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    Double-Diffusive Interleaving. Part II: Finite Amplitude, Steady State Interleaving

    Source: Journal of Physical Oceanography:;1985:;Volume( 015 ):;issue: 011::page 1542
    Author:
    McDougall, Trevor J.
    DOI: 10.1175/1520-0485(1985)015<1542:DDIPIF>2.0.CO;2
    Publisher: American Meteorological Society
    Abstract: The exponentially growing solutions of the linear stability analysis of double-diffusive interleaving are allowed to grow to finite amplitude. At this stage the double-diffusive fluxes across the intrusion boundaries must be parameterized differently to those in the growing solution because every second finger interface becomes a diffusive interface in the steady state solution. Using the wavenumbers that are set by the initial, growing intrusions from the linear stability problem, together with the changed parameterization of the double-diffusive fluxes, it is shown that a steady state is reached. The ratio of the gradients of potential temperature and salinity along any particular intrusion is the same as in the linear stability analysis. When expressed in terms of density changes, this ratio is close to 0.9 rather than the commonly assumed value of 0.5 (being the buoyancy-flux ratio of a single salt finger interface). After solving for the velocity field, the isopycnal and diapycnal fluxes of potential temperature, salinity and density are formed. The diapycnal fluxes of potential temperature, salinity and density are all found to be up-gradient, implying negative diapycnal diffusivities for all three quantities. This is an unexpected and potentially important result. Following the approach of Garrett, a basin-average diapycnal diffusivity is estimated and is found to be of comparable size, but of opposite sign, to the modern day metric of 10?5 m2 s?1.
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      Double-Diffusive Interleaving. Part II: Finite Amplitude, Steady State Interleaving

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    contributor authorMcDougall, Trevor J.
    date accessioned2017-06-09T14:47:39Z
    date available2017-06-09T14:47:39Z
    date copyright1985/11/01
    date issued1985
    identifier issn0022-3670
    identifier otherams-26907.pdf
    identifier urihttp://onlinelibrary.yabesh.ir/handle/yetl/4163853
    description abstractThe exponentially growing solutions of the linear stability analysis of double-diffusive interleaving are allowed to grow to finite amplitude. At this stage the double-diffusive fluxes across the intrusion boundaries must be parameterized differently to those in the growing solution because every second finger interface becomes a diffusive interface in the steady state solution. Using the wavenumbers that are set by the initial, growing intrusions from the linear stability problem, together with the changed parameterization of the double-diffusive fluxes, it is shown that a steady state is reached. The ratio of the gradients of potential temperature and salinity along any particular intrusion is the same as in the linear stability analysis. When expressed in terms of density changes, this ratio is close to 0.9 rather than the commonly assumed value of 0.5 (being the buoyancy-flux ratio of a single salt finger interface). After solving for the velocity field, the isopycnal and diapycnal fluxes of potential temperature, salinity and density are formed. The diapycnal fluxes of potential temperature, salinity and density are all found to be up-gradient, implying negative diapycnal diffusivities for all three quantities. This is an unexpected and potentially important result. Following the approach of Garrett, a basin-average diapycnal diffusivity is estimated and is found to be of comparable size, but of opposite sign, to the modern day metric of 10?5 m2 s?1.
    publisherAmerican Meteorological Society
    titleDouble-Diffusive Interleaving. Part II: Finite Amplitude, Steady State Interleaving
    typeJournal Paper
    journal volume15
    journal issue11
    journal titleJournal of Physical Oceanography
    identifier doi10.1175/1520-0485(1985)015<1542:DDIPIF>2.0.CO;2
    journal fristpage1542
    journal lastpage1556
    treeJournal of Physical Oceanography:;1985:;Volume( 015 ):;issue: 011
    contenttypeFulltext
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