  The L-dependence of the static potential between Nc quarks arranged in a
circle of radius L (a "baryon") immersed in the hot plasma of a gauge theory
with Nc colors defines a screening length Ls. We use the AdS/CFT correspondence
to compute this screening length for the case of heavy quarks in the plasma of
strongly coupled N=4 super Yang-Mills theory moving with velocity v relative to
the baryon. We find that in the v -> 1 limit, Ls \propto (1-v^2)^{1/4}/T, and
find that corrections to this velocity dependence are small at lower
velocities. This result provides evidence for the robustness of the analogous
behavior of the screening length defined by the static quark-antiquark pair,
which has been computed previously and in QCD is relevant to quarkonium physics
in heavy ion collisions. Our results also show that as long as the hot wind is
not blowing precisely perpendicular to the plane of the baryon configuration
that we analyze, the Nc different quarks are not all affected by the wind
velocity to the same degree, with those quarks lying perpendicular to the wind
direction screened most effectively.
