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In numerical calculations, we observe a dichotomy in the time evolution of solutions of the high-Reynolds-number, two-dimensional, incompressible Navier-Stokes equations using power-law initial modal energy spectra E(κ,0)~κ^-μ₀. The boundary is expressed in terms of critical values of viscosity νcr and microscale λcr. For both parameters initially above critical, μ approaches 4. For both parameters initially below critical, μ approaches 1 at large κ, consistent with equipartition of the vorticity spectrum. In the former case, large-scale vortex states form after a long time; and, in both cases, energy flows to the lowest wave numbers.
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Deem et al. (1971) studied this question.
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