Structure and Dynamics of the Surface Branch of the Meridional Cell in the Indian Ocean - PowerPoint PPT Presentation

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Structure and Dynamics of the Surface Branch of the Meridional Cell in the Indian Ocean

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Near-surface eastward flow in the South Indian Ocean. CLIVAR Indian Ocean ... Impact of ITF (COCO) Dynamics. Basin-wide ... (COCO) Impact of ACC (COCO) ... – PowerPoint PPT presentation

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Title: Structure and Dynamics of the Surface Branch of the Meridional Cell in the Indian Ocean


1
Near-surface eastward flow in the South Indian
Ocean
Jay McCreary, Ryo Furue, and Billy Kessler
2
Topics
  • Observations and models
  • Dynamics
  • Indonesian Throughflow
  • Basin-wide subduction (LPS theory)
  • Localized subduction/convection

3
Observations and models
4
Annual-mean near-surface circulation
There are extensive regions of eastward flow in
the South and North Pacific Ocean and in the
South Indian Ocean.
5
Annual-mean near-surface circulation
6
Annual-mean near-surface circulation
7
Dynamics Indonesian Throughflow
8
Impact of ITF (COCO)
u, T, closed
u, T, open
9
Dynamics Basin-wide subduction (LPS theory)
10
LPS theory (2½-layer model)
Equations Equations of motion for the analytic
model are
(1)
where the pressure gradients are
and
11
LPS theory (2½-layer model)
h equation Equations (1) can be solved for a
single equation in h, yielding
(2)
where
is the speed of the n 2 Rossby waves,
are the depth-averaged geostrophic currents
associated with the Sverdrup circulation, and
12
LPS theory (2½-layer model)
Subduction along ys introduces a source of n 2
Rossby signals that extend equatorward due to
dvection by the SIO Subtropical Gyre.
Courtesy of Billy Kessler
13
LPS theory (2½-layer model)
14
Dynamics Localized subduction/convection
15
Subduction (COCO)
16
Impact of ACC (COCO)
17
Summary
18
  • There is near-surface eastward flow that overlies
    westward flow across the South Pacific and South
    Indian Oceans. Such flows are referred to as
    Subtropical Countercurrents. The eastward flow
    is more extensive in the South IO than in the
    Pacific.
  • The cause of the eastward flow is not yet well
    understand. Several forcing mechanisms have been
    considered i) the ITF, ii) basin-wide subduction
    across the SIO, and iii) localized
    subduction/convection in the southeast IO and
    south of Australia.
  • Subduction and convection are sources of
    higher-order (n ? 1) baroclinic waves. Such
    waves propagate westward at their familiar linear
    wave speed AND are advected by the geostrophic
    part of the Sverdrup circulation (LPS theory).
    In the SIO, this property means that they tend to
    circulate around the SIO subtropical gyre, so
    that baroclinic sources in the far-south IO and
    south of Australia can impact flows farther north.

19
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