is a switching circuit, 2 is a transmitting circuit, 3 is a receiver, 4 is a mounting element, 5 is a pipe, 6 is a fluid, and 7
1 is a mounting element, 8 is a receiver, 9 is a receiving circuit, 10 is a difference frequency counting circuit, 11 is a multiplier circuit, 12 is a delay circuit, and 13 is a delay amount control circuit.

Claims (1)

【特許請求の範囲】[Claims] 1 被測定流体が流れるパイプの外壁に所定角度
をもつて斜めに対向して設置された一対の超音波
送受波器と、一方の送受波器が送波モードにある
ときは他方が受波モードになる様に一定時間毎に
交互に送受波の切換制御を行う切換回路と、送信
モードにある送受波器を励振する送信回路と、受
信モードにある送受波器からの微弱信号を増巾
し、受信判別を行うと共に、その出力パルスを送
信回路のトリガーとして動作させる受信回路と、
受信回路の出力パルスを時間遅延させうる可変要
素を持つた遅延回路と、送受切換に同期させ、切
換毎に遅延量を送信回路の送信回数に比例させな
がら減少させて行く遅延量制御回路と、遅延回路
からの出力パルスを逓倍する逓倍回路と、送受切
換の交互の逓倍回路の出力から時間差を算出する
差周波数計数回路とから構成され、差周波数計数
回路の時間差に基づいて被測定流体の流速・流量
を測定することを特徴とする超音波流量計測装
置。
1 A pair of ultrasonic transducers are installed diagonally opposite each other at a predetermined angle on the outer wall of a pipe through which the fluid to be measured flows, and when one transducer is in transmitting mode, the other is in receiving mode. There is a switching circuit that alternately controls the switching of transmitting and receiving waves at regular intervals so that the transmitter and receiver are in the transmitting mode, a transmitting circuit that excites the transducer in the transmitting mode, and amplifying the weak signal from the transducer in the receiving mode. , a receiving circuit that performs reception discrimination and operates the output pulse as a trigger for a transmitting circuit;
a delay circuit having a variable element capable of time-delaying the output pulse of the receiving circuit; a delay amount control circuit that is synchronized with transmission/reception switching and decreases the amount of delay in proportion to the number of transmissions of the transmitting circuit for each switching; It consists of a multiplier circuit that multiplies the output pulse from the delay circuit, and a difference frequency counting circuit that calculates the time difference from the output of the multiplier circuit that alternates transmission and reception.・An ultrasonic flow rate measurement device that measures flow rate.
JP57191893A 1982-11-02 1982-11-02 Ultrasonic flow rate measuring device Granted JPS5981515A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP57191893A JPS5981515A (en) 1982-11-02 1982-11-02 Ultrasonic flow rate measuring device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP57191893A JPS5981515A (en) 1982-11-02 1982-11-02 Ultrasonic flow rate measuring device

Publications (2)

Publication Number Publication Date
JPS5981515A JPS5981515A (en) 1984-05-11
JPH0447771B2 true JPH0447771B2 (en) 1992-08-04

Family

ID=16282196

Family Applications (1)

Application Number Title Priority Date Filing Date
JP57191893A Granted JPS5981515A (en) 1982-11-02 1982-11-02 Ultrasonic flow rate measuring device

Country Status (1)

Country Link
JP (1) JPS5981515A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS59185815A (en) * 1983-04-07 1984-10-22 Diesel Kiki Co Ltd Exhaust particle processing device of internal- combustion engine

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS584766B2 (en) * 1977-01-26 1983-01-27 横河電機株式会社 Ultrasonic fluid measuring device

Also Published As

Publication number Publication date
JPS5981515A (en) 1984-05-11

Similar Documents

Publication Publication Date Title
JP3023569B2 (en) Method and apparatus for digitally measuring acoustic burst transit time in a fluid medium
EP0713080B1 (en) Method and device for measuring with sing-around technique
US4024760A (en) Fluid flow measurement apparatus
CN112964319B (en) Multi-frequency array ultrasonic flowmeter
US3727454A (en) Ultrasonic systems for carrying out flow measurements in fluids
JPH1048009A (en) Ultrasound temperature current meter
JP3689973B2 (en) Flow measuring device
JPH0447771B2 (en)
JP2000338123A (en) Ultrasonic floe speed measuring method
JP4008741B2 (en) Ultrasonic flow velocity measuring method and apparatus
JPS5852488Y2 (en) Flow rate measurement device using correlation technology
JPH088417Y2 (en) Ultrasonic flowmeter calibration device
JP2001281032A (en) Ultrasonic flow meter
JPH1090029A (en) Ultrasonic flow meter
US20220268609A1 (en) Ultrasonic Flowmeter and Method for Determining the Velocity of a Flowing Medium
RU2085858C1 (en) Ultrasound method for detection of product volume which runs through pipe and device which implements said method
JPH0421807B2 (en)
JPH0926341A (en) Ultrasonic flow meter
RU2195635C1 (en) Method of measurement of level of liquid and loose media
JP4485641B2 (en) Ultrasonic flow meter
JPH0361892B2 (en)
JPH01100414A (en) Ultrasonic-wave flow velocity measuring apparatus
RU2066852C1 (en) Method of finding of distribution of sound velocity in liquids downwards over depth
JPH0117090B2 (en)
JPS6042405B2 (en) Pulsed ultrasonic Doppler current meter