High-Current Double Pulse ECT Technique for Inspection of Ferromagnetic Materials

dc.contributor.author Rocha, Tiago
dc.contributor.author Ramos, Helena
dc.contributor.author Ribeiro, Artur
dc.contributor.author Pasadas, Dario
dc.date 2018-02-17T22:41:05.000
dc.date.accessioned 2020-06-30T06:53:29Z
dc.date.available 2020-06-30T06:53:29Z
dc.date.issued 2016-01-01
dc.description.abstract <p>The detection of surface cracks of conductive materials that have a magnetic permeability higher than μ0, are usually made using the Magnetic Flux Leakage (MFL) technique. It requires the saturation of the specimen so that some magnetic flux lines escape the material when a defect is present. However, saturating the material can be very power consuming and if there is motion involved, eddy currents induced due to motion decrease or even null this method sensitivity as speed increases, which can be a disadvantage in cases such as railroad inspection.</p> <p>This work proposes a new technique to inspect the surface of ferromagnetic materials based on eddy currents. It is denominated high-current double pulse (Hi-CDP) ECT. The technique creates two consecutive pulses of currents (up to 1500 A) in a coil in the vicinity of the sample. Fig. 1 shows the simulation model used and the corresponding magnetic flux obtained in a point in the axis of a pancake coil (25 turns, id=15 mm, od=25 mm, heigh=10 mm), and in the vicinity of the sample material. The first pulse (starts at 0.1 ms) saturates the material, making it behave almost like a non-ferromagnetic material. The second pulse starts at 0.25 ms when the maximum current of the first pulse occurs (when the material is most saturated). When the second pulse occurs, eddy currents are induced. As the material is saturated, the ferromagnetic properties almost do not interfere with penetration depth and distribution of eddy currents, making it suitable for eddy current testing. Fig. 2 shows the derivative of the magnetic field obtained in a point located between the windings of the coil and the sample material, for a case without defect and in the presence of two similar defects with different depths (0.5 mm and 1.5 mm deep) in the vicinity of the point. It is possible to observe that the second current peak contains a perturbation that is different according to the defect. The signal derivative was chosen in order to distinguish the MFL from eddy currents perturbations.</p>
dc.format.mimetype application/pdf
dc.identifier archive/lib.dr.iastate.edu/qnde/2016/abstracts/223/
dc.identifier.articleid 4930
dc.identifier.contextkey 9239049
dc.identifier.s3bucket isulib-bepress-aws-west
dc.identifier.submissionpath qnde/2016/abstracts/223
dc.identifier.uri https://dr.lib.iastate.edu/handle/20.500.12876/61976
dc.language.iso en
dc.relation.ispartofseries Review of Progress in Quantitative Nondestructive Evaluation
dc.source.bitstream archive/lib.dr.iastate.edu/qnde/2016/abstracts/223/136_High_Current_Double.pdf|||Fri Jan 14 22:42:52 UTC 2022
dc.subject.disciplines Electromagnetics and Photonics
dc.subject.disciplines Electronic Devices and Semiconductor Manufacturing
dc.subject.disciplines Materials Science and Engineering
dc.subject.disciplines Semiconductor and Optical Materials
dc.title High-Current Double Pulse ECT Technique for Inspection of Ferromagnetic Materials
dc.type event
dc.type.genre event
dspace.entity.type Publication
relation.isSeriesOfPublication 289a28b5-887e-4ddb-8c51-a88d07ebc3f3
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