3.2      The CANDIE Forward Time Integration

In the A-grid formulation the temperature and salinity are volume averages for a cell and we interpolate the A-grid velocities to the C-grid cell faces in order to deal with the conservation equations. The basic approach goes as follows. Assume we start out knowing the velocity at both the C-grid (cell face) and the temperature, salinity and velocity at the A-grid (volume average) locations. Suppose further that these quantities are known at two successive times to and page6_1.gif. Using standard centered differences in space and a leapfrog scheme in time, the temperature T and salinity S are updated to time level page6_2.gif. Similarly, the A-grid velocity components U0 and V0 from time level to can be updated to the time level t2 for the effects of advection, diffusion and Coriolis acceleration. However, the surface pressure is not yet known at the time level t1, so only an approximation to the pressure driven acceleration can be determined. This approximation is based on the surface pressure field at the initial time level to and the density variations at the time level t1. The correction due to the change in surface pressure between to and t1 must be added on later.

How does DieCAST determine the change in surface pressure between to and t1? Mathematical details are given in Appendix A, but the basic approach is actually quite simple. Given that the velocity field is non-divergent at time to, the idea is to determine the surface pressure at time t1 that is required to insure that the velocity field at time t2 remains non-divergent. Any imbalances in continuity associated with errors in the velocity field must be balanced by changing the velocity. Because all other effects have already been accounted for, these velocity changes must be driven by the gradients in the surface pressure difference page6_3.gif between the time levels to and t1. To determine an equation for page6_3.gif, we first write the horizontal velocity components in terms of the previously estimated values at t2 plus the correction associated with the unknown page6_3.gif. Forming the depth-integrated continuity equation now results in a simple 2D elliptic equation for page6_3.gif. After solving this equation for page6_3.gif the horizontal velocity components are adjusted for the additional pressure driven acceleration and the vertical velocity is updated using the 3D continuity equation.

The above paragraph describes the basic idea. However, this approach assumes that the velocity is known at the C-grid locations in order to determine the continuity errors that need to be corrected, but the velocity updates from to to t2 were actually done at the A-grid locations. Thus, to apply this methodology, one must interpolate the velocities from the A-grid to the C-grid. The velocity field is then corrected on the C-grid and the changes must then be interpolated back to the A-grid. These technical details are relegated to Appendix A. However, it should be noted that the C-grid velocities resulting from this approach precisely satisfy the continuity equation and that the Coriolis terms do not suffer from the need for horizontal interpolations.

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