

FOLLOWUS
1.College of Meteorology and Oceanography, National University of Defense Technology, Changsha 410073, China
2.College of Frontier Interdisciplinary Sciences, National University of Defense Technology, Nanjing 211101, China
3.College of Marine Science and Technology, Zhejiang Ocean University, Zhoushan 316022, China
4.College of Marine Science and Ecological Environment, Shanghai Ocean University, Shanghai 201306, China
5.College of Marine Technology and Surveying, Jiangsu Ocean University, Lianyungang 222000, China
mingli152@163.com
Received:20 August 2025,
Accepted:11 October 2025,
Online First:26 May 2026,
Published:01 July 2026
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LI Hongchen,LI Ming,WANG Penghao,et al.Integrating machine learning and physical models for reconstructing sound speed profiles in mesoscale eddies[J].Journal of Oceanology and Limnology,2026,44(04):1323-1341.
LI Hongchen,LI Ming,WANG Penghao,et al.Integrating machine learning and physical models for reconstructing sound speed profiles in mesoscale eddies[J].Journal of Oceanology and Limnology,2026,44(04):1323-1341. DOI: 10.1007/s00343-025-5263-1.
Mesoscale eddies significantly affect sound propagation
yet their complex internal sound speed profiles suffer from substantial reconstruction errors
and only few studies specifically addressed this reconstruction. To bridge this gap
we used multi-source satellite data and Argo profiles to identify eddies and build a temperature-salinity-sound speed dataset. Sea surface parameters (temperature
height anomalies
salinity
density) and Argo density serve as inputs for a random forest (RF) algorithm to learn the surface-to-underwater sound speed mapping. Concurrently
a unified eddy dynamic model reconstructs the internal density field. By combining these environmental parameters with the reconstructed density generates eddy sound speed profiles
an integrated PIRF-DEN model that merges machine learning and physical modeling was established. Evaluations demonstrate the superiority of the model. By incorporating density input
the reconstruction accuracy was significantly improved
the mean absolute error (MAE) and root mean square error (RMSE) were reduced to 0.83 and 1.39 m/s
respectively
which is 87.3% and 83.7% less than that of the sEOFr method. Integration of the eddy model effectively characterized the vertical density structure
whose constraint lowered the overfitting risk and enhanced the accuracy and stability over sEOFr
sEOF-RF
and RF models. Propagation loss calculations using the reconstructed sound speed showed high correlation (coefficient: 0.77) with measured data
further confirming its reliability.
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