| Literature DB >> 26091524 |
Yang Li1, Guoqing Li1, Zhenhao Wang1.
Abstract
In order to overcome the problems of poor understandability of the pattern recognition-based transient stability assessment (PRTSA) methods, a new rule extraction method based on extreme learning machine (ELM) and an improved Ant-miner (IAM) algorithm is presented in this paper. First, the basic principles of ELM and Ant-miner algorithm are respectively introduced. Then, based on the selected optimal feature subset, an example sample set is generated by the trained ELM-based PRTSA model. And finally, a set of classification rules are obtained by IAM algorithm to replace the original ELM network. The novelty of this proposal is that transient stability rules are extracted from an example sample set generated by the trained ELM-based transient stability assessment model by using IAM algorithm. The effectiveness of the proposed method is shown by the application results on the New England 39-bus power system and a practical power system--the southern power system of Hebei province.Entities:
Mesh:
Year: 2015 PMID: 26091524 PMCID: PMC4475017 DOI: 10.1371/journal.pone.0130814
Source DB: PubMed Journal: PLoS One ISSN: 1932-6203 Impact factor: 3.240
Fig 1Flowchart of ELM-based rule extraction.
The input features for the New England 39-bus test system.
| No. | Input features |
|---|---|
|
| Mean value of all the mechanical power before the fault incipient time |
|
| Mean value of all the initial acceleration power |
|
| Rotor angular velocity of the machine with the biggest difference relative to the centre of inertia at |
|
| Rotor angle of the machine with the biggest difference relative to the centre of inertia at |
|
| Rotor angular velocity of the machine with the biggest difference relative to the centre of inertia at |
|
| Rotor angle of the machine with the biggest difference relative to the centre of inertia at |
|
| Rotor angular velocity of the machine with the biggest difference relative to the centre of inertia at |
The input features for the southern power system of Hebei province.
| No. | Input features |
|---|---|
|
| Mean value of all the initial acceleration power |
|
| Maximum value of all the rotor kinetic energies at |
|
| Rotor angle of the machine with the biggest difference relative to the centre of inertia at |
|
| Maximum value of the difference of rotor angles at |
|
| Kinetic energy of the machine with the maximum rotor angle at |
|
| Rotor angle of the machine with the biggest difference relative to the centre of inertia at |
|
| Maximum value of the difference of rotor angles at |
|
| Rotor angular velocity of the machine with the biggest difference relative to the centre of inertia at |
|
| Rotor angle of the machine with the biggest difference relative to the centre of inertia at |
|
| Maximum value of the difference of rotor angles at |
|
| Rotor angular velocity of the machine with the biggest difference relative to the centre of inertia at |
Fig 2Flowchart of IAM algorithm.
Fig 3New England 39-bus test system.
Fig 4Transient stable case.
Fig 5Transient unstable case.
Fig 6Influence of the two parameters on accuracy.
Fig 8Influence of the pheromone evaporation rate on accuracy (with 400 ants).
Fig 7Influence of the number of ants on accuracy (with ρ set to 0.85).
Test results in Case-1.
| Method |
|
|
| # | # |
|
|---|---|---|---|---|---|---|
|
| 97.10±0.0096 | 94.24±0.0265 | 0.9794±0.0048 | 10.5±0.24 | 3.72 | 0.9643±0.0116 |
|
| 97.20±0.0102 | 0.94.74±0.0376 | 0.9817±0.0027 | 15.2±0.41 | 4.35 | 0.9670±0.0152 |
|
| 96.36±0.0105 | 0.9468±0.0226 | 0.9824±0.0097 | 18.1±0.32 | 4.81 | 0.9643±0.0102 |
|
| 97.78±0.0088 | 94.93±0.0255 | 0.9819±0.0040 | — | — | 0.9697±0.0117 |
|
| 93.24±0.0134 | 91.64±0.0317 | 0.9671±0.0068 | — | — | 0.9386±0.0145 |
Fig 9The ROC curve in Case-1.
Fig 10The ROC curve in Case-2.
Test results in Case-2.
| Method |
|
|
| # | # |
|
|---|---|---|---|---|---|---|
|
| 95.20±0.0065 | 92.99±0.0183 | 97.76±0.0113 | 18.6±0.18 | 6.04 | 0.9532±0.0046 |
|
| 95.32±0.0079 | 93.21±0.0231 | 0.9791±0.0086 | 21.5±0.33 | 7.21 | 0.9548±0.0069 |
|
| 95.08±0.0081 | 92.88±0.0230 | 97.93±0.0081 | 25.8±0.35 | 8.62 | 0.9530±0.0078 |
|
| 96.44±0.0144 | 93.42±0.0397 | 0.9782±0.0090 | — | — | 0.9589±0.0191 |
|
| 92.36±0.0157 | 89.13±0.0401 | 0.9620±0.0127 | — | — | 0.9256±0.0174 |