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Simulation of anisotropic turbulence transport

R. Minero

Download PDF (1.72 MB)

Project description:

Anisotropic turbulence

Turbulence in engineering problems, in meteorology, or in plasma physics is mostly anisotropic. For instance the buoyancy and Coriolis forces in the ocean surpress motion in vertical direction, making the flow two-dimensional of nature. A typical property of 2D-turbulence is the self organization of the flow, resulting in large eddies (see Figure 1).

vort1.jpg  
vort2.jpg  
Figure 1 - Vorticity plots, showing the self organization of 2D turbulence, for the time t = 1 and t = 50 with Reynolds number Re = 3000 [I].

Transport

Tracer transport in anisotropic turbulence is characterized by a large scale separation between the size of the turbulent eddies and the filaments of the tracer material. For solving the tracer concentration even a higher resolution is required than for the turbulent flow field. Transport can be studied more efficiently by applying the LDC technique on a problem with a local dye distribution (see Figure 2).

transport0.jpg  
transport1.jpg  
Figure 2 - Tracer transport of an initial local dye distribution in the flow field of Figure 1 for t > 50.

Local Defect Correction (LDC)

Local Defect Correction (LDC) is a method that can be used to efficiently solve problems whose solutions exhibit large variations in a small part of the domain. LDC iteratively combines the solution over a global coarse grid and the solution over one or more local fine grids [2]; the fine grids are located where the high activity occurs (see Figure 3).

transport_ldc.jpg  
Figure 3 - Coarse and fine grid to solve a transport problem with a high activity in a small part of the domain using LDC

The global grid provides artificial boundary conditions for the fine grid interface whereas the (more accurate) local solutions provide an error estimate for the coarse grid discretization: the defect (see Figure 4). The main advantages of LDC are saving CPU time, since the grid is fine only where it needs to be, and preserving a simple data structure.

scheme_ldc.jpg
Figure 4 - Scheme of LDC

LDC: an example of application

Figure 5 shows the Finite Differences approximation of a 1D Poisson equation, whose exact solution is a tanh function, treated with LDC. LDC considerably improves the initial approximation after a single iteration.

ldc1.jpg
ldc2.jpg
ldc3.jpg
ldc4.jpg
Figure 5 - Finite differences solution of a 1D Possion equation improved using LDC

LDC seems to be a promising tool to solve transport problems in anisotropic turbulent flows.

References

[1] S.R. Maassen, PhD thesis, TUE, 2000.
[2] M.J.H. Anthonissen, PhD thesis, TUE, 2001.





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