Abstract
An efficient approach for extracting 3D local averages in spherical subdomains is proposed and applied to study the intermittency of small-scale velocity and scalar fields in direct numerical simulations of isotropic turbulence. We focus on the inertial-range scaling exponents of locally averaged energy dissipation rate, enstrophy and scalar dissipation rate corresponding to the mixing of a passive scalar in the presence of a uniform mean gradient. The Taylor-scale Reynolds number goes up to , and the Schmidt number up to (albeit at smaller ). The intermittency exponent of the energy dissipation rate is , whereas that of enstrophy is slightly larger; trends with suggest that this will be the case even at extremely large . The intermittency exponent of the scalar dissipation rate is for . These findings are in essential agreement with previously reported results in the literature. We further show that decreases monotonically with increasing , either as or a weak power law, suggesting that as , reaffirming recent results on the breakdown of scalar dissipation anomaly in this limit.
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