Title: A 2D Model for the Interleaving of Northern and Southern Atlantic Ocean Deep Waters
1A 2D Model for the Interleaving of Northern and
Southern Atlantic Ocean Deep Waters
- Guo, Xin
- October 7th 2004
- Advisor Ingersoll, Andrew P.
2Outline
- 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
3Interleaving 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.
4Equation 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.
5Possibility of Interleaving thermobaric effect
- At low pressure, salinity dominates density
variance - At high pressure, temperature dominates density
variance - At somewhere between, isopycnal is possible
6Observation
http//sam.ucsd.edu/vertical_sections/
7The 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
8The 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
9Model with Boussinesq Approximationequations to
solve
10Initial 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
11With Asymmetric Fluxes
12With Asymmetric Fluxes
13Conclusion 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
14The End
Acknowledgement
Andrew Ingersoll, Kevin Lewis, Claudia Pasquero
and Liming Li for useful guidance and discussion
15Observation
http//sam.ucsd.edu/vertical_sections/
16With Asymmetric Fluxes
17With Asymmetric Fluxes
18With Asymmetric Fluxes
19References
- 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/
20With symmetric fluxes
21With symmetric fluxes
22With symmetric fluxes
23With asymmetric fluxes
24With asymmetric fluxes
25Discussion 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
26Thermobaric Instability
- The dependence of density on temperature,
salinity and pressure allows seawater to store a
finite amount of potential energy for later
release.
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28Possibility of Interleaving thermobaric effect
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31Knauss, J.A., Introduction to Physical
Oceanography. 1978, New Jersey Prentice-Hall,
Inc.
32 Temperature Density
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