Gb. Smith et Mt. Montgomery, VORTEX AXISYMMETRIZATION - DEPENDENCE ON AZIMUTHAL WAVE-NUMBER OR ASYMMETRIC RADIAL STRUCTURE CHANGES, Quarterly Journal of the Royal Meteorological Society, 121(527), 1995, pp. 1615-1650
Intense vortices in the atmosphere and ocean exhibit a high degree of
axisymmetry despite persistent asymmetric forcing from their environme
nt. To further elucidate vortex axisymmetrization a variety of idealiz
ed initial-value models for barotropic non-divergent now is considered
. To ensure basic understanding, disturbance evolution is first examin
ed in a rectilinear system of simple shear. Particular emphasis is pla
ced on identifying how inviscid disturbance-evolution depends on the z
onal wave-number and on the meridional structure of the initial condit
ions. Insight acquired from the rectilinear problem is then applied to
a bounded Rankine vortex. Here, the dependency of disturbance evoluti
on on the azimuthal wave-number is of special interest. Recent develop
ment of a low-frequency balance theory for rapidly rotating (large Ros
sby number) vortices has provided observational evidence that the low-
azimuthal-wave-number asymmetries, especially wave number one, are dom
inant in the near-vortex region. The results of this work provide furt
her theoretical evidence of an inviscid wave-number-selection mechanis
m that preferentially damps the high-wave-number asymmetries. The radi
al structure and location of the initial conditions are found to be im
portant factors in determining how rapidly a disturbance is compressed
or elongated. This in turn controls the rate of disturbance growth or
decay. For swirling flows, a definition of an effective shear is prop
osed that accounts for both the radial variations of the initial condi
tion and the radial variation of the angular velocity. Using the recip
rocal of this effective shear, time-scales for a disturbance to decay
to half its initial energy, the half-life, are calculated for initial
conditions and symmetric wind-profiles that are found in hurricanes. S
imple-shear flow and the bounded Rankine vortex do not admit discrete
modal solutions since there is no mean-state vorticity-gradient to sup
port them. The unbounded Rankine vortex is examined to investigate how
the presence of discrete modes (Rossby edge-waves) associated with th
e radial vorticity-gradient of the Rankine swirl modifies the continuo
us spectrum solutions presented here.