In a generic pressure-based terrain following vertical coordinate ¦Ç, the governing equations of the atmosphere under the hydrostatic assumption can be derived following Kasahara (1974). This equation set, also known as the primitive equations, reads
¡¡
| (4) |
Here v is
the horizontal
velocity vector (on the sphere);
k is the unit vector
in the radial outward direction;
f is the Coriolis parameter;
is the vertical component of the relative vorticity;
is the kinetic energy per unit mass. p and T
denote pressure and temperature, respectively.
is geopotential, R is the gas constant
and Cp the
specific heat capacity of dry air under constant pressure. Note that the
momentum equation is written in the vector invariant form.
¡¡
The generalized p-sigma hybrid vertical coordinate used in ICOHDC is the same as in ECHAM5 and many other global hydrostatic models. It was first introduced by Simmons and Str¨¹fing (1981) for the grid-point forecast model of the ECMWF. The vertical domain of the model atmosphere is divided into NLEV layers. Pressure values of the interfaces between layers are given by
¡¡
| (5) |
and
are parameters independent of the
horizontal location. Near the earth¡¯s surface
equals zero and the interfaces are pure sigma
levels; near the model top
equals zero and the interfaces coincide with isobaric surfaces.
The levels in between provide a smooth transition. Pressure of the "full
levels" on which the horizontal wind and temperature are predicted is
defined as
¡¡
| (6) |
¡¡
Last modified: 2008-10-20 by Hui Wan