A Dissipation Integral with Application to Ocean Diffusivities and Structure

An integral balance is developed for steady fluid flows relating dissipation in volumes bounded by isosurfaces of a tracer (quasi-conserved quantity) and solid boundaries to the covariance of the tracer value and surface fluxes across the boundaries. The balance is used to estimate upper bounds for vertical eddy diffusion coefficients for temperature and salinity in various volumes of the ocean. The vertical temperature diffusivity is calculated to be small, O(0.1 3 1024 m2 s21), except for the warmest and coldest volumes of the ocean. The vertical salinity diffusivity for the volume that makes up most of the deep ocean is estimated to be O(1 3 1024 m2 s21). Sources of error in these calculations are discussed, and the sensitivity to errors in the surface flux data is evaluated. The dissipation integral is also applied to demonstrate some related results concerning extrema and homogenization. The Prandtl‐Batchelor theorem is a special case of one of these results. As a consequence of these results, if turbulent transfer is downgradient and there are no internal sources or sinks, a necessary (but not sufficient) condition for a climatological tracer distribution to be in a steady state is the absence of internal extrema. The climatological salinity distribution does not appear to violate this condition.

[1]  C. Rooth,et al.  Penetration of tritium into the Atlantic thermocline , 1972 .

[2]  K. Speer A note on average cross-isopycnal mixing in the North Atlantic ocean , 1997 .

[3]  R. Reynolds,et al.  The NCEP/NCAR 40-Year Reanalysis Project , 1996, Renewable Energy.

[4]  Gösta Walin,et al.  On the relation between sea‐surface heat flow and thermal circulation in the ocean , 1982 .

[5]  F. Bryan Climate Drift in a Multicentury Integration of the NCAR Climate System Model , 1998 .

[6]  K. Speer,et al.  The Relationship between Water Mass Formation and the Surface Buoyancy Flux, with Application to Phillips’ Red Sea Model , 1995 .

[7]  Josef M. Oberhuber,et al.  An Atlas Based on the COADS Data Set: the Budgets of Heat Buoyancy and Turbulent Kinetic Energy at t , 1988 .

[8]  J. Toole,et al.  Estimates of Diapycnal Mixing in the Abyssal Ocean , 1994, Science.

[9]  De Szoeke,et al.  The Dissipation of Fluctuating Tracer Variances , 1998 .

[10]  Syukuro Manabe,et al.  Transient Response of a Global Ocean-Atmosphere Model to a Doubling of Atmospheric Carbon Dioxide , 1990 .

[11]  H. E. Kallmann,et al.  Transient Response , 1945, Proceedings of the IRE.

[12]  Andrew J. Watson,et al.  Evidence for slow mixing across the pycnocline from an open-ocean tracer-release experiment , 1993, Nature.

[13]  M. Stern Ocean circulation physics , 1975 .

[14]  L. Talley,et al.  Heat and Buoyancy Budgets and Mixing Rates in the Upper Thermocline of the Indian and Global Oceans , 1998 .

[15]  Joseph Pedlosky,et al.  Ocean Circulation Theory , 1996 .

[16]  R. Lindzen Axially symmetric steady-state models of the basic state for instability and climate studies , 1977 .

[17]  K. Bryan,et al.  A water mass model of the world ocean circulation , 1979 .

[18]  R. Hide Dynamics of the Atmospheres of the Major Planets with an Appendix on the Viscous Boundary Layer at the Rigid Bounding Surface of an Electrically-Conducting Rotating Fluid in the Presence of a Magnetic Field , 1969 .

[19]  E. Schneider Axially symmetric steady-state models of the basic state for instability and climate studies , 1977 .

[20]  T. Joyce On Production and Dissipation of Thermal Variance in the Oceans , 1980 .

[21]  G. Batchelor,et al.  On steady laminar flow with closed streamlines at large Reynolds number , 1956, Journal of Fluid Mechanics.

[22]  S. Levitus Climatological Atlas of the World Ocean , 1982 .

[23]  E. Kunze,et al.  Abyssal Mixing: Where It Is Not , 1996 .