Diagnostics of diapycnal diffusion in z-level ocean models

In general ocean circulation models (OGCMs) diapycnal diffusion arises not only from the discretisation of the explicit diffusion, but also by numerically induced diffusion, caused, e.g., by common discretisations of advective transport. In the present study, three different diagnostics to analyse the mean diapycnal diffusivities of individual tracers (vertically and horizontally) are introduced: (i) The divergence method based on the work of Ledwell et al. (1998) infers the mean diapycnal diffusivity from the advection-diffusion equation. (ii) The tracer flux method based on the work of Griffies et al. (2000), that determines the diapycnal flux crossing an isopycnal layer, is modified for the analysis of mean diapycnal diffusivities of a passive tracer. (iii) The variance method based on the work of Morales Maqueda and Holloway (2006) is a more general approach as the diapycnal diffusion is analysed by the variance decay of the total tracer concentration. These methods can be used for the analysis of the diffusivity of passive tracer independent of the model set-up, e.g. the advection scheme used, but support only information about mean diapycnal diffusivity of that tracer field rather than for each individual layer. The applicability of these methods is tested in a set of 1- and 2-dimensional case studies. The effect of vertical advection and of diverging and converging isopycnals is shown separately. In all three methods used, the transformation of the tracer onto isopycnals leads to errors in the diagnosed diffusivities. It turns out that the tracer flux method is the most robust method and therefore the method of choice. In order to keep the errors as small as possible, longer time mean values should be analysed.

[1]  M. Prather Numerical advection by conservation of second-order moments. [for trace element spatial distribution and chemical interaction in atmosphere] , 1986 .

[2]  Stephen M. Griffies,et al.  Spurious Diapycnal Mixing Associated with Advection in a z-Coordinate Ocean Model , 2000 .

[3]  Andreas Oschlies,et al.  Diagnostics of diapycnal diffusivity in z-level ocean models part I: 1-Dimensional case studies , 2010 .

[4]  Laurent White,et al.  A high-order finite volume remapping scheme for nonuniform grids: The piecewise quartic method (PQM) , 2008, J. Comput. Phys..

[5]  C. Molenkamp,et al.  Accuracy of Finite-Difference Methods Applied to the Advection Equation , 1968 .

[6]  Stephen M. Griffies,et al.  Fundamentals of Ocean Climate Models , 2004 .

[7]  Patrick Marchesiello,et al.  Thermal forcing for a global ocean circulation model using a three-year climatology of ECMWF analyses , 1995 .

[8]  P. Gent,et al.  Isopycnal mixing in ocean circulation models , 1990 .

[9]  P. Smolarkiewicz A Simple Positive Definite Advection Scheme with Small Implicit Diffusion , 1983 .

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

[11]  W. R. Holland,et al.  A consideration of tracer advection schemes in a primitive equation ocean model , 1998 .

[12]  David P. Stevens,et al.  A New Tracer Advection Scheme for Bryan and Cox Type Ocean General Circulation Models , 1995 .

[13]  D. Webb,et al.  IMPROVED ADVECTION SCHEMES FOR OCEAN MODELS , 1998 .

[14]  M. A. Morales Maqueda,et al.  Second-order moment advection scheme applied to Arctic Ocean simulation , 2006 .

[15]  A. Watson,et al.  Mixing of a tracer in the pycnocline , 1998 .

[16]  Rüdiger Gerdes,et al.  The influence of numerical advection schemes on the results of ocean general circulation models , 1991 .

[17]  Rainer Bleck,et al.  An oceanic general circulation model framed in hybrid isopycnic-Cartesian coordinates , 2002 .

[18]  A. Oschlies,et al.  An eddy‐permitting coupled physical‐biological model of the North Atlantic: 1. Sensitivity to advection numerics and mixed layer physics , 1999 .

[19]  H. Burchard,et al.  Comparative quantification of physically and numerically induced mixing in ocean models , 2008 .

[20]  M. Redi Oceanic Isopycnal Mixing by Coordinate Rotation , 1982 .

[21]  Philippe Gaspar,et al.  A simple eddy kinetic energy model for simulations of the oceanic vertical mixing: Tests at Station Papa and long-term upper ocean study site , 1990 .

[22]  D. Stevens On open boundary conditions for three dimensional primitive equation ocean circulation models , 1990 .