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O' Berk Usta

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Title: O' Berk Usta


1
Simulations of Polymer Solutions in Periodic and
Confined GeometriesA Lattice-Boltzmann Approach

O. Berk Usta Anthony J. C. Ladd Jason E. Butler
Supported by the National Science Foundation
(CTS-0505929)
2
Overview Lattice-Boltzmann Method for
Polymer Simulations
  • Solve Navier-Stokes equations with Brownian
    stresses using lattice-Boltzmann method.
  • Represent polymers by a micromechanical model
    which is coupled with the solution for the flow
    field.
  • Simulate polymer as point particles having
    excluded volume (Ahlrichs and Duenweg J. Chem.
    Phys, 1999).
  • Connect point particles with potentials of choice
    (FENE, Hookean, etc.).
  • Addition of walls through simple bounce-back
    rules for the fluid-wall interactions.

3
Verification of the Model
  • Hydrodynamic Interactions
  • Fluid Response
  • Two Particle Mobility
  • Polymer Properties
  • Scaling of end-to-end distance and radius of
    gyration (RE, RG) with chain length (N)
  • Scaling of center of mass diffusion coefficient
    (DCM) with (N)
  • Effect of Schmidt number

4
Single Chain Simulations (Periodic)
O. B. Usta, A. J. C. Ladd, and J. E. Butler J.
Chem. Phys., 122, 094902, (2005)
5
Advantages of the Lattice-Boltzmann Method for
Polymer Simulations
  • Computation (primarily) scales with number of
    fluid nodes, not number of particles.
  • No need to calculate the Greens function for each
    new geometry.
  • Ideal for studying confined flows and can be
    extended to simulate semi-dilute polymer
    solutions.
  • Easy to code a basic Lattice-Boltzmann
    simulation.
  • Implementation of a parallel code is
    straightforward due to the local nature of the
    calculations.

6
Problems in Confined Geometries
  • Unidirectional Flows in Microchannels
  • Pressure Driven Flow
  • Lateral Migration
  • Dispersion and Separation
  • Simple Shear Flow
  • Lateral Migration
  • External Field Driven Flows
  • Combined Flows

7
Pressure Driven Flow
y
Vmax
H
x
z
Low Re
Flow Peclet Number
Confinement Level
8
Results
  • Wide Channels, Center of Mass Distribution

Wall
Center
9
The Mechanism (Ma Graham 2005)
Forces Polymer in tension.
Velocities Hydrodynamic lift away from wall.
10
External Forces
Particle Peclet Number
11
External Forces - Results
12
External Forces Effect of Hydrodynamic
Interactions
H/Rg8
Wall
Center
13
Mechanism 2 External Forces
  • Kinetic theory predicts a rotation of the polymer
    near the wall to a preferential orientation as
    shown.
  • Subsequently, the polymer drifts away from the
    wall due to the external force and hydrodynamic
    interactions between the beads.

14
Combined Flow
Concurrent
P1
P2
F
Countercurrent
H
15
Three Mechanisms
Rotation Due to Force Drift Due to Force
Lift Due to Shear
Rotation Due to Shear and Drift Due to Force (no
wall needed!)
F
U
F
16
Concurrent Application
17
Countercurrent Application
18
Conclusions and Continuing Work
  • The fluctuating lattice-Boltzmann method coupled
    to point particles is a flexible and efficient
    alternative for simulating polymers in solution.
  • Hydrodynamic interactions in bounded geometries
    can give rise to unexpected behavior such as
    migration.
  • Several different driving forces can induce
    migration.
  • Combination of these forces can be used to
    manipulate the migration.
  • Couple the current simulation capabilities with a
    detailed micromechanical model to predict the
    dynamics and viscoelastic properties actin
    filaments.
  • Combine with molecular scale models to simulate
    force generation by actin polymerization.
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