2.1 Eulerian reformulation of the continuous equations
Following Ritchie (1988,1991), the first step in developing a semi-Lagrangian version of the ECMWF spectral model was to convert the existing Eulerian
-D (vorticity-divergence) model to a
-
formulation, where
and
are the wind images defined by
,
(
and
are the components of the horizontal wind in spherical coordinates, and
is latitude). In this section we describe the Eulerian
-
model.
First we set out the continuous equations in
coordinates, where
is longitude and
is the hybrid vertical coordinate introduced by Simmons and Burridge (1981); thus
is a monotonic function of the pressure
, and also depends on the surface pressure
in such a way that
and . |
|
The momentum equations are
where
is the radius of the earth,
is the
-coordinate vertical velocity (
),
is geopotential,
is the gas constant for dry air, and
is the virtual temperature defined by
where
is temperature,
is specific humidity and
is the gas constant for water vapour.
and
represent the contributions of the parametrized physical processes, while
and
are the horizontal diffusion terms.
The thermodynamic equation is
where
(
is the specific heat of dry air at constant pressure),
is the
-coordinate vertical velocity (
), and
(
is the specific heat of water vapour at constant pressure).
The moisture equation is
In (2.2) and (2.3),
and
represent the contributions of the parametrized physical processes, while
and
are the horizontal diffusion terms.
The continuity equation is
where
is the horizontal gradient operator in spherical coordinates and
is the horizontal wind.
The geopotential
which appears in (2.1) and (2.2) is defined by the hydrostatic equation
while the vertical velocity
in (2.3) is given by
Expressions for the rate of change of surface pressure, and for the vertical velocity
, are obtained by integrating (2.5), using the boundary conditions
at
and at
Since we use
rather than
as the surface pressure variable, it is convenient to rewrite (2.8) as