JPH0148994B2 - - Google Patents
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- Publication number
- JPH0148994B2 JPH0148994B2 JP59225668A JP22566884A JPH0148994B2 JP H0148994 B2 JPH0148994 B2 JP H0148994B2 JP 59225668 A JP59225668 A JP 59225668A JP 22566884 A JP22566884 A JP 22566884A JP H0148994 B2 JPH0148994 B2 JP H0148994B2
- Authority
- JP
- Japan
- Prior art keywords
- signal
- ultrasonic
- wave
- polarity
- transmission
- 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
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Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N2291/00—Indexing codes associated with group G01N29/00
- G01N2291/02—Indexing codes associated with the analysed material
- G01N2291/028—Material parameters
- G01N2291/02836—Flow rate, liquid level
Landscapes
- Measurement Of Levels Of Liquids Or Fluent Solid Materials (AREA)
- Measuring Volume Flow (AREA)
- Length Measuring Devices Characterised By Use Of Acoustic Means (AREA)
- Measurement Of Velocity Or Position Using Acoustic Or Ultrasonic Waves (AREA)
Description
〔産業上の利用分野〕
本発明は超音波流量計、レベル計および厚さ計
などにおける超音波パルス信号の送受信装置に関
する。
〔従来の技術〕
第5図は従来の外壁透過型超音波流量計のブロ
ツク構成図である。第5図において、1は流体が
矢印V方向に流れる流管、2,3は超音波信号を
電気−音響変換および音響−電気変換する超音波
送受波器、4は超音波信号が超音波送受波器2か
ら3または超音波送受波器3から2、すなわち超
音波信号が流体の流れに沿う順方向または流体の
流れに逆う逆方向に伝搬するように切り替える送
受信切替回路、5は送信回路、6は受信回路、7
は超音波信号およびそれに対応した電気信号が送
信回路5から受信回路6まで伝搬する1サイクル
の時間を複数回測定し、測定した伝搬時間に基づ
いて流体の流速に対応する信号を出力する信号処
理回路、8は測定結果を表示する表示器、9はこ
の超音波流量計の各部の動作を制御するタイミン
グパルスを出力するタイマである。なお、送信回
路5の出力および受信回路6の入力は電気信号で
あり、流管1内を伝搬する信号は超音波信号であ
る。
かかる従来の外壁透過型超音波流量計の動作を
説明すると、まず送信回路5から送信波として出
力された信号は送受信切替回路4を介して超音波
送受波器3に入力され、流体中を逆方向に伝搬し
て超音波受波器2に到達し、さらに送受信切替回
路4を介して受信波として受信回路6に入力され
る。この超音波信号の逆方向の伝搬が複数回行な
われた後、送受信切替回路4が切り替えられる
と、送信回路5から出力された信号は送受信切替
回路4を介して超音波送受波器2に入力され、流
体中を順方向に伝搬して超音波送受波器3に到達
し、さらに送受信切替回路4を介して受信回路6
に入力される。超音波信号波の順方向の伝搬も複
数回行なわれる。
信号処理回路7は超音波信号波の順方向および
逆方向の伝搬時間に基づいて、シングアイランド
法、PLL法および時間差法などにより、流体の
流速および流量などを検出する。
次に、第6図は上述した送信波および受信波の
波形の一例を示す図である。送信回路5から出力
される送信波は第6図aまたは第6図bに示すよ
うな波形である。これに対して受信回路6に入力
される受信波は第6図cに示すような波形とな
る。超音波信号が超音波送受波器2または3と管
壁および管壁と流体の各境界で反射、屈折および
拡散を繰り返し、複雑な伝搬経路を経て超音波送
受波器2または3に到達するため、さらには超音
波信号が複雑な伝搬経路を経て超音波送受波器2
または3に到達した後、直ちに消滅せず次に送出
される送信波に重畳されるため受信回路6に入力
される受信波が送信波に対して、本来受信される
べき信号波と、上述したように複雑な伝搬経路を
経ることおよび次に送出される送信波に重畳され
ることにより、超音波信号の伝搬時間に誤差が生
じることになるが、受信波は信号波に対し発生時
刻が略一致し、かつ周波数帯域がほぼ同一である
波(以下、妨害波という)とを合成した合成波に
なつているので、受信回路の信号処理では妨害波
を除去できない。この妨害波の影響の度合は信号
波と妨害波のSN比および順逆方向の超音波信号
の位相差などによつて異なるものである。例え
ば、超音波信号の周波数が1MHz、位相差が0、
流管1の直径が50mm、流体の流速が1m/sの場
合、順逆両方向に超音波信号を伝搬させたときの
伝搬時間差は約40nSとなる。ここで、信号波と
妨害波のSN比を40dBとすると0.8nSの誤差が生
じるので、0.8/40=0.02となり、約2%の測定
誤差となる。また信号波と妨害波のSN比を40dB
にすることは実際上かなり困難であり測定誤差は
2%以上になる。また、流管1の直径が小さいと
きおよび流体の流速が遅いときなどは測定誤差が
拡がることになる。
〔発明が解決しようとする問題点〕
かかる妨害波の影響を避けるため、従来は送信
波を出力させる間隔、すなわち1サイクルの周期
を十分に長くとり、送信波を出力させるサイクル
以前のサイクルで生じた妨害波を消滅させるよう
にしていた。
しかし、1サイクルの周期を長くすることによ
り、単位時間当りの伝搬時間測定回数が減り、流
体の流速を測定するのに時間がかかつてしまうと
いう問題があつた。
本発明は上記問題点を解決する目的でなされた
もので、1サイクルの周期を長くせずに、妨害波
の影響で除去できる超音波パルスの送受信装置を
提供するものである。
〔問題点を解決するための手段〕
そこで本発明では、互いに逆極性の関係にある
正極性の超音波信号と負極性の超音波信号のいず
れか一方を、予め設定されたシーケンスあるいは
ランダムなシーケンスに従つて選択出力し、被計
測媒体中に伝搬させる超音波信号出力手段と、該
選択出力された超音波信号の極性に対応して、前
記被計測媒体中を伝搬した超音波受信信号の極性
を変化させ、伝搬時間を検出する超音波信号検出
手段と、該超音波信号検出手段により検出された
双方の極性による伝搬時間の平均時間を行う平均
処理手段とを設ける。
〔作用〕
上記構成の超音波パルスの送受信方式は、超音
波信号出力手段が互いに逆極性の関係にある正極
性の超音波信号と負極性の超音波信号のいずれか
一方を、予め設定されたシーケンスまたはランダ
ムなシーケンスに従つて選択出力し、被計測媒体
中に伝搬させ、超音波信号検出手段が前記選択出
力された超音波信号の極性に対応して、前記被計
測媒体中に伝搬した超音波受信信号の極性を変化
させ伝搬時間を検出し、平均処理手段が前記超音
波信号検出手段により検出された双方の極性によ
る伝搬時間の平均処理を行ない平均時間を計測す
る。
〔実施例〕
以下、本発明の一実施例を添付図面を参照して
詳細に説明する。
第1図は本発明に係る超音波パルス信号の送受
信方式を適用した超音波流量計の主要部分のブロ
ツク回路図である。第1図において、10は互い
に逆極性の関係にある正極性の信号または負極性
の信号のいずれか一方を、予め設定されたシーケ
ンスまたはランダムなシーケンスに従つて選択し
て、送信波として出力する送信信号出力手段であ
つて、パルス発生回路11、ドライブ回路12、
トランジスタ13Aと13Bからなる送信増幅回
路13および第5図に示した送受信切替回路4を
介して超音波送受波器2,3に接続される送信端
子14から構成されている。20は送信信号出力
手段10から出力され、第5図に示した流管1の
流体(被計測媒体)中を伝搬し、受信波として入
力される信号の到達時刻を検出する受信信号検出
手段であつて、受信端子、21入力された受信波
に対し、同極性および逆極性(逆位相)の信号を
出力する端子OUT1およびOUT2を有する受信
増幅回路22、アナログスイツチ23Aと23B
からなり、増幅回路22から出力される互いに逆
極性の受信波のいずれか一方を選択して出力する
受信波極性切替回路23、入力端子IN1とIN2
を有する増幅回路24および比較基準レベルが
OVに設定され、受信波の零クロス点を検出する
比較回路25から構成されている。30はドライ
ブ回路12および受信波極性切替回路23を制御
し、所定のシーケンスに従い超音波信号出力手段
10から互いに逆極性の送信波を選択させるとと
もに、該送信波の極性に応じて受信波の極性を切
り替えさせるコントローラである。40は信号処
理回路であつて、送信信号出力手段10から出力
される送信波の立上り時刻を送信信号の送出時
刻、受信信号検出手段20に入力される受信波の
零クロス点通過時刻を受信信号の到達時刻、到達
時刻と送出時刻の差を伝搬時間とし、超音波信号
を逆方向および順方向にそれぞれ複数回ずつ伝搬
させたときの伝搬時間tuおよびtdの時間差△t
(△t=tu−td)に基づいて、シングアラウンド
法、PLL法あるいは時間差法などによつて流体
の流速に対応した信号を出力するものである。9
は各部の動作タイミングを制御するタイマであ
る。
なお、送信信号出力手段10はトランジスタ1
3Aをオン、トランジスタ13Bをオフにして正
極性の送信信号を出力し、トランジスタ13Aを
オフ、トランジスタ13Bをオンにして負極性の
送信信号を出力する。また受信信号検出手段20
はアナログスイツチ23Aを端子OUT1側、ア
ナログスイツチ23Bを端子OUT2側に切り替
えて、受信した超音波信号を増幅回路24に加
え、アナログスイツチ23Aを端子OUT2側、
アナログスイツチ23Bを端子OUT1側に切り
替えて、受信した信号を反転して増幅回路24に
加える。
ところで、前述した如く受信信号検出手段20
に入力される受信波は送信波を順逆どちらの方向
に伝搬させた場合であつても、、第2図に示すよ
うに送信波Tに対し本来受信すべき信号波Sと妨
害波Nを重畳した合成波Rとなる。妨害波Nの影
響は、例えば送信波を逆方向に伝搬させた場合は
妨害波Nの影響がないときの伝搬時間tuに対し、
伝搬時間を時間αだけ遅くする(第2図a参照)。
また、送信波を順方向に伝搬させた場合は妨害波
Nの影響がないときの伝搬時間tdに対し、伝搬時
間をαだけ速くする(第2図b参照)。したがつ
て、超音波を逆方向に伝搬させたときの伝搬時間
tuと超音波を順方向に伝搬させたときの伝搬時間
tdとの差である伝搬時間差△tは(tu−td+2α)
となり、時間2αだけの誤差を生じてしまう。
このため、本発明においては送信信号出力手段
10は互いに逆極性の関係にある正極性の送信信
号と負極性の送信信号のいずれか一方を予め設定
したシーケンスまたはランダムなシーケンスに従
つて選択して送信波として出力する。受信信号検
出手段20は送信波の極性に応じて受信波極性切
替回路23を切り替え、受信波の特定のポイン
ト、例えば受信波が正から負に変化するときの零
クロス点を検出する。さらに、信号処理回路40
は上述したようにして送受信される超音波信号を
逆方向および順方向に伝搬させることによつて得
られる伝搬時間差の測定を複数回行なわせ、その
平均をとることによつて、妨害波の影響を除去し
た伝搬時間差を得る。
表は妨害波を前回のサイクルにおける送信波の
残影によるものとし、互いに逆極性の関係にある
正極性の超音波信号と負極性の超音波信号のいず
れか一方を、種々のシーケンスに従つて選択出力
した場合における伝搬時間差および伝搬時間差の
平均を示すものである。
[Industrial Application Field] The present invention relates to an ultrasonic pulse signal transmitting/receiving device in an ultrasonic flow meter, a level meter, a thickness meter, etc. [Prior Art] FIG. 5 is a block diagram of a conventional external wall transmission type ultrasonic flow meter. In Fig. 5, 1 is a flow tube through which fluid flows in the direction of arrow V, 2 and 3 are ultrasonic transducers that convert ultrasound signals into electric-acoustic and acoustic-electrical converters, and 4 is an ultrasonic signal that transmits and receives ultrasonic waves. Transducer 2 to 3 or ultrasonic transducer 3 to 2, that is, a transmission/reception switching circuit that switches the ultrasonic signal to propagate in the forward direction along the fluid flow or in the reverse direction against the fluid flow; 5 is a transmission circuit; , 6 is a receiving circuit, 7
is a signal processing method that measures the time of one cycle in which an ultrasonic signal and its corresponding electric signal propagate from the transmitting circuit 5 to the receiving circuit 6 multiple times, and outputs a signal corresponding to the fluid flow velocity based on the measured propagation time. The circuit includes a display device 8 for displaying measurement results, and a timer 9 for outputting timing pulses for controlling the operation of each part of this ultrasonic flowmeter. Note that the output of the transmitting circuit 5 and the input of the receiving circuit 6 are electrical signals, and the signals propagating within the flow tube 1 are ultrasonic signals. To explain the operation of such a conventional external wall transmission type ultrasonic flowmeter, first, a signal output as a transmission wave from the transmission circuit 5 is input to the ultrasonic transducer 3 via the transmission/reception switching circuit 4, and is reversely transmitted through the fluid. The waves propagate in the same direction, reach the ultrasonic wave receiver 2, and are further input to the reception circuit 6 as a reception wave via the transmission/reception switching circuit 4. After this ultrasonic signal propagates in the opposite direction multiple times, when the transmission/reception switching circuit 4 is switched, the signal output from the transmission circuit 5 is input to the ultrasonic transducer 2 via the transmission/reception switching circuit 4. It propagates in the fluid in the forward direction, reaches the ultrasonic transducer 3, and then passes through the transmission/reception switching circuit 4 to the reception circuit 6.
is input. The forward propagation of the ultrasound signal wave is also performed multiple times. The signal processing circuit 7 detects the flow velocity and flow rate of the fluid based on the forward and reverse propagation times of the ultrasonic signal waves using the sing island method, the PLL method, the time difference method, and the like. Next, FIG. 6 is a diagram showing an example of the waveforms of the above-mentioned transmitted waves and received waves. The transmission wave output from the transmission circuit 5 has a waveform as shown in FIG. 6a or FIG. 6b. On the other hand, the received wave input to the receiving circuit 6 has a waveform as shown in FIG. 6c. Because the ultrasonic signal is repeatedly reflected, refracted, and diffused at each boundary between the ultrasonic transducer 2 or 3 and the tube wall, and between the tube wall and the fluid, it reaches the ultrasonic transducer 2 or 3 through a complicated propagation path. , furthermore, the ultrasonic signal passes through a complicated propagation path to the ultrasonic transducer 2.
Or, after reaching 3, the received wave input to the receiving circuit 6 does not disappear immediately and is superimposed on the next transmitted wave, so that the received wave input to the receiving circuit 6 is the signal wave that should originally be received with respect to the transmitted wave. An error occurs in the propagation time of the ultrasonic signal due to the complicated propagation path and being superimposed on the next transmitted wave. The interference wave cannot be removed by the signal processing of the receiving circuit because it is a composite wave that is composed of waves that match and have almost the same frequency band (hereinafter referred to as interference waves). The degree of influence of this interference wave varies depending on the SN ratio between the signal wave and the interference wave, the phase difference between the forward and reverse ultrasonic signals, and the like. For example, the frequency of the ultrasound signal is 1MHz, the phase difference is 0,
When the diameter of the flow tube 1 is 50 mm and the flow velocity of the fluid is 1 m/s, the propagation time difference when an ultrasonic signal is propagated in both forward and reverse directions is about 40 nS. Here, if the SN ratio between the signal wave and the interference wave is 40 dB, an error of 0.8 nS will occur, so 0.8/40 = 0.02, resulting in a measurement error of about 2%. Also, the SN ratio of signal waves and interference waves is 40dB.
In practice, it is quite difficult to achieve this, and the measurement error is 2% or more. Furthermore, when the diameter of the flow tube 1 is small or when the flow rate of the fluid is slow, measurement errors will increase. [Problem to be solved by the invention] In order to avoid the influence of such interference waves, conventionally, the interval at which the transmitted waves are outputted, that is, the period of one cycle, is set sufficiently long, and the interval between the outputs of the transmitted waves, that is, the period of one cycle, is set sufficiently long, and the interval between the outputs of the transmitted waves is made sufficiently long. It was designed to eliminate any interference waves. However, by increasing the period of one cycle, the number of times the propagation time is measured per unit time decreases, resulting in a problem that it takes time to measure the flow velocity of the fluid. The present invention has been made to solve the above-mentioned problems, and provides an ultrasonic pulse transmitting/receiving device that can eliminate interference waves without increasing the period of one cycle. [Means for Solving the Problem] Therefore, in the present invention, either a positive polarity ultrasound signal or a negative polarity ultrasound signal, which have opposite polarity to each other, is transmitted in a preset sequence or a random sequence. an ultrasonic signal output means for selectively outputting the ultrasonic signal and propagating it in the medium to be measured, and a polarity of the ultrasonic reception signal propagated in the medium to be measured corresponding to the polarity of the selectively outputted ultrasonic signal; and an averaging processing means for averaging the propagation times of both polarities detected by the ultrasonic signal detecting means. [Operation] In the ultrasonic pulse transmission/reception method having the above configuration, the ultrasonic signal output means transmits either a positive polarity ultrasonic signal or a negative polarity ultrasonic signal, which have opposite polarities to each other. The ultrasonic signal is selectively output according to a sequence or a random sequence and propagated into the medium to be measured, and the ultrasonic signal detecting means detects the ultrasonic wave propagated into the medium to be measured in accordance with the polarity of the selected and outputted ultrasonic signal. The propagation time is detected by changing the polarity of the sonic reception signal, and the averaging processing means averages the propagation time of both polarities detected by the ultrasonic signal detection means to measure the average time. [Example] Hereinafter, an example of the present invention will be described in detail with reference to the accompanying drawings. FIG. 1 is a block circuit diagram of the main parts of an ultrasonic flowmeter to which the ultrasonic pulse signal transmission/reception method according to the present invention is applied. In FIG. 1, 10 selects either a positive polarity signal or a negative polarity signal, which have opposite polarities to each other, according to a preset sequence or a random sequence, and outputs it as a transmission wave. The transmission signal output means includes a pulse generation circuit 11, a drive circuit 12,
It consists of a transmission amplifier circuit 13 made up of transistors 13A and 13B, and a transmission terminal 14 connected to the ultrasonic transducers 2 and 3 via a transmission/reception switching circuit 4 shown in FIG. Reference numeral 20 denotes a received signal detection means for detecting the arrival time of a signal outputted from the transmitted signal output means 10, propagated in the fluid (measured medium) of the flow tube 1 shown in FIG. 5, and inputted as a received wave. There is a receiving terminal, 21 a receiving amplifier circuit 22 having terminals OUT1 and OUT2 that output signals of the same polarity and opposite polarity (opposite phase) to the input received wave, and analog switches 23A and 23B.
a received wave polarity switching circuit 23 that selects and outputs one of the received waves of opposite polarity output from the amplifier circuit 22, and input terminals IN1 and IN2.
and a comparison reference level.
It is set to OV and consists of a comparison circuit 25 that detects the zero cross point of the received wave. 30 controls the drive circuit 12 and the received wave polarity switching circuit 23 to select transmitted waves of opposite polarity from the ultrasonic signal output means 10 according to a predetermined sequence, and also changes the polarity of the received wave according to the polarity of the transmitted waves. This is a controller that allows you to switch. Reference numeral 40 denotes a signal processing circuit, which uses the rising time of the transmission wave outputted from the transmission signal output means 10 as the transmission time of the transmission signal, and the time when the reception wave inputted to the reception signal detection means 20 passes the zero cross point as the reception signal. The arrival time of , and the difference between the arrival time and the sending time are the propagation time, and the time difference △t between the propagation times tu and td when the ultrasonic signal is propagated multiple times in the backward and forward directions, respectively.
(Δt=tu−td), a signal corresponding to the flow velocity of the fluid is output by the sing-around method, PLL method, or time difference method. 9
is a timer that controls the operation timing of each part. Note that the transmission signal output means 10 is a transistor 1.
3A is turned on and transistor 13B is turned off to output a positive polarity transmission signal, and transistor 13A is turned off and transistor 13B is turned on to output a negative polarity transmission signal. Also, the received signal detection means 20
switches the analog switch 23A to the terminal OUT1 side and the analog switch 23B to the terminal OUT2 side, applies the received ultrasonic signal to the amplifier circuit 24, and switches the analog switch 23A to the terminal OUT2 side,
The analog switch 23B is switched to the terminal OUT1 side, and the received signal is inverted and applied to the amplifier circuit 24. By the way, as mentioned above, the received signal detection means 20
Regardless of whether the transmitted wave is propagated in the forward or reverse direction, the received wave that is input to the transmitter superimposes the signal wave S that should originally be received and the interference wave N on the transmitted wave T, as shown in Figure 2. The result is a composite wave R. The influence of the interference wave N is, for example, when the transmitted wave propagates in the opposite direction, with respect to the propagation time tu when there is no influence of the interference wave N.
The propagation time is delayed by a time α (see Figure 2a).
Furthermore, when the transmitted wave is propagated in the forward direction, the propagation time is increased by α compared to the propagation time td when there is no influence of the interference wave N (see FIG. 2b). Therefore, the propagation time when the ultrasound propagates in the opposite direction
tu and the propagation time when the ultrasound propagates in the forward direction
The propagation time difference △t, which is the difference from td, is (tu−td+2α)
Therefore, an error of only time 2α occurs. Therefore, in the present invention, the transmission signal output means 10 selects either a positive polarity transmission signal or a negative polarity transmission signal, which have opposite polarities to each other, according to a preset sequence or a random sequence. Output as a transmitted wave. The received signal detection means 20 switches the received wave polarity switching circuit 23 according to the polarity of the transmitted wave, and detects a specific point of the received wave, for example, a zero crossing point when the received wave changes from positive to negative. Furthermore, the signal processing circuit 40
The method measures the propagation time difference obtained by propagating the transmitted and received ultrasonic signals in the reverse and forward directions multiple times as described above, and then averages them to determine the influence of interference waves. Obtain the propagation time difference with . The table assumes that the interference waves are the residual effects of the transmitted waves from the previous cycle, and that either a positive polarity ultrasonic signal or a negative polarity ultrasonic signal, which have opposite polarities to each other, is transmitted according to various sequences. It shows the propagation time difference and the average of the propagation time differences in the case of selective output.
【表】【table】
以上説明したように本発明によれば、互いに逆
極性の関係、にある正極性または負極性の送信信
号のいずれか一方を、予め設定したシーケンスま
たはランダムなシーケンスに従つて選択出力し、
選択出力した送信信号の極性にかかわらず、受信
信号が所定の変化点に到達したときを超音波信号
の到達時刻とすることによつて得られる伝搬時間
差の平均効果により妨害波の影響を除去すること
ができる。
As explained above, according to the present invention, either one of positive polarity or negative polarity transmission signals having opposite polarity to each other is selectively outputted according to a preset sequence or a random sequence,
Regardless of the polarity of the selectively output transmitted signal, the influence of interference waves is removed by the average effect of the propagation time difference obtained by setting the arrival time of the ultrasonic signal to the time when the received signal reaches a predetermined change point. be able to.
第1図は本発明に係る超音波パルス信号の送受
信装置を適用した超音波流量計の主要部分のブロ
ツク回路図、第2図は送信波の波形の一例を示す
波形図、第3図および第4図は本発明に係る超音
波パルス信号の送受信方式を適用した超音波流量
計の他の実施例を示すブロツク回路図、第5図は
従来の外壁透過型超音波流量計のブロツク構成
図、第6図は送信波および受信波の波形の一例を
示す波形図である。
10……送信信号出力手段、11……パルス発
生回路、12……ドライブ回路、13……送信増
幅回路、14……送信端子、20……受信信号検
出手段、21……受信端子、22……受信増幅回
路、23,26……極性切替回路、24……増幅
回路、25,27,28……比較回路、29……
オアゲート、30……コントローラ、40……信
号処理回路。
Fig. 1 is a block circuit diagram of the main parts of an ultrasonic flowmeter to which an ultrasonic pulse signal transmitting/receiving device according to the present invention is applied, Fig. 2 is a waveform diagram showing an example of the waveform of a transmitted wave, Figs. Fig. 4 is a block circuit diagram showing another embodiment of an ultrasonic flowmeter to which the ultrasonic pulse signal transmission/reception method according to the present invention is applied, and Fig. 5 is a block diagram of a conventional external wall transmission type ultrasonic flowmeter. FIG. 6 is a waveform diagram showing an example of the waveforms of the transmitted wave and the received wave. DESCRIPTION OF SYMBOLS 10... Transmission signal output means, 11... Pulse generation circuit, 12... Drive circuit, 13... Transmission amplifier circuit, 14... Transmission terminal, 20... Reception signal detection means, 21... Reception terminal, 22... ...Reception amplifier circuit, 23, 26...Polarity switching circuit, 24...Amplification circuit, 25, 27, 28...Comparison circuit, 29...
OR gate, 30...controller, 40...signal processing circuit.
Claims (1)
号と負極性の超音波信号を、予め設定されたシー
ケンスまたはランダムなシーケンスに従つて選択
出力し、被計測媒体中に伝搬させる超音波信号出
力手段と、 該選択出力された超音波信号の極性に対応し
て、前記被計測媒体中を伝搬した超音波受信信号
の極性を変化させ、伝搬時間を検出する超音波検
出手段と、 該超音波信号検出手段により検出された双方の
極性による伝搬時間の平均処理を行う平均処理手
段とを備えたことを特徴とする超音波パルスの送
受信装置。[Claims] 1. A positive polarity ultrasonic signal and a negative polarity ultrasonic signal having opposite polarities to each other are selectively outputted according to a preset sequence or a random sequence, and are outputted into a medium to be measured. ultrasonic signal output means for propagating; and ultrasonic detection for detecting propagation time by changing the polarity of the ultrasonic reception signal propagated in the medium to be measured in accordance with the polarity of the selectively outputted ultrasonic signal. What is claimed is: 1. An ultrasonic pulse transmitting/receiving device comprising: means for averaging propagation times of both polarities detected by the ultrasonic signal detecting means.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59225668A JPS61104276A (en) | 1984-10-29 | 1984-10-29 | System for transmitting and receiving ultrasonic pulse |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59225668A JPS61104276A (en) | 1984-10-29 | 1984-10-29 | System for transmitting and receiving ultrasonic pulse |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS61104276A JPS61104276A (en) | 1986-05-22 |
| JPH0148994B2 true JPH0148994B2 (en) | 1989-10-23 |
Family
ID=16832907
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP59225668A Granted JPS61104276A (en) | 1984-10-29 | 1984-10-29 | System for transmitting and receiving ultrasonic pulse |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS61104276A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2009085972A (en) * | 2009-01-28 | 2009-04-23 | Panasonic Corp | Ultrasonic flow meter |
Families Citing this family (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| GB8805105D0 (en) * | 1988-03-03 | 1988-03-30 | Scan Technologies Ltd | Improvements relating to instruments |
| NZ243294A (en) * | 1991-06-25 | 1995-04-27 | Commw Scient Ind Res Org | Time of flight of acoustic wave packets through fluid: reduction of higher order acoustic mode effects |
| JP4825367B2 (en) * | 2001-06-11 | 2011-11-30 | 愛知時計電機株式会社 | Ultrasonic flow meter |
| WO2012094298A1 (en) * | 2011-01-06 | 2012-07-12 | The Lubrizol Corporation | Ultrasonic measurement |
| JP6665792B2 (en) * | 2017-01-16 | 2020-03-13 | 株式会社デンソー | Liquid level detector |
-
1984
- 1984-10-29 JP JP59225668A patent/JPS61104276A/en active Granted
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2009085972A (en) * | 2009-01-28 | 2009-04-23 | Panasonic Corp | Ultrasonic flow meter |
Also Published As
| Publication number | Publication date |
|---|---|
| JPS61104276A (en) | 1986-05-22 |
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