The scattering of electromagnetic waves from counter-rotating vortex s
treets associated with nonlinear convective cells in uniform plasmas h
as been considered. The vortex street solution of the Navier-Stokes or
the Hasegawa-Mima (and of the ''sinh-Poisson'') equation is adopted a
s a scatterer. Assuming arbitrary polarization and profile function fo
r the incident electromagnetic field, a compact expression for the sca
ttering cross section has been obtained. Specific results for the diff
erential cross section are obtained for the case in which the incident
beam has a Gaussian profile and propagates as an ordinary mode. The r
esults show that when the characteristic wavelength of the vortex stre
et (lambda(upsilon) = 2 pi/a) is larger than that of the incident elec
tromagnetic wave (lambda(i) = 2 pi/k(i)), the differential cross secti
on d sigma/d Omega has a very well-defined angular periodicity; in fac
t, it is a collection of Gaussians varying as exp[-f(k(i)w)(2)], where
w is the waist and f is a function expressing a kind of ''Bragg condi
tion.'' On the other hand, for lambda(i)>lambda(upsilon) the incident
electromagnetic beam is unable to distinguish the periodic structure o
f the vortex street. The effects of the vortex street as well as the i
ncident beam parameters on the scattering cross section are examined.
(C) 1996 American Institute of Physics.