Seasonal variability of ?15N in settling particles in the Arabian Sea and its palaeogeochemical significance

1993 ◽  
Vol 80 (11) ◽  
pp. 511-513 ◽  
Author(s):  
P. Sch�fer ◽  
V. Ittekkot
2008 ◽  
Vol 43 (3) ◽  
pp. 147-152 ◽  
Author(s):  
TVS Udaya Bhaskar ◽  
Debadatta Swain ◽  
M Ravichandran

1998 ◽  
Vol 103 (C1) ◽  
pp. 1167-1176 ◽  
Author(s):  
Prabir K. Patra ◽  
Shyam Lal ◽  
S. Venkataramani ◽  
Mangesh Gauns ◽  
V. V. S. S. Sarma

2011 ◽  
Vol 8 (6) ◽  
pp. 2377-2415 ◽  
Author(s):  
F. M. Bingham ◽  
G. R. Foltz ◽  
M. J. McPhaden

Abstract. The seasonal variability of surface layer salinity (SLS), evaporation (E), precipitation (P) and E-P over the global ocean is examined using in situ salinity data and the National Center for Environmental Prediction's Climate System Forecast Reanalysis. Seasonal amplitudes and phases are calculated using harmonic analysis and presented in all areas of the open ocean between 60° S and 60° N. Areas with large amplitude SLS seasonal variations include: the intertropical convergence zone in the Atlantic, Pacific and Indian Oceans; western marginal seas of the Pacific; and the Arabian Sea. The median value in areas that have statistically significant seasonal cycles of SLS is 0.19. Between about 60° S and 60° N, 37 % of the ocean surface has a significant seasonal cycle of SLS and 75 % a seasonal cycle of E-P. Phases of SLS have a bimodal distribution, with most areas of the ocean peaking in SLS in either March/April or September/October. The same calculation is done with surface freshwater flux using a mixed-layer depth climatology. With the exception of an area near the western boundaries of the North Atlantic and North Pacific, seasonal variability is dominated by precipitation. Surface freshwater fluxes also have a bimodal distribution, with peaks in January and July, 1–2 months before the peaks of SLS. The amplitudes and phases of SLS and surface fluxes compare well in a qualitative sense, suggesting that much of the variability in SLS is due to E-P forcing. However, the amplitudes of SLS are somewhat larger than would be expected and the peak of SLS comes typically about one month earlier than expected. The differences of the amplitudes of the two quantities is largest in such areas as the Amazon River plume, the Arabian Sea, the ITCZ and the eastern equatorial Pacific and Atlantic, indicating that other processes such as ocean mixing and lateral transport must be important, especially in the tropics.


2008 ◽  
Vol 38 (3) ◽  
pp. 624-638 ◽  
Author(s):  
Pankajakshan Thadathil ◽  
Prasad Thoppil ◽  
R. R. Rao ◽  
P. M. Muraleedharan ◽  
Y. K. Somayajulu ◽  
...  

Abstract The formation mechanisms of the barrier layer (BL) and its seasonal variability in the Arabian Sea (AS) are studied using a comprehensive dataset of temperature and salinity profiles from Argo and other archives for the AS. Relatively thick BL of 20–60 m with large spatial extent is found in the central-southwestern AS (CSWAS), the convergence zone of the monsoon wind, during the peak summer monsoon (July–August) and in the southeastern AS (SEAS) and northeastern AS (NEAS) during the winter (January–February). Although the BL in the SEAS has been reported before, the observed thick BL in the central-southwestern AS during the peak summer monsoon and in the northeastern AS during late winter are the new findings of this study. The seasonal variability of BL thickness (BLT) is closely related to the processes that occur during summer and winter monsoons. During both seasons, the Ekman processes and the distribution of low-salinity waters in the surface layer show a dominant influence on the observed BLT distributions. In addition, Kelvin and Rossby waves also modulate the observed BL thickness in the AS. The relatively low salinity surface water overlying the Arabian Sea high-salinity water (ASHSW) provides an ideal ground for strong haline stratification in the CSWAS (during summer monsoon) and in NEAS (during winter monsoon). During summer, northward advection of equatorial low-salinity water by the Somali Current and the offshore advection of low-salinity water from the upwelling region facilitate the salinity stratification that is necessary to develop the observed BL in the CSWAS. In the SEAS, during winter, the winter monsoon current (WMC) carries less saline water over relatively high salinity ambient water to form the observed BL there. The winter West India Coastal Current (WICC) transports the low-salinity water from the SEAS to the NEAS, where it lies over the subducted ASHSW leading to strong haline stratification. Ekman pumping together with the downwelling Kelvin wave in the NEAS deepen the thermocline to cause the observed thick BL in the NEAS.


1998 ◽  
Vol 45 (10-11) ◽  
pp. 2001-2025 ◽  
Author(s):  
T. Dickey ◽  
J. Marra ◽  
D.E. Sigurdson ◽  
R.A. Weller ◽  
C.S. Kinkade ◽  
...  

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