The number of degrees of freedom of three-dimensional Navier--Stokes turbulence
arXiv:0912.2000 · doi:10.1063/1.3276295
Abstract
In Kolmogorov's phenomenological theory of turbulence, the energy spectrum in the inertial range scales with the wave number as and extends up to a dissipation wave number , which is given in terms of the energy dissipation rate and viscosity by . This result leads to Landau's heuristic estimate for the number of degrees of freedom that scales as , where is the Reynolds number. Here we consider the possibility of establishing a quantitative basis for these results from first principles. In particular, we examine the extent to which they can be derived from the three-dimensional Navier--Stokes system, making use of Kolmogorov's hypothesis of finite and viscosity-independent energy dissipation only. It is found that the Taylor microscale wave number (a close cousin of ) can be expressed in the form $k_T \le CU/ν= (CU/\norm{\u})^{1/2}(ε/ν^3)^{1/4}$. Here and $\norm{\u}$ are, respectively, a ``microscale'' velocity and the root mean square velocity, and is a dynamical parameter. This result can be seen to be in line with Kolmogorov's prediction for . Furthermore, it is shown that the minimum number of greatest Lyapunov exponents whose sum becomes negative does not exceed , where is defined in terms of an average energy dissipation rate, the system length scale, and . This result is in a remarkable agreement with the Landau estimate, up to a presumably slight discrepancy between the conventional and the present energy dissipation rates used in the definition of .
6--7 journal pages, to appear in Physics of Fluids