1. Institute for Information and Communication Technologies, University of Applied Sciences and Arts Western Switzerland (HES-SO), Yverdon-les-Bains,Switzerland
2. Ecole Polytechnique Fédérale de Lausanne (EPFL), Electromagnetic Compatibility Laboratory,Lausanne,Switzerland
3. Department of Electrical and Electronic Engineering, Imperial College London,London,UK
4. State Key Laboratory of Electrical Insulation and Power Equipment, School of Electrical Engineering, Xi'an Jiaotong University,Xi'an,China
5. Department of Electrical Engineering, Bu-Ali Sina University, Hamedan,Iran
纸质出版:2025
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Hamidreza Karami, Zhaoyang Wang, Parsa Khorasani, 等. An experimental proof of concept of time-reversal single-sensor acoustic source localisation: Application to partial discharges[J]. 高电压(英文), 2025,10(2).
Hamidreza Karami, Zhaoyang Wang, Parsa Khorasani, et al. An experimental proof of concept of time-reversal single-sensor acoustic source localisation: Application to partial discharges[J]. High Voltage, 2025, 10(2).
Hamidreza Karami, Zhaoyang Wang, Parsa Khorasani, 等. An experimental proof of concept of time-reversal single-sensor acoustic source localisation: Application to partial discharges[J]. 高电压(英文), 2025,10(2). DOI: 10.1049/hve2.70008.
Hamidreza Karami, Zhaoyang Wang, Parsa Khorasani, et al. An experimental proof of concept of time-reversal single-sensor acoustic source localisation: Application to partial discharges[J]. High Voltage, 2025, 10(2). DOI: 10.1049/hve2.70008.
In this paper
for the first time
an experimental proof of concept for utilising time reversal (TR) in the acoustic regime to localise partial discharge (PD) sources was presented using a single sensor. To achieve this
an experimental setup comprising a water tank
acoustic transducers for signal transmission and reception
and 2D scanners was developed. The performance of the proposed method was evaluated across various scenarios
encompassing different PD source locations and sensor placements
barriers obstructing the line of sight between the receiving sensor and PD sources
varying levels of noise
and different frequency bandwidths for the PD sources. The experimental results demonstrate a near-zero localisation error in all considered examples. The achieved resolution was approximately half of the minimum wavelength. Furthermore
the acoustic TR method exhibits remarkable precision in source localisation
even when faced with obstacles such as a multi-layered metallic cylinder and in scenarios lacking a direct line of sight between the sensor and the source. The accuracy of acoustic TR's localisation remained robust in the presence of noise
showcasing resilience at signal-to-noise ratio levels as low as −20 dB. Additionally
the performance of the acoustic TR method remained consistent across a broad frequency spectrum
spanning from 60 to 200 kHz.
In this paper
for the first time
an experimental proof of concept for utilising time reversal (TR) in the acoustic regime to localise partial discharge (PD) sources was presented using a single sensor. To achieve this
an experimental setup comprising a water tank
acoustic transducers for signal transmission and reception
and 2D scanners was developed. The performance of the proposed method was evaluated across various scenarios
encompassing different PD source locations and sensor placements
barriers obstructing the line of sight between the receiving sensor and PD sources
varying levels of noise
and different frequency bandwidths for the PD sources. The experimental results demonstrate a near-zero localisation error in all considered examples. The achieved resolution was approximately half of the minimum wavelength. Furthermore
the acoustic TR method exhibits remarkable precision in source localisation
even when faced with obstacles such as a multi-layered metallic cylinder and in scenarios lacking a direct line of sight between the sensor and the source. The accuracy of acoustic TR's localisation remained robust in the presence of noise
showcasing resilience at signal-to-noise ratio levels as low as −20 dB. Additionally
the performance of the acoustic TR method remained consistent across a broad frequency spectrum
spanning from 60 to 200 kHz.
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