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Kolmogorov constants for the second-order structure function and the energy spectrum
1Department of Physics, The Chinese University of Hong Kong, Shatin, Hong Kong, China.
Kolmogorov constants C(2), C(k), and C(k1) depend on the microscale Reynolds number R(λ). The ratio C(2)=4.02C(k1) is only valid for R(λ) above 10^5.
Area of Science:
- Fluid dynamics
- Turbulence theory
- Statistical physics
Background:
- The Kolmogorov theory provides a framework for understanding turbulence.
- Kolmogorov constants are crucial for characterizing energy transfer in turbulent flows.
- Previous studies assumed these constants are independent of the Reynolds number.
Purpose of the Study:
- To investigate the behavior of Kolmogorov constants C(2), C(k), and C(k1).
- To determine the dependence of these constants and their ratios on the microscale Reynolds number R(λ).
- To re-evaluate the validity of commonly used relationships between these constants.
Main Methods:
- Analysis of the second-order longitudinal structure function.
- Examination of the three-dimensional and one-dimensional longitudinal energy spectra.
- Correlation of constant ratios with the microscale Reynolds number R(λ).
Main Results:
- The ratios C(2)/C(k1) and C(k)/C(k1) show a clear dependence on R(λ).
- A specific relationship was found: (C(k1)/C(2)-0.25)=1.95R(λ)(-0.68).
- The widely accepted relation C(2)=4.02C(k1) is only asymptotically valid for R(λ) ≥ 10^5.
Conclusions:
- Kolmogorov constants are not universally independent of the Reynolds number.
- The dependence varies among C(2), C(k), and C(k1), with C(2) showing stronger R(λ) dependence.
- Differences in real-space and wave-number space inertial ranges explain the varying R(λ) dependence.
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