Mesoscale%20modelling%20with%20the%20Lattice%20Boltzmann%20model - PowerPoint PPT Presentation

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Mesoscale%20modelling%20with%20the%20Lattice%20Boltzmann%20model

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Weighting factors chosen to ensure isotropic hydrodynamics. ... time hydrodynamic regime dominated by viscosity. Late-time inertial hydrodynamic regime: domains ... – PowerPoint PPT presentation

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Title: Mesoscale%20modelling%20with%20the%20Lattice%20Boltzmann%20model


1
Mesoscale modelling with the Lattice Boltzmann
model
  • Jonathan Chin

ltj.chin_at_qmul.ac.ukgt
2
Lattice Boltzmann Method
  • Fluids represented by fictional particles with
    discrete velocities, occupying sites on a
    discrete lattice.
  • Particles described by real-valued distribution
    function
  • Density of single component ? given by
  • Momentum of single component given by

3
Time Evolution
  • Advection step particles move to adjacent sites.
  • Collision step distribution function relaxes to
    equilibrium value via BGK operator.

4
  • The equilibrium distribution is a function only
    of density and velocity at a given site.
  • Weighting factors chosen to ensure isotropic
    hydrodynamics.
  • Bounce-back boundaries give non-slip walls.

5
  • Velocity is perturbed to take account of
    collisions with other components, and forcing
    term.
  • Force term includes gravity and Shan-Chen
    immiscibility force.
  • Immiscibility force proportional to
    single-component density gradient, repelling
    differing components.

6
Spinodal decomposition
  • Two fluids may mix above some temperature
  • A mixture quenched below this temperature will
    separate into its component fluids this process
    is called Spinodal Decomposition.
  • Simulation performed of demixing process using
    periodic boundary conditions.

7
Phase separation images
Timestep 0
500
1000
2000
4000
8000
32000
50000
8
Growth Regimes
  • Very early time exponential growth in structure
    factor as interfaces form according to a
    Cahn-Hilliard model.
  • Early-time hydrodynamic regime dominated by
    viscosity.
  • Late-time inertial hydrodynamic regime domains
    grow as two-thirds power of time.
  • Very late time turbulent mixing regime postulated
    but not seen.

9
Early-time Cahn-Hilliard Growth
  • Circularly-averaged structure factor S(k) retains
    shape but grows exponentially in magnitude as
    domains form.
  • Although the model does not define any free
    energies, it produces results in agreement with
    free-energy models of phase separation.

10
Domain Growth Laws
Porod Law structure
Power law growth
11
Breakdown of scaling
  • Many theories assume that a phase-separating
    system contains a single length scale evolving in
    time.
  • Simulation shows regime with multiple length
    scales due to competition between different
    growth mechanisms.

12
Surface tension measurement
  • Laplaces Law states that the pressure drop
    across the interface of a bubble is inversely
    proportional to its radius.
  • Bubbles simulated with different coupling
    constants to measure surface tension.
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