We study the pattern selection and the dynamics of a bifurcating system such as Taylor-Couette flow or Rayleigh-B\'enard convection, subject to an externally imposed cross flow using the complex Ginzburg-Landau equation 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 semi-infinite domain [0,+∞), with a homogeneous condition at x0ex0ex=0ex0ex0, exists only when the basic state is linearly absolutely unstable. We derive the scaling law for the characteristic growth size, which varies as ε^-1/2 ( ε being the criticality parameter), and compares satisfactorily with numerical and experimental results from the literature.
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Couairon et al. (1997) studied this question.
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