Английская Википедия:Batchelor scale
In fluid and molecular dynamics, the Batchelor scale, determined by George Batchelor (1959),[1] describes the size of a droplet of fluid that will diffuse in the same time it takes the energy in an eddy of size Шаблон:Mvar to dissipate. The Batchelor scale can be determined by:[2]
- <math>\lambda_B= \frac{ \eta }{ \sqrt{\mathrm{Sc}}} = \left( \frac{\nu D^2}{\varepsilon} \right)^\frac{1}{4} </math>
where:
- <math>\eta = ( \nu^3 / \varepsilon )^{1/4}</math> is the Kolmogorov length scale.
- Шаблон:Math is the Schmidt number.
- Шаблон:Mvar is the kinematic viscosity.
- Шаблон:Mvar is the mass diffusivity.
- Шаблон:Mvar is the rate of dissipation of turbulence kinetic energy per unit mass.
Similar to the Kolmogorov microscales – which describe the smallest scales of turbulence before viscosity dominates – the Batchelor scale describes the smallest length scales of fluctuations in scalar concentration that can exist before being dominated by molecular diffusion. It is important to note that for Шаблон:Math, which is common in many liquid flows, the Batchelor scale is small when compared to the Kolmogorov microscales. This means that scalar transport occurs at scales smaller than the smallest eddy size.
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