Power Generation Technology ›› 2025, Vol. 46 ›› Issue (2): 361-369.DOI: 10.12096/j.2096-4528.pgt.23115
• Power Generation and Environmental Protection • Previous Articles
Lifeng ZHANG, Xianghu DONG
Received:
2024-09-14
Revised:
2024-10-20
Published:
2025-04-30
Online:
2025-04-23
Supported by:
CLC Number:
Lifeng ZHANG, Xianghu DONG. Reconstruction of Temperature Distribution in Acoustic Tomography Based on Robust Regularized Extreme Learning Machine[J]. Power Generation Technology, 2025, 46(2): 361-369.
重建算法 | EARE | ERMSE |
---|---|---|
Tikhonov | 6.59 | 11.11 |
ART | 4.36 | 6.92 |
Landweber | 4.68 | 7.19 |
ELM | 0.26 | 0.38 |
RELM-IRLS | 0.16 | 0.22 |
Tab. 1 Reconstruction errors of single-peak temperature distribution
重建算法 | EARE | ERMSE |
---|---|---|
Tikhonov | 6.59 | 11.11 |
ART | 4.36 | 6.92 |
Landweber | 4.68 | 7.19 |
ELM | 0.26 | 0.38 |
RELM-IRLS | 0.16 | 0.22 |
重建算法 | EARE | ERMSE |
---|---|---|
Tikhonov | 8.10 | 11.70 |
ART | 6.35 | 9.18 |
Landweber | 6.43 | 8.83 |
ELM | 0.44 | 0.62 |
RELM-IRLS | 0.29 | 0.40 |
Tab. 2 Reconstruction errors of double-peak temperature distribution
重建算法 | EARE | ERMSE |
---|---|---|
Tikhonov | 8.10 | 11.70 |
ART | 6.35 | 9.18 |
Landweber | 6.43 | 8.83 |
ELM | 0.44 | 0.62 |
RELM-IRLS | 0.29 | 0.40 |
重建算法 | EARE | ERMSE |
---|---|---|
Tikhonov | 9.02 | 11.59 |
ART | 7.98 | 10.32 |
Landweber | 7.24 | 9.09 |
ELM | 0.54 | 0.72 |
RELM-IRLS | 0.41 | 0.54 |
Tab. 3 Reconstruction errors of four-peak temperature distribution
重建算法 | EARE | ERMSE |
---|---|---|
Tikhonov | 9.02 | 11.59 |
ART | 7.98 | 10.32 |
Landweber | 7.24 | 9.09 |
ELM | 0.54 | 0.72 |
RELM-IRLS | 0.41 | 0.54 |
重建算法 | 单峰 | 双峰 | 四峰 |
---|---|---|---|
Tikhonov | 0.001 | 0.003 | 0.002 |
ART | 0.328 | 0.312 | 0.334 |
Landweber | 0.120 | 0.121 | 0.136 |
ELM | 0.031 | 0.031 | 0.029 |
RELM-IRLS | 0.052 | 0.051 | 0.043 |
Tab. 4 Reconstruction time
重建算法 | 单峰 | 双峰 | 四峰 |
---|---|---|---|
Tikhonov | 0.001 | 0.003 | 0.002 |
ART | 0.328 | 0.312 | 0.334 |
Landweber | 0.120 | 0.121 | 0.136 |
ELM | 0.031 | 0.031 | 0.029 |
RELM-IRLS | 0.052 | 0.051 | 0.043 |
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