Turbulence and Lorenz Attractor

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SUMMARY

The discussion centers on the nature of turbulence and its relationship with deterministic processes, particularly through the lens of the Navier-Stokes (N-S) equations and the Lorenz Attractor. While Direct Numerical Simulation (DNS) of the N-S equations can accurately depict turbulent structures, the challenge lies in validating these results against experimental data due to the complexity of initial and boundary conditions. The conversation highlights the paradox of deterministic equations producing chaotic behavior, questioning whether this chaos arises from the equations themselves or from numerical instabilities in simulations. The insights shared are part of ongoing PhD research focused on uncovering mechanisms within the N-S equations that may explain this apparent chaos.

PREREQUISITES
  • Understanding of Navier-Stokes equations
  • Familiarity with Direct Numerical Simulation (DNS)
  • Knowledge of turbulence and chaotic systems
  • Concept of initial and boundary conditions in fluid dynamics
NEXT STEPS
  • Research the implications of high Reynolds numbers on turbulence
  • Explore the mathematical properties of the Lorenz Attractor
  • Investigate numerical methods for simulating fluid dynamics
  • Study the relationship between chaos theory and fluid dynamics
USEFUL FOR

Fluid dynamicists, researchers in chaos theory, and anyone interested in the complexities of turbulence and deterministic systems will benefit from this discussion.

Clausius2
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When one tries to have an insight into what the turbulence regime really is, one comes across the question of: is the turbulence a deterministic process or not? Even though we are able to simulate accurately turbulence with Direct Numerical Simulation (DNS) of the Navier-Stokes Equations, it is very difficult to test the results unless done assumming an statistically steady state. What I mean is that even though the DNS and its results are showing the major turbulent coherent structures and it comes from a deterministic model (N-S equations), it is very difficult to test its results with experiments unless the numerical results are averaged and compared with those flow experimentally averaged quantities.

Nowadays fluid dynamicists are prone to think that a turbulent process is governed by a set of deterministic equations such as N-S equations. That is, the process itself seems to be deterministic (how the coherent structures evolutes in time in space seems to have a physical explanation), but it is not quite the case of how the turbulence is triggered. The onset of turbulence seems to me to be influenciated by lot of random variables. I mean, even though we are able to use DNS, the whole key stays in the Initial and Boundary Conditions of integration. Those are kind of random and extraordinarily difficult to account for. The IC and BC in a laboratory facility may be impossible to simulate because they could belong to the randomness of some environmental conditions. As the Reynolds number becomes large, the sensivity of the flow to these small perturbations grows enormously, triggering the global instability.

What about the Lorenz Attractor http://mathworld.wolfram.com/LorenzAttractor.html?? Lorenz worked out this model thinking of the instabilty of a pure convective regime (large Rayleigh Number). It seems to me that this system is a generator of randomness even it is "deterministically determined" by a set of differential equations. My question is, what is triggering this apparently chaotic behavior?? i) Is it because the proper nature of the equations? ii) Or is it because a numerical instability impossible to overcome with nowadays methods??.

If i) is true, the lorenz attractor seems to me contradictory, because then a mathematical model is not as deterministic as I thought. But if ii) is true, that is the instability is caused by the numerical integration, I think it is telling us that despites we are unable of integrate the equations properly, the process is deterministic at the bottom. The Lorenz attractor seems a great comparison with the N-S equations at high Reynolds Numbers. Are they instable per se, generators of randomness, or on the contrary are we unable of integrating the properly propagating numerical errors which trigger finally the instability??.
 
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Interesting topic indeed... It is the current focus of my PhD study program... :-)

The turbulence behaviour could appear to be chaotic, when observed correctly - rather than using the typical statistical perspective favoured by many Fluid Dynamicists. There is a further physical mechanism however which seems to link back quite nicely with the 'chaotic' theme in the sense of determinism within turbulence, & in fact overlays a sense of order over this apparent chaos. Most Fluid Dynamicists have unfortunately been looking too hard in the wrong places... :-)

I have discovered this mechanism contained within the Navier-Stokes equations themselves & am presently writing a paper series describing this phenomenon. All of a sudden, much of the mystery surrounding these 'magic equations' has been exposed. Not all Fluids folks will, however, agree.

I'll have to contain my input at this point in order not to pre-empt my papers, but suffice it to say that I am able to substantiate these findings in numerous high-resolution numerical simulations.

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I'll look more deeply into the Lorenz Attractor & see if it could link back into my current findings. Why not? :-)
 

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