EP1754025A2 - Determination of the reception time for an ultrasound signal by means of pulse shape detection - Google Patents
Determination of the reception time for an ultrasound signal by means of pulse shape detectionInfo
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- EP1754025A2 EP1754025A2 EP05733644A EP05733644A EP1754025A2 EP 1754025 A2 EP1754025 A2 EP 1754025A2 EP 05733644 A EP05733644 A EP 05733644A EP 05733644 A EP05733644 A EP 05733644A EP 1754025 A2 EP1754025 A2 EP 1754025A2
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- European Patent Office
- Prior art keywords
- time
- signal
- ultrasonic
- ultrasound
- receiving unit
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01F—MEASURING VOLUME, VOLUME FLOW, MASS FLOW OR LIQUID LEVEL; METERING BY VOLUME
- G01F1/00—Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow
- G01F1/66—Measuring 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
Definitions
- the invention relates to an ultrasonic flow sensor according to the preamble of patent claim 1 and a method for determining the time of reception of an ultrasonic signal according to the preamble of patent claim 7.
- Ultrasonic flow sensors are used in particular to measure the volume or mass flow or the flow rate of a gaseous or liquid medium flowing through a pipeline.
- a known type of ultrasound flow sensor comprises two ultrasound transducers arranged offset in the flow direction, each of which generates ultrasound signals and emits them to the other ultrasound transducer.
- the ultrasonic signals are received by the other transducer and evaluated using electronics.
- the transit time difference between the signal in the flow direction and the signal in the opposite direction is a measure of the flow velocity of the fluid.
- the desired measurement variable e.g. a volume or mass flow can be calculated.
- Fig. 1 shows a typical arrangement of an ultrasonic flow sensor with two ultrasonic transducers A, B, which are arranged within a pipe 3 and face each other at a distance L.
- a fluid 1 flows in the pipeline 3 at a speed v in the direction of the arrow 2.
- the measuring section L is opposite to the
- the ultrasonic transducers A, B send each other ultrasonic signals that are either slowed or accelerated by the flow, depending on the direction.
- the transit times of the sound signals are a measure of the flow velocity to be determined.
- Fig. 2 shows a highly simplified schematic representation of a transducer arrangement with an associated control and evaluation electronics 4.
- the flow sensor can e.g. work according to the so-called "sing-around" process.
- the reception of an ultrasonic signal AO or B0 at one of the transducers A, B triggers an ultrasonic signal in the opposite direction.
- the "reception time" of the signal A0, B0 is defined here as the first zero crossing No of the signal after the signal amplitude Amp has a predetermined threshold value SW (the so-called pretrigger
- the time to would be the time of reception of the signal. (Alternatively, the reception time of the signal could also be determined differently, e.g. by evaluating the phase of the signal.)
- Contamination, drifting or aging of the ultrasonic transducers, or turbulence in the flowing fluid can lead to the amplitude of the ultrasonic signals A0, B0 varying greatly.
- the zero crossing detection is hardly impaired, since the same zero crossing (based on the entire signal) is always detected as the reception time and the frequency of the signal remains essentially the same.
- the amplitude of the half-wave lying before the time to falls below the threshold value SW incorrect measurements of the time of reception can occur, since the
- the ultrasound signal then exceeds the threshold value SW at a later point in time and thus an incorrect zero crossing is detected as the reception time.
- the receiving unit 4 shows the signal curve of the ultrasonic signal A0, B0 or converter output signal 5 with a reduced amplitude Amp. This signal only exceeds the fixed threshold value SW at a later point in time. In this case, the receiving unit 4 determines the zero crossing Ni and thus an incorrect zero crossing N as the reception time t o of the ultrasonic signal A0, B0.
- An essential aspect of the invention is the point in time of the form of the ultrasound signal characteristic size (eg the time of the maximum
- a reception time e.g. a zero crossing
- the time shift between the reference time and the reception event remains unchanged as long as the threshold lies between the same two amplitudes of the ultrasound signal. If the amplitude of the ultrasound signal or the associated transducer output signal changes so strongly that the threshold lies between two other amplitudes of the signal, the time difference between the characteristic quantity and the detected reception event changes suddenly. This can be recognized by the receiving unit of the ultrasonic flow sensor and the time of reception can be corrected accordingly.
- the characteristic quantity is preferably a quantity which is independent of the signal amplitude, e.g. the time of the maximum amplitude, the signal center of gravity or the center of gravity of the envelope.
- the point in time of the center of gravity of the envelope curve determines the reference point in time.
- the temporal focus of the envelope can e.g. can be calculated in a processor unit according to the following relationship:
- the receiving unit comprises a device for determining the maximum amplitude of the ultrasound signal.
- the characteristic quantity is the maximum amplitude of the ultrasound signal.
- the choice of the maximum amplitude of the ultrasound signal as the reference point in time provides the same result as the choice of the center of gravity of the envelope, provided that the position of the maximum amplitude does not change relative to the other amplitudes. However, if the position of the maximum amplitude shifts relative to the other amplitudes, incorrect measurements can occur since the time interval between the detected reception time to and the reference time changes by n * 2pi.
- the receiving unit preferably comprises a comparator, at the input of which the transducer output signal generated by the ultrasonic transducer and a reference signal (e.g. a threshold voltage) are present, the receiving unit providing information about the reference time (e.g. time of the maximum amplitude or the center of gravity of the comparator) from the output signal of the comparator Envelope curve).
- a comparator at the input of which the transducer output signal generated by the ultrasonic transducer and a reference signal (e.g. a threshold voltage) are present, the receiving unit providing information about the reference time (e.g. time of the maximum amplitude or the center of gravity of the comparator) from the output signal of the comparator Envelope curve).
- the reception event is preferably a zero crossing, but can also be another predetermined criterion.
- the receiving unit is preferably able to correct the reception time depending on its position in time at the reference time.
- 1 shows an ultrasonic flow sensor known from the prior art with two ultrasonic transducers; 2 shows an ultrasonic flow sensor with associated control and reception circuit;
- Receiving time to an ultrasonic signal A0, B0 by means of zero crossing detection is detected as the reception time to.
- a predetermined threshold value SW is detected as the reception time to.
- another event e.g. exceeding a threshold value, could also be defined as a reception event.
- the receiving unit 4 (FIG. 2) also determines the time to of the maximum signal amplitude Amp max and the time difference ⁇ t between the reception time to and the time ti. (You can also choose the time of another characteristic quantity, for example the time of the center of gravity of the envelope curve 6 can be determined as the reference time ti.)
- the incorrect zero crossing (here Ni) is detected as the reception time t 0 .
- the time difference ⁇ t changes abruptly by integral multiples of 1 / f or 1 / (2f), where f is the ultrasound frequency. This is recognized by the reception unit 4 and the reception time to is corrected accordingly.
- FIG. 5 shows a known logic circuit for zero crossing detection, with which the reception time to can be determined.
- the circuit comprises a first comparator 10, at whose input (-) the ultrasound signal US or the corresponding converter output signal 5 is present, and at whose other input (+) a threshold voltage U sw is supplied as a reference.
- the output of the comparator 10 always goes into the "high" state when the amplitude of the ultrasonic signal A0, B0 exceeds the reference voltage U sw . From the duration of the high phases, the
- Time of the maximum amplitude Amp max can be determined.
- the second comparator 11 of FIG. 5 is used for zero crossing detection.
- the second comparator 11 receives the ultrasound signal US at its positive input (+) and a corresponding reference voltage (here 0V) at its negative input (-).
- the output signal K 1, K 2 of the comparators 10, 11 is shown in FIG. 6.
- FIG. 6 shows the pulse-width-modulated output signal Ki of the first comparator 10.
- the individual high phases of the signal Ki can be stored and evaluated, for example, in different counters.
- the longest high phase indicates the maximum amplitude Ampmax of the ultrasonic signal A0 or B0.
- the comparator output signal could be processed further analog or digital or evaluated arithmetically. For example, a cross-correlation of different output signals Ki could be carried out.
- the center of gravity T s of the envelope curve 6 of the ultrasonic signal A0, B0 is used as a characteristic variable which is set in relation to the detected reception time to.
- the temporal focus of the envelope 6 can be determined, for example, from the following relationship:
- k is a running index, which is the number of positive half-waves of the ultrasound signal after the
- Threshold value SW describes.
- a (k) is the amplitude of the kth half-wave after the threshold value has been exceeded (trigger time).
- a (k) Since a higher amplitude A (k) also results in a larger high time of the first comparator 10, A (k) can be replaced by the high time of the signal Ki in a rough but sufficiently good approximation.
- the first sum of the aforementioned equation can be implemented without arithmetic functions, for example by means of a counter, the clock input of which is enabled by the high level of the pulse-width-modulated comparator output signal Ki.
- the multiplication by the running index k can be achieved without arithmetic, by increasing or decreasing the clock frequency of the counter every half wave.
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- Electromagnetism (AREA)
- Fluid Mechanics (AREA)
- General Physics & Mathematics (AREA)
- Measuring Volume Flow (AREA)
Abstract
The invention relates to an ultrasound flow sensor, comprising at least one ultrasound converter (A,B) for the transmission and receiving of ultrasound signals (A0,B0) and a receiver unit (4) arranged on the ultrasound converter (A,B) which detects a zero transition (N) of the ultrasound signal (A0,B0) as reception time, after the ultrasound signal (A0,B0) has exceeded a given threshold value (SW). The measurement accuracy of the sensor can be significantly improved, if the receiver unit (4) detects the time of a parameter characterizing the ultrasound signal (A0,B0) and records the relative time shift (deltat) of the characteristic parameter (Ampmax,Ts) as the zero transition (N0 or N1) detected as reception time (to).
Description
Beschreibungdescription
Bestimmung des EmpfangsZeitpunkts eines Ultraschallsignals mittels PulsformerfassungDetermination of the reception time of an ultrasound signal by means of pulse shape detection
Die Erfindung betrifft einen Ultraschall-Strömungssensor gemäß dem Oberbegriff des Patentanspruchs 1, sowie ein Verfahren zur Bestimmung des EmpfangsZeitpunkts eines Ultraschallsignals gemäß dem Oberbegriff des Patentanspruchs 7.The invention relates to an ultrasonic flow sensor according to the preamble of patent claim 1 and a method for determining the time of reception of an ultrasonic signal according to the preamble of patent claim 7.
Ultraschall-Strömungssensoren dienen insbesondere dazu, den Volumen- oder Massestrom oder die Strömungsgeschwindigkeit eines gasförmigen oder flüssigen Mediums zu messen, das durch eine Rohrleitung strömt. Ein bekannter Typ von Ultraschall- StrömungsSensoren umfasst zwei in Strömungsrichtung versetzt angeordnete Ultraschallwandler, die jeweils Ultraschallsignale erzeugen und diese an den jeweils anderen Ultraschallwandler aussenden. Die Ultraschallsignale werden vom jeweils anderen Wandler empfangen und mittels einer Elektronik ausgewertet. Der Laufzeitunterschied zwischen dem Signal in Strömungsrichtung und dem Signal in Gegenrichtung ist dabei ein Maß für die Strömungsgeschwindigkeit des Fluids . Daraus kann die gewünschte Messgröße, wie z.B. ein Volumen- oder Massestrom, berechnet werden.Ultrasonic flow sensors are used in particular to measure the volume or mass flow or the flow rate of a gaseous or liquid medium flowing through a pipeline. A known type of ultrasound flow sensor comprises two ultrasound transducers arranged offset in the flow direction, each of which generates ultrasound signals and emits them to the other ultrasound transducer. The ultrasonic signals are received by the other transducer and evaluated using electronics. The transit time difference between the signal in the flow direction and the signal in the opposite direction is a measure of the flow velocity of the fluid. The desired measurement variable, e.g. a volume or mass flow can be calculated.
Fig. 1 zeigt eine typische Anordnung eines Ultraschall- Strömungssensors mit zwei Ultraschallwandlern A,B, die innerhalb einer Rohrleitung 3 angeordnet sind und sich in einem Abstand L gegenüberstehen. In der Rohrleitung 3 strömt ein Fluid 1 mit einer Geschwindigkeit v in Richtung des Pfeils 2. Die Messtrecke L ist gegenüber derFig. 1 shows a typical arrangement of an ultrasonic flow sensor with two ultrasonic transducers A, B, which are arranged within a pipe 3 and face each other at a distance L. A fluid 1 flows in the pipeline 3 at a speed v in the direction of the arrow 2. The measuring section L is opposite to the
Strömungsrichtung 2 um eine Winkel CC geneigt. Während einer
Messung senden sich die Ultraschallwandler A,B gegenseitig Ultraschallsignale zu, die je nach Richtung von der Strömung entweder verlangsamt oder beschleunigt werden. Die Laufzeiten der Schallsignale sind dabei ein Maß für die zu bestimmende Strömungsgeschwindigkeit .Flow direction 2 inclined by an angle CC. During one Measurement, the ultrasonic transducers A, B send each other ultrasonic signals that are either slowed or accelerated by the flow, depending on the direction. The transit times of the sound signals are a measure of the flow velocity to be determined.
Fig. 2 zeigt eine stark vereinfachte schematische Darstellung einer Wandleranordnung mit einer daran angeschlossenen Steuer- und Auswerteelektronik 4. Der Strömungssensor kann z.B. nach dem sogenannten "sing-around"-Verfahren arbeiten. Dabei wird durch den Empfang eines Ultraschallsignals AO bzw. B0 an einem der Wandler A,B unmittelbar ein Ultraschallsignal in Gegenrichtung ausgelöst.Fig. 2 shows a highly simplified schematic representation of a transducer arrangement with an associated control and evaluation electronics 4. The flow sensor can e.g. work according to the so-called "sing-around" process. The reception of an ultrasonic signal AO or B0 at one of the transducers A, B triggers an ultrasonic signal in the opposite direction.
Für die LaufZeitmessung eines Ultraschallsignals AO bzw. B0 ist es von wesentlicher Bedeutung, dass der EmpfangsZeitpunkt des Ultraschallsignals A0,B0 eindeutig und genau bestimmt wird. Ein aus dem Stand der Technik bekanntes Verfahren zur Bestimmung eines EmpfangsZeitpunkts wird im Folgenden anhand von Fig. 3 erläutert.For the transit time measurement of an ultrasound signal AO or B0, it is essential that the reception time of the ultrasound signal A0, B0 is clearly and precisely determined. A method known from the prior art for determining a reception time is explained below with reference to FIG. 3.
Fig. 3 zeigt den Signalverlauf eines einzelnen Ultraschallsignals AO bzw. B0. Der "EmpfangsZeitpunkt" des Signals A0,B0 ist hier als der erste Nulldurchgang No des Signals definiert, nachdem die Signalamplitude Amp einen vorgegebenen Schwellenwert SW (den sogenannten Pretrigger3 shows the signal curve of an individual ultrasonic signal AO or B0. The "reception time" of the signal A0, B0 is defined here as the first zero crossing No of the signal after the signal amplitude Amp has a predetermined threshold value SW (the so-called pretrigger
Level) überschritten hat. In dem dargestellten Beispiel wäre somit der Zeitpunkt to der Empfangszeitpunkt des Signals. (Der EmpfangsZeitpunkt des Signals könnte alternativ auch anders, z.B. durch Auswertung der Phase des Signals bestimmt werden.)Level) has exceeded. In the example shown, the time to would be the time of reception of the signal. (Alternatively, the reception time of the signal could also be determined differently, e.g. by evaluating the phase of the signal.)
Verschmutzungen, Driften oder Alterung der Ultraschallwandler, oder Turbulenzen im strömenden Fluid können dazu führen, dass die Amplitude der Ultraschallsignale A0,B0 stark variiert. Solange die Signalamplitude sich nicht zu stark ändert, wird die Nulldurchgangsdetektion kaum
beeinträchtigt, da immer der gleiche Nulldurchgang (bezogen auf das gesamte Signal) als EmpfangsZeitpunkt detektiert wird und die Frequenz des Signals im wesentlichen gleich bleibt. Sobald die Amplitude der vor dem Zeitpunkt to liegenden Halbwelle jedoch den Schwellenwert SW unterschreitet, kann es zu Fehlmessungen des Empfangszeitpunkts kommen, da dasContamination, drifting or aging of the ultrasonic transducers, or turbulence in the flowing fluid can lead to the amplitude of the ultrasonic signals A0, B0 varying greatly. As long as the signal amplitude does not change too much, the zero crossing detection is hardly impaired, since the same zero crossing (based on the entire signal) is always detected as the reception time and the frequency of the signal remains essentially the same. As soon as the amplitude of the half-wave lying before the time to falls below the threshold value SW, incorrect measurements of the time of reception can occur, since the
Ultraschallsignal den Schwellenwert SW dann zu einem späteren Zeitpunkt überschreitet und somit ein falscher Nulldurchgang als EmpfangsZeitpunkt detektiert wird.The ultrasound signal then exceeds the threshold value SW at a later point in time and thus an incorrect zero crossing is detected as the reception time.
Fig. 4 zeigt den Signalverlauf des Ultraschallsignals A0,B0 bzw. Wandler-Ausgangssignals 5 mit verminderter Amplitude Amp. Dieses Signal übersteigt den festen Schwellenwert SW erst zu einem späteren Zeitpunkt. Die Empfangseinheit 4 ermittelt in diesem Fall den Nulldurchgang Ni und damit einen falschen Nulldurchgang N als EmpfangsZeitpunkt to des Ultraschallsignals A0,B0. Die LaufZeitmessung des Ultraschallsignals A0,B0 verschiebt sich somit um ganzzahlige Vielfache von +-l/f bzw. +-1/ (2f) (f=Ultraschallfrequenz) , wodurch die Messgenauigkeit stark beeinträchtigt wird. Durch starkes Anwachsen der Amplitude Amp des Ultraschallsignals A0,B0 bzw. des entsprechenden Wandler-Ausgangsignals 5 kann sich der detektierte Empfangszeitpunkt to auch in Richtung früherer Nulldurchgänge N verschieben (nicht gezeigt) .4 shows the signal curve of the ultrasonic signal A0, B0 or converter output signal 5 with a reduced amplitude Amp. This signal only exceeds the fixed threshold value SW at a later point in time. In this case, the receiving unit 4 determines the zero crossing Ni and thus an incorrect zero crossing N as the reception time t o of the ultrasonic signal A0, B0. The transit time measurement of the ultrasound signal A0, B0 thus shifts by integral multiples of + -l / f or + -1 / (2f) (f = ultrasound frequency), which greatly impairs the measurement accuracy. Due to a strong increase in the amplitude Amp of the ultrasonic signal A0, B0 or the corresponding transducer output signal 5, the detected reception time to can also shift in the direction of earlier zero crossings N (not shown).
Es ist daher die Aufgabe der vorliegenden Erfindung, dieIt is therefore the object of the present invention that
Messgenauigkeit eines Ultraschall-Strömungssensors bei stark schwankender Signalamplitude des Ultraschallsignals zu verbessern.To improve the measurement accuracy of an ultrasonic flow sensor in the case of a strongly fluctuating signal amplitude of the ultrasonic signal.
Gelöst wird diese Aufgabe gemäß der Erfindung durch die im Patentanspruch 1 sowie im Patentanspruch 7 angegebenen Merkmale. Weitere Ausgestaltungen der Erfindung sind Gegenstand von Unteransprüchen.This object is achieved according to the invention by the features specified in claim 1 and in claim 7. Further embodiments of the invention are the subject of dependent claims.
Ein wesentlicher Aspekt der Erfindung besteht darin, den Zeitpunkt einer die Form des Ultraschallsignals
kennzeichnenden Größe (z.B. den Zeitpunkt der maximalenAn essential aspect of the invention is the point in time of the form of the ultrasound signal characteristic size (eg the time of the maximum
Amplitude oder des Signalschwerpunkts oder des Schwerpunkts der Hüllkurve) als Referenzzeitpunkt, einen Empfangszeitpunkt (z.B. einen Nulldurchgang), sowie die relative zeitliche Verschiebung des Referenzzeitpunkts zum EmpfangsZeitpunkt zu ermitteln. Die zeitliche Verschiebung zwischen dem Referenzzeitpunkt und dem Empfangsereignis bleibt unverändert, so lange der Schwellenwert zwischen denselben beiden Amplituden des Ultraschallsignals liegt. Ändert sich die Amplitude des Ultraschallsignals bzw. des zugehörigen Wandler-Ausgangssignals so stark, dass der Schwellenwert zwischen zwei anderen Amplituden des Signals liegt, ändert sich die Zeitdifferenz zwischen der kennzeichnenden Größe und dem detektierten Empfangsereignis sprungartig. Dies kann von der Empfangseinheit des Ultraschall-Strömungssensors erkannt und der EmpfangsZeitpunkt entsprechend korrigiert werden.To determine the amplitude or the signal center of gravity or the center of gravity of the envelope) as the reference time, a reception time (e.g. a zero crossing), and the relative time shift of the reference time to the reception time. The time shift between the reference time and the reception event remains unchanged as long as the threshold lies between the same two amplitudes of the ultrasound signal. If the amplitude of the ultrasound signal or the associated transducer output signal changes so strongly that the threshold lies between two other amplitudes of the signal, the time difference between the characteristic quantity and the detected reception event changes suddenly. This can be recognized by the receiving unit of the ultrasonic flow sensor and the time of reception can be corrected accordingly.
Die kennzeichnende Größe ist vorzugsweise eine Größe, die von der Signalamplitude unabhängig ist, wie z.B. der Zeitpunkt der maximalen Amplitude, des Signalschwerpunkts oder des Schwerpunkts der Hüllkurve.The characteristic quantity is preferably a quantity which is independent of the signal amplitude, e.g. the time of the maximum amplitude, the signal center of gravity or the center of gravity of the envelope.
Gemäß einer bevorzugten Ausführungsform der Erfindung bestimmt der Zeitpunkt des Schwerpunkts der Hüllkurve den Referenzzeitpunkt. Der zeitliche Schwerpunkt der Hüllkurve kann z.B. in einer Prozessoreinheit nach folgender Beziehung berechnet werden:According to a preferred embodiment of the invention, the point in time of the center of gravity of the envelope curve determines the reference point in time. The temporal focus of the envelope can e.g. can be calculated in a processor unit according to the following relationship:
T3~ k*A(k)/£ A(k) *=ι *=1T 3 ~ k * A (k) / £ A (k) * = ι * = 1
wobei k ein Laufindex ist, der die Nummer der positiven Halbwellen des Ultraschallsignals nach Überschreiten des Schwellenwertes beschreibt. A(k) ist die Amplitude der k-ten Halbwelle nach dem Überschreiten des Schwellenwerts (Triggerzeitpunkt) .
Nach einer anderen Ausführungsform der Erfindung umfasst die Empfangseinheit eine Einrichtung zur Bestimmung der maximalen Amplitude des Ultraschallsignals. In diesem Fall ist die kennzeichnende Größe die maximale Amplitude des Ultraschallsignals. Die Wahl der maximalen Amplitude des Ultraschallsignals als Referenzzeitpunkt liefert prinzipiell das gleiche Ergebnis wie die Wahl des Schwerpunkts der Hüllkurve, unter der Vorraussetzung, dass sich die Position der maximalen Amplitude relativ zu den anderen Amplituden nicht ändert. Verschiebt sich die Position der maximalen Amplitude jedoch relativ zu den übrigen Amplituden, kann es zu Fehlmessungen kommen, da sich das Zeitintervall zwischen dem detektierten EmpfangsZeitpunkt to und dem ReferenzZeitpunkt um n*2pi verändert.where k is a running index that describes the number of positive half-waves of the ultrasound signal after the threshold value has been exceeded. A (k) is the amplitude of the kth half-wave after the threshold value has been exceeded (trigger time). According to another embodiment of the invention, the receiving unit comprises a device for determining the maximum amplitude of the ultrasound signal. In this case, the characteristic quantity is the maximum amplitude of the ultrasound signal. The choice of the maximum amplitude of the ultrasound signal as the reference point in time provides the same result as the choice of the center of gravity of the envelope, provided that the position of the maximum amplitude does not change relative to the other amplitudes. However, if the position of the maximum amplitude shifts relative to the other amplitudes, incorrect measurements can occur since the time interval between the detected reception time to and the reference time changes by n * 2pi.
Die Empfangseinheit umfasst vorzugsweise einen Komparator, an dessen Eingang das vom Ultraschallwandler erzeugte Wandler- Ausgangssignal und ein Referenzsignal (z.B. eine Schwellenspannung) anliegt, wobei die Empfangseinheit aus dem Ausgangssignal des Komparators eine Information über den Referenzzeitpunkt (z.B. Zeitpunkt der maximalen Amplitude oder des Schwerpunkts der Hüllkurve) ermittelt.The receiving unit preferably comprises a comparator, at the input of which the transducer output signal generated by the ultrasonic transducer and a reference signal (e.g. a threshold voltage) are present, the receiving unit providing information about the reference time (e.g. time of the maximum amplitude or the center of gravity of the comparator) from the output signal of the comparator Envelope curve).
Das Empfangsereignis ist vorzugsweise ein Nulldurchgang, kann aber auch ein anderes vorgegebenes Kriterium sein.The reception event is preferably a zero crossing, but can also be another predetermined criterion.
Die Empfangseinheit ist vorzugsweise in der Lage, den EmpfangsZeitpunkt in Abhängigkeit von seiner zeitlichen Position zum Referenzzeitpunkt zu korrigieren.The receiving unit is preferably able to correct the reception time depending on its position in time at the reference time.
Die Erfindung wird nachstehend anhand der beigefügten Zeichnungen beispielhaft näher erläutert. Es zeigen:The invention is explained in more detail below by way of example with reference to the accompanying drawings. Show it:
Fig. 1 einen aus dem Stand der Technik bekannten Ultraschall- Strömungssensor mit zwei Ultraschallwandlern;
Fig. 2 einen Ultraschall-Strömungssensor mit zugehöriger Steuer- und Empfangsschaltung;1 shows an ultrasonic flow sensor known from the prior art with two ultrasonic transducers; 2 shows an ultrasonic flow sensor with associated control and reception circuit;
Fig. 3 den Signalverlauf eines einzelnen Ultraschallsignals mit großer Amplitude;3 shows the signal curve of a single ultrasonic signal with a large amplitude;
Fig. 4 den Signalverlauf eines einzelnen Ultraschallsignals mit kleiner Amplitude;4 shows the signal curve of an individual ultrasonic signal with a small amplitude;
Fig. 5 eine aus dem Stand der Technik bekannte Schaltung zur Nulldurchgangsdetektion;5 shows a circuit for zero crossing detection known from the prior art;
Fig. 6 einen typischen Verlauf des Signalschwerpunkts in Abhängigkeit vom Verhältnis Schwellenspannung/Signalamplitude; und6 shows a typical course of the signal center of gravity as a function of the ratio of the threshold voltage / signal amplitude; and
Fig. 7 den Verlauf des Schwerpunkts einer Hüllkurve des Ultraschallsignals in Abhängigkeit vom Verhältnis Schwellenspannung/Signalamplitude.7 shows the course of the center of gravity of an envelope curve of the ultrasound signal as a function of the ratio of the threshold voltage / signal amplitude.
Bezüglich der Erläuterung der Fig. 1-4 wird auf die Beschreibungseinleitung verwiesen .With regard to the explanation of FIGS. 1-4, reference is made to the introduction to the description.
Fig. 3 zeigt, wie erwähnt, die Bestimmung des3 shows, as mentioned, the determination of the
EmpfangsZeitpunkts to eines Ultraschallsignals A0,B0 mittels Nulldurchgangsdetektion. Dabei wird der erste Nulldurchgang No des Signals A0 bzw. B0, nachdem das Signal A0,B0 einen vorgegebenen Schwellenwert SW überschritten hat, als EmpfangsZeitpunkt to detektiert. (Wahlweise könnte auch ein anderes Ereignis, z.B. das Überschreiten eines Schwellenwerts als Empfangsereignis definiert werden.)Receiving time to an ultrasonic signal A0, B0 by means of zero crossing detection. The first zero crossing No of the signal A0 or B0, after the signal A0, B0 has exceeded a predetermined threshold value SW, is detected as the reception time to. (Alternatively, another event, e.g. exceeding a threshold value, could also be defined as a reception event.)
Die Empfangseinheit 4 (Fig. 2) ermittelt ferner den Zeitpunkt to der maximalen Signalamplitude Ampmax und die Zeitdifferenz Δt zwischen dem EmpfangsZeitpunkt to und dem Zeitpunkt ti. (Wahlweise kann auch der Zeitpunkt einer anderen
kennzeichnenden Größe, z.B. der Zeitpunkt des Schwerpunkts der Hüllkurve 6 als Referenzzeitpunkt ti ermittelt werden.)The receiving unit 4 (FIG. 2) also determines the time to of the maximum signal amplitude Amp max and the time difference Δt between the reception time to and the time ti. (You can also choose the time of another characteristic quantity, for example the time of the center of gravity of the envelope curve 6 can be determined as the reference time ti.)
Bei einer starken Änderung der Signalamplitude Amp des Ultraschallsignals (siehe Fig. 4) wird der falsche Nulldurchgang (hier Ni) als EmpfangsZeitpunkt t0 detektiert. Die Zeitdifferenz Δt ändert sich dadurch sprungartig um ganzzahlige Vielfache von 1/f oder 1/ (2f) , wobei f die Ultraschallfrequenz ist. Dies wird von der Empfangseinheit 4 erkannt und der EmpfangsZeitpunkt to entsprechend korrigiert.In the event of a strong change in the signal amplitude Amp of the ultrasound signal (see FIG. 4), the incorrect zero crossing (here Ni) is detected as the reception time t 0 . As a result, the time difference Δt changes abruptly by integral multiples of 1 / f or 1 / (2f), where f is the ultrasound frequency. This is recognized by the reception unit 4 and the reception time to is corrected accordingly.
Fig. 5 zeigt eine bekannte Logikschaltung zur Nulldurchgangsdetektion, mit der der EmpfangsZeitpunkt to bestimmt werden kann. Die Schaltung umfasst einen ersten Komparator 10, an dessen Eingang (-) das Ultraschallsignal US bzw. das entsprechende Wandler-Ausgangssignal 5 anliegt, und an dessen anderem Eingang (+) eine Schwellenspannung Usw als Referenz zugeführt wird. Der Ausgang des Komparators 10 geht immer dann in den Zustand "high", wenn die Amplitude des Ultraschallsignals A0,B0 die Referenzspannung Usw überschreitet. Aus der Dauer der High-Phasen kann derFIG. 5 shows a known logic circuit for zero crossing detection, with which the reception time to can be determined. The circuit comprises a first comparator 10, at whose input (-) the ultrasound signal US or the corresponding converter output signal 5 is present, and at whose other input (+) a threshold voltage U sw is supplied as a reference. The output of the comparator 10 always goes into the "high" state when the amplitude of the ultrasonic signal A0, B0 exceeds the reference voltage U sw . From the duration of the high phases, the
Zeitpunkt der maximalen Amplitude Ampmax bestimmt werden.Time of the maximum amplitude Amp max can be determined.
Der zweite Komparator 11 von Fig. 5 dient zur Nulldurchgangsdetektion. Der zweite Komparator 11 erhält hierzu an seinem positiven Eingang (+) das Ultraschallsignal US und an seinem negativen Eingang (-) eine entsprechende Referenzspannung (hier 0V) . Das Ausgangssignal Kι,K2 der Komparatoren 10,11 ist in Fig. 6 dargestellt.The second comparator 11 of FIG. 5 is used for zero crossing detection. For this purpose, the second comparator 11 receives the ultrasound signal US at its positive input (+) and a corresponding reference voltage (here 0V) at its negative input (-). The output signal K 1, K 2 of the comparators 10, 11 is shown in FIG. 6.
Fig. 6 zeigt das pulsweitenmodulierte Ausgangssignal Ki des ersten Komparators 10. Die einzelnen High-Phasen des Signals Ki können z.B. in verschiedenen Zählern gespeichert und ausgewertet werden. Die längste High-Phase indiziert dabei die maximale Amplitude Ampmax des Ultraschallsignals A0 bzw. B0.
Das Komparator-Ausgangssignal könnte analog oder digital weiterverarbeitet oder arithmetisch bewertet werden. So könnte z.B. eine Kreuzkorrelation verschiedener Ausgangssignale Ki durchgeführt werden.6 shows the pulse-width-modulated output signal Ki of the first comparator 10. The individual high phases of the signal Ki can be stored and evaluated, for example, in different counters. The longest high phase indicates the maximum amplitude Ampmax of the ultrasonic signal A0 or B0. The comparator output signal could be processed further analog or digital or evaluated arithmetically. For example, a cross-correlation of different output signals Ki could be carried out.
Gemäß einer bevorzugten Ausführungsform der Erfindung wird der Schwerpunkt Ts der Hüllkurve 6 des Ultraschallsignals A0,B0 als charakteristische Größe herangezogen, die in Relation zum detektierten EmpfangsZeitpunkt to gesetzt wird. Der zeitliche Schwerpunkt der Hüllkurve 6 kann beispielsweise aus folgender Beziehung ermittelt werden:According to a preferred embodiment of the invention, the center of gravity T s of the envelope curve 6 of the ultrasonic signal A0, B0 is used as a characteristic variable which is set in relation to the detected reception time to. The temporal focus of the envelope 6 can be determined, for example, from the following relationship:
Ts~ k*A<k)/£ A(k),T s ~ k * A <k) / £ A (k),
wobei k ein Laufindex ist, der die Nummer der positiven Halbwellen des Ultraschallsignals nach Überschreiten deswhere k is a running index, which is the number of positive half-waves of the ultrasound signal after the
Schwellenwertes SW beschreibt. A(k) ist dabei die Amplitude der k-ten Halbwelle nach dem Überschreiten des Schwellenwerts (Triggerzeitpunkt) .Threshold value SW describes. A (k) is the amplitude of the kth half-wave after the threshold value has been exceeded (trigger time).
Fig. 7 zeigt den Verlauf des Signalschwerpunkts Ts in7 shows the course of the signal center of gravity T s in
Abhängigkeit vom Verhältnis der Schwellenspannung USW zur Signalamplitude Amp. Immer dann, wenn sich die Amplitude Amp des Ultraschallsignals A0,B0 so stark ändert, dass der Schwellenwert USW eine Signalperiode früher oder später überschritten wird, hat das Signal Ts einen Sprung.Dependence on the ratio of the threshold voltage USW to the signal amplitude Amp. Whenever the amplitude Amp of the ultrasonic signal A0, B0 changes so much that the threshold value USW is exceeded one signal period sooner or later, the signal T s has a jump.
Da eine höhere Amplitude A(k) auch eine größere High-Zeit des ersten Komparators 10 nach sich zieht, kann A(k) in einer groben, aber ausreichend guten Nährung durch die High-Zeit des Signals Ki ersetzt werden. Die erste Summe der vorstehend genannten Gleichung kann ohne arithmetische Funktionen z.B. mittels eines Zählers realisiert werden, dessen Takteingang vom High-Pegel des pulsweitenmodulierten Komparator- Ausgangssignals Ki freigeschaltet wird. Die Multiplikation mit dem Laufindex k kann ohne Arithmetik erreicht werden,
indem die Taktfrequenz des Zählers bei jeder Halbwelle entsprechend erhöht oder erniedrigt wird.
Since a higher amplitude A (k) also results in a larger high time of the first comparator 10, A (k) can be replaced by the high time of the signal Ki in a rough but sufficiently good approximation. The first sum of the aforementioned equation can be implemented without arithmetic functions, for example by means of a counter, the clock input of which is enabled by the high level of the pulse-width-modulated comparator output signal Ki. The multiplication by the running index k can be achieved without arithmetic, by increasing or decreasing the clock frequency of the counter every half wave.
BezugszeichenlisteLIST OF REFERENCE NUMBERS
1 Fluid1 fluid
2 Strömungsrichtung2 flow direction
3 Rohrleitung3 pipeline
4 Steuer- und Auswerteeinheit 5 Wandler-Ausgangssignal4 control and evaluation unit 5 converter output signal
6 Hüllkurve6 envelope
10 erster Komparator10 first comparator
11 zweiter Komparator11 second comparator
12 Monoflop 13 Verarbeitungseinheit12 Monoflop 13 processing unit
14 UND-Gatter14 AND gates
Ki Komparator-AusgangssignalKi comparator output signal
K2 Komparator-AusgangssignalK 2 comparator output signal
SW Schwellenwert A,B UltraschallwandlerSW threshold A, B ultrasonic transducer
A0,BÖ UltraschallsignaleA0, BÖ ultrasonic signals
Ampmax maximale Amplitude to EmpfangsZeitpunktAmp max maximum amplitude to receive time
Δt Zeitverschiebung USW SchwellenspannungΔt time shift USW threshold voltage
US UltraschallsignaleingangUS ultrasonic signal input
Ts Schwerpunkt der Hüllkurve
T s center of gravity of the envelope
Claims
1. Ultraschall-Strömungssensor, umfassend1. Ultrasonic flow sensor, comprising
- wenigstens einen Ultraschallwandler (A,B) zum Aussenden und Empfangen von Ultraschallsignalen (A0,B0), und eine am Ultraschallwandler (A,B) angeschlossene Empfangseinheit (4) , die ein vorgegebenes Ereignis (N) des Ultraschallsignals (A0,B0) als EmpfangsZeitpunkt (to) detektiert, dadurch gekennzeichnet, dass die Empfangseinheit (4) derart realisiert ist, dass sie den Zeitpunkt (ti) einer das Ultraschallsignal (A0,B0) kennzeichnenden Größe (Ampmax,Ts), sowie die zeitliche Verschiebung (Δt) des Zeitpunkts (ti) zum- At least one ultrasound transducer (A, B) for transmitting and receiving ultrasound signals (A0, B0), and a receiving unit (4) connected to the ultrasound transducer (A, B) which detects a predetermined event (N) of the ultrasound signal (A0, B0) detected as the reception time (to), characterized in that the reception unit (4) is implemented in such a way that it records the time (ti) of a variable (Amp max , T s ) characterizing the ultrasound signal (A0, B0), as well as the time shift ( Δt) of the time (ti) at
EmpfangsZeitpunkt (to) ermittelt.Received time (to) determined.
2. Ultraschall-Strömungssensor nach Anspruch 1, dadurch gekennzeichnet, dass die Empfangseinheit (4) eine maximale Amplitude (Ampmax) des Ultraschallsignals (A0,B0) als kennzeichnende Größe ermittelt.2. Ultrasonic flow sensor according to claim 1, characterized in that the receiving unit (4) determines a maximum amplitude (Amp max ) of the ultrasonic signal (A0, B0) as a characteristic variable.
3. Ultraschall-Strömungssensor nach Anspruch 1, dadurch gekennzeichnet, dass die Empfangseinheit (4) die zeitliche Lage (Ts) des Schwerpunkts des Ultraschallsignals (A0,B0) oder seiner Hüllkurve (6) als kennzeichnende Größe bestimmt.3. Ultrasonic flow sensor according to claim 1, characterized in that the receiving unit (4) determines the temporal position (T s ) of the center of gravity of the ultrasonic signal (A0, B0) or its envelope (6) as a characteristic variable.
4. Ultraschall-Strömungssensor nach einem der vorhergehenden Ansprüche, dadurch gekennzeichnet, dass die Empfangseinheit4. Ultrasonic flow sensor according to one of the preceding claims, characterized in that the receiving unit
(4) einen Komparator (10) umfasst, an dessen Eingang ein Wandler-Ausgangssignal (5) und ein Referenzsignal (SW) anliegt, und dass die Empfangseinheit (4) aus dem Ausgangssignal des Komparators (10) eine Information über den Zeitpunkt (ti) der kennzeichnenden Größe (Ampmax,Ts) ermittelt. (4) comprises a comparator (10), at the input of which a converter output signal (5) and a reference signal (SW) are present, and that the receiving unit (4) from the output signal of the comparator (10) provides information about the time (ti ) of the characteristic size (Amp max , T s ).
5. Ultraschall-Strömungssensor nach Anspruch 4, dadurch gekennzeichnet, dass das am Komparator (10) anliegende Referenzsignal ein Schwellenwert (SW) ungleich Null ist und das Ausgangssignal des Komparators (10) ein pulsweiten- moduliertes Signal (Kl) ist, aus dem der Zeitpunkt (ti) der kennzeichnenden Größe (Ampmax,Ts) ermittelt wird.5. Ultrasonic flow sensor according to claim 4, characterized in that the reference signal applied to the comparator (10) is a threshold value (SW) not equal to zero and the output signal of the comparator (10) is a pulse width modulated signal (Kl) from which the Time (ti) of the characteristic quantity (Amp max , T s ) is determined.
6. Ultraschall-Strömungssensor nach einem der vorhergehenden Ansprüche, dadurch gekennzeichnet, dass der Empfangszeitpunkt (to) in Abhängigkeit von der zeitlichen Verschiebung (Δt) korrigiert wird.6. Ultrasonic flow sensor according to one of the preceding claims, characterized in that the time of reception (to) is corrected as a function of the time shift (Δt).
7. Verfahren zur Detektion eines Ultraschallsignals (A0,B0) an einem Ultraschallwandler (A,B) mittels einer Empfangseinheit (4), die ein vorgegebenes Ereignis (N) des Ultraschallsignals (A0,B0) als Empfangszeitpunkt (to) detektiert, dadurch gekennzeichnet, dass die Empfangseinheit (4) den Zeitpunkt (ti) einer das Ultraschallsignal (A0,B0) kennzeichnenden Größe (Ampmax,Ts), sowie die zeitliche Verschiebung (Δt) des Zeitpunkts (ti) zum EmpfangsZeitpunkt (t0) ermittelt.7. A method for detecting an ultrasonic signal (A0, B0) on an ultrasonic transducer (A, B) by means of a receiving unit (4), which detects a predetermined event (N) of the ultrasonic signal (A0, B0) as the time of reception (to), characterized that the receiving unit (4) determines the point in time (ti) of a quantity (Amp max , T s ) characterizing the ultrasonic signal (A0, B0) and the time shift (Δt) of the point in time (ti) to the point in time of reception (t 0 ).
8. Verfahren nach Anspruch 7, dadurch gekennzeichnet, dass die Empfangseinheit (4) eine maximale Amplitude (Ampmax) des Ultraschallsignals (A0,B0) als kennzeichnende Größe ermittelt.8. The method according to claim 7, characterized in that the receiving unit (4) determines a maximum amplitude (Ampmax) of the ultrasonic signal (A0, B0) as a characteristic variable.
9. Verfahren nach Anspruch 7, dadurch gekennzeichnet, dass die Empfangseinheit (4) die zeitliche Lage des Schwerpunkts des Ultraschallsignals (A0,B0) oder seiner Hüllkurve (6) als kennzeichnende Größe bestimmt. 9. The method according to claim 7, characterized in that the receiving unit (4) determines the temporal position of the center of gravity of the ultrasonic signal (A0, B0) or its envelope (6) as a characteristic variable.
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
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DE102004025243A DE102004025243A1 (en) | 2004-05-22 | 2004-05-22 | Determining the time of reception of an ultrasound signal by means of pulse shape detection |
PCT/EP2005/051761 WO2005114112A2 (en) | 2004-05-22 | 2005-04-21 | Determination of the reception time for an ultrasound signal by means of pulse shape detection |
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EP1754025A2 true EP1754025A2 (en) | 2007-02-21 |
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US (1) | US8744785B2 (en) |
EP (1) | EP1754025A2 (en) |
JP (1) | JP4976287B2 (en) |
DE (1) | DE102004025243A1 (en) |
WO (1) | WO2005114112A2 (en) |
Cited By (2)
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CN110799810A (en) * | 2017-06-27 | 2020-02-14 | 萨基姆通讯能源及电信联合股份公司 | Method for measuring fluid velocity |
CN111157066A (en) * | 2019-12-31 | 2020-05-15 | 浙江大学 | Gas ultrasonic flowmeter transit time calculation method based on first envelope contact ratio |
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JP4904098B2 (en) * | 2006-07-05 | 2012-03-28 | Jfeアドバンテック株式会社 | Physical quantity measuring device and ultrasonic flow measuring device |
DE102008019991B4 (en) * | 2008-04-21 | 2015-10-22 | Mib Gmbh Messtechnik Und Industrieberatung | Concentration determination method and measuring device |
EP2182349A1 (en) * | 2008-10-28 | 2010-05-05 | Axsensor AB | Method for determining the starting instant of a periodically oscillating signal response |
DE202011005427U1 (en) * | 2011-04-19 | 2012-07-20 | Acam-Messelectronic Gmbh | Apparatus for measuring the transit time of an ultrasonic signal in a flowing liquid |
JP6101020B2 (en) * | 2012-08-29 | 2017-03-22 | 日立オートモティブシステムズメジャメント株式会社 | Ultrasonic flow meter |
CN102967334B (en) * | 2012-09-26 | 2015-08-26 | 朱作行 | Utilize system and method signal envelope process being measured to fluid flow |
CN108548578B (en) * | 2018-03-29 | 2020-01-03 | 中国计量大学 | Ultrasonic echo signal characteristic peak identification method based on self-adaptive threshold |
JP7298186B2 (en) * | 2019-02-26 | 2023-06-27 | セイコーエプソン株式会社 | Ultrasonic measuring device and ultrasonic measuring method |
CN112833999B (en) * | 2021-03-04 | 2024-08-02 | 宁波水表(集团)股份有限公司 | Quick meter calibrating method for ultrasonic water meter |
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CN111157066B (en) * | 2019-12-31 | 2020-11-20 | 浙江大学 | Gas ultrasonic flowmeter transit time calculation method based on first envelope contact ratio |
Also Published As
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JP4976287B2 (en) | 2012-07-18 |
WO2005114112A3 (en) | 2006-04-13 |
US20070186680A1 (en) | 2007-08-16 |
US8744785B2 (en) | 2014-06-03 |
JP2007538240A (en) | 2007-12-27 |
DE102004025243A1 (en) | 2005-12-08 |
WO2005114112A2 (en) | 2005-12-01 |
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