Abstract

High-resolution ocean general circulation model (OGCM) simulations are employed to investigate interannual variability of the upper-ocean temperature in the tropical Indian Ocean (20°S–20°N). The seasonal cycle and interannual variability in the upper-ocean temperature in the tropical Indian Ocean in the forced ocean simulation are in good agreement with available observation and reanalysis products. Two further sensitivity OGCM simulations are used to separate the relative contributions of heat flux and wind stress. The comparison of the model simulations reveals the depth-dependent influences of heat flux and wind stress on the ocean temperature variability in the tropical Indian Ocean. Generally, heat flux dominates the temperature variability in the top 30 m, while wind stress contributes most strongly to the subsurface temperature variability below 30 m. This implies that a transition depth should exist at each location, where the dominant control of the ocean temperature variability switched from heat flux to wind stress. We define the depth of this transition point as the ‘crossing depth’ and make use of this concept to better understand the depth-dependent impacts of the heat flux and wind stress on the upper-ocean temperature variability in the tropical Indian Ocean. The crossing depth tends to be shallower in the southern tropical Indian Ocean (20°S-EQ), including the Seychelles-Chagos Thermocline Ridge (SCTR) and the eastern part of the Indian Ocean Dipole (IOD), suggesting the dominance of forcing due to wind stress and the resulting ocean dynamical processes in the temperature variability in those regions. The crossing depth also shows prominent seasonal variability in the southern tropical Indian Ocean. In the SCTR, the variability of the subsurface temperature forced by the wind stress dominates largely in boreal winter and spring, resulting in the shallow crossing depth in these seasons. In contrast, the intensified subsurface temperature variability with shallow crossing depth in the eastern part of the IOD is seen during boreal autumn. Overall, our results suggest that the two regions within the tropical Indian Ocean, the SCTR and the eastern part of the IOD, are the primary locations where the ocean dynamics due to wind-stress forcing control the upper-ocean temperature variability.

Highlights

  • Prominent warming has been observed throughout the global upper-ocean since the 1950 s (Levitus et al 2009, 2012)

  • Depth-dependent effect of heat flux and wind stress forcing on the interannual variability of the upper-ocean temperature fields Previous studies have shown that interannual variability of the upper-ocean temperature in the tropical Indian Ocean features a significant seasonal phaselocking related to El Niño-Southern Oscillation (ENSO) and Indian Ocean Dipole (IOD) (e.g. Behera et al 2000, Huang and Kinter 2002)

  • WS underestimates the variability seen in ALL in the surface layer, only to become comparable to ALL in the deeper ocean. This highlights the depth-dependent role of wind stress and heat flux forcing in determining interannual variability of upper-ocean temperature in the tropical Indian Ocean

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Summary

Introduction

Prominent warming has been observed throughout the global upper-ocean since the 1950 s (Levitus et al 2009, 2012). Existing studies indicate that atmospheric circulation patterns are closely related to the upper-ocean temperature and sea surface temperature (SST) variability in the tropical Indian Ocean (e.g. Ashok et al 2004, Annamalai et al 2005, Trenary and Han 2012). Net heat flux and wind stress are the main drivers of the variability in SST and subsurface ocean temperature on seasonal to interannual timescales (e.g. Behera et al 2000, Rao and Sivakumar 2000, Schott et al 2009, Sayantani and Gnanaseelan 2015). Is the net heat flux the main driver for seasonal variability of upper-ocean temperature in most areas of the tropical Indian Ocean (Rao and Sivakumar 2000, Cyriac et al 2019), but it plays a vital role in controlling interannual SST variations associated with the El Niño-Southern Oscillation (ENSO) (Behera et al 2000). Heat flux into the ocean in the tropical Indian Ocean is shown to be enhanced during the El Niño years in association with the induced atmospheric circulation changes (i.e. atmospheric bridge) (Klein et al 1999, Alexander et al 2002, Lau and Nath 2003, Liu and Alexander 2007), often inducing basin-wide warming during boreal winter (Shinoda et al 2004a, Zhong et al 2005)

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