Beam shaping acoustic signal travel time flow meter

Abstract

A method and corresponding device are provided for determining a flow speed in a fluid conduit. The fluid conduit is provided with first, second and third ultrasonic wet transducers, wherein respective connection lines between transducers extend outside of a direction of average flow of the fluid conduit. First and second measuring signals are applied to the first ultrasonic wet transducer and received at the second and the third ultrasonic wet transducer, respectively. The measuring signals comprise a respective reversed signal portion with respect to time of a response signal. Respective first and second response signals are measured and the flow speed is derived from at least one of the first and second response signals.

Claims

1. A method for determining a flow speed of a fluid in a fluid conduit comprising: providing the fluid conduit with a fluid that has a predetermined velocity with respect to the fluid conduit, providing the fluid conduit with a first ultrasonic wet transducer, a second ultrasonic wet transducer and a third ultrasonic wet transducer, wherein respective connection lines between the first ultrasonic wet transducer, the second ultrasonic wet transducer and the third ultrasonic wet transducer extend outside of a direction of average flow within the fluid conduit, applying a first measuring signal to the first ultrasonic wet transducer, and measuring a first response signal of the first measuring signal at the second ultrasonic wet transducer, applying a second measuring signal to the first ultrasonic wet transducer, measuring a second response signal of the second measuring signal at the third ultrasonic wet transducer, wherein the first measuring signal and the second measuring signal respectively comprise a reversed signal portion with respect to time of a response signal of a corresponding impulse signal or of a signal derived therefrom, deriving a flow speed of the fluid from at least one of the first response signal and the second response signal.

2. The method according to claim 1, comprising: applying a first reverse direction measuring signal to the second ultrasonic wet transducer, and measuring a first reverse direction response signal of the first reverse direction measuring signal at the first ultrasonic wet transducer, applying a second reverse direction measuring signal to the third ultrasonic wet transducer, measuring a second reverse direction response signal of the second reverse direction measuring signal at the first ultrasonic wet transducer, wherein the first reverse direction measuring signal and the second reverse direction measuring signal respectively comprise a reversed signal portion with respect to time of a response signal of a corresponding impulse signal or of a signal derived therefrom, deriving a flow speed of the fluid from at least one of the first response signal, the first reverse direction response signal, the second response signal and the second reverse direction response signal.

3. The method according to claim 1, comprising: applying a third measuring signal to the second ultrasonic wet transducer, measuring a third response signal of the second measuring signal at the third ultrasonic wet transducer, wherein the third measuring signal comprises a reversed signal portion with respect to time of a response signal of a corresponding impulse signal or of a signal derived therefrom, deriving at least one flow speed of the fluid from the third response signal.

4. The method according to claim 3, comprising: applying a third reverse direction measuring signal to the third ultrasonic wet transducer, measuring a third reverse direction response signal of the third reverse direction measuring signal at the second ultrasonic wet transducer, wherein the third reverse direction measuring signal comprises a reversed signal portion with respect to time of a response signal of a corresponding impulse signal or of a signal derived therefrom deriving at least one flow speed of the fluid from the third response signal and the third reverse direction response signal.

5. The method according to claim 1, wherein the signal portion that is used to derive the respective measuring signals comprises a first portion around a maximum amplitude of a response signal and a trailing signal portion, the trailing signal portion extending in time behind the arrival time of the maximum amplitude.

6. The method according to claim 1, comprising processing of at least one of the response signals for determining a change in the wall thickness of the conduit or for determining material characteristics of the conduit walls by determining longitudinal and transversal sound wave characteristics.

7. The method according to claim 1, comprising providing the fluid conduit with a fluid, providing a first impulse signal to one of the first or the second ultrasonic wet transducer, receiving a first response signal of the first impulse signal at the other one of the first or the second ultrasonic wet transducer, receiving a second response signal of the second impulse signal at the other one of the first or the third ultrasonic wet transducer, deriving the first measuring signal from the first response signal, deriving the second measuring signal from the second response signal, the derivation of the respective first and second measuring signals comprising selecting a signal portion of the respective first and second response signals or of a signal derived therefrom and reversing the signal portion with respect to time, storing the first measuring signal and the second measuring signal for later use.

8. The method according to claim 7, comprising repeating the steps of applying an impulse signal and receiving a corresponding response signal multiple times, thereby obtaining a plurality of response signals, deriving the respective measuring signal from an average of the received response signals.

9. The method according to claim 7, wherein the derivation of the respective measuring signal comprises digitizing the corresponding response signal or a signal derived therefrom with respect to amplitude.

10. The method according to claim 9, comprising increasing the bit-resolution of the digitized signal for increasing an amplitude of a response signal to the respective measuring signal.

11. The method according to claim 9, comprising decreasing the bit-resolution of the digitized signal for increasing an amplitude of a response signal to the respective measuring signal.

12. The method according to claim 9, wherein the bit resolution of the digitized signal with respect to the amplitude is a low bit resolution.

13. A computer readable program code comprising computer readable instructions for executing the method according to claim 1.

14. A computer readable memory, the computer readable memory comprising the computer readable program code of claim 13.

15. An application specific electronic component, which is operable to execute the method according to claim 1.

16. A method for determining whether a test device is measuring a flow speed of a fluid in a fluid conduit according to the method for determining a flow speed of a fluid in a fluid conduit of claim 1, comprising: providing the fluid conduit with a fluid that has a predetermined velocity with respect to the fluid conduit, providing the fluid conduit with a first testing ultrasonic wet transducer and a second testing ultrasonic wet transducer, applying a test impulse signal to the first testing ultrasonic wet transducer of the test device, receiving a test response signal of the test impulse signal at the second testing ultrasonic wet transducer of the test device, deriving a test measuring signal from the test response signal, the derivation of the test measuring signal comprising reversing the respective first or second response signal, or a portion thereof, with respect to time, comparing the first test measuring signal with a first measuring signal that is emitted at an ultrasonic wet transducer of the test device, wherein it is determined that the test device is using the method to determine a flow speed of a fluid in a fluid conduit, if the first test measuring signal and the first measuring signal are similar.

17. The method according to claim 16, comprising: providing the fluid conduit with a third testing ultrasonic wet transducer, applying a test impulse signal to the first testing ultrasonic wet transducer of the test device or to the second testing ultrasonic wet transducer of the test device, receiving a second test response signal of the test impulse signal at the at the third testing ultrasonic wet transducer of the test device, deriving a second test measuring signal from the second test response signal, comparing the second test measuring signal with a second measuring signal that is emitted at the ultrasonic wet transducer of the test device, wherein it is determined that the test device is using the method for determining a flow speed of a fluid in a fluid conduit if the first test measuring signal and the first measuring signal are similar.

18. The method of claim 16, wherein each of the first testing ultrasonic wet transducer, the second testing ultrasonic wet transducer correspond to one of the first ultrasonic wet transducer, the second ultrasonic wet transducer, and the third ultrasonic wet transducer.

19. A device for measuring a flow speed of a fluid in a conduit with a travel time ultrasonic flow meter, comprising: a first connector for connecting a first ultrasonic wet transducer, a second connector for connecting a second ultrasonic wet transducer, a third connector for connecting a third ultrasonic wet transducer, a transmitting unit for sending impulse signals and for sending measuring signals, a receiving unit for receiving response signals, a processing unit for deriving a first measuring signal from a first inverted signal, for deriving a second measuring signal from a second inverted signal and for storing the first measuring signal and the second measuring signal, wherein the derivation of the first inverted signal and of the second inverted signal comprises reversing a signal portion of a response signal of a corresponding impulse signal or of a signal derived therefrom with respect to time, and wherein the transmitting unit is further operative to apply the first measuring signal to the first connector, and to apply the second measuring signal to the first connector, the receiving unit is further operative to receive a first response signal of the first measuring signal at the second connector, and to receive a second response signal of the second measuring signal at the third connector, and the processing unit is further operative to derive a flow speed of the fluid from at least one of the first response signal and the second response signal.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

(1) The subject matter of the present specification is now explained in further detail with respect to the following Figures, wherein

(2) FIG. 1 shows a first flow meter arrangement with two piezoelectric elements,

(3) FIG. 2 shows the flow meter arrangement of FIG. 1, one direct signal and two scattered signals,

(4) FIG. 3 shows the flow meter arrangement of FIG. 1 when viewed in the direction of flow,

(5) FIG. 4 shows a second flow meter arrangement with four piezoelectric elements and four direct signals,

(6) FIG. 5 shows the flow meter arrangement of FIG. 4 when viewed in the direction of flow,

(7) FIG. 6 shows a schematic diagram of a test signal,

(8) FIG. 7 shows a schematic diagram of a test signal response,

(9) FIG. 8 shows a schematic diagram of an inverted signal,

(10) FIG. 9 shows a schematic diagram of a response from the inverted signal,

(11) FIG. 10 shows a first inverted signal in high resolution,

(12) FIG. 11 shows a response of the inverted signal of FIG. 10,

(13) FIG. 12 shows a further inverted signal in high resolution,

(14) FIG. 13 shows a response of the inverted signal of FIG. 12,

(15) FIG. 14 shows a further inverted signal in high resolution,

(16) FIG. 15 shows a response of the inverted signal of FIG. 14,

(17) FIG. 16 shows a further inverted signal in high resolution,

(18) FIG. 17 shows a response of the inverted signal of FIG. 16,

(19) FIG. 18 shows a further inverted signal in high resolution,

(20) FIG. 19 shows a response of the inverted signal of FIG. 18,

(21) FIG. 20 shows a further inverted signal in high resolution,

(22) FIG. 21 shows a response of the inverted signal of FIG. 20,

(23) FIG. 22 shows a further inverted signal in high resolution,

(24) FIG. 23 shows a response of the inverted signal of FIG. 22,

(25) FIG. 24 shows a further inverted signal in high resolution,

(26) FIG. 25 shows a response of the inverted signal of FIG. 24,

(27) FIG. 26 shows a further inverted signal in high resolution,

(28) FIG. 27 shows a response of the inverted signal of FIG. 26,

(29) FIG. 28 shows a further inverted signal in 12-bit resolution,

(30) FIG. 29 shows a response of the signal of FIG. 28,

(31) FIG. 30 shows a further inverted signal in 3-bit resolution,

(32) FIG. 31 shows a response of the signal of FIG. 30,

(33) FIG. 32 shows a further inverted signal in 2-bit resolution,

(34) FIG. 33 shows a response of the signal of FIG. 32,

(35) FIG. 34 shows a further inverted signal in 1-bit resolution,

(36) FIG. 35 shows a response of the signal of FIG. 34,

(37) FIG. 36 shows a short impulse at a piezoelectric element of the flow meter of FIG. 1,

(38) FIG. 37 shows a signal of a piezoelectric element of the flow meter of FIG. 1, which is derived from the inverted response of the signal of FIG. 36,

(39) FIG. 38 shows a response of the signal of FIG. 37,

(40) FIG. 39 shows an upstream and a downstream cross correlation function,

(41) FIG. 40 shows a sectional enlargement of FIG. 39,

(42) FIG. 41 shows a response signal of an inverted signal for a 12-degree misalignment against an opposite arrangement of piezoelectric elements,

(43) FIG. 42 shows a many-to-one sensor arrangement for a flow measurement according to the present specification,

(44) FIG. 43 shows a one-to-many sensor arrangement for a flow measurement according to the present specification,

(45) FIG. 44 shows a one-to-one sensor arrangement for a flow measurement in a layer according to the present specification,

(46) FIG. 45 shows a multi-sensor arrangement for flow measure-ment in multiple layers according to the present specification,

(47) FIG. 46 shows a device for measuring a flow speed according to the present specification,

(48) FIG. 47 shows a direct digital synthesizer for use in the device of FIG. 46,

(49) FIG. 48 shows a longitudinal cross section of an asymmetric transducer arrangement,

(50) FIG. 49 shows a transverse cross section of the arrangement of FIG. 49,

(51) FIG. 50 shows a one cycle measuring signal of a time of flight measurement,

(52) FIG. 51 shows a ten cycle measuring signal of a time of flight measurement,

(53) FIG. 52 show a measuring signal that is derived from a time reversed signal,

(54) FIG. 53 shows a response signal of the signal of FIG. 50, wherein the transmission channel is provided by the asymmetric arrangement of FIGS. 48 and 49,

(55) FIG. 54 shows a response signal of the signal of FIG. 51 for the arrangement of FIGS. 48 and 49,

(56) FIG. 55 shows a response signal of the Signal of FIG. 52 for the arrangement of FIGS. 48 and 49,

(57) FIG. 56 shows a procedure for obtaining measuring signals corresponding to two signal paths in a three transducer arrangement,

(58) FIG. 57 shows a TOF flow measurement using the measuring signals obtained in the method of FIG. 56,

(59) FIG. 58 shows two different arrangements of two transducers on a conduit,

(60) FIG. 59 shows pressure distributions of measuring signals obtained in the arrangement of FIG. 58, and

(61) FIG. 60 illustrates an example of determining whether a device under test uses the same method of flow measurement as a verification device.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS

(62) In the following description, details are provided to describe the embodiments of the present specification. It shall be apparent to one skilled in the art, however, that the embodiments may be practiced without such details.

(63) Some parts of the embodiments, which are shown in the FIGS., have similar parts. The similar parts have the same names or similar part numbers with a prime symbol or with an alphabetic symbol. The description of such similar parts also applies by reference to other similar parts, where appropriate, thereby reducing repetition of text without limiting the disclosure.

(64) FIG. 1 shows a first flow meter arrangement 10. In the flow meter arrangement, a first piezoelectric element 11 is placed at an outer wall of a pipe 12, which is also referred as a tube 12. A second piezoelectric element 13 is placed at an opposite side of the pipe 12 such that a direct line between the piezoelectric element 11 and the downstream piezoelectric element 13 is oriented at an angle β to the direction 14 of average flow, which is at the same time also the direction of the pipe's 12 symmetry axis. The angle β is chosen to be approximately 45 degrees in the example of FIG. 1 but it may also be steeper, such as for example 60 degrees, or shallower, such as for example 30 degrees.

(65) A piezoelectric element, such as the piezoelectric elements 11, 13 of FIG. 1 may in general be operated as an acoustic transmitter and as an acoustic sensor. An acoustic transmitter and an acoustic sensor may be provided by the same piezoelectric element or by different regions of the same piezoelectric element. In this case, a piezoelectric element or transducer is also referred to as piezoelectric transmitter when it is operated as transmitter or sound source and it is also referred to as acoustic sensor or receiver when it is operated as acoustic sensor.

(66) When a flow direction is as shown in FIG. 1, the first piezoelectric element 11 is also referred to as “upstream” piezoelectric element and the second piezoelectric element 13 is also referred to as “downstream” piezoelectric element. A flow meter according to the present specification works for both directions of flow in essentially the same way and the flow direction of FIG. 1 is only provided by way of example.

(67) FIG. 1 shows a flow of electric signals of FIG. 1 for a configuration in which the upstream piezoelectric element 11 is operated as a piezoelectric transducer and the downstream piezoelectric element 13 is operated as an acoustic sensor. For the purpose of clarity, the application works upstream and downstream, i.e. the position of the piezoelectric elements can be interchanged.

(68) A first computation unit 15 is connected to the upstream piezoelectric element 11 and a second computation unit 16 is connected to the downstream piezoelectric element 13. The first computation unit 15 comprises a first digital signal processor, a first digital analog converter (DAC) and a first analog digital converter (ADC). Likewise, the second computation unit 16 comprises a second digital signal processor, a second digital analog converter (DAC) and a second analog digital converter (ADC). The first computation unit 15 is connected to the second computation unit 16.

(69) The arrangement with two computation units 15, 16 shown in FIG. 1 is only provided by way of example. Other embodiments may have different numbers and arrangements of computation units. For example, there may be only one central computation unit or there may be two AD/DC converters and one central computation unit, or there may be two small-scale computation units at the transducers and one larger central computation unit.

(70) A computation unit or computation units can be provided by microcontrollers or application specific integrated circuits (ASICs), or field programmable gate arrays (FPGAs), for example. Specifically, the synthesis of an electrical signal from a stored digital signal may be provided by a direct digital synthesizer (DDS), which comprises a digital to analog converter (DA, DAC).

(71) A method for generating a measuring signal according to the present specification comprises the following steps.

(72) A pre-determined digital test signal is generated by synthesizing an acoustic signal with the digital signal processor of the first computation unit 15. The digital test signal is sent from the first computation unit 15 to the piezoelectric transducer 11 along signal path 17. The piezoelectric transducer 11 generates a corresponding ultrasound test signal. Units 15 and 16 can also be provided in one single unit.

(73) The test signal is provided as a short pulse, for example by a single 1 MHz oscillation or by 10 such oscillations. In particular, the test signal may be provided by a small number of oscillations with constant amplitude, thereby approximating a rectangular signal. The oscillation or the oscillations may have a sinusoidal shape, a triangular shape, a rectangular shape or also other shapes.

(74) The ultrasound test signal travels through the liquid in the pipe 12 to the piezoelectric sensor 13. In FIG. 1, a direct signal path of the ultrasound signal is indicated by an arrow 18. Likewise, a direct signal path of the ultrasound signal in the reverse direction is indicated by an arrow 19. A response signal is picked up by the piezoelectric sensor 13, sent to the second computation unit 16 along signal path 20, and digitized by the second computation unit 16.

(75) In a further step, a digital measuring signal is derived from the digitized response signal. The derivation of the measurement refers to a reversal of the digitized response signal with respect to time. According to further embodiments, the derivation comprises further steps such as a conversion to a reduced resolution in the amplitude range, a bandwidth filtering of the signal to remove noise, such as low frequency noise and high frequency noise. In particular, the step of bandwidth filtering may be executed before the step of reversing the signal with respect to time.

(76) The signal reversal may be carried out in various ways, for example by reading out a memory area in reverse direction or by reversing the sign of sinus components in a Fourier representation.

(77) In one embodiment, a suitable portion of the digitized response signal is selected that contains the response from the direct signal. The portion of the response signal is then turned around or is inverted with respect to time. In other words, signal portions of the response signal that are received later are sent out earlier in the inverted measuring signal. If a signal is represented by a time ordered sequence of amplitude samples, by way of example, the abovementioned signal inversion amounts to inverting or reversing the order of the amplitude samples.

(78) The resulting signal, in which the direction, or the sign, of time has been inverted, is also referred to as an “inverted signal”. The expression “inverted” in this context refers to an inversion with respect to the direction of time, and not to an inversion with respect to a value, such as the amplitude value.

(79) FIGS. 10 to 19 show, by way of example digital signals according to the present specification.

(80) In a flow meter according to one embodiment of the present specification, the same measuring signal is used for both directions 18, 19, the downstream and the upstream direction, providing a simple and efficient arrangement. According to other embodiments, different measuring signals are used for both directions. In particular, the measuring signal may be applied to the original receiver of the test signal. Such arrangements may provide benefits for asymmetric conditions and pipe shapes.

(81) A method of measuring a flow speed of a liquid through a pipe, which uses the abovementioned-inverted signal as a measuring signal, comprises the following steps.

(82) The abovementioned measuring signal is sent from the first computation unit 15 to the piezoelectric transducer 11 along signal path 17. The piezoelectric transducer 11 generates a corresponding ultrasound-measuring signal. Examples for such a measuring signal are provided in FIGS. 10, 12, 14, 16, 18, 20, 22, 24, 26, 28, 30, 32, 34, 37, and 38.

(83) The ultrasound-measuring signal travels through the liquid in the pipe 12 to the piezoelectric sensor 13. A response signal is picked up by the piezoelectric sensor 13, sent to the second computation unit 16 along signal path 20, and digitized by the second computation unit 16.

(84) The second computation unit 16 sends the digitized response signal to the first computation unit 15. The first computation unit 15 determines a time of flight of the received signal, for example by using one of the methods described further below.

(85) A similar process is carried out for a signal travelling in the reverse direction 19, namely the abovementioned measuring signal is applied to the downstream piezoelectric element 13, and a response signal is measured by the upstream piezoelectric element 11 to obtain an upstream time of flight TOF_up in the reverse direction 19. The first computation unit 15 determines a velocity of flow, for example according to the formula

(86) $v=\frac{c^2}{2.Math.L.Math.\cos \beta }.Math.\left({\mathrm{TOF}}_{\mathrm{up}}-{\mathrm{TOF}}_{\mathrm{down}}\right),$

(87) wherein L is the length of the direct path between the piezoelectric elements 11, 13, β is the angle of inclination of the direct path between the piezoelectric elements 11, 13 and the direction of the average flow, and c is the velocity of sound in the liquid under the given pressure and temperature conditions.

(88) The squared velocity of sound c{circumflex over ( )}2 can be approximated to second order by the expression

(89) $c^2\approx \frac{L^2}{{\mathrm{TOF}}_{\mathrm{up}}*{\mathrm{TOF}}_{\mathrm{down}}}$

(90) which leads to the formula

(91) $v=\frac{L}{2*\cos \beta }.Math.\frac{{\mathrm{TOF}}_{\mathrm{up}}-{\mathrm{TOF}}_{\mathrm{down}}}{{\mathrm{TOF}}_{\mathrm{up}}*{\mathrm{TOF}}_{\mathrm{down}}}$

(92) Thereby, it is not necessary to determine temperature or pressure, which in turn determine the fluid density and the sound velocity, or to measure the sound velocity or the fluid density directly. By contrast, the first order of the error does not cancel out for only one measurement direction.

(93) Instead of using a factor 2.Math.L.Math.cos β, a proportionality constant can be derived from a calibration measurement with a known flow speed. The proportionality constant of the calibration takes into account further effects such as flow profiles and contributions from sound waves that were scattered and did not travel along a straight line.

(94) According to a further embodiment, the process of generating an impulse signal, recording a response signal and deriving an inverted measuring signal from the response signal is simulated in a computer. Relevant parameters, such as the pipe diameter of the pipe 12 and the sensor placements are provided as input parameters to the simulation.

(95) According to yet another embodiment, the measuring signal, which is to be supplied to a transmitting piezoelectric element, is synthesized using a shape of a typical response signal to an impulse signal, such as the signal shapes shown in FIGS. 37 and 38. For example, the measuring signal may be provided by a 1 MHz sinusoidal oscillation, which is amplitude modulated with an envelope according to a Gaussian probability function having a half width of 10 microseconds. The half-width may be chosen as an input parameter, which depends on the actual arrangement, such as the pipe diameter and the sensor placement.

(96) A flow meter according to the present specification may also be provided as a pre-defined flow meter in which the measuring signal is generated during a test run at a factory site, in particular when the flow meter is supplied together with a pipe section.

(97) According to a simple embodiment of the present specification, a time of flight in upstream and in downstream direction is determined by evaluating a time of a peak amplitude of a received signal with respect to a sending time of the measuring signal. To achieve a higher precision, the maximum may be determined using an envelope of the received signal. According to a further embodiment, the measurement is repeated multiple times and an average time of flight is used.

(98) According to a further embodiment of the present specification, the time of flight of a signal is evaluated using a cross-correlation technique. In particular, the respective time shifts can be evaluated by cross correlating the received downstream or upstream signal with the received signal at zero flow speed according to the formula:

(99) $\mathrm{CCorr}\left(\tau \right)=\underset{t=-\infty }{\overset{\infty }{.Math.}}{\mathrm{Sig}}_{\mathrm{Flow}}\left(t\right).Math.{\mathrm{Sig}}_{\mathrm{NoFlow}}\left(t+\tau \right),$

(100) wherein Sig_Flow represents an upstream or downstream signal under measurement conditions, when there is a fluid flow through the pipe, and wherein Sig_NoFlow represents a signal under calibration conditions at zero flow. The infinite sum limits represent a sufficiently large time window [−T1, +T2]. In more general words, −T1 and +T2 do not need to be same and for practical reasons this can be advantageous for the flow meter.

(101) The time shift TOF_up-TOF_down is then obtained by comparing the time of the maximum of the upstream correlation function with the time of the maximum of the downstream correlation function. The envelope of the correlation function may be used to determine the location of the maximum more accurately.

(102) In a further embodiment, a separate evaluation unit is provided between the first computation unit 15 and the second computation unit 16, which performs the calculation of the signal arrival times and the flow speed.

(103) In general, the measured signal of the acoustic sensor results from a superposition of scattered signals and a direct signal. The scattered signals are reflected from the inner and outer walls of the pipe once or multiple times including additional scattering processes within the pipe wall. This is shown, by way of example, in FIG. 2.

(104) The transducer configuration of FIG. 1 is a direct-line or “Z” configuration. Other arrangements, which make use of reflections on an opposite side of the pipe, are possible as well, such as the “V” and the “W” configuration. V and W configuration work based on reflections on the pipe wall, which induce more scatterings than the Z configuration. The subject matter of the application will benefit from these configurations as long as the paths are understood properly.

(105) In a V-configuration, the two transducers are mounted on the same side of the pipe. For recording a 45-degree reflection, they are placed about a pipe diameter apart in the direction of the flow. The W-configuration makes use of three reflections. Similar to the V-configuration, the two transducers are mounted on the same side of the pipe. For recording a signal after two 45-degree reflections, they are placed two pipe diameters apart in the direction of the flow.

(106) FIG. 2 shows, by way of example a first acoustic signal “1”, which travels directly from the piezoelectric element 11 to the piezoelectric element 13 and a third signal 3, which is scattered three times at the periphery of the pipe 12.

(107) For simplicity, the scattering events are shown as reflections in FIGS. 2 to 5 but the actual scattering process can be more complicated. In particular, the most relevant scattering occurs typically in the pipe wall or at material that is mounted in front of the piezoelectric transducers. FIG. 3 shows a view of FIG. 2 in flow direction in the viewing direction A-A.

(108) FIGS. 4 and 5 show a second sensor arrangement in which a further piezoelectric element 22 is positioned at a 90-degree angle to the piezoelectric element 11 and a further piezoelectric element 23 is positioned at a 90-degree angle to the piezoelectric element 13.

(109) Furthermore, FIGS. 4 and 5 show direct or straight line, acoustic signal paths for a situation in which the piezoelectric elements 11, 22 are operated as piezo transducers and the piezoelectric elements 13, 23 are operated as acoustic sensors. Piezoelectric element 23, which is on the back of the pipe 12 in the view of FIG. 4 is shown by a dashed line in FIG. 4.

(110) FIGS. 6 to 9 show, in a simplified way, a method of generating a measuring signal from a response of a test signal. In FIGS. 6 to 9, losses due to scattering are indicated by hatched portions of a signal and by arrows.

(111) For the considerations of FIGS. 6 to 9, it is assumed that the acoustic signal only propagates along a straight line path, along a first scattering channel with a time delay of Δt, and along a second scattering channel with a time delay of 2Δt. Signal attenuation along the paths is not considered.

(112) A test signal in the form of a rectangular spike is applied to the piezoelectric element 11. Due to scattering, a first portion of the signal amplitude is lost due to the first scattering path and appears after a time Δt, and a second portion of the signal amplitude is lost due to the second scattering path and appears after a time 2Δt. This yields a signal according to the white columns in FIG. 7, which is recorded at the piezoelectric element 13.

(113) A signal processor inverts this recorded signal with respect to time and is applies the inverted signal to the piezoelectric element 11. The same scattering process as explained before now applies to all three-signal components. As a result, a signal according to FIG. 9 is recorded at the piezoelectric element 13, which is approximately symmetric.

(114) In reality, the received signals will be distributed over time and there often is a “ballistic wave”, which has travelled through material of the pipe and arrives before the direct signal. This surface wave is discarded by choosing a suitable time window for generating the inverted measuring signal. Likewise, signals that stem from multiple reflections and arrive late can be discarded by limiting the time window and/or by choosing specific parts of the signal.

(115) The following table 1 shows measured time delays for a direct alignment, or, in other words, for a straight-line connection between clamped-on piezoelectric elements on a DN 250 pipe in a plane perpendicular to the longitudinal extension of the DN 250 pipe. The flow rate refers to a flow of water through the DN 250 pipe.

(116) Herein “TOF 1 cycle” refers to an impulse such as the one shown in FIG. 36, that is generated by a piezoelectric element, which is excited by an electric signal with 1 oscillation having a 1 μs period. “TOF 10 cycle” refers to a signal that is generated by a piezoelectric element, which is excited by an electric signal with 10 sinusoidal oscillations of constant amplitude having a 1 μs period.

(117) TABLE-US-00001 Flowrate/Method 21 m.sup.3/h 44 m.sup.3/h 61 m.sup.3/h TOF 1 cycle 7 ns 18 ns 27 ns TOF 10 cycle 9 ns 19 ns 26 ns Time reversal 8 ns 18 ns 27 ns

(118) The following table shows measured time delays for a 12 degree misalignment against a straight line connection between clamped-on piezoelectric elements in a DN 250 pipe in a plane perpendicular to the longitudinal extension of the DN 250 pipe (see also FIGS. 48 & 49).

(119) TABLE-US-00002 Flowrate/Method 21 m.sup.3/h 44 m.sup.3/h 61 m.sup.3/h TOF 1 cycle 10 ns 21 ns 28 ns TOF 10 cycle  9 ns 17 ns 26 ns Time reversal  4 ns 12 ns 26 ns

(120) FIGS. 9-27 show high resolution inverted signals and their respective response signals. The voltage is plotted in arbitrary units over the time in microseconds.

(121) The time axes in the upper Figures show a transmitting time of the inverted signal. The transmitting time is limited to the time window that is used to record the inverted signal. In the example of FIGS. 9-27 the time window starts shortly before the onset of the maximum, which comes from the direct signal and ends 100 microseconds thereafter.

(122) The time axes in the lower Figures are centered around the maximum of the response signals and extend 100 microseconds, which is the size of the time window for the inverted signal, before and after the maximum of the response signals.

(123) FIGS. 28-35 show digitized inverted signals in a high resolution and in 12, 3, 2 and 1 bit resolution in the amplitude range and their respective response signals. The voltage is plotted in Volt over the time in microseconds. The signals of FIG. 28-25 were obtained for a water filled DN 250 pipe.

(124) The length of the time window for the inverted signal is 450 microseconds. Hence, the time window of FIGS. 28-35 is more than four times larger than in the preceding FIGS. 9-27.

(125) In FIGS. 28-35 it can be seen that even a digitization with 1 bit resolution produces a sharp spike. It can be seen that the spike becomes even more pronounced for the lower resolutions. A possible explanation for this effect is that in the example of FIGS. 28-35 the total energy of the input signal is increased by using a coarser digitization in the amplitude range while the response signal remains concentrated in time.

(126) FIG. 36 shows a signal that is generated by a piezoelectric element after receiving an electric pulse that lasts for about 0.56 microseconds, which is equivalent to a frequency of 3.57 MHz. Due to the inertia of the piezoelectric element, the maximum amplitude for the negative voltage is smaller than for the positive voltage and there are multiple reverberations before the piezoelectric element comes to rest.

(127) FIG. 37 shows an electric signal that is applied to a piezoelectric element, such as the upstream piezoelectric element 11 of FIG. 1. The signal of FIG. 37 is derived by forming an average of ten digitized response signals to a signal of the type shown in FIG. 36 and time reversing the signal, wherein the response signals are received by a piezoelectric element such as the downstream piezoelectric element 13 of FIG. 1.

(128) In the example of FIG. 37, the digitized signals are obtained by cutting out a signal portion from the response signal that begins approximately 10 microseconds before the onset of envelope of the response signal and that ends approximately 55 microseconds behind the envelope of the response signal. The envelope shape of the response signal of FIG. 37 is similar to the shape of a Gaussian probability distribution, or, in other words, to a suitable shifted and scaled version of exp(−x{circumflex over ( )}2).

(129) FIG. 38 shows a portion of a response signal to the signal shown in FIG. 37, wherein the signal of FIG. 37 is applied to a first piezoelectric element, such as the upstream piezoelectric element 11, and is received at a second piezoelectric element, such as the downstream piezoelectric element 13 of FIG. 1.

(130) FIG. 39 shows a an upstream cross correlation function and a downstream cross correlation function, which are obtained by cross correlating the upstream signal and the downstream signal of the arrangement of FIG. 1 with a signal obtained at zero flow, respectively.

(131) FIG. 40 shows a sectional enlargement of FIG. 39. Two position markers indicate the positions of the respective maxima of the upstream and downstream cross correlation function. The time difference between the maxima is a measure for the time difference between the upstream and the downstream signal.

(132) FIG. 41 shows a response signal, which was obtained under similar conditions as for the response signal of FIG. 37. Different from the arrangement of FIG. 37, the piezoelectric elements are misaligned by 12 degrees against a straight-line arrangement along the perimeter of the pipe. This offset is shown in the inset of FIG. 41. FIG. 41 shows that even under misalignment conditions there is a reasonably well defined response signal.

(133) FIGS. 42 to 45 show, by way of example, different arrangements of clamp-on piezoelectric transducers for which a flow measurement according to the present specification can be used. Especially for clamp-on transducers a flow measurement method according to the present specification may lead to an improvement of the signal to noise ratio in the arrangements of FIGS. 42 to 45 or in other, similar transducer arrangements. Furthermore, the flow measurement method may provide energy savings by providing an increased signal amplitude of the response signal for a given sending signal power. Thereby, a signal sending power can be reduced.

(134) FIGS. 42 to 45 are aligned such that a gravity force on a liquid in the pipe 12 points downwards. However, arrangements, which are rotated relative to the arrangements of FIGS. 42 to 45, may also be used. The viewing direction of FIGS. 42 to 45 is along the longitudinal axis of the pipe 12. An upstream or downstream position of a transducer is not indicated in FIGS. 42 to 45.

(135) In the arrangement of FIG. 42, an array of five piezoelectric elements 31-35 is provided in a first location and a further piezoelectric element 36 is placed upstream or downstream of the first location. The array of piezoelectric elements 31-35 may be used to obtain a pre-determined wave front and to achieve an improved focusing of an acoustic wave in a pre-determined direction, when the array of five elements 31-35 is used as a transmitter and the further element 36 is used as a receiver.

(136) In the arrangement of FIG. 43, a single piezoelectric element 37 is provided in a first location and an array of five piezoelectric elements 38-42 is placed upstream or downstream of the first location. The array of piezoelectric elements 38-42 may be used to obtain an improved recording of the wave front of the response signal. The improved recording can then be used to obtain an improved flow-measuring signal, which is then applied to the single piezoelectric element 37.

(137) FIG. 44 shows an arrangement of two piezoelectric elements 43, 44 wherein one element is placed downstream with respect to the other. A distance d of the connection line between the piezoelectric elements 43, 44 to the symmetry axis of the pipe 12 is about half the radius of the pipe 12, such that a flow layer at a distance d to the central axis of the pipe 12 can be measured.

(138) Especially for clamp-on transducers, such as the piezoelectric elements 43, 44 shown in FIG. 44, the flow measurement according to the present specification provides an improved signal at the receiving piezoelectric element 44, 43 through beam forming.

(139) FIG. 45 shows an arrangement of eight piezoelectric elements 45-52, which are spaced at 45 degrees apart. Several arrangements are possible with respect to upstream-downstream placements.

(140) In one arrangement, the sensors locations alternate between upstream and downstream along the perimeter, for example 45, 47, 49, 51 upstream and 46, 48, 50, 52 downstream.

(141) In another arrangement, first four consecutive elements, such as 45-48, along the perimeter are placed upstream or downstream relative to the other four elements, such as 49-52. In a further arrangement with 16 piezoelectric elements, all the piezoelectric elements 45-52 of FIG. 45 are placed in one plane and the arrangement of FIG. 45 is repeated in upstream or downstream direction.

(142) FIG. 46 shows, by way of example, a flow measurement device 60 for measuring a flow in the arrangement in FIG. 1 or other arrangements according to the specification. In the arrangement of FIG. 1, the flow measurement device 60 is provided by the first and second computation units 15, and 16.

(143) The flow measurement device 60 comprises a first connector 61 for connecting a first piezoelectric transducer and a second connector 62 for connecting a second piezoelectric transducer. The first connector 61 is connected to a digital to analog converter (DAC) 64 over a multiplexer 63. The second connector 62 is connected to an analog to digital converter 65 over a demultiplexer 66.

(144) The ADC 65 is connected to a signal selection unit 67, which is connected to a signal inversion unit 68, which is connected to a band pass filter 69, which is connected to a computer readable memory 70. Furthermore, the ADC 65 is connected to a velocity computation unit 71.

(145) The DAC 64 is connected to an impulse signal generator 72 and a measuring signal generator 73. The measuring signal generator is connected to the impulse generator 72 over a command line 74. The velocity computation unit 71 is connected to the measuring signal generator 73 via a second command line 75.

(146) In general, the impulse signal generator 72 and the measuring signal generator comprise hardware elements, such as an oscillator, and software elements, such as an impulse generator module and a measuring signal generator module. In this case, the command lines 74, 75 may be provided by software interfaces between respective modules.

(147) During a signal-generating phase, the impulse signal generator sends a signal to the DAC 64, the selection unit 67 receives a corresponding incoming signal over the ADC 65 and selects a portion of an incoming signal. The inversion unit 68 inverts the selected signal portion with respect to time, the optional bandpass filter 69 filters out lower and upper frequencies and the resulting measuring signal is stored in the computer memory 70. When the word “signal” is used with reference to a signal manipulation step, it may in particular refer to a representation of a signal in a computer memory.

(148) In particular, a signal representation can be defined by value pairs of digitized amplitudes and associated discrete times. Other representations comprise, among others, Fourier coefficients, wavelet coefficients and an envelope for amplitude modulating a signal.

(149) FIG. 47 shows a second embodiment of a flow measurement device 60′ for measuring a flow in the arrangement in FIG. 1 or other arrangements according to the specification. The flow measurement device 60′ comprises a direct digital synthesizer (DDS) 76. For simplicity, only the components of the DDS 76 are shown. The DDS 76 is also referred to as an arbitrary waveform generator (AWG).

(150) The DDS 76 comprises a reference oscillator 77, which is connected to a frequency controller register 78, a numerically controlled oscillator (NCO) 79 and to the DAC 64. An input of the NCO 79 for N channels is connected to an output of the frequency control register 78. An input of the DAC 64 for M channels is connected to the NCO 79 and an input of a reconstruction low pass filter is connected to the DAC 64. By way of example, a direct numerically controlled oscillator 79 with a clock frequency of 100 MHz may be used to generate an amplitude modulated 1 MHz signal.

(151) An output of the reconstruction low pass filter 80 is connected to the piezoelectric transducers 11, 13 of FIG. 1.

(152) Due to the inertia of an oscillator crystal, it is often advantageous to use an oscillator with a higher frequency than that of a carrier wave in order to obtain a predetermined amplitude modulated signal, for example by using a direct digital synthesizer, as shown in FIG. 47.

(153) In particular, the method steps of storing a digital representation of a signal and performing operations such as selection a signal portion, time reversing a signal and filtering a signal may be interchanged. For example, a signal may be stored in a time inverted form or it may be read out in reverse order to obtain a time inverted signal.

(154) While the present invention is explained with respect to a round DN 250 pipe, it can be readily applied to other pipe sizes or even to other pipe shapes. Although the embodiments are explained with respect to clamp-on transducers, wet transducers, which protrude into a pipe, may be used as well.

(155) FIGS. 48 and 49 show an asymmetric transducer arrangement, wherein a second transducer is offset by 12 degrees with respect to a symmetry axis of the conduit 12.

(156) FIG. 50 shows a one cycle measuring signal of a time of flight measurement, and FIG. 51 shows a ten cycle measuring signal of a time of flight measurement. The signals shown in FIGS. 50 and 51 can be used for a time of flight measurement. Furthermore, the signals can also be used to generate a measurement signal according to the present specification using an inversion with respect to time of a received response signal, such as the response signals of FIGS. 52 and 53.

(157) FIG. 52 shows an example of a measuring signal that is derived from a time-reversed signal, which is stored at a low resolution.

(158) FIGS. 53 to 55 show response signals to the respective signals of FIGS. 50 to 52. The response signal is picked up by a receiving transducer 11, 13 of the asymmetric arrangement of FIGS. 48, 49 in response to a signal of a sending transducer, which is excited by the signal of FIG. 50.

(159) In particular, FIG. 53 shows a response signal of the signal of FIG. 50, FIG. 54 shows a response signal of the signal of FIG. 51 for the arrangement of FIGS. 48 and 49 and FIG. 55 shows a response signal of the Signal of FIG. 52 for the arrangement of FIGS. 48 and 49. In the examples shown, the response signal is more concentrated in time, has a higher amplitude and has a more well-defined envelope as compared to the signals of FIGS. 52 and 53.

(160) The result of FIG. 55 demonstrates that the benefits of inversion of the impulse response with respect to time, which allow, among others, to use smaller energy signals, can be retained for coarse-grained resolution and asymmetric transducer arrangements.

(161) The results of FIG. 55 demonstrate that using an inverted signal with respect to time according to the present specification is able to provide short time delays as compared with conventional time of flight Doppler shift measurements using a signal with 1 or 10 oscillation cycles. FIG. 55 as a result of the arrangement shown in FIG. 48 and FIG. 49 furthermore shows that a measuring signal according to the present specification can be used for beam shaping purposes.

(162) Table 2 shows results time delays for the asymmetric arrangement shown in FIGS. 48, 49 and for respective flow rates of 21, 44, and 61 cubic metres per hour.

(163) TABLE-US-00003 Flowrate Methods 21 m.sup.3/h 44 m.sup.3/h 61 m.sup.3/h TOF 1 cycle 10 ns 21 ns 28 ns TOF 10 cycle  9 ns 17 ns 26 ns inverted  4 ns 12 ns 26 ns signal

(164) The FIGS. 56 to 59 illustrate further examples of beam shaping applications. In general, there are Σ.sub.i=1.sup.N-1i=N*(N−1)/2 direct transmission channels between N transducers not considering reflections at the pipe walls, which are provided on a conduit. These transmission channels have in general different properties and lead to different response signals.

(165) In the event that all of the N transducers are mounted at different heights with respect to a flow direction or a longitudinal direction of the conduit, all of these transmission channels can be used for flow measurements. A signal propagation between transducers that is perpendicular to the mean flow is in general not useful for capturing flow velocity components but can still be used to determine contaminations and material changes of the conduit and changes in the properties of the transducers and their coupling to the conduit.

(166) A TOF flow measurement comprises a measurement in both directions with respect to a given transmission channel between two of the transducers. A TOF flow measurement that involves transmission channels between a first transducer and N−1 other transducers requires at least N consecutive measurements: a first measurement with a measurement signal applied to the first transducer and N−1 consecutive measurements with measurement signals applied to each one of the N−1 other transducers.

(167) In general, the required measurement signals are different for each transmission channel and separate forward and a backward measurements are needed for each transmission channel. Thus, 2×(N−1) measurements are required. For example, max 2×(3−1)=4 measurements are possible, but not necessarily required, in the example of FIG. 57.

(168) The signals of FIGS. 41 and 55 are produced by transducers, which radiate mainly in a preferred direction, with a maximum angle of about 12 degrees to both sides of the preferred direction. The directionality of the transducers is achieved, among others, by adjusting the form of the transducers and their attachment to the conduit. Depending on the angle between the transducers, not all paths may yield a sufficiently strong signal at a receiver side, especially if the sender has a high directionality. Applying the common known techniques only results as shown in FIG. 53 and FIG. 54 can be achieved with are typically too noisy for establishing flow measurements. However with the proposed method using inverted measurements signals, sufficiently good signals like those shown in FIG. 55 can be achieved.

(169) The use of a measuring signal according to the application, which uses a reversion with respect to time makes it possible to provide transducers with less directionality. The measuring signal focuses the signal energy at the receiver and the received signal is still strong enough.

(170) Similar to a measurement using just two transducers or just one transmission channel, the flow measurement can be performed using a pre-determined measuring signal or a signal that is obtained by a prior calibration. During the calibration step, the measuring signals are derived from response signals to the impulse signals. According to one example, an impulse signal is applied to a transducer to obtain one or more response signals at the other transducers. The measurement signals are derived by applying an inversion with respect to time to the response signals or a portion thereof.

(171) In one example, in which there are four measurement paths, consecutive measurements are taken along the first path, the second path, the third path and the fourth path. The consecutive measurements are used to derive an overall flow and/or flows in at a predetermined layer or position.

(172) One or more flow speeds can then be derived by comparing the measurements with a pre-determined flow profile. By way of example, the pre-determined flow profile can be obtained by a simulation. In another embodiment, a flow speed for a specific layer or position is estimated by using results from one or more measuring signals and known methods to calculate the flow profile. In one embodiment, an overall volume flow is derived by applying a calculated or simulated flow profile to a cross section area of the conduit.

(173) FIGS. 56 and 57 illustrate a time of flight flow measurement using three transducers and two transmission paths.

(174) FIGS. 58 and 59 show a pressure measurement in a two-transducer arrangement. The pressure scale of FIG. 59 is displayed in arbitrary units (a.u.).

(175) A measurement signal according to the present application is applied to the first transducer 11 and the resulting pressure distribution is measured at the periphery of the conduit 12. The transducers 11, 13 are offset in the longitudinal direction, similar to the arrangement of FIG. 1.

(176) In a first example, a measuring signal which adapted to the signal path between the transducer 11 and the transducer 13 is sent from the transducer 11 to the opposite transducer 13 and the resulting pressure distribution is measured. This yields a curve similar to the pressure distribution 90 of FIG. 59, which has a peak at the position of the transducer 13.

(177) In a second example, a measuring signal which adapted to the signal path between the transducer 11 and the transducer 13 is sent from the transducer 11 to transducer 13′ and the resulting pressure distribution is measured. Different from the first arrangement, the transducer 13′ is offset by an angle of 45 degrees with respect to a connection line through the first transducer and the center of the conduit 12. Even in this situation, the resulting pressure distribution is peaked around the position of the transducer 13′ and consequently the energy of the signal is concentrated around the position of the transducer 13′

(178) Thus, a measuring signal according to the application, which is obtaining using a reversal with respect to time of a signal between the respective transducers, leads to a pressure signal that is not only concentrated in time, as shown in the respective second Figure of the Figure sets 10-35, but the resulting pressure distribution is also concentrated in space.

(179) By using a standard signal, such as an impulse signal, a concentration in space can still be achieved, but only at a fixed location close to the opposite side of the sending transducer. However, by using a signal according to the present specification, which comprises a time reversed portion the peak of the pressure concentration can be moved.

(180) The ultrasonic transducers 11, 13, 23 of FIGS. 56-59 can be provided by mounted transducers, which are mounted to the outside of the conduit, or wet by transducers, which are protruding into the interior of the conduit 12 from outside of the conduit 12.

(181) FIG. 60 show an example of determining whether a test device uses the same method of flow measurement as a verification device. In a first step, the verification device selects a test impulse signal. For example, this may comprise the selection of a signal shape for performing an amplitude modulation of a sine wave out of a set of stored signal shapes, such as rectangular shape, a sinusoidal shape, a saw tooth shape etc.

(182) In a further step, the test impulse signal is applied to a first transducer. In a further step, a corresponding test response signal is received at the second transducer. In further steps, the test response signal, or a portion of it, is inverted and a test measuring signal is derived. The transducers to which the verification device is connected are preferably the transducers of the test device.

(183) In a further step, the test measuring signal is compared with the actual measuring signal of the test device. If the test measuring signal is similar to the measuring signal of the test device, it is decided that the test device uses the same method as the verification device. Alternatively or in addition, the verification device can apply the test measuring signal to a transducer, receive a corresponding test response signal and compare this test response signal with the response signal to the measuring signal of the test device.

(184) The verification device may receive or measure the signals of the test device as electric signals via tapping a wire connection of the test device to the transducers or, alternatively, the signals can be measured by placing a microphone in the conduit and receiving a signal of the microphone.

(185) If the signals are not similar, the same process is repeated with further available test impulse signals to see whether one of the test impulse signals leads to a test measuring signal and/or a response signal to it which resembles the measuring signal and/or the response signal to it. In the event that an impulse signal of the test device is available, the verification device may choose the available impulse signal or a similar impulse signal instead of testing various test impulse signals or it may narrow down the selection of test impulse signals.

(186) For a test device which uses several signal paths and/or combinations of pairs of sending and receiving transducers for the flow measurement, the verification device repeats the method of FIG. 60 for the multiple signal paths and/or for the multiple transducer combinations and the respective measuring signals and/or response signals to the measuring signals are compared.

(187) Although the above description contains much specificity, these should not be construed as limiting the scope of the embodiments but merely providing illustration of the foreseeable embodiments. The method steps may be performed in different order than in the provided embodiments, and the subdivision of the measurement device into processing units and their respective interconnections may be different from the provided embodiments.

(188) Especially, the above stated advantages of the embodiments should not be construed as limiting the scope of the embodiments but merely to explain possible achievements if the described embodiments are put into practice. Thus, the scope of the embodiments should be determined by the claims and their equivalents, rather than by the examples given.

(189) The embodiments of the present specification can also be described with the following lists of elements being organized into items. The respective combinations of features which are disclosed in the item list are regarded as independent subject matter, respectively, that can also be combined with other features of the application.

Embodiment 1

(190) A method for determining a flow speed of a fluid in a fluid conduit comprising: providing the fluid conduit with a fluid that has a predetermined velocity with respect to the fluid conduit, providing the fluid conduit with a first ultrasonic transducer, a second ultrasonic transducer and a third ultrasonic transducer, wherein respective connection lines between the first ultrasonic transducer, the second ultrasonic transducer and the third ultrasonic transducer extend outside of a symmetry axis of the fluid conduit, applying a first measuring signal to the first ultrasonic transducer, and measuring a first response signal of the first measuring signal at the second ultrasonic transducer, applying a second measuring signal to the first ultrasonic transducer, measuring a second response signal of the second measuring signal at the third ultrasonic transducer, wherein the first measuring signal and the second measuring signal respectively comprise a reversed signal portion with respect to time of a response signal of a corresponding impulse signal or of a signal derived therefrom, deriving a flow speed of the fluid from at least one of the first response signal and the second response signal.

Embodiment 2

(191) The method according to embodiment 1, comprising: applying a first reverse direction measuring signal to the second ultrasonic transducer, and measuring a first reverse direction response signal of the first reverse direction measuring signal at the second ultrasonic transducer, applying a second reverse direction measuring signal to the third ultrasonic transducer, measuring a second reverse direction response signal of the second reverse direction measuring signal at the first ultrasonic transducer, wherein the first reverse direction measuring signal and the second reverse direction measuring signal respectively comprise a reversed signal portion with respect to time of a response signal of a corresponding impulse signal or of a signal derived therefrom, deriving a flow speed of the fluid from at least one of the first response signal, the first reverse direction response signal, the second response signal and the second reverse direction response signal.

Embodiment 3

(192) The method according to embodiment 1 or embodiment 2, comprising: applying a third measuring signal to the second ultrasonic transducer, measuring a third response signal of the second measuring signal at the third ultrasonic transducer, wherein the third measuring signal comprises a reversed signal portion with respect to time of a response signal of a corresponding impulse signal or of a signal derived therefrom deriving at least one flow speed of the fluid from the third response signal.

Embodiment 4

(193) The method according to embodiment 3, comprising: applying a third reverse direction measuring signal to the third ultrasonic transducer, measuring a third reverse direction response signal of the third reverse direction measuring signal at the second ultrasonic transducer, wherein the third reverse direction measuring signal comprises a reversed signal portion with respect to time of a response signal of a corresponding impulse signal or of a signal derived therefrom deriving at least one flow speed of the fluid from the third response signal and the third reverse direction response signal.

Embodiment 5

(194) A method for determining a flow speed of a fluid in a fluid conduit comprising: providing the fluid conduit with a fluid that has a predetermined velocity with respect to the fluid conduit, providing the fluid conduit with a first ultrasonic clamp-on transducer and a second ultrasonic clamp-on transducer, wherein a connection line between the first ultrasonic clamp-on transducer and the second ultrasonic clamp-on transducer extends outside of a symmetry axis of the fluid conduit, applying a measuring signal to the first ultrasonic clamp-on transducer, measuring a response signal of the measuring signal at the second ultrasonic clamp-on transducer, wherein the measuring signal comprises a reversed signal portion with respect to time of a response signal of a corresponding impulse signal or of a signal derived therefrom, deriving a flow speed of the fluid from the response signal.

Embodiment 6

(195) The method according to embodiment 5, comprising: applying a reverse direction measuring signal to the second ultrasonic clamp-on transducer, measuring a reverse direction response signal of the measuring signal at the first ultrasonic clamp-on transducer, wherein the measuring signal comprises a reversed signal portion with respect to time of a response signal of a corresponding impulse signal or of a signal derived therefrom, deriving a flow speed of the fluid from the response signal.

Embodiment 7

(196) The method according to one of the preceding embodiments, wherein the signal portion that is used to derive the respective measuring signals comprises a first portion around a maximum amplitude of a response signal and a trailing signal portion, the trailing signal portion extending in time behind the arrival time of the maximum amplitude.

Embodiment 8

(197) The method according to one of the preceding embodiments, comprising processing of at least one of the response signals for determining a change in the wall thickness of the conduit or for determining material characteristics of the conduit walls by determining longitudinal and transversal sound wave characteristics.

Embodiment 9

(198) The method according to embodiment 1, comprising: providing the fluid conduit with a fluid, providing a first impulse signal to one of the first or the second ultrasonic transducer, receiving a first response signal of the first impulse signal at the other one of the first or the second ultrasonic transducer, providing a second impulse signal to one of the first or the third ultrasonic transducer, receiving a second response signal of the second impulse signal at the other one of the first or the third ultrasonic transducer, deriving the first measuring signal from the first response signal, deriving the second measuring signal from the second response signal, the derivation of the respective first and second measuring signals comprising selecting a signal portion of the respective first and second response signals or of a signal derived therefrom and reversing the signal portion with respect to time, storing the first measuring signal and the second measuring signal for later use.

Embodiment 10

(199) The method according to embodiment 5, comprising: providing the fluid conduit with a fluid, providing an impulse signal to one of the first ultrasonic clamp-on transducer and the second ultrasonic clamp-on transducer, receiving a response signal of the impulse signal at the other one of the first ultrasonic clamp-on transducer and the second ultrasonic clamp-on transducer, deriving the measuring signal from the response signal, the derivation of the measuring signal comprising selecting a signal portion of the respective response signal or of a signal derived therefrom and reversing the signal portion with respect to time, storing the measuring signal for later use.

Embodiment 11

(200) The method according to embodiment 9 or embodiment 10, comprising repeating the steps of applying an impulse signal and receiving a corresponding response signal multiple times, thereby obtaining a plurality of response signals, deriving the respective measuring signal from an average of the received response signals.

Embodiment 12

(201) The method according to one of the embodiments 9 to 11,

(202) wherein the derivation of the respective measuring signal comprises digitizing the corresponding response signal or a signal derived therefrom with respect to amplitude.

Embodiment 13

(203) The method according to embodiment 12, comprising increasing the bit-resolution of the digitized signal for increasing an amplitude of a response signal to the respective measuring signal.

Embodiment 14

(204) The method according to embodiment 12, comprising decreasing the bit-resolution of the digitized signal for increasing an amplitude of a response signal to the respective measuring signal.

Embodiment 15

(205) The method according to embodiment 12, wherein the bit resolution of the digitized signal with respect to the amplitude is a low bit resolution.

Embodiment 16

(206) A computer readable program code comprising computer readable instructions for executing the method according to one of embodiments 1 to 15.

Embodiment 17

(207) A computer readable memory, the computer readable memory comprising the computer readable program code of embodiment 16.

Embodiment 18

(208) An application specific electronic component, which is operable to execute the method according to one of the embodiments 1 to 15.

Embodiment 19

(209) A device for measuring a flow speed of a fluid in a conduit with a travel time ultrasonic flow meter, comprising a first connector for connecting a first ultrasonic element, a second connector for connecting a second ultrasonic element, a third connector for connecting a third ultrasonic element, a transmitting unit for sending impulse signals and for sending measuring signals, a receiving unit for receiving response signals, a processing unit for deriving a first measuring signal from a first inverted signal, for deriving a second measuring signal from a second inverted signal and for storing the first measuring signal and the second measuring signal, wherein the derivation of the first inverted signal and of the second inverted signal comprises reversing a signal portion of a response signal of a corresponding impulse signal or of a signal derived therefrom with respect to time, and wherein the processing unit, the transmitting unit and the receiving unit are operative to apply the first measuring signal to the first connector, and to receive a first response signal of the first measuring signal at the second connector, to apply a second measuring signal to the first connector, to receive a second response signal of the second measuring signal at the third connector, and to derive a flow speed of the fluid from at least one of the first response signal and the second response signal.

Embodiment 20

(210) A device for measuring a flow speed of a fluid in a conduit with a travel time ultrasonic flow meter, comprising a first connector, a first ultrasonic clamp-on transducer which is connected to the first connector, a second connector, a second ultrasonic clamp-on transducer which is connected to the second connector, a portion of a conduit, the first ultrasonic clamp-on transducer being mounted to the conduit portion at a first location, and the second ultrasonic clamp-on transducer being mounted to the conduit portion at a location, wherein respective connection lines between the first ultrasonic clamp-on transducer and the second clamp-on ultrasonic transducer extend outside of a symmetry axis of the fluid conduit, a transmitting unit for sending impulse signals and for sending measuring signals, a receiving unit for receiving response signals, a processing unit for deriving a measuring signal from an inverted signal, wherein the derivation of the inverted signal comprises reversing a signal portion of a response signal of a corresponding impulse signal or of a signal derived therefrom with respect to time, and wherein the processing unit, the transmitting unit and the receiving unit are operative to apply the measuring signal to the first connector, to receive a response signal of the first measuring signal at the second connector, and to derive a flow speed of the fluid from the response signal.

Embodiment 21

(211) The device of embodiment 20, further comprising: a D/A converter, the D/A converter being connected to the first connector, an A/D converter, the A/D converter being connected to the second connector, a computer readable memory for storing the measuring signal.

Embodiment 22

(212) The device of embodiment 20, further comprising a selection unit, the selection unit being operative to select a portion of a received response signal to the impulse signal or a signal derived therefrom, and an inverting unit, the inverting unit being operative to invert the selected portion of the received response signal with respect to time to obtain the inverted signal.

Embodiment 23

(213) The device according to embodiment 20, the device comprising

(214) a direct digital signal synthesizer, the direct digital signal synthesizer comprising the ADC,

(215) a frequency control register, a reference oscillator, a numerically controlled oscillator and a reconstruction low pass filter, the ADC being connectable to the first and the second connector over the reconstruction low pass filter.

Embodiment 24

(216) The device according to embodiment 20, comprising a portion of a conduit, the first ultrasonic transducer being mounted to the conduit portion at a first location,

(217) and the second ultrasonic transducer being mounted to the conduit portion at a second location.

Embodiment 25

(218) A method for determining whether a test device is measuring a flow speed of a fluid in a fluid conduit according to one of the embodiments 1 to 5, comprising: providing the fluid conduit with a fluid that has a pre-determined velocity with respect to the fluid conduit, providing the fluid conduit with a first ultrasonic transducer and a second ultrasonic transducer, applying a test impulse signal to the first ultrasonic transducer of the test device, receiving a test response signal of the test impulse signal at the second ultrasonic transducer of the test device, deriving a test measuring signal from the test response signal the derivation of the test measuring signal comprising reversing the respective first or second response signal, or a portion thereof, with respect to time, comparing the first test measuring signal with a first measuring signal that is emitted at a transducer of the test device, wherein it is determined that the test device is using a method to determine a flow speed of a fluid in a fluid conduit according to one of the items 1 to 5, if the first test measuring signal and the first measuring signal are similar.

Embodiment 26

(219) Method according to embodiment 25, comprising: providing the fluid conduit with a third ultrasonic transducer, applying a test impulse signal to the first ultrasonic transducer of the test device or to the second ultrasonic transducer of the test device, receiving a second test response signal of the test impulse signal at the at the third ultrasonic transducer of the test device, deriving a second test measuring signal from the second test response signal, comparing the second test measuring signal with a second measuring signal that is emitted at a transducer of the test device, wherein it is determined that the test device is using a method to determine a flow speed of a fluid in a fluid conduit according to item 1, if the first test measuring signal and the first measuring signal are similar.

REFERENCE

(220) 10 flow meter arrangement 11 upstream piezoelectric element 12 pipe 13 downstream piezoelec-tric element 14 direction of average flow 15 first computation unit 16 second computation unit 17 signal path 20 signal path 22 piezoelectric element 23 piezoelectric element 31-52 piezoelectric ele-ments 60, 60′ flow measurement de-vice 61 first connector 62 second connector 63 multiplexer 64 DAC
65 ADC 66 demultiplexer 67 signal selection unit 68 signal inversion unit 69 bandpass filter 70 memory 71 velocity computation unit 72 impulse signal genera-tor 73 measuring signal gener-ator 74 command line 75 command line 76 DDS 77 reference oscillator 78 frequency controller register 79 numerically controlled oscillator 80 low pass filter