journal article·2024-10-02

Distributed point source method for eddy current modelling

Pu Huang, Xiaofei Huang, Zhiying Li, Yuedong Xie

Publisher page

Abstract

Distributed point source method (DPSM) has been gradually applied to the field of nondestructive testing (NDT). As a semi-analytical modelling technique, DPSM is extremely powerful and straightforward for solving various engineering problems, such as ultrasonic fields and electromagnetic field. In this paper, the technique is extended to model the eddy current field including sweep frequency measurement and scanning defect. The configuration of eddy current sensors consists of excitation coil and solid-state magnetic field measurement sensors such as Hall device and giant magnetoresistive sensor. Besides that, the wave propagation has been described and magnetic field created by eddy current has been calculated. The results obtained by DPSM is compared with that calculated by finite element method (FEM) in terms of accuracy and computation time, which indicates DPSM can improve calculation speed while ensuring calculation accuracy.
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Research context

OpenAlex topics: Non-Destructive Testing Techniques · Geophysical Methods and Applications · Ultrasonics and Acoustic Wave Propagation

SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.

Affiliations

Key Laboratory of Precision Opto-mechatronics Technology of Education Ministry, School of Instrumentation and Opto-Electronic Engineering, Beihang University, Beijing, China

Funding

Fundamental Research Funds for the Central Universities · National Natural Science Foundation of China · Academic Excellence Foundation of BUAA for PhD Students

References (25)

Show source-provided references
1. Liu G, Gao W, Liu W, et al. LFM-Chirp-square pulse-compression thermography for debonding defects detection in honeycomb sandwich composites based on THD-processing technique. Case Stud NondestrTest Eval. 2023;1–14.
2. 10.1080/10589759.2016.122630310.1080/10589759.2016.1226303 ↗
3. 10.1109/TIM.2008.92377710.1109/TIM.2008.923777 ↗
4. 10.1080/10589759.2020.171461410.1080/10589759.2020.1714614 ↗
5. 10.1080/10589759.2022.207793910.1080/10589759.2022.2077939 ↗
6. 10.1109/TIM.2022.318802910.1109/TIM.2022.3188029 ↗
7. 10.1016/j.ndteint.2016.02.01010.1016/j.ndteint.2016.02.010 ↗
8. 10.1109/JSEN.2020.296520110.1109/JSEN.2020.2965201 ↗
9. 10.1016/j.sna.2012.10.01110.1016/j.sna.2012.10.011 ↗
10. 10.1063/1.165668010.1063/1.1656680 ↗
11. 10.1063/1.165839910.1063/1.1658399 ↗
12. 10.1109/TMAG.2005.84483810.1109/TMAG.2005.844838 ↗
13. 10.1109/TMAG.2007.90493010.1109/TMAG.2007.904930 ↗
14. 10.1109/TMAG.2022.315205810.1109/TMAG.2022.3152058 ↗
15. 10.1109/TMAG.2019.295432310.1109/TMAG.2019.2954323 ↗
16. 10.1109/TAP.2020.304855010.1109/TAP.2020.3048550 ↗
17. 10.1109/TIM.2022.318607310.1109/TIM.2022.3186073 ↗
18. 10.1109/TMECH.2014.238253210.1109/TMECH.2014.2382532 ↗
19. 10.1016/j.ultras.2009.12.00310.1016/j.ultras.2009.12.003 ↗
20. 10.1016/j.ultras.2018.09.00210.1016/j.ultras.2018.09.002 ↗
21. 10.1016/j.ultras.2010.12.01110.1016/j.ultras.2010.12.011 ↗
22. 10.1016/j.ultras.2017.03.00910.1016/j.ultras.2017.03.009 ↗
23. 10.2528/PIER1403240510.2528/PIER14032405 ↗
24. 10.1016/j.ultras.2009.02.00810.1016/j.ultras.2009.02.008 ↗
25. 10.1002/978047014240010.1002/9780470142400 ↗