In this essay, we recall the specificities of the transition to turbulence in
wall-bounded flows and present recent achievements in the understanding of this
problem. The transition is abrupt with laminar-turbulent coexistence over a
finite range of Reynolds numbers, the transitional range. The archetypical
cases of Poiseuille pipe flow and plane Couette flow are first reviewed at the
phenomenological level, together with a few other flow configurations.
Theoretical approaches are then examined with particular emphasis on the
existence of special nontrivial solutions to the Navier-Stokes equations at
finite distance from laminar flow. Dynamical systems theory is most appropriate
to analyze their role, in particular with respect to the transient character of
turbulence in the lower transitional range. The extensions needed to deal with
the prominent spatiotemporal features of the transition are then discussed.
Turbulence growth/decay in terms of statistical physics of many-body systems
and the relevance of directed percolation as a stochastic process able to
account for it are next scrutinized. To conclude, we advocate the recourse to
well-designed modeling able to provide us with a conceptually coherent picture
of the full transitional range and put forward some open issues.Comment: to appear in "Mechanical Engineering Review", Vol. 3, No. 2, July
1st, 201