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Anisotropy in homogeneous rotating turbulence
1Instituto de Matemáticas y Física Fundamental, CSIC, Serrano 123, 28006 Madrid, Spain.
Physical Review. E, Statistical, Nonlinear, and Soft Matter Physics
|December 20, 2003
Summary
Turbulent rotating fluids exhibit anisotropic effective stress tensors. This study introduces a general axisymmetric viscosity tensor, revealing new large-scale turbulent forces and angular momentum nonconserving terms.
Area of Science:
- Fluid dynamics
- Turbulence theory
- Rheology
Background:
- Homogeneous turbulent rotating fluids exhibit anisotropic effective stress tensors.
- Understanding these anisotropies is crucial for accurate fluid modeling.
Purpose of the Study:
- To derive the most general axisymmetric four-rank viscosity tensor for a Newtonian fluid.
- To identify new terms in the large-scale turbulent effective force arising from this tensor.
- To explore axisymmetry constraints on response functions and velocity correlations.
Main Methods:
- Derivation of the general axisymmetric four-rank viscosity tensor.
- Analysis of the resulting turbulent effective force terms, including couplings to vorticity.
- Investigation of angular momentum nonconserving effects in the rotating frame.
- Application of axisymmetry constraints to response functions and two-point velocity correlations.
Main Results:
- The effective stress tensor in homogeneous turbulent rotating fluids is anisotropic.
- New terms in the large-scale turbulent effective force arise from the generalized viscosity tensor.
- Some terms exhibit couplings to vorticity, while others are angular momentum nonconserving.
- Axisymmetry imposes specific constraints on the response function and velocity correlations.
Conclusions:
- The generalized axisymmetric viscosity tensor provides a more complete description of turbulent rotating fluids.
- The identified new force terms and nonconserving effects are significant for large-scale dynamics.
- Comparison with existing models highlights the advancements in describing anisotropic turbulence.