![]() ·Table of Contents ·General | Ultrasonic flow detection for small and medium diameter pipe bendsAuthor: Shao-he Song (senior electrical engineer)Adress: Boiler Inspection Office, Gansu Electric Powere Test & Research Institute Gansu Province, China Co-Author: Xin Zhang ( electrical engineer) Adress: Boiler Inspection Office, Gansu Electric Powere Test & Research Institute Gansu Province, China Jin-qiang Hu ( electrical engineer) Adress: Gansu 803 Electric Powere plant, Gansu Province, China Contact |
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2.1 RT Flaw Detection
In spite of its high sensitivity, the method of the radioisotope test has very limited uses because it is time-consuming, difficult to operate, small in detection scale, dangerous to the operator. Besides, when several bends are arranged in parallel, detection can not be carried out.
2.2 Traditional UT Detector
Because of the point-to-point or line-to-line contact between the conventional detector and the testing sample, it is rather difficult for the detector to beam ultrasonic wave into the pipe bends due to the unregular convex surface of the outer-arc at a pipe bend. To achieve a good contact, the detector need to have a concave surface through grinding (see Fig.3). However, such a grinding process will change all the other pre-set parameters of the detector. Besides, the thickness of the ground wedge of the ultrasonic detector will be greatly reduced and the operation life of the detector will be substantially shortened. Also, the noise level on the monitoring screen will be increased and the accuracy of flaw recognition will be affected (see Fig.4).
Fig 3
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Fig 4 |
Another factor limiting the use of traditional ultrasonic detector is the thickness of pipe walls, which falls in the range of 4~12mm. The near-field distance of a ultrasonic wave is computed from the following equation,
| (1) |
The angle of the detector or is determined by (see Fig.5):
| (2) |
Fig 5 |
In practice R and r will both increase after bending. Based on experimental data, the following mean values are chosen:
R=70mm, r=62mm
Therefore sina=62/70 a »62.30
Since 
sina=2700/3200, b»48.3°
hence l=c/f, l=3200/2500»1.28
If the dimension of the piezocrystal selected for the detector is 9×9mm2, and L is 4mm. Substituting them into (1), we have
N=11.7.
The far field is defined as a=3N,hence
a =3N=11.7×3=35.1
Because the testing object to be inspected has a thickness of 4-12mm,it is obvious that the traditional detector is not feasible for inspection of such pipe bends.
Considering all the factors stated above, it is clear that traditional ultrasonic detectors can not possibly be used to conduct flaw inspection for small and medium diameter pipe bends.
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Fig 7
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Fig 8
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3.2 As stated above, if traditional flat-surface detectors are used for the convex outer-arc of the bend, the detector and the testing object cannot fit each other properly. If the detector is ground to have a concave surface, effective operation thickness of the detector wedge will be reduced and the noise level will rise. To solve these problems, one additional wedge is installed at the trailing edge of the detector (see Fig.7).
3.3 Determining of q
In practical inspection operations, the value of q should be decided according to the thickness of the testing object, so that the focus of two piezocrystal can be targeted at where flaws may most probably occur. A smallerq value will lead to a focus deeper from the surface and form a long, narrow diamond area, which is suitable for inspection of testing object with large thickness. In contrast, a larger q value will result in a focus closer to the surface and form a shorter but wider diamond area. The value of q can be determined through calculation as follows. From Fig.8 it can be seen that the distance between the center of the piezocrystal and the center of emission is 4mm, and the detection depth is 8mm. Therefore
tga=4/8=0.5,a=26.6°, sinq/sinb=2700/3200, q=22°.
The ultrasonic detector developed is shown in Fig.9.
Fig 9:
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Fig 10: |
5.1 Determining the incidence point:
Point a is the incidence point of the detector when it is place at position I and the reflected signal reaches the highest level.
5.2 Adjusting the rate of sweep speed:
Find out the position of the 0.5mm line cuts at distance of 5mm and 10mm by placing the detector at positions II and III on the testing block, respectively. Then adjustment is made to achieve scales of 1:1 or 2:1 on the monitoring screen.
Fig 11
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Fig 12 |
5.3 Sensitivity Adjustment:
In accordance with industrial regulations, the sensitivity for flaw detection on a new pipe should be set at 8% or 10%of the reflection amplitude. However, no sensitivity standard has yet been made for inspecting operating pipelines. If a 0.5mm line cut is used for sensitivity adjustment for inspecting an operating pipeline, the detector may fail to detect some flaws. This is because in practice it has been found out that after the formation of cracks in operating pipelines, corrosion products, such as Fe3O4, in the cracks will absorb some ultrasonic wave so that the reflected signal will be weakened. Therefore, in order to successfully detect a 0.5mm crack, the detector sensitivity required must be higher than that set for the 0.5mm line cut on a new pipe. Experiment shows that this will require a 3~8dB increase on the basis of the 80% amplitude for 0.5mm line cut detection. In practice, an increase of 5mm or 10mm is chosen, depending on the thickness of the testing object. For testing objects with a thickness of 4-6mm, sensitivity adjustment should use the line cut at the place of 5mm; for thickness between 8-12mm,use the line cut at the place of 10mm. Fig.12 shows the actual wave pattern during a flaw detection operation.
5.4 Determining the Type of Flaws
Wave patterns indicating flaws need to be analyzed carefully to decide they might imply a corrosion pit or a crack. Corrosion pits usually do not exceed a length of 10mm, and are scattered all over, i.e., they can be found at different locations on the pipe wall. A crack flaw can be distinctly identified if it is longer than 12mm, and is located within 45°to both sides of the outer-arc, and within 10mm from both sides of the normal direction.
Photo 1: Inner wall crack in the No.2 Boiler down comer at 803 power plant
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Photo 2: Inner wall crack in the No.7 Boiler down comer at Xigu Thermal Power Plant |
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