Q. Xu et W. Gu, Baroclinic Eady wave and fronts. Part II: Geostrophic potential vorticity dynamics in semigeostrophic space, J ATMOS SCI, 57(6), 2000, pp. 861-872
The geostrophic coordinate transformation is applied to the viscous semigeo
strophic (SG) Eady wave. In the transformed space, called the SG space, the
potential temperature anomaly can be treated as a delta-function anomaly o
f geostrophic potential vorticity (GPV) at the physical boundary or imagina
ry boundary (along the top of the boundary layer). Since the delta-function
anomaly is analogous to the surface charge of a problem in electrostatics
with the induced geopotential playing the role of the electric potential, t
he development of the Eady wave and fronts can be interpreted in terms of t
he interaction between the "surface charges" at two imaginary boundaries. I
t is shown that this interpretation and related GPV thinking for the viscou
s SG Eady wave can be made nearly as concise as its inviscid paradigm durin
g the boundary stage (until the inviscid surface front collapses in physica
l space).
When the viscous SG Eady wave develops into the interior stage, strong inte
rior GPV anomalies, analogous to "body charges," are generated by the diffu
sive GPV flux. These body charges form two domes in the SG space. The geost
rophic flow field induced by the body charge in each dome produces diffusiv
e GPV fluxes that converge at the upstream edge of each dome and thus keep
the body charge in step against the horizontal advection. The growth of the
geometric area of each dome of body charge (or the penetration of the fron
t into the interior in physical space), however, is caused mainly by the ag
eostrophic circulation forced by the geostrophic flow. It is also shown tha
t the body charge in each dome can be represented by the surface charge (po
tential temperature anomaly) on an imaginary boundary that covers the dome
(above the boundary layer). The growth of these surface charges can be expl
ained by a simplified GPV thinking applied only to the nearly inviscid inte
rior region, similar to its inviscid counterpart for the interior stage (be
yond the time that the inviscid surface front collapses in physical space).