A. Masuda et K. Miki, ON THE STABILITY OF BAROCLINIC VORTEX STREETS COMPOSED OF QUASI-GEOSTROPHIC POINT EDDIES, Deep-sea research. Part 1. Oceanographic research papers, 42(4), 1995, pp. 437-453
The stability of quasi-geostrophic vortex streets is investigated for
a single, a symmetric double, and a staggered double row, where compon
ent baroclinic point vortices are discriminated from ordinary ones by
concentrated potential vorticity instead of concentrated vorticity. Th
e former two types of rows always turn out unstable, though the growth
rate itself decreases monotonically with increasing F, an index of h
orizontal divergence, or the inverse of the deformation radius nondime
nsionalized in terms of the longitudinal spacing of the vortex street.
As regards a staggered double row, a critical value F-c = 3.04 divid
es F into two regimes. Below F-c*, only one value of b* = b(s)* is ne
utrally stable, where b = b/a is the aspect ratio of the vortex stree
t with a and b the separations between eddies along and perpendicular
to the street, respectively. The stable configuration b(s) slowly inc
reases with F from the Karman ratio 0.281 at F* = 0 to 0.322 at F* =
F-c. For F* above F-c*, the staggered double row is stable for a band
of b. The appearance of the stable region is explained by a near-fie
ld approximation, where an eddy is assumed to exert its vortex force o
nly on adjacent eddies. The near-field approximation yields a stabilit
y diagram which agrees well with that obtained from rigorous calculati
on for large F. In particular, the configuration b* greater than or e
qual to root 3/2 is shown to be unstable irrespective of F.