We study the pattern selection and the dynamics of a bifurcating syste
m such as Taylor-Couette flow or Rayleigh-Benard convection, subject t
o an externally imposed cross flow using the complex Ginzburg-Landau e
quation as a qualitative model. We show that the bifurcation scenario
is radically modified by the introduction of a cross flow, and that a
nonlinear global mode, i.e., a nonlinear oscillating solution in a Sem
i-infinite domain [0, +infinity), with a homogeneous condition at x =
0, exists only when the basic state is linearly absolutely unstable. W
e derive the scaling law for the characteristic growth size, which var
ies as epsilon(-1/2) (epsilon being the criticality parameter), and co
mpares satisfactorily with numerical and experimental results from the
literature.