EGU24-1943, updated on 08 Mar 2024
https://doi.org/10.5194/egusphere-egu24-1943
EGU General Assembly 2024
© Author(s) 2024. This work is distributed under
the Creative Commons Attribution 4.0 License.

Annual evolution of the ice–ocean interaction beneath landfast ice in Prydz Bay, East Antarctica

Haihan Hu1,2, Jiechen Zhao3,4, Petra Heil5, Zhiliang Qin3,4, Jingkai Ma6, Fengming Hui1,2, and Xiao Cheng1,2
Haihan Hu et al.
  • 1School of Geospatial Engineering and Science, Sun Yat-sen University, and Southern Marine Science and Engineering Guangdong Laboratory (Zhuhai), Zhuhai 519082, China
  • 2Key Laboratory of Comprehensive Observation of Polar Environment (Sun Yat-sen University), Ministry of Education, Zhuhai 519082, China
  • 3Qingdao Innovation and Development Base (Centre) of Harbin Engineering University, Qingdao, 266500, China
  • 4College of Underwater Acoustic Engineering, Harbin Engineering University, Harbin 150001, China
  • 5Australia Antarctic Division & Australian Antarctic Programmer Partnership, Private Bag 80, Hobart TAS 7001, Australia
  • 6Key Laboratory of Research on Marine Hazards Forecasting, National Marine Environmental Forecasting Centre, Beijing 100081, China

High-frequency observations of the ice–ocean interaction and high-precision estimation of the ice–ocean heat exchange are critical to understanding the thermodynamics of the landfast ice mass balance in Antarctica. To investigate the oceanic contribution to the evolution of the landfast ice, an integrated ocean observation system, including an acoustic Doppler velocimeter (ADV), conductivity–temperature–depth (CTD) sensors, and a sea ice mass balance array (SIMBA), was deployed on the landfast ice near Chinese Zhongshan Station in Prydz Bay, East Antarctica from April to November 2021. The CTD sensors recorded the ocean temperature and salinity. The ocean temperature experienced a rapid increase in late April, from −1.62°C to the maximum of −1.30°C, and then, it gradually decreased to −1.75°C in May and remained at this temperature until November. The seawater salinity and density exhibited similar increasing trends during April and May, with mean rates of 0.04 psu day1 and 0.03 kg m3 day1, respectively, which was related to the strong salt rejection caused by freezing of the landfast ice. The ocean current observed by the ADV had mean horizontal and vertical velocities of 9.5±3.9 cm s1 and 0.2±0.8 cm s1, respectively. The domain current direction was ESE (120°)–WSW (240°), and the domain velocity (79%) was 5–15 cm s1. The oceanic heat flux (Fw) estimated using the residual method reached a peak of 41.3±9.8 W m2 in April, and then, it gradually decreased to a stable level of 7.8±2.9 W m2 from June to October. The Fw values calculated using three different bulk parameterizations exhibited similar trends with different magnitudes due to the uncertainties of the empirical friction velocity. The spectral analysis results suggest that all of the observed ocean variables exhibited a typical half-day period, indicating the strong diurnal influence of the local tidal oscillations. The large-scale sea ice distribution and ocean circulation contributed to the seasonal variations in the ocean variables, revealing the important relationship between the large-scale and local phenomena. The high frequency and cross-seasonal observations of oceanic variables obtained in this study allow us to deeply investigate their diurnal and seasonal variations and to evaluate their influences on the landfast ice evolution.

How to cite: Hu, H., Zhao, J., Heil, P., Qin, Z., Ma, J., Hui, F., and Cheng, X.: Annual evolution of the ice–ocean interaction beneath landfast ice in Prydz Bay, East Antarctica, EGU General Assembly 2024, Vienna, Austria, 14–19 Apr 2024, EGU24-1943, https://doi.org/10.5194/egusphere-egu24-1943, 2024.