Power Transformer Partial Discharge (PD) Acoustic Signal Detection using Fiber Sensors and Wavelet Analysis, Modeling, and Simulation

dc.contributor.authorTsai, Shu-Jen Stevenen
dc.contributor.committeechairLiu, Yiluen
dc.contributor.committeememberPhadke, Arun G.en
dc.contributor.committeememberde Wolf, David A.en
dc.contributor.departmentElectrical and Computer Engineeringen
dc.date.accessioned2014-03-14T20:49:02Zen
dc.date.adate2002-12-12en
dc.date.available2014-03-14T20:49:02Zen
dc.date.issued2002-12-06en
dc.date.rdate2003-12-12en
dc.date.sdate2002-12-06en
dc.description.abstractIn this work, we first analyze the behavior of the acoustic wave from the theoretical point of view using a simplified 1-dimensional model. The model was developed based on the conservation of mass, the conservation of momentum, and the state equation; in addition, the fluid medium obeys Stokes assumption and it is homogeneous, adiabatic and isentropic. Experiment and simulation results show consistency to theoretical calculation. The second part of this thesis focuses on the PD signal analysis from an on-site PD measurement of the in-house design fiber optic sensors (by Virginia Tech, Center for Photonics Technology). Several commercial piezoelectric transducers (PZTs) were also used to compare the measurement results. The signal analysis employs the application of wavelet-based denoising technique to remove the noises, which mainly came from vibration, EMI, and light sources, embedded in the PD signal. The denoising technique includes the discrete wavelet transform (DWT) decomposition, thresh-holding of wavelet coefficients, and signal recovery by inverse discrete wavelet transform. Several approaches were compared to determine the optimal mother wavelet. The threshold limits are selected to remove the maximum Gaussian noises for each level of wavelet coefficients. The results indicate that this method could extract the PD spike from the noisy measurement effectively. The frequency of the PD pulse is also analyzed; it is shown that the frequencies lie in the range of 70 kHz to 250 kHz. In addition, with the assumed acoustic wave propagation delay between PD source and sensors, it was found that all PD activities occur in the first and third quadrant in reference to the applied sinusoidal transformer voltage.en
dc.description.degreeMaster of Scienceen
dc.identifier.otheretd-12062002-152858en
dc.identifier.sourceurlhttp://scholar.lib.vt.edu/theses/available/etd-12062002-152858/en
dc.identifier.urihttp://hdl.handle.net/10919/35983en
dc.publisherVirginia Techen
dc.relation.haspartChapter4.pdfen
dc.relation.haspartChapter1.pdfen
dc.relation.haspartVita.pdfen
dc.relation.haspartChapter2.pdfen
dc.relation.haspartChapter3.pdfen
dc.relation.haspartChapter6.pdfen
dc.relation.haspartBibliography.pdfen
dc.relation.haspartAppendixes.pdfen
dc.relation.haspartFront.pdfen
dc.relation.haspartChapter5.pdfen
dc.rightsIn Copyrighten
dc.rights.urihttp://rightsstatements.org/vocab/InC/1.0/en
dc.subjectAcoustic Emissionen
dc.subjectFiber Optic Sensoren
dc.subjectPower Transformeren
dc.subjectPartial Discharge (PD)en
dc.subjectWavelet Transform Denoisingen
dc.titlePower Transformer Partial Discharge (PD) Acoustic Signal Detection using Fiber Sensors and Wavelet Analysis, Modeling, and Simulationen
dc.typeThesisen
thesis.degree.disciplineElectrical and Computer Engineeringen
thesis.degree.grantorVirginia Polytechnic Institute and State Universityen
thesis.degree.levelmastersen
thesis.degree.nameMaster of Scienceen

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