College of Aviation Electromechanical Equipment Maintenance, Changsha Aeronautical Vocational and Technical College, Changsha 410124, China.
Key Laboratory of Nondestructive Testing, Ministry of Education, Nanchang Hangkong University, Nanchang 330063, China.
Sensors (Basel). 2023 Jan 18;23(3):1135. doi: 10.3390/s23031135.
Fundamental theory and methods are investigated of inspecting tubing and casing simultaneously using pulsed eddy current testing by numerical simulations and experiments. The distribution and variation of eddy current field are given in the finite element simulation for the inspection of undamaged and corroded casing and tubing combinations, with tubing outer diameter 73.8 mm, wall thickness 5.7 mm, corrosion depth 1.25 mm, 2.5 mm, 3.75 mm, and casing outer diameter 141.5 mm, wall thickness 7.7 mm, corrosion depth 1.25 mm, 2.5 mm, and 3.75 mm, respectively. The results show that eddy current field propagates around and to the depth after the direct section of the exciting current is cut off and the intensity center of eddy current field shifts gradually from the inner side of the tubing to the casing, which forms the basis of analyzing inspection mechanism. Corrosion at a particular depth is related to a particular optimum time slice of the induced voltage (namely with deepest concave) and a highest sensitivity is obtained at this slice. The time associated with this slice is in accordance with the time when the intensity center of eddy current reaches the corrosion. Corrosion at different depths has different voltage time slices starting to show signal of defect, which can be used to estimate the depth of the defect in order to judge the defect coming from tubing or casing. Furthermore, sinking degree of the time slice reflects the size of the defect. All machined defects can be recognized in the experiments and the optimum time slice appears at 0.01 s and 0.008 s after the excitation current is cut off for the tubing corrosion of 1.25 mm and 2.5 mm, respectively. The optimum time slice appears at the last moment of cut-off period, 0.625, for the casing corrosion. Experimental results agree well with the simulations and show the existence of the optimum correspondence between depth of corrosion and starting time of the defect signal of time slice, relations between sinking degree of the time slice, and corrosion size.
本文通过数值模拟和实验研究了采用脉冲涡流检测技术同时检测油管和套管的基本理论和方法。针对外径为 73.8mm、壁厚为 5.7mm、腐蚀深度为 1.25mm、2.5mm 和 3.75mm 的油管和外径为 141.5mm、壁厚为 7.7mm、腐蚀深度为 1.25mm、2.5mm 和 3.75mm 的套管的无损伤和腐蚀组合体的检测,给出了有限元模拟中涡流场的分布和变化。结果表明,激励电流直接部分切断后,涡流场在周围传播并深入,涡流场强度中心逐渐从油管内侧向套管移动,这为分析检测机理奠定了基础。在特定深度的腐蚀与特定的感应电压最佳时片(即具有最深凹度)有关,并且在该时片处获得最高的灵敏度。与该时片相关联的时间与涡流强度中心到达腐蚀的时间一致。不同深度的腐蚀具有不同的起始缺陷信号的电压时片,可以用来估计缺陷的深度,以判断缺陷来自油管还是套管。此外,时片的下沉程度反映了缺陷的大小。在实验中可以识别所有加工缺陷,并且对于壁厚为 1.25mm 和 2.5mm 的油管腐蚀,激励电流切断后最佳时片分别出现在 0.01s 和 0.008s 之后。套管腐蚀的最佳时片出现在截止周期的最后时刻,即 0.625 之后。实验结果与模拟结果吻合较好,表明腐蚀深度与时间切片缺陷信号起始时间之间存在最佳对应关系,时间切片下沉程度与腐蚀尺寸之间存在关系。