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HYCOM
was run with KPP mixing
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and
relaxation boundary conditions
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to
produce the “best” possible
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simulation.
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Many
of the observed differences
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between
the simulated and observed
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fields
can be attributed at least in
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part
to the lack of river runoff and
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sea
ice in the model, not to mention
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forcing
errors and the poor estimate
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|
of
observed mixed layer thickness
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obtained
from the smooth Levitus
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climatology.
Errors in the simulated
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dynamical
fields are partly related
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|
to
the errors in the simulated
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thermodynamical
fields.
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