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LBM: Approximate Invariant Manifolds and Stability Alexander Gorban (Leicester) Tuesday 07 September 2010, 16:50-17:30 Seminar Room 1, Newton Institute.

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Presentation on theme: "LBM: Approximate Invariant Manifolds and Stability Alexander Gorban (Leicester) Tuesday 07 September 2010, 16:50-17:30 Seminar Room 1, Newton Institute."— Presentation transcript:

1 LBM: Approximate Invariant Manifolds and Stability Alexander Gorban (Leicester) Tuesday 07 September 2010, 16:50-17:30 Seminar Room 1, Newton Institute 1

2 In LBM “Nonlinearity is local, non-locality is linear” (Sauro Succi) Moreover, in LBM non-locality is linear, exact and explicit 2

3 Plan Two ways for LBM definition Building blocks: Advection-Macrovariables- Collisions- Equilibria Invariant manifolds for LBM chain and Invariance Equation, Solutions to Invariance Equation by time step expansion, stability theorem Macroscopic equations and matching conditions Examples 3

4 Scheme of LBM approach Microscopic model (The Boltzmann Equation) Asymptotic Expansion “Macroscopic” model (Navier-Stokes) Discretization in velocity space Finite velocity model Discretization in space and time Discrete lattice Boltzmann model Approximation 4

5 Simplified scheme of LBM “Macroscopic” model (Navier-Stokes) after initial layer Dynamics of discrete lattice Boltzmann model Time step expansion for IM 5

6 Elementary advection 6

7 Advection 7 Microvariables – f i

8 Macrovariables: 8

9 Properties of collisions 9

10 Equilibria 10

11 LBM chain 11 f→advection(f) → collision(advection(f))→ advection(collision(advection(f) )) → collision(advection(collision(advection(f))) →...

12 Invariance equation 12

13 Solution to Invariance Equation 13

14 LBM up to the kth order 14

15 Stability theorem: conditions 15 Contraction is uniform:

16 Stability theorem 16 There exist such constants That for The distance from f(t) to the kth order invariant manifold is less than Cε k+1

17 Macroscopic Equations 17

18 Construction of macroscopic equations and matching condition 18

19 19 Space discretization: if the grid is advection-invariant then no efforts are needed 19 ●●●●●●●● ●●●●●●●● ●●●●●●●● ●●●●●●●● ●●●●●●●● ●●●●●●●● ●●●●●●●● ●●●●●●●●

20 1D athermal equilibrium, v={0,±1}, T=1/3, matching moments, BGK collisions 20 c~1,u≤Ma

21 2D Athermal 9 velocities model (D2Q9), equilibrium 21

22 2D Athermal 9 velocities model (D2Q9) 22 c~1,u≤Ma

23 References 23 Succi, S.: The lattice Boltzmann equation for fluid dynamics and beyond. Oxford University Press, New York (2001) He, X., Luo., L. S.: Theory of the lattice Boltzmann method: From the Boltzmann equation to the lattice Boltzmann Equation. Phys Rev E 56(6) (1997) 6811–6817 Gorban, A. N., Karlin, I. V.: Invariant Manifolds for Physical and Chemical Kinetics. Springer, Berlin – Heidelberg (2005) Packwood, D.J., Levesley, J., Gorban A.N.: Time Step Expansions and the Invariant Manifold Approach to Lattice Boltzmann Models, arXiv:1006.3270v1 [cond-mat.stat-mech]arXiv:1006.3270v1

24 Questions please 24 Vorticity, Re=5000


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