Fiber Optic Fabry-Perot Sensor with Stabilization Technology for Acoustic Emission Detection of Partial Discharge

Author(s):  
Wei-chao ZHANG ◽  
Qi-chao CHEN ◽  
Li-yong ZHANG ◽  
Hong ZHAO
2004 ◽  
Vol 124 (2) ◽  
pp. 274-280 ◽  
Author(s):  
Tadamitsu Kaneko ◽  
Akito Takemura ◽  
Osamu Takenouchi ◽  
Youl-Moon Sung ◽  
Masahisa Otsubo ◽  
...  

2015 ◽  
Vol 23 (11) ◽  
pp. 3069-3076
Author(s):  
赵江海 ZHAO Jiang-hai ◽  
章小建 ZHANG Xiao-jian

Author(s):  
Yomna Omran Shaker

<span>Partial discharge is one the most important factor that leads to deteroration and failure of the power transformer transformer. Acoustic emission detection is effective method to evaluate the health index of the power transformer.      Using acoustic emission (AE) sensors for partial discharge (PD) measurement is considered as one of the most promising techniques to detect and localize PD activities inside the transformer tank. On the other hand, AE waves suffer from high attenuation and reflections while traveling from the PD source to the AE sensor. The modeling of the AE wave can help to understand the behavior of the AE PD signal during its travel. In this paper, the AE PD signal is assumed to be composed of different frequencies. This work aims to investigate the influence of the frequency value on the attenuation and arrival time of the acoustic wave.</span>


2021 ◽  
Vol 29 (11) ◽  
pp. 2613-2621
Author(s):  
Wen-rong SI ◽  
◽  
Chen-zhao FU ◽  
Jian BU ◽  
He-li NI ◽  
...  

2021 ◽  
pp. 18-29
Author(s):  
A. N. Seryeznov ◽  
L. N. Stepanova ◽  
S. I. Kabanov ◽  
I. S. Kabanov ◽  
V. V. Chernova ◽  
...  

The issues are considered of acoustic emission (AE) signals location generated by various simulators (Su–Nielsen, electronic simulator, metal balls of various diameter from 0.5 to 1.5 mm, dropped from different heights). Signals generated by built-in electronic simulator with a frequency of 1 Hz location is analyzed performed by an antenna consisting of two Fabry–Perot fiber-optic sensors (FOS) and two piezoelectric transducers, mounted on samples made of duralumin and T800 carbon fiber. A carbon fiber reinforced plastic sample with the defined above antenna mounted was tested with a VEDS-10 vibration stand. AE signals were registered under the vibration frequency of 20…50 Hz in the acceleration range of 0.3…0.8g. The influence of the time drift recorded by the piezoelectric transducers on the measurement results is determined. It was found that the time drift was not recorded by fiber-optic FOS sensors, but their sensitivity is more than 14 times less than that of piezoelectric transducers.


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