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A 2D Model for the Interleaving of Northern and Southern Atlantic Ocean Deep Waters

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Submitted to Journal of Physical Oceanography, 2004. ... Knauss, J.A., Introduction to Physical Oceanography. 1978, New Jersey: Prentice-Hall, Inc. ... – PowerPoint PPT presentation

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Title: A 2D Model for the Interleaving of Northern and Southern Atlantic Ocean Deep Waters


1
A 2D Model for the Interleaving of Northern and
Southern Atlantic Ocean Deep Waters
  • Guo, Xin
  • October 7th 2004
  • Advisor Ingersoll, Andrew P.

2
Outline
  • The Interleaving phenomenon in northern and
    southern Atlantic ocean deep waters
  • The reason for interleaving
  • The 2D model
  • Results of simulation
  • Conclusion and future work

3
Interleaving of Atlantic Waters
  • Northern Atlantic water is warmer and saltier
    than southern Atlantic water
  • Atlantic source water (North Atlantic water)
    could be denser at the surface and less dense at
    the bottom than the Antarctic source water (South
    Atlantic water)
  • Ingersoll 2004 suggests that the level of neutral
    buoyancy would be about 3.5km below the sea level

Hartmann, D.L., Global Physical Climatology.
International Geophysics Series, ed. R. Dmowska
and J.R. Holton. Vol. 56. 1994, San Diego
Academic Press.
4
Equation of State
  • Cold Fresh Water (CFW) vs Warm Salty Water (WSW)
    at different depths
  • Thermobaric Effect Thermal coefficient of
    expansion increases with pressure

Hartmann, D.L., Global Physical Climatology.
International Geophysics Series, ed. R. Dmowska
and J.R. Holton. Vol. 56. 1994, San Diego
Academic Press.
Knauss, J.A., Introduction to Physical
Oceanography. 1978, New Jersey Prentice-Hall,
Inc.
5
Possibility of Interleaving thermobaric effect
  • At low pressure, salinity dominates density
    variance
  • At high pressure, temperature dominates density
    variance
  • At somewhere between, isopycnal is possible

6
Observation
http//sam.ucsd.edu/vertical_sections/
7
The Real Ocean
Depth1 2km North Water 1024.4438 kg/m3 South
Water 1024.3979 kg/m3 Depth2 5km North Water
1024.119 kg/m3 South Water 1024.1518 kg/m3
8
The Real Ocean
Depth1 4km North Water 1024.4664 kg/m3 South
Water 1024.6752 kg/m3 Depth2 0.5km North
Water 1024.7035 kg/m3 South Water 1024.6918
kg/m3
9
Model with Boussinesq Approximationequations to
solve
10
Initial condition and boundary condition
  • Initial conditions
  • Homogenous stream function
  • Homogenous potential temperature
  • Homogenous salinity
  • Boundary conditions
  • No-slip boundaries at sides and bottom
  • None-stress top boundary
  • Specific salinity flux on surface
  • Relaxation thermal flux
  • Zero geothermal heat flux

11
With Asymmetric Fluxes
12
With Asymmetric Fluxes
13
Conclusion and future work
  • The dependence of density on various parameters
    and thermobaric effect is presented in the real
    ocean, which can explain the interleaving
  • This 2D model shows its potential to reproduce
    the interleaving in thermohaline circulation
  • Effects of boundary condition, initial condition
    and parameters need further exploration
  • Model is simple, longitudinal circulation and sea
    floor topography could play important role

14
The End
Acknowledgement
Andrew Ingersoll, Kevin Lewis, Claudia Pasquero
and Liming Li for useful guidance and discussion
  • Thank you for listening

15
Observation
http//sam.ucsd.edu/vertical_sections/
16
With Asymmetric Fluxes
17
With Asymmetric Fluxes
18
With Asymmetric Fluxes
19
References
  • Ingersoll, A., Boussinesq and Anelastic
    Approximations Revisited Potential Energy
    Release during Thermobaric Instability. Submitted
    to Journal of Physical Oceanography, 2004.
  • Hartmann, D.L., Global Physical Climatology.
    International Geophysics Series, ed. R. Dmowska
    and J.R. Holton. Vol. 56. 1994, San Diego
    Academic Press.
  • Knauss, J.A., Introduction to Physical
    Oceanography. 1978, New Jersey Prentice-Hall,
    Inc.
  • Vellinga, M., Instability of Two-Dimensional
    Thermohaline Circulation. Journal of Physical
    Oceanography, 1996. 26(3) p. 305-319.
  • http//sam.ucsd.edu/vertical_sections/

20
With symmetric fluxes
21
With symmetric fluxes
22
With symmetric fluxes
23
With asymmetric fluxes
24
With asymmetric fluxes
25
Discussion on the picture of interleaving
  • Thermobaric effect works
  • Different levels where pole-to-pole convection
    happens
  • Diffusion coefficient helps build temperature and
    salinity gradient
  • Boundary fluxes and relaxation time
  • Initial condition would affect the transient
    stages but not final steady stages

26
Thermobaric Instability
  • The dependence of density on temperature,
    salinity and pressure allows seawater to store a
    finite amount of potential energy for later
    release.

27
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28
Possibility of Interleaving thermobaric effect
29
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30
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31
Knauss, J.A., Introduction to Physical
Oceanography. 1978, New Jersey Prentice-Hall,
Inc.
32
Temperature Density
33
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