• 专利附录
  • 专利说明
  • 权利要求
  • 类似技术
  • 同族专利
  • 引用文献
  • 法律状态
  • 优先权
    • 专利摘要:
    The invention relates to a method for ultrasonic detection of defects in a material, comprising the following steps: - emission of ultrasound from an ultrasonic transmitter transducer placed against the material at an emission position, - acquisition, by a ultrasonic receiver transducer placed against the material at the receiving position, at least one time signal, - for each measurement position, determining a normalization term from the values taken by the time signal during an initial portion of the measurement duration corresponding to the reception of ultrasonic waves propagated on the surface of the material; - for each measurement position, normalization of the time signal over the measurement time by using the normalization term to obtain a standardized time signal, - processing of standardized time signals for different measurement positions to detect defects in the material.
    公开号:FR3051913A1
    申请号:FR1654708
    申请日:2016-05-25
    公开日:2017-12-01
    发明作者:Nicolas Paul；Paul Kassis
    申请人:Electricite de France SA；
    IPC主号:
    专利说明:

    METHOD OF ULTRASOUND DETECTION OF DEFECTS IN A
    MATERIAL
    GENERAL TECHNICAL FIELD AND CONTEXT OF THE INVENTION
    The present invention relates to the non-destructive testing of materials, and more specifically to the ultrasonic detection and characterization of defects in a material.
    Ultrasound is commonly used for the implementation of non-destructive testing of materials. An ultrasonic probe placed on the surface of the material to be examined, which emits ultrasonic waves into the material, is used for this purpose. These waves transform and propagate in the material in different directions depending on its structure. The transducer receives a portion of these propagated waves, and their analysis can detect any defects in the material.
    US Patent Application 2007/0006651 Aldecrit a non-destructive testing method using ultrasonic waves, based on comparing the amplitude of the frequency spectrum of a selection of the signal with a reference amplitude. This application mentions the possibility of performing the measurements at different positions and evokes the combination of these measurements to obtain a mean measurement signal in the spatial sense. However, such a method is not entirely satisfactory, and the signal remains tainted with noise.
    In fact, most of the parts inspected have surface heterogeneities, such as deformations, roughness variations, surface accidents, or welds (including coatings), which can lead to significant variations in the quality of the acoustic coupling between the probe and the material to be inspected. However, the quality of this coupling has a direct influence on the measurements made and therefore on the result of the detection of defects.
    In particular, for a heterogeneous material, that is to say a polycrystalline material whose grain size is of the order of the ultrasonic wavelength in this material, the ultrasonic wave diffusion phenomenon by the structure of the material becomes preponderant. This diffusion can then lead to the generation of a structure noise, that is to say to an ultrasound signal of significant amplitude received by the probe and having characteristics similar to those that would emit a wave reflected by a default. It is then necessary to be able to distinguish finely between the noise of structure and possible defects. However, surface heterogeneities, by the attenuation of signal amplitudes and the variations they induce, may interfere with this detection. By way of illustrative example, FIG. 1 illustrates an example of measurement results obtained on an internal portion of a metal tube, with a shade that is all the clearer for the measurement points that the signal received is high. This is a map of the maximum values of the time signal portions corresponding to the diffraction zones of said time signals, that is to say to the representative parts of the structure noise. The material here is free of internal defects, and the patterns presented by the map of Figure 1 show the structure noise, which is relatively homogeneous in the material, except for two anomalies around which two black frames 2, 3 have been placed. At these anomalies, the amplitude of the received signal shows a discontinuity and is substantially lower than for the rest of the card.
    These two discontinuities correspond to coupling defects between the probe and the material for these measurement points, caused by surface inhomogeneities of the material. These coupling faults are reflected in the measurements by characteristics similar to those caused by defects inside the material, which pollutes the detection of faults or makes it impossible.
    More generally, the surface heterogeneities will hinder the interpretations of the signals in several ways: the strong variations of amplitudes that they induce can be confused with the presence of a defect; the coupling faults, by the small amplitude of the waves emitted or received, can mask faults which are then not detected; some fault detection methods exploit the statistical constancy of the signals, in particular the structure noise, and the small amplitudes induced by the coupling faults pollute these statistics.
    PRESENTATION OF THE INVENTION
    The object of the present invention is to provide a method for ultrasonic detection of defects in a material that makes it possible to reduce the influence of the surface heterogeneities of the material on the coupling between the transducer and the material, the variations of which taint the harvested data. For this purpose, there is provided a method for ultrasonic detection of defects in a material, comprising the following steps, for a plurality of transmitting position and receiving position couples: - emitting ultrasound from a ultrasonic transmitter transducer placed against the material at an emission position, - acquisition, by an ultrasonic receiver transducer placed against the material at the reception position corresponding to said transmission position, of at least one time signal representative of the amplitude of the ultrasound propagated in the material as a function of time during a measurement period at a measurement position, characterized in that the method comprises the following steps: for each measurement position, determining a normalization term from the values taken by at least the time signal at said measurement position during an initial portion of the measurement duration corresponding to the ception of ultrasonic waves propagated on the surface of the material; - for each measurement position, normalization of the time signal over the measurement time by using the normalization term to obtain a standardized time signal, - processing of standardized time signals for different measurement positions to detect defects in the material. The invention is advantageously completed by the following characteristics, taken alone or in any of their technically possible combination: the ultrasound is emitted by the ultrasonic transmitter transducer during a pulse duration, and the initial part of the measurement duration corresponds at a time less than the propagation time of the ultrasonic waves propagating on the surface of the material between the emission position and the reception position plus two times the pulse duration, taken from the beginning of the pulse; the normalization term is determined from the temporally average power of the values taken by the time signal during the initial portion of the measurement duration corresponding to the reception of ultrasonic waves propagated on the surface of the material; for a measurement position, the square of the normalization term is proportional to the temporally average power of the values taken by the time signal during the initial portion of the measurement duration corresponding to the reception of ultrasonic waves propagated on the surface of the material ; the method further comprises determining the propagation times between the transmission position and the corresponding reception position for the ultrasonic waves, and wherein the normalization term for a measurement position is determined from the propagation times to different measurement positions. the propagation time at a measurement position can be determined by correlating the time signal with a reference signal representative of the reception of an ultrasonic wave; for each time group of a plurality of propagation time groups, the temporally average power is determined, for the measurement positions having a propagation time belonging to said time group, of the values taken by the time signal during the part. initial measurement duration corresponding to the reception of ultrasonic waves propagated on the surface of the material, and - the term of normalization of a measurement position is determined from the temporally average powers of the measuring positions of the time group of propagation corresponding to the propagation time presented by the measuring position; the normalization term of a measurement position is determined from the mean of the temporally average powers of the measurement positions of the group of propagation time corresponding to the propagation time presented by the measurement position; a spatial filtering corresponding to measurement positions distributed over a surface portion of the material is used to filter the normalization term of a measurement position belonging to said surface portion. The invention also relates to an automated data processing system comprising a processor and a memory and configured to implement the method according to the invention, such a system comprising a memory and a processor. The invention also relates to a computer program product comprising program code instructions for executing the method according to the invention when said program is executed on a computer.
    PRESENTATION OF THE FIGURES The invention will be better understood, thanks to the following description, which relates to a preferred embodiment, given by way of non-limiting example and explained with reference to the accompanying diagrammatic drawings, in which: FIG. 1, already discussed, shows a map illustrating an example of the maximum values of the time signal portions corresponding to the diffraction zones of said time signals for a plurality of measurement positions and highlighting structural noise and coupling defects; FIG. 2 illustrates the inspection of a tube by an ultrasonic probe; FIG. 3 illustrates an example of an altitude / time two-dimensional representation for a given angle, showing the different parts of a temporal measurement signal; FIG. 4 shows a map of normalization terms for the example of FIG. 1 in a possible embodiment of the invention; FIG. 5 shows a map illustrating the maximum values of the standardized time signals for a plurality of measurement positions in a possible embodiment of the invention, taking again the example of FIG. 1; FIG. 6 shows a map of the propagation times for the ultrasonic waves taking again the example of FIG. 1; FIG. 7 shows a map of the normalization terms for the example of FIG. 1 in a possible embodiment of the invention.
    DETAILED DESCRIPTION For purposes of illustration, the following description will be made in the context of non-destructive testing of a tube of metallic material by means of ultrasonic transducers. Other types of surface may be inspected, and the invention is not restricted to a tube. Such an acquisition of transducer measurements is commonly performed, in particular for the implementation of the so-called diffraction path time measurement technique, better known by the acronym TOFD for the English "time of flight diffraction", whose protocol data acquisition can be implemented for the present invention. By way of example, the frequency of the ultrasonic waves generally used in non-destructive testing can range from 0.1 to 50 MHz, the 2-10 MHz band being the most commonly used. The wavelength, in this band, is therefore substantially, for metals such as steel or aluminum, between 3 mm and 0.5 mm.
    FIG. 2 illustrates a probe 1 disposed on the surface 11 of a tube 10 and inspecting the tube 10 presenting the defect 13. The emitting transducer 14 and the receiving transducer 15 of the probe 1 are arranged so as to be aligned in the longitudinal axis of the tube 10. They are therefore in a plane parallel to said longitudinal axis of the tube 10.
    The probe 1 moves on the surface of the material, and for each measurement position, emits and receives ultrasonic waves whose amplitudes define the measurement at this measurement position. The measurement position taken into account depends on the approach considered. It may for example be the reception position of the ultrasonic waves, the transmission position, or another position, for example a point of the probe 1 equidistant from the receiving position and the position of program. The definition of the measuring position affects only the geometric correspondence between the measuring positions and the material. Moving from one definition of the measurement position to another simply translates the measurements with respect to the surface of the tube 10.
    The data thus acquired are defined by an amplitude as a function of time related to each measurement position. By noting z the measurement position and x the amplitude of the signals, the time signal received by the probe for the measurement position z is recorded as x (z, t). It should be noted that the example given here, the position z is defined by an altitude h and an angle Θ. We can therefore also note x (z, t) = x (h, 0, t). The pitch of the altitude and the angle depends on the desired accuracy and the dimensional characteristics of the beams of emission and reception of the transducers. By way of example, it will be possible to take an altitude step of between 0.1 and 2 mm and an angular pitch of between 1 and 3 °.
    For measurements, ultrasound is emitted from the ultrasonic emitter transducer 14 placed against the material. The probe traverses the tube, and for a plurality of emission positions, ultrasonic wave firing is performed, generally taking the form of a pulse for a short pulse duration. This pulse can for example take the form of a gate signal or attenuated sinusoid. The ultrasonic waves emitted by the transmitter transducer 14 penetrate into the tube 10 at its inner wall 11, then propagate in the material of said tube 10.
    For a plurality of transmitting position and receiving position couples, the method according to the invention thus comprises emitting ultrasound from the ultrasonic transmitter transducer 14 placed against the material at an emission position, and acquiring, by the ultrasonic receiver transducer 15 placed against the material at the receiving position corresponding to said transmission position, at least one temporal signal representative of the amplitude of the ultrasound propagated in the material as a function of time during a measuring time at a measuring position.
    The time signal generally takes the form of a representation A, or A-scan, which is a time signal for a measurement position, whose data is denoted x (h, 0, t) or x (z, t). Other representations can obviously be defined, such as a representation B with a two-dimensional angle / time signal for a given altitude or altitude / time for a given angle.
    Another representation will also be used for illustrative purposes. It is the representation C, or C-scan, which is a two-dimensional signal corresponding to the maximum amplitudes (in absolute value) measured for each measurement position:
    Figure 1 previously discussed is for example a C-scan.
    The ultrasonic waves propagate to the ultrasonic receiver transducer 15. The waves received by the ultrasonic receiver transducer 15 may take several paths, as shown in FIG. 2. A first path 16 corresponds to the shortest path for the ultrasonic waves, which here corresponds to the surface of the material between the ultrasound emitter transducer 14 and the ultrasonic receiver transducer 15. This is called lateral waves for ultrasonic waves propagated on the surface of the material. Other paths 17 constitute other paths for the ultrasonic waves inside the material, which are diffracted by the defect 13 towards the receiving transducer 15. Finally, the longest path 18 constitutes the long path for the waves ultrasound, which are reflected towards the receiving transducer 15 by the opposite surface of the material, in this case the outer wall 12 of the tube 10.
    These different paths translate on the A-scan temporal signal by different zones that can be identified. To illustrate this effect, Figure 3 shows a B-scan altitude / time for a given angle.
    In this FIG. 3, a first zone 21 can be identified corresponding to the reception of ultrasonic waves propagated on the surface of the material. This is the initial part of the measurement time since these waves have taken the shortest path 16 between the ultrasonic transmitter transducer and the ultrasonic receiver transducer. An ultrasonic wave propagated on the surface of the material can thus be designated as a side wave. In FIG. 3, this initial part corresponding to lateral foundation lies in the first sixty steps of time.
    A second zone 22 corresponds to the reception of the ultrasonic waves propagated inside the surface of the material and which have been diffracted by the material, and in particular by the defects and heterogeneities inside thereof. We are talking about a diffraction zone. It is this second zone 22 which is mainly used to detect defects inside the material.
    Moreover, it can be seen that inside this diffraction zone 22 there are, for example, portions representative of a structure noise 24, or portions representative of defects 25.
    The third zone 23 corresponds to the background echo, and thus consists of the ultrasonic waves that have been reflected by the outer surface 12. These are the waves having taken the longest path 18, and which are therefore logically at the end of the measurement, after the 180 ^ "no time. The invention proposes to exploit the values taken by the time signals during an initial portion of the measurement duration corresponding to the reception of ultrasonic waves propagated on the surface of the material in order to normalize each time signal in its entirety, to compensate for the influence of surface heterogeneity. For this purpose, it is proposed for each measurement position to determine a normalization term from the values taken by at least the time signal at the measurement position during an initial portion of the measurement duration corresponding to the reception of ultrasonic waves propagated on the surface of the material, then normalize the time signal over the measurement time by using the normalization term to obtain a normalized time signal. Preferably, the normalization term is determined from the values taken by time signals of a plurality of measurement positions.
    The initial part of the measurement time can be defined as grouping the data acquired at the beginning of the measurement up to the acquisition of the measurements of the lateral waves including. There are therefore measurements of lateral waves, but possibly other measures such as ultrasonic waves propagated by the shortest path, which may differ from lateral waves. Indeed, when the surface of the material is flat, as in the example of Figure 2, the ultrasonic waves propagated by the shortest path in the material are the waves propagating on the surface of the material. The same goes for a concave surface.
    On the other hand, for a convex surface, ultrasonic waves propagating directly in the material between the emission position and the reception position arrive before the ultrasonic waves propagating on the surface of the material. These ultrasonic waves propagating by a direct path are also measured during the initial part. In this case, the initial portion of the measurement duration corresponding to the reception of ultrasonic waves propagated on the surface of the material covers not only said reception of ultrasonic waves propagated on the surface of the material, but also the prior reception of ultrasonic waves. propagated by the direct route.
    The initial portion extends to the time taken by the ultrasonic waves to propagate on the surface of the material between the transmission position 4 and the receiving position 5. The initial portion can thus for example correspond to a duration less than the time. propagation of ultrasonic waves propagating on the surface of the material between the transmission position 4 and the receiving position 5, plus two times the transmission duration, to ensure that all side waves have been received. The duration is taken from the beginning of the show. It will also be possible to rely on measurements made to define the limit chosen for this initial part, as for example in FIG. 3, where this initial duration corresponds approximately to the first 60 steps of time.
    Thus, to normalize a time signal, not the time signals in their entirety, but only the portions of the time signals corresponding to the initial portion of the measurement duration corresponding to the reception of ultrasonic waves propagated on the surface of the material. , that is to say, the reception of lateral waves. The normalization terms are not determined from the following portions of the time signals. In particular, the normalization terms are not determined from the parts of the measurement period corresponding to the reception of ultrasonic waves whose propagation path is longer than the propagation on the surface of the material.
    For example, it is possible, for example, to provide a preliminary step of selecting or extracting the portion of the time signals corresponding to the initial portion of the measurement duration, by deleting data used for this standardization measurements that follow the wave reception periodically. ultrasound propagated on the surface of the material, that is to say the reception of lateral waves.
    The normalization term can be determined from the temporally average power of the values taken by the time signal during the initial portion of the measurement time corresponding to the reception of ultrasonic waves propagated on the surface of the material. For example, for a measurement position, the square of the normalization term may be proportional to the temporally average power of the values taken by the time signal during the initial portion of the measurement duration corresponding to the reception of ultrasonic waves propagated to the surface of the material.
    Noting C (z) the normalization term for a measurement position z, we have, for example:
    with Nonde lateral the number of measurements belonging to the initial part of the measurement duration corresponding to the reception of ultrasonic waves propagated on the surface of the material.
    It should be noted that the temporally average power of the lateral wave Pol (z) corresponds to:
    Although such a normalization term determined from the temporally average power of the amplitude values can be used to directly normalize the time signal of the corresponding measurement position, a relatively strong variability of this normalization term can be observed, especially because of structural noise.
    Thus, preferably, the normalization term is determined from the values taken by time signals of a plurality of measurement positions. Spatial filtering corresponding to measurement positions distributed over a surface portion of the material may be used to filter the normalization term of a measurement position belonging to said surface portion. For example, a median spatial filter, i.e. constructed from the median of the considered values, is applied as a sliding window. The average could also be used, but the median is preferred to the average to avoid smoothing possible abrupt variations of plating. The filter window should be large enough to significantly reduce noise, and small enough not to mask small local variations in plating. For example, it is possible to take a window having a size of between 5 mm and 20 mm and between 15 degrees and 35 degrees (for a tube, with the steps mentioned above).
    FIG. 4 shows a map of the normalization terms obtained in this way for the example of FIG. 1, with the lowest values in dark and the highest values in the clear. In the black boxes 2, 3, there are areas where the surface heterogeneities cause a coupling fault. The low values taken by the normalization terms in these areas, and conversely, the higher values of the normalization terms, make it possible to compensate for the small amplitude of the temporal signals affected by the coupling defects. These normalization terms may be used to normalize the A-scan time signals, for example by dividing the values thereof by the normalization terms.
    FIG. 5 is a C-scan showing the result of the normalization of the A-scan used for FIG. 1 by the normalization terms determined as in the example as a result of their spatial filtering, restricted to the part corresponding to the diffraction zone. , and therefore representative of the structure noise. There is a strong attenuation of the irregularities due to the coupling faults, which had been identified by the black frames 2, 3 in FIG.
    It is also possible, to determine the normalization term for a measurement position, to use the propagation time of the ultrasonic waves corresponding to said measurement position. Here again the time signals of a plurality of measurement positions are used during the initial portion of the measurement period corresponding to the reception of the ultrasonic waves propagated on the surface of the material. For this purpose, the propagation times between the transmission position 4 and the corresponding reception position 5 for the ultrasonic waves for each measurement position are determined. The propagation time at a measurement position can be determined by correlating the time signal with a reference signal representative of the reception of an ultrasonic wave propagated along the shortest path in the inspected area. This path may for example be at the surface of the material, in which case the reference signal is representative of the reception of an ultrasonic wave propagated on the surface, or it may be a direct path in the material, especially if the surface is convex, in which case the reference signal is representative of the reception of an ultrasonic wave propagated by this direct path.
    This reference signal may for example be an ideal theoretical signal, or calculated by simulation. It is also possible to define it empirically from a set of measurements corresponding to the reception of lateral waves. For example, the spatially averaged values of a previously acquired set of ultrasonic wave reception measurements can be taken to define the reference signal.
    The peak of correlation corresponds to the reception of an ultrasonic wave, and thus allows, knowing the moment of emission impulse of the ultrasonic wave, to determine the propagation time of this ultrasonic wave. In addition to the moment of the transmit pulse, any other fixed time reference with respect to the moment of the transmit pulse can be used. This reference may in particular be the beginning of the measurement duration if the temporal position thereof is fixed with respect to the transmission pulse moment.
    FIG. 6 thus shows a map of propagation time established for the example illustrated in FIG. 1, with in dark the shortest travel times and in clear the longest travel times. We find, in black frames 2, 3, areas where surface heterogeneities cause a coupling fault. It is therefore noted that the surface heterogeneities can be demonstrated by means of the propagation times, and that it is therefore possible to exploit them to normalize the time signals in order to compensate for the influence of the coupling faults. For example, a relationship between the lateral wave delay and the sideband received power can be used to determine the normalization term. It is thus possible to construct the normalization term C (z) for the measurement position z from the temporally average power of the lateral base.
    More specifically: for each time group of a plurality of propagation time groups, the temporally average power is determined, for the measurement positions having a propagation time belonging to said time group, of the values taken by the time signal. during the initial portion of the measurement period corresponding to the reception of ultrasonic waves propagated on the surface of the material, and - the term of normalization of a measurement position is determined from the temporally average powers of the measurement positions of the grouping propagation time corresponding to the propagation time presented by the measuring position.
    In particular, the term of normalization of a measurement position can be determined from the average of the temporally average powers of the measurement positions of the group of propagation time corresponding to the propagation time presented by the measurement position.
    Thus, a corrected temporally average power is obtained which associates an average power with each grouping of time:
    where Nt is the number of measurement positions for which the propagation time of the lateral wave belongs to the measurement group of time t, and where
    The corrected corrected temporal average power Pol, is then used to determine the normalization term C (z):
    FIG. 7 shows a map of the normalization terms obtained in this way for the example of FIG. 1, with the lowest values in dark and the highest values in the clear. In the black boxes 2, 3, the areas where the surface heterogeneities lead to a coupling fault, which had already been highlighted with the propagation delay map shown in Figure 6, show the low values. by the normalization terms in these areas, and conversely, the higher values of the normalization terms elsewhere, make it possible to compensate for the small amplitude of the time signals affected by the coupling defects.
    As before, these normalization terms can be used to normalize the A-scan time signals, for example by dividing the values of these by the normalization terms.
    Moreover, as previously, it is possible to implement a spatial filtering corresponding to measurement positions distributed over a surface portion of the material to filter the normalization term of a measurement position belonging to said surface portion.
    Once the time signal is normalized, a known method of detecting defects can then be implemented, for example by comparing the normalized values with thresholds or by using more elaborate methods allowing not only to detect defects, but also to characterize them.
    It is possible in particular to construct one of the evoked representations, typically a C-scan, from normalized time signals restricted to the diffraction zone, that is to say to the measurement duration corresponding to the reception of ultrasonic waves propagated to the inside of the material, excluding lateral waves or background echo, then from this representation detect the defects by an analysis of the variations of the values of this representation.
    The method described is typically implemented by a computer provided with a processor and a memory. For this purpose, there is provided a computer program product comprising program code instructions for executing the method according to the invention when said program is executed on a computer. The invention is not limited to the embodiment described and shown in the accompanying figures. Modifications are possible, particularly from the point of view of the constitution of the various elements or by substitution of technical equivalents, without departing from the scope of protection of the invention.
    权利要求:
    Claims (11)
    [1" id="c-fr-0001]
    claims
    A method of ultrasonic detection of defects in a material, comprising the following steps, for a plurality of transmitting position and receiving position couples: - emitting ultrasound from an ultrasonic transmitter transducer (14) placed against the material at an emission position (4), - acquisition, by an ultrasonic receiver transducer (15) placed against the material at the receiving position (5) corresponding to said emission position, of at least one temporal signal representative of the amplitude of the ultrasound propagated in the material as a function of time during a measurement period at a measurement position, characterized in that the method comprises the following steps: for each measurement position, determination of a normalization term from the values taken by at least the time signal at said measurement position during an initial portion of the measurement duration corresponding to the reception of ultrasound propagated on the surface of the material; - for each measurement position, normalization of the time signal over the measurement time by using the normalization term to obtain a standardized time signal, - processing of standardized time signals for different measurement positions to detect defects in the material.
    [2" id="c-fr-0002]
    The method of claim 1, wherein the ultrasound is emitted by the ultrasonic emitter transducer (14) during a pulse duration, and the initial portion of the measurement duration corresponds to a time less than the propagation time of the ultrasonic waves. propagating on the surface of the material between the emission position (4) and the receiving position (5) plus two times the pulse duration, taken from the beginning of the pulse.
    [3" id="c-fr-0003]
    3. Method according to one of the preceding claims, wherein the normalization term is determined from the temporally average power of the values taken by the time signal during the initial portion of the measurement duration corresponding to the reception of ultrasonic waves. propagated on the surface of the material.
    [4" id="c-fr-0004]
    4. Method according to claim 3, wherein for a measurement position, the square of the normalization term is proportional to the temporally average power of the values taken by the time signal during the initial portion of the measurement duration corresponding to the reception of the signal. ultrasonic waves propagated on the surface of the material.
    [5" id="c-fr-0005]
    The method according to any one of the preceding claims, further comprising determining the propagation times between the transmission position (4) and the corresponding reception position (5) for the ultrasonic waves, and wherein the term Normalization for a measurement position is determined from the propagation times at different measurement positions.
    [6" id="c-fr-0006]
    6. Method according to the preceding claim, wherein the propagation time at a measurement position can be determined by correlating the time signal with a reference signal representative of the reception of an ultrasonic wave.
    [7" id="c-fr-0007]
    7. Method according to one of claims 5 to 6, wherein: - for each time group of a plurality of groups of propagation time, the temporally average power is determined, for the measurement positions having a propagation time belonging to said time group, values taken by the time signal during the initial part of the measurement period corresponding to the reception of ultrasonic waves propagated on the surface of the material, and - the term of normalization of a position of measuring from the temporally average powers of the measuring positions of the propagation delay group corresponding to the propagation time presented by the measurement position.
    [8" id="c-fr-0008]
    8. Method according to the preceding claim, wherein the term of normalization of a measurement position is determined from the mean of the temporally average powers of the measurement positions of the group of propagation time corresponding to the propagation time presented by the position. measurement.
    [9" id="c-fr-0009]
    9. Method according to one of the preceding claims, wherein a spatial filtering corresponding to measurement positions distributed over a surface portion of the material is used to filter the normalization term of a measurement position belonging to said surface portion. .
    [10" id="c-fr-0010]
    An automated data processing system comprising a processor and a memory and configured to implement the method of any one of the preceding claims.
    [11" id="c-fr-0011]
    A computer program product comprising program code instructions for executing the method according to any one of claims 1 to 9 when said program is run on a computer.
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    EP3465197B1|2020-04-01|
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    优先权:
    申请号 | 申请日 | 专利标题
    FR1654708A|FR3051913B1|2016-05-25|2016-05-25|ULTRASONIC DETECTION PROCESS OF DEFECTS IN A MATERIAL|FR1654708A| FR3051913B1|2016-05-25|2016-05-25|ULTRASONIC DETECTION PROCESS OF DEFECTS IN A MATERIAL|
    CN201780032628.1A| CN109196350B|2016-05-25|2017-05-24|Method for detecting defects in materials by ultrasound|
    PCT/FR2017/051282| WO2017203166A1|2016-05-25|2017-05-24|Method for detecting by ultrasound defects in a material|
    ES17732500T| ES2794825T3|2016-05-25|2017-05-24|Ultrasonic detection procedure for defects in a material|
    CA3025465A| CA3025465C|2016-05-25|2017-05-24|Method for detecting by ultrasound defects in a material|
    EP17732500.8A| EP3465197B1|2016-05-25|2017-05-24|Method for detecting defects in a material by ultrasound|
    US16/304,119| US10551352B2|2016-05-25|2017-05-24|Method for detecting defects in a material by ultrasounds|
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