NL2003154C2 - Method for ultrasonic sizing. - Google Patents
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- NL2003154C2 NL2003154C2 NL2003154A NL2003154A NL2003154C2 NL 2003154 C2 NL2003154 C2 NL 2003154C2 NL 2003154 A NL2003154 A NL 2003154A NL 2003154 A NL2003154 A NL 2003154A NL 2003154 C2 NL2003154 C2 NL 2003154C2
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- 238000000034 method Methods 0.000 title claims description 115
- 238000004513 sizing Methods 0.000 title description 29
- 230000007547 defect Effects 0.000 claims description 197
- 230000004927 fusion Effects 0.000 claims description 48
- 230000005540 biological transmission Effects 0.000 claims description 30
- GNFTZDOKVXKIBK-UHFFFAOYSA-N 3-(2-methoxyethoxy)benzohydrazide Chemical compound COCCOC1=CC=CC(C(=O)NN)=C1 GNFTZDOKVXKIBK-UHFFFAOYSA-N 0.000 claims description 12
- 238000004088 simulation Methods 0.000 claims description 8
- FGUUSXIOTUKUDN-IBGZPJMESA-N C1(=CC=CC=C1)N1C2=C(NC([C@H](C1)NC=1OC(=NN=1)C1=CC=CC=C1)=O)C=CC=C2 Chemical compound C1(=CC=CC=C1)N1C2=C(NC([C@H](C1)NC=1OC(=NN=1)C1=CC=CC=C1)=O)C=CC=C2 FGUUSXIOTUKUDN-IBGZPJMESA-N 0.000 claims description 6
- 230000003993 interaction Effects 0.000 claims description 5
- 229910000831 Steel Inorganic materials 0.000 claims description 4
- YTAHJIFKAKIKAV-XNMGPUDCSA-N [(1R)-3-morpholin-4-yl-1-phenylpropyl] N-[(3S)-2-oxo-5-phenyl-1,3-dihydro-1,4-benzodiazepin-3-yl]carbamate Chemical compound O=C1[C@H](N=C(C2=C(N1)C=CC=C2)C1=CC=CC=C1)NC(O[C@H](CCN1CCOCC1)C1=CC=CC=C1)=O YTAHJIFKAKIKAV-XNMGPUDCSA-N 0.000 claims description 4
- 239000010959 steel Substances 0.000 claims description 4
- 238000005457 optimization Methods 0.000 claims 3
- 238000005259 measurement Methods 0.000 description 8
- 229930195733 hydrocarbon Natural products 0.000 description 6
- 150000002430 hydrocarbons Chemical class 0.000 description 6
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N29/00—Investigating or analysing materials by the use of ultrasonic, sonic or infrasonic waves; Visualisation of the interior of objects by transmitting ultrasonic or sonic waves through the object
- G01N29/04—Analysing solids
- G01N29/07—Analysing solids by measuring propagation velocity or propagation time of acoustic waves
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N29/00—Investigating or analysing materials by the use of ultrasonic, sonic or infrasonic waves; Visualisation of the interior of objects by transmitting ultrasonic or sonic waves through the object
- G01N29/22—Details, e.g. general constructional or apparatus details
- G01N29/30—Arrangements for calibrating or comparing, e.g. with standard objects
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N29/00—Investigating or analysing materials by the use of ultrasonic, sonic or infrasonic waves; Visualisation of the interior of objects by transmitting ultrasonic or sonic waves through the object
- G01N29/44—Processing the detected response signal, e.g. electronic circuits specially adapted therefor
- G01N29/4409—Processing the detected response signal, e.g. electronic circuits specially adapted therefor by comparison
- G01N29/4436—Processing the detected response signal, e.g. electronic circuits specially adapted therefor by comparison with a reference signal
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N2291/00—Indexing codes associated with group G01N29/00
- G01N2291/01—Indexing codes associated with the measuring variable
- G01N2291/011—Velocity or travel time
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N2291/00—Indexing codes associated with group G01N29/00
- G01N2291/02—Indexing codes associated with the analysed material
- G01N2291/028—Material parameters
- G01N2291/0289—Internal structure, e.g. defects, grain size, texture
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N2291/00—Indexing codes associated with group G01N29/00
- G01N2291/04—Wave modes and trajectories
- G01N2291/044—Internal reflections (echoes), e.g. on walls or defects
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N2291/00—Indexing codes associated with group G01N29/00
- G01N2291/26—Scanned objects
- G01N2291/267—Welds
- G01N2291/2675—Seam, butt welding
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- Investigating Or Analyzing Materials By The Use Of Ultrasonic Waves (AREA)
Description
Title: Method for ultrasonic sizing
The invention relates to a method for ultrasonic sizing of at least one defect located at or adjacent to a fusion face of a weld in a wall of an object to be inspected such as a pipeline or a tank.
A pipeline or a tank used for fluidum transport or storage usually 5 has one or more welds. These welds can form connections between parts of the pipeline or the tank, or can form connections to another pipeline or tank. Usually such welds form a relatively vulnerable part of the pipeline or the tank. Practical experience shows that defects can relatively easily occur at or adjacent to fusion faces of the welds. If such defects occur, fluidum may leak 10 from the pipeline or the tank into an environment of the pipeline or the tank, which is in general unwanted. The connection may even fail starting from these defects, leading to desintegration of the pipeline or the tank in addition to large spoilage of the fluidum.
A class of pipelines or tanks where prevention of leakage is of utmost 15 importance are pipelines or tanks used for transport or storage of hydrocarbons. Loss of hydrocarbons to the environment of the pipeline or the tank is in general costly, brings damage to the environment and creatures living therein, and is dangerous as often these hydrocarbons are of an inflammable nature.
20 In practical conditions, pipelines or tanks used for hydrocarbon transport or storage are often loaded heavily. In case of floating off-shore facilities that are used in production and transport of hydrocarbons, welded connections of the pipeline near the facility are subject to relatively large dynamic mechanical loads as a result of tide. Over time, such dynamical loads 25 can easily lead to defects as a result of fatigue. To prevent failure of the welds as a result of fatigue, regular inspection of the welds is necessary. Such inspection can be performed non-destructively by automatic ultrasonic testing. If a defect is detected, it is important to correctly determine its size as this 2 forms important input to methods for assessing a risk of failure and/or leakage from the detected defect.
As hydrocarbons are found in and produced from increasingly deeper waters nowadays, loads on welds steadily increase and risks become 5 unacceptable already for relatively small defect sizes. This causes a continuous demand for improved methods for sizing defects, so that risks can be assessed more accurately.
It is therefore an object of the present invention to provide an improved method for ultrasonic sizing of a defect located at or adjacent to a 10 weld in a wall of an object to be inspected such as a pipeline or a tank.
Thereto the invention provides a method for ultrasonic sizing of at least one defect located at or adjacent to a fusion face of a weld in a wall of an object to be inspected such as a pipeline or a tank, including the steps of: a) dividing the fusion face to be inspected in a plurality of facets i (/=1,2,...n); b) 15 selecting a facet of the plurality of facets; c) transmitting a first ultrasonic signal to the facet selected in step b); d) receiving the first ultrasonic signal transmitted in step c) after being reflected on the selected facet of the object to be inspected; e) transmitting a second ultrasonic signal to a reference facet of a calibration object, which reference facet is associated with the selected facet in 20 step b), wherein the calibration object comprises an artificial defect in the reference facet, wherein the artificial defect has predetermined dimensions; f) receiving the second ultrasonic signal transmitted in step e) after being reflected on the reference facet of the calibration object; g) comparing the received first ultrasonic signal in step d) with the received second ultrasonic 25 signal in step f) for determining a size of a possible defect in the facet selected in step b) of the object to be inspected. Such a combination of using a calibration object and receiving the reflected first ultrasonic signal, enables an accurate and improved method of sizing. Preferably, the reflection of the first ultrasonic signal on the selected facet is caused by the possible defect.
30 Preferably, the reflection of the second ultrasonic signal on the reference facet 3 is caused by the artificial defect. Using such reflective measurements enables the detection of amounts of acoustic energy that are relatively small with respect to a transmitted amount of acoustic energy, so that the sensitivity of the method is high.
5 The method may be carried out by using zones for obtaining facets, in the object to be inspected and/or in the calibration object, instead of defining the facets directly. It may be clear that, then, dividing the wall of the object to be inspected in a plurality of zones / (/=1,2,...n) leads to dividing the fusion face to be inspected in a plurality of facets / (/=1,2,...n). When the fusion face at 10 least partly crosses one of the zones, that zone defines a facet.
Preferably, the selected facet and/or the reference facet have a planar shape, so that a first direction along the selected facet and/or the reference facet can be distinguished from a second direction transverse to the selected facet and/or the reference facet. Preferably, the selected facet is 15 positioned along the fusion face of the weld, so that the first direction is directed along the fusion face of the weld.
Preferably, determining a type of the weld may precede dividing in step a). Different weld types in general have different shapes. The dividing into facets of step a) preferably is different for each weld type. If the weld type 20 is determined before dividing in step a), a facet division that is optimum for that weld type can be made in step a).
The reference facet of step e) is associated with the facet selected in step b). For example, this means that an angle of incidence of the first ultrasonic signal on the facet selected in step b) is similar to an angle of 25 incidence of the second ultrasonic signal on the reference facet. Alternatively, or additionally, this for example means that a first travel distance of the first ultrasonic signal to and from the facet selected in step b) is similar to a second travel distance of the second ultrasonic signal to and from the reference facet. Alternatively, or additionally, this for example means that a first geometry of a 30 travel path of the first ultrasonic signal to and from the facet selected in step 4 b) is similar to a second geometry of a travel path of the second ultrasonic signal to and from the reference facet. Alternatively, or additionally, this for example means that the facet selected in step b) and the reference facet have a similar size and/or shape.
5 In an embodiment, steps e) and f) are carried out before steps c) and d) are carried out. This offers the advantage that positions of one or more transducers used in steps c) and d) can be optimized based on results obtained in steps e) and f).
It may further be clear that, preferably, dividing in step a) is carried 10 out automatically, and is optionally checked and possibly corrected by an operator. Preferably, the dividing in step a) is physically realised by choosing a beam width and/or a beam position of the first ultrasonic signal at or adjacent to the fusion face. The beam width may for example be defined by a -3 dB point, or by a -6 dB point, with respect to a maximum effective power inside 15 the beam. Such choosing may include focussing the beam of the first ultrasonic signal. Hence, dividing in step a) may include focussing the beam of the first ultrasonic signal.
In an embodiment, the method further includes: selecting another facet of the object to be inspected in a step h), wherein step h) further includes 20 repeating steps c)-g) for the other facet selected in step h). In this way, an additional facet can be inspected. Optionally, the reference facet associated with the facet selected in step b), and the reference facet associated with the other facet, are located in distinct calibration objects. However, alternatively they may be located in one and the same calibration object.
25 In an embodiment, in a step i) step h) is repeated for each of the facets obtained in step a) additionally to the facet and the other facet. In this way, all of the plurality of facets can be inspected.
In an embodiment, a first transmitter is used for transmitting in step c), a first receiver is used for receiving in step d), a second transmitter is 30 used for transmitting in step e), and a second receiver is used for receiving in 5 step f). Preferably, the first transmitter and the first receiver are positioned with respect to the facet selected in step b) similarly as the second receiver and the second transmitter are positioned with respect to the reference facet. In this way, the reference facet of step e) can be associated with the facet selected 5 in step b). For example, in this way it can be achieved that an angle of incidence of the first ultrasonic signal on the facet selected in step b) is similar to an angle of incidence of the second ultrasonic signal on the reference facet.
Preferably, a first plurality of mutually similar transmitters that includes the first transmitter is used for transmitting the respective first 10 ultrasonic signals in steps c) and h). Preferably, a first plurality of mutually similar receivers that includes the first receiver is used for receiving the respective first ultrasonic signals in steps d) and h). Preferably, a second plurality of mutually similar transmitters that includes the second transmitter is used for transmitting the respective second ultrasonic signals in steps e) and 15 h). Preferably, a second plurality of mutually similar receivers that includes the second receiver is used for receiving the respective second ultrasonic signals in steps f) and h).
In an embodiment, one and the same receiving transducer forms the first receiver and the second receiver, and/or one and the same transmitting 20 transducer forms the first transmitter and the second transmitter. This enables more accurate comparing in step g), as errors that occur from differences between individual transducers used for receiving in steps d) and f), and/or differences between individual transducers used for transmitting in steps c) and e), are prevented.
25 In an embodiment, the method includes the step: j) optimizing a position, with respect to the reference facet, of the second transmitter and the second receiver on the calibration object based on a shape of the fusion face of the weld, wherein optimizing includes pursuing for oblique impact of the transmitted second ultrasonic signal on the artificial defect or includes 30 pursuing for impact of the second ultrasonic signal on the reference facet with 6 an angle between 35 degrees and 70 degrees with a normal of the reference facet, further including using a similar position, with respect to the facet selected in step b), of the first transmitter and the first receiver on the object to be inspected. With these angles, disturbing mode conversions on the reference 5 facet may be substantially prevented. Such optimizing enables an improved way of sizing the possible defect. It is recognised by the inventor that the shape of the fusion face of the weld usually is different between various types of welds that are used in practice. In addition, the inventor recognised that the reflection of the first ultrasonic signal depends on a direction of the first 10 ultrasonic signal relative to an orientation of the possible defect. This orientation is usually strongly influenced by the shape of the fusion face of the weld, as the fusion face usually forms a relatively weak part of the weld. Typically, the possible defect has a planar elongated shape (for example pennyshaped) that is oriented with its plane in a plane of the fusion face of the weld. 15 As the direction of the first ultrasonic signal is determined by the position of the first ultrasonic transducer, optimising this position is important as it may allow for substantially maximizing the amplitude of the second reflected ultrasonic signal. In this way even a small defect, which only reflects a small amount of ultrasonic energy, can still be detected.
20 In an embodiment, optimizing in step j) is, at least partly, carried out automatically using dedicated design software. The use of such software significantly diminishes a probability for making errors.
In an embodiment, the first ultrasonic signal transmitted in step c) reaches the facet selected in step b) in a direction transverse to the facet 25 selected in step b), and the second ultrasonic signal transmitted in step e) reaches the reference facet in a direction transverse to the reference facet. This enables that one and the same first ultrasonic transducer forms the first receiver and the first transmitter, and one and the same second ultrasonic transducer form the second receiver and the second transmitter. This enables 30 an efficient use of transducers.
7
In an embodiment, the first ultrasonic signal transmitted in step c) reaches the facet selected in step b) with an angle between 35 degrees and 70 degrees with a normal of the facet selected in step b), and the second ultrasonic signal transmitted in step e) reaches the reference facet with an angle between 5 35 degrees and 70 degrees with a normal of the reference facet. In this way, facets that cannot be reached with the one and the same first transducer, can still be inspected.
In an embodiment, a size of the facet of the plurality of facets is small enough for determining a required minimum detectable size of the 10 possible defect. The minimum detectable size for example is 0.5 mm or 0.3 mm. If the size of the facet is too large, a signal-to-noise ratio of the first ultrasonic signal reflected from the first defect may be too small. Preferably, a ratio of the size of the facet and the required minimum detectable size is below a predetermined value, this value for example being smaller than twenty, 15 preferably smaller than ten. Preferably, the required minimum detectable size is inferred from a safety criterium for the object to be inspected. Preferably, the required minimum detectable size is smaller than or equal to a maximum size that is still considered safe based on the safety criterium.
In an embodiment, the plurality of facets substantially covers the 20 whole fusion face. It may be clear that, in an embodiment, the plurality of facets cover the whole thickness of the wall of the object. This greatly enhances reliability of the method.
In an embodiment, at least a number of, and preferably all, of the plurality of facets mutually overlap. In this way, interaction criteria between 25 defects in neighbouring facets can be applied more reliably. In addition, it can be more reliably determined whether neighbouring defects are part of one and the same physical defect.
In an embodiment, at least a number of, and preferably all, of the plurality of facets are mutually contiguous. In contiguous facets there may be 30 little, for example less than 10%, overlap between the facets. This enables an 8 efficient use of transducers, for example a total number of transducers for covering the whole wall of the object to be inspected can be relatively low.
In an embodiment, a first number of the plurality of facets mutually overlap and a second number of the plurality of facets are mutually 5 contiguous. Preferably, the sum of the first number and the second number equals the total amount of facets in the plurality of facets. Preferably, overlapping facets are used in relatively weak parts of a weld where defects are known to occur relatively often, and for example contiguous facets are used elsewhere. In this way, the advantages of contiguous facets and overlapping 10 facets can be combined.
In an embodiment, the method includes the step: k) determining a first reflection amplitude Ai of the first ultrasonic signal received in step d) and a second reflection amplitude A2 of the second ultrasonic signal received in step f), wherein determining in step g) is based on the first reflection 15 amplitude Ai and the second reflection amplitude A2. After carrying out step k), a set of data containing the second reflection amplitude A2 and the size of the artificial defect are known. Using a similar transducer configuration for, in step k), determining the second reflection amplitude A2 and for determining the first reflection amplitude Ai, i.e. having the second ultrasonic transducer 20 positioned relative to a location of the artificial defect in a similar way as the first transducer is positioned relative to a location of the possible defect, allows for the quantitative interpretation of the first reflection amplitude Ai. Using the calibration object in combination with the reflective measurement of this embodiment allows for a high sizing accuracy, and leads to an improved sizing 25 method. One of the advantages of such improved sizing is that the number of unnecessary repair jobs can be decreased.
In an embodiment, determining in step g) is further based on a ratio A1/A2 of the first reflection amplitude Ai and the second reflection amplitude A2, and preferably is based on a multiplication factor times the ratio A1IA2.
9
In an embodiment, the method includes the step: 1) determining a first transmission amplitude Bi of the first ultrasonic signal transmitted in step c), and determining a second transmission amplitude B2 of the second ultrasonic signal transmitted in step e); wherein determining in step g) is 5 further based on the first transmission amplitude Bi and the second transmission amplitude B2. As the first transmission amplitude Bi and the second transmission amplitude B2 will influence respectively the first reflection amplitude Ai and the second reflection amplitude A2, it may be important to take these into account for determining the size of the possible defect. In this 10 embodiment, the first transmission amplitude Bi and the second transmission amplitude B2 need not necessarily be similar, but can be allowed to be different from each other as well.
In an embodiment, determining in step g) is further based on a ratio B2/B1 of the second transmission amplitude B2 and the first transmission 15 amplitude Bi, and preferably is based on the product of the ratio A1IA2 and the ratio B2/B1.
In an embodiment, determining in step g) includes determining the size of the possible defect by using a predetermined sizing relation that relates the first reflection amplitude Ai to the size of the possible defect, wherein the 20 predetermined sizing relation is based on, at least, the second reflection amplitude A2 and the predetermined size of the artificial defect, and/or is based on numerical simulations. Preferably, the predetermined sizing relation is further based on the first transmission amplitude Bi and/or on the second transmission amplitude B2. In these numerical simulations, at least steps c)-f) 25 are simulated numerically. The inventor recognised the added value of determining the predetermined sizing relation based on, at least, the second reflection amplitude A2 and the predetermined size of the artificial defect, and on the numerical simulations. This combines the inherent practical reliability of experimental methods and the inherent versatility of numerical methods.
10
In an embodiment, the size of the possible defect is a surface area of the possible defect and the predetermined size of the artificial defect is a predetermined surface area of the artificial defect. As the first reflection amplitude Ai and the second reflection amplitude A2 are proportional to 5 respectively the surface area of the possible defect and the predetermined surface area of the artificial defect, this embodiment is especially suitable for sizing.
In an embodiment, step g) includes determining the surface area of the first defect by determining the product of the predetermined surface area 10 of the artificial defect and the ratio A1/A2 of the first reflection amplitude Ai and the second reflection amplitude A2.
In an embodiment, carrying out steps g) and h) includes determining a size of a plurality of defects that includes the possible defect, which plurality of defects is located at or adjacent to the fusion face. Although being detected 15 for more than one facet, at least a number of the plurality of defects may in fact be formed by one and the same defect. Alternatively or additionally, at least a number of the plurality of defects may mutually interact. Preferably, the method includes determining whether the plurality of sized defects mutually interact, preferably using interaction criteria inferred from at least 20 one of the API 1104 standard, the British standard BS 7910, and steel catenary riser criteria.
In an embodiment, the method includes determining whether the plurality of sized defects are formed by one and the same physical defect. This is important, as the size of each possible defect may otherwise be 25 underestimated. Preferably, the method includes using a time-of-flight- diffraction measurement of the plurality of first defects. In this way it can be determined whether the plurality of first defects are formed by one and the same physical defect. However, another method can be used for this as well.
Preferably, a creep-wave measurement along a surface of the wall 30 may be used to determine whether the possible defect or the one and the same 11 defect extends up to or near a surface of the wall. Using creep waves, with or without time-of-flight diffraction, is especially useful in combination with the reflective measurement of the invention as creep wave measurements yield valuable information of near-wall regions that would be difficult to obtain with 5 other methods.
According to an aspect of the invention, the method includes the step: m) designing a dimension of the calibration object based on a type of the weld, so that a position of the artificial defect in the calibration object corresponds with a position of the fusion face of the weld in the object to be 10 inspected. Carrying out such a designing step is especially advantageous for defect sizing as expressed by at least the steps a)-g), as it further improves the sizing accuracy. However, it is recognised by the inventor that it is not necessary to carry out step m) in combination with all of steps a)-g), but that it can be carried out independently as well, or in combination with one or more of 15 steps a)-l). The inventor recognised that especially combination of steps j) and m) is advantageous, as optimizing in step j) may be strongly linked with designing in step m).
In an embodiment, the artificial defect is a hole in the calibration object.
20 In an embodiment, the hole is a, preferably circular, bore.
In an embodiment, the bottom face of the bore is substantially flat, i.e. the bore has a flat bottom hole. In this way favourable reflections can be obtained.
In an embodiment, a material of the calibration object has similar 25 acoustic properties as a material of the wall of the pipeline or the tank.
In an embodiment, the pipeline is a catenary riser pipeline.
The invention will now be described, in a non-limiting way, with reference to the accompanying drawings, in which: 12
Figure 1 shows a cross-section of a wall of a pipeline parallel with a longitudinal direction of the pipeline and transverse to the wall;
Figure 2 shows a calibration object, wherein a artificial defect is located that has a predetermined size; 5 Figure 2A shows a close-up of a part of figure 2;
Figure 2B shows a top angle a of a notch;
Figure 3 shows a case wherein distinct transducers are used for sending and receiving;
Figure 4A shows an artificial defect in cross section substantially 10 parallel with a calibration face;
Figure 4B shows a cross section of the wall of figure 1 along the possible defect, substantially parallel with a fusion face; and
Figure 5 shows geometrical properties of a calibration face.
15 Unless stated otherwise, like reference numerals refer to like elements throughout the drawings.
Figure 1 shows a cross-section of a wall 2 of a pipeline parallel with a longitudinal direction of the pipeline and transverse to the wall 2. A weld 4, for example a girth weld, is present in the pipeline. The pipeline for example is 20 a catenary riser. Inspection of such catenary riser pipelines is important as dynamic loads can be relatively high for these kind of pipelines, in particular for girth welds present therein. On an outer surface 6 of the wall 2, a first ultrasonic transducer 8 may be positioned. The first ultrasonic transducer may be arranged for transmitting a first ultrasonic signal 10 and receiving the first 25 ultrasonic signal, respectively into and from the wall 2. The first ultrasonic transducer 8 thus forms both a first transmitter and a first receiver. A possible defect 12 is located adjacent to a fusion face 14 of the weld 4. The wall 2 is an example of an object to be inspected.
Figure 2 shows a calibration object 20, wherein an artificial defect 30 22 is located that has a predetermined size. The artificial defect 22 may be 13 located on an imaginary surface, herein referred to as a calibration face 24.
The calibration face 24 has a shape similar to the fusion face 14 of the weld 4, as is clear for example from comparison of figures 1 and 2. Preferably, a material of the calibration object has similar acoustic properties as a material 5 of the wall of the pipeline or the tank, so that it is representative for the wall of the pipeline or the tank. The calibration object may be made of steel. The calibration object 20 may have a first surface 25 and be similarly shaped and have similar dimensions as a part of the pipeline 2 of figure 1. For example, a wall thickness Di of the pipeline 2 may be similar to a thickness D2 of the 10 calibration object. The artificial defect 22 may be one of a plurality of mutually similar artificial defects 22.i The artificial defect 22 may he formed by a hole, for example a circular bore 23, in the calibration object 20. In that case, a bottom part of the bore 23 is regarded as the artificial defect 22. In this example, the plurality of artificial defects 22.i is formed by circular flat 15 bottomed holes 23 (see figure 2A). The calibration object is designed in such a way in this example that the plurality of bores 23 end at or near the calibration face 24. As a result, the plurality of artificial defects 22.i is located at or near the calibration face 24. The calibration face 24 may be located, with respect to the first surface 25, at a similar position as the fusion face 14 of the 20 weld 4 is located with respect to the outer surface 6.
It may be clear that, in addition to the bores 23 shown in figure 2, additional artificial defects such as bores and slots may be present in the calibration object 20. As a result, the plurality of artificial defects 22.i may substantially cover the whole calibration face 24. It may be clear that such 25 whole coverage still allows for spaces in between the artificial defects 22.i, and may refer to coverage along one direction along the calibration face 24. The additional bores are not shown in figure 2 for clarity. More in general, the artificial defects 22.i may be distributed over more than one calibration object 20.
14
Figure 2 further shows a second ultrasonic transducer 26 positioned on the first surface 25 of the calibration object 20. The second ultrasonic transducer 26 may be arranged for transmitting and for receiving a second ultrasonic signal 28 respectively into and from the calibration object 20. The 5 second ultrasonic transducer 26 thus forms both a second transmitter and a second receiver. In this example, the second ultrasonic transducer 26 is positioned relative to a location of the artificial defect 22 in a similar way as the first transducer 8 is positioned relative to a location of the possible defect 12. This may mean that a distance vector from the artificial defect 22 to the 10 second ultrasonic transducer 26 has a similar magnitude and direction as a distance vector from the possible defect 12 to the first ultrasonic transducer 8.
As a result of their similar thicknesses Di and D2, the object to be inspected 2 and the calibration object 20 have a similar size respectively in a direction of transmitting the first ultrasonic signal 10 and in a direction of 15 transmitting the second ultrasonic signal 28.
The first and/or second ultrasonic signal may contain ultrasonic shear waves. Preferably, the first ultrasonic signal predominantly contains ultrasonic shear waves, so that most of the energy of the first ultrasonic signal is carried by ultrasonic shear waves. Preferably, the second ultrasonic signal 20 predominantly contains ultrasonic shear waves, so that most of the energy of the second ultrasonic signal is carried by ultrasonic shear waves.
Figure 2A shows a close-up of a part 29 of figure 2, wherein the bottom of one of the plurality of artificial defects 22.i is indicated. The bore 23 may have a circular cross-section. The bottom face of the bore 23 may be 25 substantially flat. More in general, the bottom faces of the artificial defects 22 may be substantially parallel with the calibration face 24.
A first embodiment of a method for ultrasonic sizing according to the invention, hereinafter referred to as the first method, is now illustrated with reference to figures 1 and 2.
15
The first method includes the step of dividing the fusion face to be inspected in a plurality of facets i (i=l,2,...ri). In figure 1, the plurality of facets is indicated with reference numeral Zi. In the example of figure 1, n equals twelve and each one of the facets 1, 2, ...n is indicated with reference numeral 5 Zi. Such selecting may be carried out automatically and/or by an operator.
The first method further includes the step of selecting a facet of the plurality of facets. In this example, the facet Z8 is the selected facet. Selecting may be carried out by choosing a position of the first transducer 8 and by choosing a beam width of the first ultrasonic signal at the fusion face 14.
10 The first method further includes the step of transmitting the first ultrasonic signal 10 to the selected facet Z8 of the plurality of facets, and further includes receiving the transmitted first ultrasonic signal after it is reflected on the selected facet, in this example facet Z8, of the wall 2.
The first method further includes transmitting the second ultrasonic 15 signal 28 to a reference facet R8 of the calibration object 20. In general, the reference facet may be one of a plurality of reference facets l,2,...n. The reference facet R8 is associated with the selected facet Z8. The calibration object 2 comprises an artificial defect, in this example formed by a bore 23, in the reference facet R8 wherein the artificial defect 22 has predetermined 20 dimensions. The first method includes receiving the transmitted second ultrasonic signal 28 after it is reflected on the reference facet of the calibration object, which reflection is caused by the artificial defect 22.
The first method further includes comparing the received first ultrasonic signal 10 with the received second ultrasonic signal 28 for 25 determining a size of the possible defect 12, in the selected facet Z8 of the wall 2. Such comparing may include comparing a first characteristic of the received ultrasonic signal 10 with a second characteristic of the received second ultrasonic signal 28. Such a first characteristic includes for example a maximum amplitude or a power spectrum of the first ultrasonic signal. The 30 second characteristic includes for example a maximum amplitude or a power 16 spectrum of the second ultrasonic signal. Such characteristics may be sensitive to respectively the size of the possible defect and the predetermined size of the artificial defect. If the first and second characteristic are similar, it may be determined that the size of the possible defect 12 is similar to the size of the 5 artificial defect 22. For such determining, preferably the transmitted first ultrasonic signal before it is reflected on the selected facet is similar to the transmitted second ultrasonic signal before it is reflected on the artificial defect.
The first method may further include selecting another facet of the 10 wall 2, and may include repeating the steps of transmitting and receiving the first ultrasonic signal 10 and the second ultrasonic signal 28 for the other facets Zi in addition to facet Z8 in the wall 2 and for the other reference facets Ri in addition to reference facet R8 in the calibration object 20. This may be achieved by using a first plurality of mutually similar first transducers that 15 includes the first transducer 8 for transmitting and receiving the respective first ultrasonic signals 10 for the plurality of facets Zi. In addition, a second plurality of mutually similar second transducers that includes the second transducer 26 may be used for transmitting and receiving the respective second ultrasonic signals 28 for the plurality of reference facets Ri.
20 The first method may also include repeating the comparing of the received first ultrasonic signal 10 with the received second ultrasonic signal 28 for determining a size of a possible defect 12, for the other combinations of selected facet and reference facet in addition to the combination of the selected facet Z8 and the reference facet R8.
25 It may be clear that, in figures 1 and 2, the first transmitter and the first receiver are positioned with respect to the selected facet Z8 similarly as the second receiver and the second transmitter are positioned with respect to the reference facet.
In the first method, the first ultrasonic signal 10 transmitted by the 30 first ultrasonic transducer 8 reaches the facet Z8 selected in step b) in a 17 direction transverse to the selected facet Z8. In addition, in the first method the second ultrasonic signal 28 transmitted by the second ultrasonic transducer 26 reaches the reference facet R8 in a direction transverse to the reference facet R8. In the first method, one and the same first transducer 8 5 forms the first receiver and the first transmitter, and one and the same second transducer 26 forms the second receiver and the second transmitter.
While thus in the first method one and the same second transducer 26 was used for both sending and receiving, the inventor recognised that for some parts of the calibration face 24 it is advantageous to use distinct 10 transducers for sending and receiving. Such a case is illustrated for a second embodiment of a method according to the invention (further referred to as the second method) with reference to figure 3, which shows two distinct ultrasonic transducers which respectively form the second transmitter 30 and the second receiver 31. A similar configuration may be used for the first transmitter and 15 the first receiver.
In the second method, a first plurality of mutually similar transmitters that includes the first transmitter may be used for transmitting the respective first ultrasonic signals for the plurality of facets Ri, and a first plurality of mutually similar receivers that includes the first receiver may be 20 used for receiving the respective first ultrasonic signals. In addition, a second plurality of mutually similar transmitters that includes the second transmitter 30 may used for transmitting the respective second ultrasonic signals 28, and a second plurality of mutually similar receivers that includes the second receiver 31 may be used for receiving the respective second ultrasonic signals 28.
25 In the second method, the first ultrasonic signal 10 transmitted by the first transmitter may reach the selected facet with an angle between 35 degrees and 70 degrees with a normal of the selected facet. Analogously, the second ultrasonic signal 28 transmitted by the second transmitter 30 may reach the reference facet, in this example reference facet R2, with an angle 30 between 35 degrees and 70 degrees with a normal of the reference facet. Thus, 18 the second ultrasonic signal 28 reaches the reference facet, here reference facet R2, at an angle of incidence |3 (figure 3) with a normal to the calibration face 24 that is between 35 degrees and 70 degrees. Such a situation is illustrated in figure 3.
5 It may be clear that the artificial defect 22 usually extends in a plane of the calibration face 24. Thus, in the first method, an ultrasonic beam of the second ultrasonic signal 28 reaches the artificial defect 22 transversely to the calibration face 24. Such a situation is illustrated in figure 2. Thus, in the second method, the ultrasonic beam of the second ultrasonic signal 28 10 reaches the calibration face 24 under an angle with the calibration face 24. Such a situation is illustrated in figure 3. It may be clear that the possible defect 12 usually extends in a plane of the fusion face 12. Thus, in the first method, an ultrasonic beam of the first ultrasonic signal 10 reaches the defect 12 transversely to the fusion face 12. Such a situation is illustrated in figure 1. 15 Thus, in the second method, an ultrasonic beam of the first ultrasonic signal 10 reaches the defect 12 under an angle with the fusion face 12 (not illustrated).
It may be clear that, in the first and second method, the first ultrasonic signal 10 and the second ultrasonic signal 28 may be significantly 20 changed by reflection against respectively the possible defect 12 and the artificial defect 28.
The second method may further include steps similar to steps of the first method. In particular, the second method includes the step of dividing the fusion face 12 to be inspected in the plurality of facets i (i=l,2,...ri), and the 25 step of comparing the received first ultrasonic signal 10 with the received second ultrasonic signal 28 for determining the size of the possible defect in the selected facet of the object to be inspected. Such dividing and comparing are further described for the first method.
A third embodiment of a method according to the invention (further 30 referred to as the third method) includes determining a first reflection 19 amplitude Ai of the received first ultrasonic signal 10 and a second reflection amplitude A2 of the received second ultrasonic signal 28. The first receiver may be used for determining the first reflection amplitude Ai, after the first ultrasonic signal is reflected from the possible defect. The second receiver may 5 be used for determining the second reflection amplitude A2, after the second ultrasonic signal is reflected from the artificial defect. In the third method, determining the size of the possible defect is based on the first reflection amplitude Ai and the second reflection amplitude A2.
The third method may be carried out in combination with the first 10 method or the second method. However, it may lack steps of the first method or the second method that do not correspond with steps c)-g) of claim 1.
The third method may further include determining a first transmission amplitude Bi of the transmitted first ultrasonic signal 10, and determining a second transmission amplitude B2 of the transmitted second 15 ultrasonic signal 28. In the third method, determining the size of the possible defect may further be based on the first and second transmission amplitude Bi, B2.
More in general, one way of determining the size of the possible defect may include comparing the first reflection amplitude Ai and the second 20 reflection amplitude A2, and assign a size to the possible defect 12 that is proportional to the first reflection amplitude Ai and the predetermined size of the possible defect, and inversely proportional to the second reflection amplitude A2. In such a method, the first and second transmission amplitudes Bi, B2 may still be unknown as long as they have a similar value. For example, 25 the size of the possible defect may be determined to be similar, for example equal, to the product of the predetermined surface area of the artificial defect and the ratio A1/A2 of the first reflection amplitude Ai and the second reflection amplitude A2. Alternatively or additionally, the size of the possible defect 12 may be determined to be equal to the product of the predetermined surface 30 area of the artificial defect and the ratio A1/A2, times a multiplication factor.
20
The multiplication factor may be determined experimentally, numerically, and/or theoretically.
In the third method, determining the size of the possible defect may be carried out by using a predetermined sizing relation that relates the first 5 reflection amplitude Ai to the size of the possible defect, wherein the predetermined sizing relation is based on, at least, the second reflection amplitude A2 and the predetermined size of the artificial defect, and/or is based on numerical simulations.
Determining the size of the possible defect 12 by using the 10 predetermined sizing relation will now be illustrated for a variation of the third method. This variation may include transmitting the first ultrasonic signal 10 and determining the first transmission amplitude Bi of the first ultrasonic signal 10 before it is reflected from the possible defect 12. It may further include transmitting the second ultrasonic signal 28 and determining 15 the second transmission amplitude B2 of the second ultrasonic signal 28 before it is reflected from the artificial defect 22.
The predetermined sizing relation relates the first reflection amplitude Ai to the size of the possible defect 12, and is based on, at least, the second reflection amplitude A2 and the predetermined size of the artificial 20 defect 22. In the variation of the third method, the predetermined sizing relation is further based on the first transmission amplitude Bi and the second transmission amplitude B2.
It may be clear that in general the possibility exists that in practice the reflective properties of the artificial defect and the possible defect are 25 somewhat different. To further improve the predetermined sizing relation, the predetermined sizing relation may be determined by using numerical simulation results as well. Such simulations enable determining a simulated first reflection amplitude Ai of a simulated possible defect that has a size similar to the predetermined size of the artificial defect. In the numerical 30 simulations, the influence of small variations in the orientation of the 21 simulated possible defect on the simulated first reflection amplitude Ai may for example be determined. This adds to reliability of determination of the size of the possible defect.
Such a predetermined sizing relation may be set up by using the 5 second reflection amplitude A2, the second transmission amplitude B2, and the predetermined size of the artificial defect. For example, a plurality of second ultrasonic signals 28 may be generated for a number of positions of the second ultrasonic transducer 26 on the first surface 25 of the calibration object. More in general, additionally or alternatively, the size of one or more of the artificial 10 defects may be varied when setting up the predetermined sizing relation. Additionally or alternatively, the second transmission amplitude B2 may be varied, although the inventor recognised that this is not always necessary due to the highly linear nature of ultrasonic wave propagation and reflection. Using mathematical fitting techniques based on the results, a mathematical 15 function may be generated that relates, for a certain position of the second ultrasonic transducer and a certain value of the first transmission amplitude Bi, the size of the possible defect with the second reflection amplitude A2.
The size of the possible defect may be a surface area of the possible defect and the predetermined size of the artificial defect may be a 20 predetermined surface area of the artificial defect. In this case, in a first approximation, the size of the possible defect is proportional to the first reflection amplitude Ai and the predetermined size of the artificial defect, and inversely proportional to the second reflection amplitude A2. This is further illustrated with reference to figures 4A and 4B. This choice for the size of the 25 possible defect and the artificial defect is of practical importance, as the surface area of the possible defect is a good indicator for strength reduction of the weld 4.
Figure 4A shows the artificial defect 22, in this example the bottom part of the circular bore, in a cross section of the calibration object 20 30 substantially parallel with the calibration face 24 in figure 2. Figure 4B shows 22 a cross section of the wall 2 of figure 1 along the possible defect 12, substantially parallel with the fusion face. Figures 4A and 4B also show respectively the reference facet Ri and the facet Zi around respectively the artificial defect 22 and the possible defect 12. The facet Zi and the reference 5 facet Ri may respectively coincide with a beam cross section of the first ultrasonic signal 10 and the second ultrasonic signal 28.
In a fourth embodiment of a method according to the invention (further referred to as the fourth method), a step is carried out that includes optimizing a position, with respect to the reference facet, of the second 10 transmitter and the second receiver on the calibration object based on a shape of the fusion face of the weld, further including using a similar position, with respect to the facet selected in step b), of the first transmitter and the first receiver on the object to be inspected.
The fourth method is based on the first, second, and/or third method 15 and may include one or more steps thereof. Carrying out the optimizing of the fourth method for the second ultrasonic transducer positioned on the calibration object offers the advantage that well-controlled laboratory conditions can be used. Once an optimal position in the laboratory is employed, this position can be used for the first transmitter and the first receiver in field 20 practice as well. More in general, optimizing may be carried out for substantially maximizing the amplitude of the second reflected ultrasonic signal. This may increase for example a signal-to-noise-ratio of the received amplitude and thus increases the quality of sizing.
Optimizing in the fourth method combined with the second method 25 may be carried out for the second plurality of transmitters and the second plurality of receivers. Optimizing in the fourth method combined with the first method may be carried out for the second plurality of transducers Alternatively or additionally, optimizing in the fourth method may, at least partly, be carried out automatically using dedicated design software.
23
The fourth method may include optimizing the positions of the second ultrasonic transducers on the calibration object based on the shape of the fusion face of the weld. In this way optimizing can be carried out for the plurality of second ultrasonic transducers.
5 A variation of the fourth method includes optimizing a number of the plurality of second transducers, for achieving a required resolution along the fusion face of the weld and/or for covering the whole, or at least a substantial part, of the fusion face of the weld. For example, a required resolution along the fusion face as shown in figure 1 may be achieved by 10 setting the number of the plurality of ultrasonic transducers high enough.
Typically, this number is in a range from six to twelve on each side of the weld. This number may be chosen depending on the wall thickness and weld design. The facet height may typically be in a range from 2 to 3 millimeter. More in general, the minimum detectable defect size is smaller than the facet height. 15 More in general, the minimum detectable defect size is around 0.5 millimeter, possibly smaller than 0.5 millimeter, such as 0.3 millimeter or 0.2 millimeter.
A fifth embodiment of a method according to the invention (further referred to as the fifth method) includes determining a plurality of sizes of a respective plurality of defects, which plurality of defects includes the possible 20 defect. The plurality of defects is located at or adjacent to the fusion face. Such a plurality of defects can be detected for example by the repeated transmission and reception of the first ultrasonic signal 10 in the first and second method, by using the first plurality of receivers and the first plurality of transmitters.
The fifth method may include determining whether the plurality of 25 sized defects mutually interact. Such interaction is present for example if a mutual orientation and separation of a first one of the defects and a second one of the defects is such that a stress field around the first one of the defects significantly influences a stress field near the second one of the defects. In this situation, the second defect is significantly weakened by the first defect.
30 Interaction criteria inferred from at least one of the API 1104 standard, the 24
British standard BS 7910, and steel catenary riser criteria may be used for determining whether the plurality of sized defects mutually interact.
Alternatively or additionally, the fifth method may include determining whether the plurality of sized defects are formed by one and the 5 same physical defect. One way to do this is to determine whether the sized defects are neighbouring defects. If this is the case, the sized defects may be formed by one and the same physical defect. Determining whether the plurality of possible defects are formed by one and the same physical defect is especially relevant when the beam of the first ultrasonic signal does not 10 completely cover the possible defect. In that case, one or more other neighbouring beams will detect the rest of the possible defects. Only after determining whether the plurality of possible defects are determined by one and the same physical defect, the size of the physical defect can be determined.
In the fifth method (and possibly also in other embodiments), 15 information of the size of the possible defect is not limited by the beam width of one transducer, but information from various transducers may be combined. In general, in this way defects that have a size, for example a surface area, that falls outside the beam width of the first ultrasonic signal, can still be detected by combining results from more than one of the plurality of first 20 ultrasonic transducers.
A method according to the invention in a sixth embodiment (the sixth method) can be combined with the first, second, third, fourth, and/or fifth method. However, it can be applied on itself as well, for example without steps a)-g) of claim 1. The sixth method includes designing a dimension of the 25 calibration object, preferably based on a type of the weld, the wall thickness Di, and/or a diameter of the pipe or the tank. As a result of designing, a position of the artificial defect in the calibration object corresponds with a position of the fusion face of the weld in the object to be inspected. More in general this may mean that the artificial defect is positioned on the calibration 30 face. Designing may, at least partly, be carried out automatically using 25 dedicated design software. In general, the use of such software significantly diminishes a probability for making errors.
More in general, designing of the calibration object may further include at least one, and preferably all, of the steps: 5 1) choosing the type of weld that corresponds with the weld 4 (figure 1), on which a shape of the calibration face 24 is based. Examples of different types of welds among which can be chosen may include a CRC weld type, a narrow gap weld type, a Serimer weld type, a Swiss weld type, a V-bevel weld type, a J-bevel weld type and a compound bevel weld type, including single 10 sided weld types and double sided weld types. All these weld types are known as such to the skilled person so that a further description is deemed superfluous. In general, all of these weld types have a mutually different shape of the fusion face, so that for a specific weld type a dedicated shape of the calibration face may be chosen. Preferably, the shape and dimensions of the 15 calibration face coincide with the shape and dimensions of the fusion face.
2) Choosing a required number of reference facets for different parts of the calibration face 24, such as a cap part 36A, a fill part 36B, a hot pass part, an LCP part 36D, and a root part 36E, all indicated in figure 5. These parts correspond with similar parts of the weld 4, which parts as such are 20 known to the skilled person. Each part 36A-E has a corresponding part height 38A-E. In general, each of the parts 36A-E may be subdivided into a number of the reference facets. For the fill part 36B, these reference facets are indicated in figure 5 with reference numeral Ri. There may be one bore related to each reference facet Ri. In general, different parts can be indentified for different 25 types of welds. As a result, step 2) depends on the type of weld that is chosen in step 1).
The chosen weld type and the required number of reference facets may be entered into the dedicated design software. The software in turn may yield a suggestion for the number of reference facets per part of the weld, 30 dependent on the wall thickness.
26
More in particular, it may be clear that dividing the fusion face 14 to be inspected in the plurality of facets Zi, may be achieved indirectly by dividing the weld 4 in a number of weld zones that extend through the weld 4 parallel with the wall. In that case, the weld zones are associated with the 5 plurality of facets Zi, which can be selected. Each facet Zi that can be selected may substantially coincide with an intersection of the associated weld zone and the fusion face 14. In addition, selecting a facet of the plurality of facets Zi may be achieved by selecting a weld zone of the plurality of weld zones. Preferably, the shape of the fusion face and/or the weld type is determined 10 before the dividing of the fusion face to be inspected in the plurality of facets.
3) determining the diameter of the pipeline, and optionally entering a value of this diameter into the design software.
4) Determining the wall thickness 2 of the pipeline, and optionally entering a value of this thickness into the design software.
15 5) Determining dimensions, i.e. part heights 38A-E and/or angles ya-
Ye with a direction 39 perpendicular to the first surface 25 and/or the second surface, of the parts 36A-E of the calibration face 24 (figure 5), and optionally entering values of these dimensions into the design software.
6) Determining dimensions, such as the thickness D2, of the 20 calibration object 20, and optionally drawing the calibration object 20.
Drawing may be carried out by using the software.
7) Choosing, for each of the reference facets Ri, a required diameter db of the bore (figure 2A), an angle cp of the bore (figure 2), and a vertical offset (in a direction transverse to the wall 2). An option is to choose to give all bores 25 a similar diameter. An option is to have a number of bores aligned with each other, i.e. these bores end on one and the same plane, preferable a part of the calibration face. Optionally, the software determines the number of reference facets Ri and height of the reference facets Ri, preferably followed by checking whether the summed height of all reference facets equals the wall thickness.
27 8) Choosing whether a first notch is present at the first surface 25 and/or whether a second notch is present at a second surface of the calibration object opposite to the first surface 25. The first and second notch may be representative for surface breaking defects (like cracks or lack of fusion) in or 5 adjacent to the weld. These surface breaking defects may extend along the weld. If one or both of the first notch and the second notch are chosen to be present, a notch depth, a notch width, a notch length, a position of the notch, and/or a rotation angle of the notch may be chosen for one of the first and second notch, or for both notches. An orientation of the notch typically 10 corresponds with an orientation of the corresponding part of the calibration face. The rotation angle, here defined as the angular difference of a depth direction of the notch and a normal to the first surface 25 or to the second surface, for example equals the angle Ja or the angle Ye. The notch may be positioned adjacent to the cap portion and/or the root.
15 9. Choosing whether a third notch 41 is present in the calibration object 20, that can be used for a time-of-flight diffraction measurement. The included top angle a is for example at most 60 degrees, in order to enable diffraction instead of reflection (see figure 2B). Depending on the required coverage with the time-of-flight diffraction measurement multiple notches with 20 different depths can be used located at the first surface 25 and/or the second surface.
10. Choosing whether a transverse notch is present in the calibration object. Such a transverse notch may be representative for a defect oriented transverse to the weld direction). In addition, designing may include 25 assigning a width, length, height and shape of the transverse notch.
Each of these steps 1)-10) on itself is already valuable for designing the calibration object, while the combination of two or more steps, especially all steps, is valuable for further improving designing of the calibration object 20. It is recognised by the inventor that, more in general, steps 1) and 2) may 30 be important for optimising the position of the second ultrasonic transducer 28 and the plurality of ultrasonic transducers in the second and third method.
The software may be arranged for determining an optimal position of the second ultrasonic transducer and the plurality of second ultrasonic transducers.
5 In one or more of the first, second, third, fourth, fifth, and sixth embodiment, the first ultrasonic transducer may be a piezoelectric transducer, and transmitting the first ultrasonic signal and determining the first reflection amplitude Ai may be carried out by means of a suitable signal processing system, known as such to the skilled person. The piezoelectric first electronic 10 transducer may be arranged for generating an electrical signal based on the received first ultrasonic signal. The signal processing system is arranged for measuring a maximum of the electrical signal relative to a base level of the electrical signal. This maximum may represent the first reflection amplitude Ai. In this way the first reflection amplitude Ai can be determined by means of 15 the signal processing system.
It may be clear that the second ultrasonic transducer may as well be a piezoelectric ultrasonic transducer, while transmitting the second ultrasonic signal and determining the second reflection amplitude A2 may be carried out in a similar way as transmitting the first ultrasonic signal and determining 20 the first reflection amplitude Ai.
The invention is not limited to any embodiment herein described and, within the purview of the skilled person, modifications are possible which may be considered within the scope of the appended claims. For example, the invention is also applicable to welds that extend along the pipeline. Equally all 25 kinematic inversions are considered inherently disclosed and to be within the scope of the present invention. The use of expressions like: "preferably", “in particular”, “typically”, “especially”, etc. is not intended to limit the invention. The indefinite article “a” or “an” does not exclude a plurality. Features which are not specifically or explicitly described or claimed may be additionally 29 included in the structure according to the present invention without deviating from its scope.
Claims (26)
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| NL2003154A NL2003154C2 (en) | 2009-07-08 | 2009-07-08 | Method for ultrasonic sizing. |
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| NL2003154A NL2003154C2 (en) | 2009-07-08 | 2009-07-08 | Method for ultrasonic sizing. |
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Citations (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| WO2002031487A2 (en) * | 2000-10-13 | 2002-04-18 | Chicago Bridge & Iron Company | Ultrasonic austenitic weld seam inspection method and apparatus |
| US20050223807A1 (en) * | 2002-06-17 | 2005-10-13 | Olivier Bardoux | Method for ultrasonic control of weld joints |
| WO2008075943A2 (en) * | 2006-12-01 | 2008-06-26 | Röntgen Technische Dienst B.V. | A method for configuring an array of transducers in an ultrasonic test apparatus |
| WO2008105109A1 (en) * | 2007-02-28 | 2008-09-04 | Jfe Steel Corporation | Calibration method of ultrasonic flaw detection and quality control method and production method of tubular body |
-
2009
- 2009-07-08 NL NL2003154A patent/NL2003154C2/en not_active IP Right Cessation
Patent Citations (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| WO2002031487A2 (en) * | 2000-10-13 | 2002-04-18 | Chicago Bridge & Iron Company | Ultrasonic austenitic weld seam inspection method and apparatus |
| US20050223807A1 (en) * | 2002-06-17 | 2005-10-13 | Olivier Bardoux | Method for ultrasonic control of weld joints |
| WO2008075943A2 (en) * | 2006-12-01 | 2008-06-26 | Röntgen Technische Dienst B.V. | A method for configuring an array of transducers in an ultrasonic test apparatus |
| WO2008105109A1 (en) * | 2007-02-28 | 2008-09-04 | Jfe Steel Corporation | Calibration method of ultrasonic flaw detection and quality control method and production method of tubular body |
| EP2116847A1 (en) * | 2007-02-28 | 2009-11-11 | JFE Steel Corporation | Calibration method of ultrasonic flaw detection and quality control method and production method of tubular body |
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