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. 1997 Nov 25;94(24):12762–12764. doi: 10.1073/pnas.94.24.12762

Figure 4.

Figure 4

The dimensionless critical length ζ0 as a function of the basic parameter λ in the case of developed turbulent flow. Note the collapse of the curves starting from rather moderate values of λ in a large range of Reynolds number, and the scaling law ζ0 ∼ λ−9/4 at large supercritical values of λ.