Classification of Partial Discharges Recorded by the Method Using the Phenomenon of Scintillation
Abstract
:1. Introduction
2. Methodology
- the electrical discharge generation system, which consisted of a set of spark gaps, a high-voltage transformer, a voltage divider and a control panel,
- a wireless system for controlling the measurement panel, which consisted of an XBee module and an integrated circuit,
- a system for measuring high-energy radiation, consisting of a scintillation detector based on a scintillation crystal, a photomultiplier and a measurement card.
- type 1: electrodes in oil, blade-to-blade configuration,
- type 2: electrodes in oil with argon bubbles, blade-to-blade configuration,
- type 3: electrodes in oil with air bubbles, blade-to-blade configuration, detector distance 0 mm,
- type 4: electrodes in oil with air bubbles, blade-to-blade configuration, detector distance 80 mm,
- type 5: electrodes in oil with air bubbles, blade-to-blade configuration, detector distance 120 mm.
3. Results and Discussion
4. Conclusions
- the best classifiers for the first group of data turned out to be the linear discriminant analysis algorithm and the SVM support vector machine, for which the accuracy was more than 99%,
- the best classifiers for the second group of data were packed decision trees, for which the accuracy was more than 95%,
- it was possible to achieve high classification efficiency for both data sets, as shown by the values of the measures collected in the tables close to the value of 1.
Author Contributions
Funding
Conflicts of Interest
References
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The Value of the Gamma Parameter | The k Value of Cross-Validation | Sensitivity | Specificity | Precision | Accuracy | F1-Score | Average |
---|---|---|---|---|---|---|---|
0 | 5 | 0.99 | 1.00 | 0.99 | 0.99 | 0.99 | 1.00 |
10 | 0.99 | 1.00 | 0.99 | 0.99 | 0.99 | 1.00 | |
15 | 0.99 | 1.00 | 0.99 | 0.99 | 0.99 | 1.00 | |
0.5 | 5 | 0.99 | 0.99 | 0.99 | 0.99 | 0.99 | 0.99 |
10 | 0.99 | 0.99 | 0.99 | 0.99 | 0.99 | 0.99 | |
15 | 0.99 | 0.99 | 0.99 | 0.99 | 0.99 | 0.99 | |
1 | 5 | 0.98 | 0.99 | 0.98 | 0.98 | 0.98 | 0.98 |
10 | 0.96 | 0.98 | 0.96 | 0.96 | 0.96 | 0.97 | |
15 | 0.98 | 0.99 | 0.98 | 0.98 | 0.98 | 0.98 |
The Value of the KernelScale Parameter | The k Value of Cross-Validation | Sensitivity | Specificity | Precision | Accuracy | F1-Score | Average |
---|---|---|---|---|---|---|---|
0 | 5 | 1.00 | 1.00 | 1.00 | 1.00 | 1.00 | 1.00 |
10 | 0.99 | 1.00 | 0.99 | 0.99 | 0.99 | 0.99 | |
15 | 0.99 | 1.00 | 0.99 | 0.99 | 0.99 | 1.00 | |
10 | 5 | 0.96 | 0.98 | 0.96 | 0.96 | 0.96 | 0.96 |
10 | 0.96 | 0.98 | 0.96 | 0.96 | 0.96 | 0.97 | |
15 | 0.96 | 0.98 | 0.96 | 0.96 | 0.96 | 0.97 | |
15 | 5 | 0.33 | 0.67 | 0.66 | 0.34 | 0.34 | 0.47 |
10 | 0.33 | 0.67 | 0.67 | 0.34 | 0.34 | 0.47 | |
15 | 0.33 | 0.67 | 0.66 | 0.34 | 0.34 | 0.47 |
NumLearning Cycles Parameter Value | The k Value of Cross-Validation | Sensitivity | Specificity | Precision | Accuracy | F1-Score | Average |
---|---|---|---|---|---|---|---|
30 | 5 | 0.90 | 0.98 | 0.98 | 0.95 | 0.94 | 0.95 |
10 | 0.90 | 0.98 | 0.97 | 0.94 | 0.94 | 0.95 | |
15 | 0.90 | 0.99 | 0.99 | 0.95 | 0.94 | 0.96 | |
50 | 5 | 0.90 | 0.99 | 0.98 | 0.95 | 0.94 | 0.95 |
10 | 0.90 | 0.99 | 0.99 | 0.95 | 0.94 | 0.96 | |
15 | 0.89 | 0.99 | 0.99 | 0.95 | 0.94 | 0.95 | |
100 | 5 | 0.89 | 0.99 | 0.99 | 0.95 | 0.94 | 0.95 |
10 | 0.90 | 0.99 | 0.98 | 0.95 | 0.94 | 0.95 | |
15 | 0.89 | 0.99 | 0.98 | 0.94 | 0.94 | 0.95 |
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Płużek, A.; Nagi, Ł. Classification of Partial Discharges Recorded by the Method Using the Phenomenon of Scintillation. Energies 2023, 16, 201. https://doi.org/10.3390/en16010201
Płużek A, Nagi Ł. Classification of Partial Discharges Recorded by the Method Using the Phenomenon of Scintillation. Energies. 2023; 16(1):201. https://doi.org/10.3390/en16010201
Chicago/Turabian StylePłużek, Aleksandra, and Łukasz Nagi. 2023. "Classification of Partial Discharges Recorded by the Method Using the Phenomenon of Scintillation" Energies 16, no. 1: 201. https://doi.org/10.3390/en16010201
APA StylePłużek, A., & Nagi, Ł. (2023). Classification of Partial Discharges Recorded by the Method Using the Phenomenon of Scintillation. Energies, 16(1), 201. https://doi.org/10.3390/en16010201