Dual-row split meander-line coil EMAT for circumferential A0-mode Lamb waves with full-range magnetic field coupling
Source abstract
Abstract
Electromagnetic acoustic transducers (EMATs) often exhibit poor conversion efficiency and weak output signals when inspecting circumferential defects in thin-walled pipelines. To address this, a novel EMAT employing a dual-row split meander-line coil (DS-MLC-EMAT) is proposed to enhance detection signal energy. This design incorporates a dual-magnet array to improve bias magnetic field uniformity, with the coil specifically tailored for efficient coupling between the magnetic field and induced eddy currents. Three-dimensional multiphysics simulations confirm a significant enhancement in Lorentz force generation: the peak X-component increases by 40%, and the Z-component within the local focal region triples compared to the conventional structure. Consequently, strain energy for the A0 mode becomes more concentrated, amplifying the displacement response by 109.3%. Experimental results show that the optimised sensor with a 0.5 mm row spacing achieves the maximum received signal amplitude, representing a 144.2% increase over the conventional single-magnet EMAT. This novel full-range magnetic field coupling approach provides an effective new solution for circumferential pipeline inspection.
Source: openalex_inverted_index · Quality: baseline
Research context
OpenAlex topics: Acoustic Wave Resonator Technologies · Ultrasonics and Acoustic Wave Propagation · Magnetic properties of thin films
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
Affiliations
North University of China
Shanxi Jinxi Precision Machinery Co. Ltd, Jinxi Industries Group Co. Ltd
China Special Equipment Inspection & Research Institute
Funding
the National Natural Science Foundation of China · Science and Technology Program of the State Administration for Market Regulation of China
References (34)
Show source-provided references
1. 10.1007/s11661-016-3939-z10.1007/s11661-016-3939-z ↗
2. 10.1016/j.ptlrs.2020.11.00110.1016/j.ptlrs.2020.11.001 ↗
3. 10.1016/j.tafmec.2022.10373010.1016/j.tafmec.2022.103730 ↗
4. 10.1016/S0020-7683(96)00197-710.1016/S0020-7683(96)00197-7 ↗
5. 10.1016/S0041-624X(96)00098-410.1016/S0041-624X(96)00098-4 ↗
6. 10.1088/0964-1726/18/8/08501110.1088/0964-1726/18/8/085011 ↗
7. 10.1016/j.ultras.2020.10609410.1016/j.ultras.2020.106094 ↗
8. 10.1016/j.jsv.2006.01.02010.1016/j.jsv.2006.01.020 ↗
9. 10.1143/JJAP.45.454110.1143/JJAP.45.4541 ↗
10. 10.1109/JSEN.2022.322232510.1109/JSEN.2022.3222325 ↗
11. 10.1016/j.ultras.2022.10672910.1016/j.ultras.2022.106729 ↗
12. 10.1016/j.ijpvp.2016.11.00710.1016/j.ijpvp.2016.11.007 ↗
13. 10.1016/j.ndteint.2019.10214210.1016/j.ndteint.2019.102142 ↗
14. 10.1016/j.ultras.2024.10749310.1016/j.ultras.2024.107493 ↗
15. 10.1109/TUFFC.2016.255846710.1109/TUFFC.2016.2558467 ↗
16. 10.1109/JSEN.2023.328882710.1109/JSEN.2023.3288827 ↗
17. 10.1007/s10921-021-00771-z10.1007/s10921-021-00771-z ↗
18. 10.3233/JAE-23014710.3233/JAE-230147 ↗
19. 10.1016/j.ultras.2014.06.01210.1016/j.ultras.2014.06.012 ↗
20. 10.3390/s2321884310.3390/s23218843 ↗
21. 10.1080/10589759.2024.235663610.1080/10589759.2024.2356636 ↗
22. 10.1515/teme-2019-012410.1515/teme-2019-0124 ↗
23. 10.1016/j.ultras.2019.06.00710.1016/j.ultras.2019.06.007 ↗
24. 10.1016/j.ndteint.2021.10249210.1016/j.ndteint.2021.102492 ↗
25. 10.1016/j.ultras.2017.05.01410.1016/j.ultras.2017.05.014 ↗
26. 10.1109/JSEN.2021.311145610.1109/JSEN.2021.3111456 ↗
27. 10.3390/s1705102310.3390/s17051023 ↗
28. 10.1088/1674-1056/27/8/08430110.1088/1674-1056/27/8/084301 ↗
29. 10.1109/JSEN.2023.334847710.1109/JSEN.2023.3348477 ↗
30. 10.1016/j.ndteint.2024.10323110.1016/j.ndteint.2024.103231 ↗
31. 10.1109/TUFFC.2019.295671110.1109/TUFFC.2019.2956711 ↗
32. 10.1016/j.ndteint.2024.10317210.1016/j.ndteint.2024.103172 ↗
33. 10.3390/mi1604036710.3390/mi16040367 ↗
34. 10.1016/j.ndteint.2013.05.00310.1016/j.ndteint.2013.05.003 ↗