| NDT.net - November 1999, Vol. 4 No. 11 |
| TABLE OF CONTENTS |
![]() Fig 1: Illustration of a shrinkage crack TOFD indication of a shrink crack |
![]() Fig 1: Probe positioning for typical longitudinal or spiral seam weld inspections |
Attention was drawn to the problem when eventually a radiograph was required on a suspect indication and a linear indication was seen on the radiograph. TransCanada Pipelines decided to investigate further so required a Time of Flight Diffraction (TOFD) technique be used on all pipe of the affected lot in the mill. A TOFD configuration was quickly incorporated into the system and operated in parallel with the standard mechanised (final) UT system. Results of the scanning are summarised in the Table 1.
| Number of Pipe Seams tested | Number of Indications detected using Mechanised OD UT (>80% reference) | Number of Indications detected using TOFD | Number of Indications detected using ID UT |
| 149 | 20 | 35 | 34 |
With a nearly vertical orientation, the shrink crack defect was ideally suited to be detected using TOFD. The principles of TOFD are illustrated in Figure 3.
![]() Fig 3: Principles of the TOFD techniqueTOFD indication of a shrink crack |
![]() Fig 5: TOFD indication of a shrink crack |
When a defect was detected using TOFD it was then investigated using a Pulse-Echo technique using a nominal 70° probe from the inside surface. Figure 4 shows the positioning of the probe for the ID surface scan. Table 1 indicates that the standard mechanised UT from the outside surface was not always effective in detecting the defects, yet reasonable correlation existed between the TOFD and ID pulse-echo techniques. Evidence from this evaluation has raised concerns as to the reliability of UT using the minimum requirements of the procedures outlined in CSA-Z245 and other codes using the same principles.
![]() Fig 4: ID pulse-echo technique |
Use of TOFD in this particular instance was very effective in identifying areas of concern. However, TOFD requires special equipment and evaluation of results is generally slow. Training and comprehension of operators would need to be far more elaborate than the present training provided for the "go/no-go" approach presently used.
Figure 5 illustrates an example of the signal obtained from the flaws in the cracked weld seams. The distinct angled indication between the parallel signals formed by the lateral (top surface) and backwall (ID surface) indicate the defect originates near the middle of the weld and propagates to a point very near the ID surface.
Figure 6 illustrates the ideal positioning of the full skip probe/beam in the traditional pipe seam inspection. Typically sensitivity calibration involves setting a response off the corner reflector geometry provided by a hole drilled in the weld on the weld centreline. Holes are of three types; through, 50% through from the OD and 50% through from the ID. The hole is normally 1.6 mm diameter (1/16 ") and the signal is set to about 80% full screen height. The fact that a slightly lower amplitude signal is received off the holes drilled half through the wall as compared to the through wall holes seems to assure the operators that they are truly looking at the inside and outside volumes separately. This is of course not strictly true but the operator assumes that the beam spread is adequate to provide all the coverage needed in the midwall region.
![]() Fig 6: Beam coverage for full skip Submerged Arc Weld inspection |
Figure 6 illustrates the beam pattern from a 9x9mm 5MHz probe positioned so the centre of beam intersects with the top midpoint of the through hole of a calibration target in a pipe with wall thickness 15.3mm. This clearly shows that although ideally positioned for the OD near surface, the region in the midwall receives only the lower beam edge.
The first assumption is reasonable for 45° refracted beams and adequate for 70° beams but fails for beams near 60°.
Since the average pipe mill UT operator does not practice manual weld inspection, they do not use echo-dynamics to evaluate flaw position and characteristics. In the pipe mill, acceptance criteria is based solely on a "go/no-go" philosophy. Therefore the second and third assumptions lead the operator to think that any signal in the gate arises from discontinuities along the beam axis. Since their fixed "standoff" from the weld cap edge allows no forward and backward motion pipe mill UT operators cannot determine if the indication is near the toe of the weld or near the midwall. This lack of probe motion coupled with an extensive use of "reject" (also called "suppression") makes flaw characterisation impossible and even approximate positioning of the flaw in the vertical plane is not possible.
Since the ID pulse-echo technique is more effective than the OD pulse-echo technique, another question is raised. Why is there such a difference? The answer lies primarily in the geometry configuration. It is always assumed that the centreline of the weld cap is adequate to describe the centre of the double-vee bevel (note: the term 'double-vee' is used loosely here as most SAW situations for such thin wall do not actually prepare a bevelled edge. Instead, the plate edges are left square). However, alignment of the wire in the submerged arc process is not so precise. If the OD cap is offset from the actual centreline by 2-3 mm and the ID cap is offset in the opposite direction by 2-3 mm the UT inspection may not be providing the coverage expected. This effect will be more pronounced for the ID looking probes. By placing the ID probes 6 mm further away from the centreline, the upper edge of the beam will be well away from the midwall region on one side. Any defects in the midwall region will be missed by one probe and the other probe will have the beam positioned to be more centred on the defect. When such a non-symmetric response was observed in the mill the pipe was sent for radiography. Since no flaw was seen on the radiograph the pipe was accepted. See Figure 7 for an illustration of the effect on beam coverage that results from offset weld caps.
| Fig 7: The effects of asymmetry between outside and inside weld caps |
![]() Symmetry of positioning maintained for weld cap on same side as probe. |
![]() Beam position symmetry lost for weld on opposite side of plate when position reference is made relative to the weld cap. Centre of beam moved to toe of weld. |
![]() Beam position symmetry lost for weld on opposite side of plate when position reference is made relative to the weld cap. Centre of beam moved to midwall region of weld. |
Using the top surface weld edge as the reference for positioning of the probe stand-off makes no change in the relative position of the beam for the upper half of the weld. However, this places the beam in the wrong position for the lower half of the weld when a cap offset exists. On the side where the lower half is offset further away, the beam is more sensitive to the weld cap edge and the midwall region is virtually missed. On the side where the lower half of the weld is closer the beam misses the far surface in the region of the weld toe and more of the central beam is directed at the midwall region of the lower weld bead. This dilemma of offset welds is exacerbated by standard tracking systems which can vary the probe standoff position by 4-5mm, or more, each side of the OD weld cap. It is conceivable under extreme conditions that with offset welds and poor tracking the ID probes might be looking at pipe plate instead of weld metal, if the combined error of 9mm is reached (depending on wall thickness).
Several options may be considered to overcome these shortcomings:
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