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Spatial Temporal Analysis of Fieldwise Flow in Microvasculature
Published on: November 18, 2019
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Flow of Spatiotemporal Turbulentlike Random Fields.
Jason Reneuve1, Laurent Chevillard2
1Laboratoire des Ecoulements Géophysiques et Industriels, Université Grenoble Alpes, CNRS, Grenoble-INP, F-38000 Grenoble, France.
Physical Review Letters
|July 18, 2020
Summary
Researchers studied rough, multifractal random vector fields to understand turbulence. Numerical simulations showed Lagrangian trajectories mirrored the field
Area of Science:
- Fluid dynamics
- Statistical physics
- Turbulence modeling
Background:
- Turbulence at infinite Reynolds numbers exhibits rough, multifractal properties in space and time.
- Understanding Lagrangian trajectories in such fields is crucial for turbulence phenomenology.
Purpose of the Study:
- To investigate Lagrangian trajectories in statistically isotropic, homogeneous, and stationary divergence-free spatiotemporal random vector fields.
- To design an advecting Eulerian velocity field that is asymptotically rough and multifractal.
- To analyze the roughness and intermittency of trajectories in such fields.
Main Methods:
- Designing a specific type of advecting Eulerian velocity field.
- Numerically solving flow equations for a differentiable version of this field.
- Analyzing Lagrangian trajectories using the Hurst exponent and identifying intermittent corrections.
Main Results:
- Lagrangian trajectories become rough, exhibiting a Hurst exponent similar to the advecting field.
- Additional intermittent corrections are observed in the Lagrangian framework, even with fractional Gaussian fields.
- The numerical findings suggest a connection between the advecting field's properties and trajectory behavior.
Conclusions:
- The study provides numerical evidence for rough and multifractal Lagrangian trajectories in designed random vector fields.
- The observed intermittency in Lagrangian trajectories warrants further rigorous theoretical investigation.
- This approach offers insights into the long-standing problem of turbulence at infinite Reynolds numbers.
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