Turbulent diffusion, advection, and water structure in the North Indian Ocean

Typescript. Bibliography: leaves 131-133. xi, 133 l charts, graphs, maps, tables Contraction of volume that occurs when sea waters mix is shown to be the mechanism which controls density structure at intermediate depths in the North Indian Ocean. This is the main result of a study in which mean annu...

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Bibliographic Details
Main Author: Bennett, Edward Bertram
Format: Thesis
Language:English
Published: [Honolulu] 1970
Subjects:
Online Access:http://hdl.handle.net/10125/11775
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Summary:Typescript. Bibliography: leaves 131-133. xi, 133 l charts, graphs, maps, tables Contraction of volume that occurs when sea waters mix is shown to be the mechanism which controls density structure at intermediate depths in the North Indian Ocean. This is the main result of a study in which mean annual distributions of temperature, salinity, dissolved oxygen, and density in the North Indian Ocean are considered to represent a steady state, and delineation of the significant physical processes responsible for the distributions is attempted. Strong lateral mixing is evident, but cannot be accounted for by current shear in the mean annual pattern of geostrophic flow. At the density of the Red Sea salinity maximum in the Arabian Sea (700 m depth) there are monsoonal variations, with typical current speeds of 10 cm s^-1, which result in intensive lateral mixing. The horizontal coefficient of eddy diffusivity is 7 x 10^7 cm^2s^-1 for mixing at a length scale of 200 km, or 3 x 10^8 cm^2s^-1 for a length scale of 1000 km. Considerations of the conservation of heat and salt lead to definition of three depth zones: a layer of uniform vertical advection, deeper than 1700 m; a layer of constant vertical diffusive flux from 400 to 1200 m depth; and an intermediate transition zone. In the deep zone of uniform vertical advection, the water properties are exponential functions of depth. The vertical exchange coefficient has the constant value 2.5 2 -1 cm s Ascending motion of 4 x 10^-5 cm s^-1 occurs from 3000 m depth in the Arabian Sea, and from 2100 m depth in the Bay of Bengal, and near the equator. The upward transport of 4 x 10 6 m^3 s^-1 is supplied by northerly flow at depths 2000 m and greater. Near 2500 m depth, North Atlantic Deep Water probably penetrates northward to the equator in the western North Indian Ocean, and to the head of the Bay of Bengal in the east. At the equator, maximum southward return flow of speed 0.2 cm s^-1 occurs near 1000 m depth, within the zone of constant vertical diffusive flux. In ...