Transcript Document

A stochastic Molecular Dynamics method for multiscale
modeling of blood platelet phenomena
•PIs: G.E. Karniadakis, P.D. Richardson, M.R. Maxey
•Collaborators: Harvard Medical School, Imperial College, Ben Gurion
•Arterioles/venules 50 microns
activated platelets
•Platelet diameter is 2-4 µm
•Normal platelet concentration in
blood is 300,000/mm3
•Functions: activation, adhesion to
injured walls, and other platelets
•Multiscale Simulation of Arterial Tree on TeraGrid
Platelet and Fibrin Aggregation
1
2
3
4
Creation of Fibrin Threads
•Fibrinogen consists of three pairs of protein chains
•Prothrombin/thrombin activate fibrinogen
•Fibrinogen monomers create fibrin threads
Objectives
•
Develop new algorithms that will make coarse-grained molecular
dynamics (MD), and DPD in particular, a very effective simulation
tool for biological flows.
•
Couple DPD-MD at the molecular level (protein interactions, scales
less than 10 nm), and DPD-continuum at the large scales (hybrid
3D/1D arterial tree model).
•
Validate simulations of platelet aggregation against existing in-vivo
and in-vitro experiments and quantify uncertainties.
•
Study thrombous formation and migration in the circulatory
system.
•
Disseminate algorithmic framework for multiscale coupling and
software to interested parties.
•
Involve undergraduates in this research and introduce high-school
students to computational science and cyber-infrastructure.
Computational Methods
• Force Coupling
Method (FCM)
(continuum)
• Dissipative Particle
Dynamics (DPD)
(mesoscopic)
• Molecular Dynamics
(LAMMPS)
Dissipative Particle Dynamics (DPD) – Coarse-Grained MD
MD
DPD
•Momentum-conserving
•Galilean-invariant
•Off-lattice
•Soft-potentials
•Conservative
•Speed-up w.r.t. MD (N mol/DPD)
•Dissipative
•1000 x N8/3; e.g. N=10: 500,000 times
•Random
Periodic
F
Periodic
•Drag coefficient
Periodic
•viscosity
Periodic
Intra-Polymer Forces – Combinations Of the Following:
• Lennard-Jones Repulsion
• Stiff (Fraenkel) / Hookean Spring
• Finitely-Extensible Non-linear Elastic (FENE) Spring
Intra-Polymer Forces (continued)
• Marko-Siggia WormLike Chain
Can be adjusted if M>2
(Underhill, Doyle 2004)
Stiff: Schlijper, Hoogerbrugge, Manke, 1995
Hookean + Lennard-Jones: Nikunen, Karttunen, Vattulainen, 2003
FENE: Chen, Phan-Thien, Fan, Khoo, 2004
Radius of Gyration for Polymer Chains
Rg  (M 1)0.50
Rg  (M 1)0.59
Linear, ideal
Rg
2
Excluded volume, real
1

M
M

i 1
Flory Formula
 
100 beads
3
d  2
50 beads
20 beads
10 beads
5 beads
( Ri  Rcm ) 2
Mixing Soft-Hard Potentials
Motivation for 2 different time-steps (Δt,δt):
Symeonidis & Karniadakis, J. Comp. Phys., on line, 2006
Solvent
(soft repulsive)
Polymer
Lennard-Jones
(hard repulsive)
Forrest+Suter, (J. Chem. Phys., 1995)
idea of pre-averaging - in the spirit of
conservative forces in DPD solvent
DNA Dynamics: Shear Flow – Wormlike Chain
Sc ~ 35
Sc ~ 690
Sc ~ 2574
Sc ≈ 1.4 x Γ2
kBT=0.2
FENE Chains in Poiseuille Flow
10 beads
H/2Rg=3.96
Center-of-Mass Distribution From Wall
60 beads
H/2Rg=1.32
Stochastic Model - First Simulation of Begent & Born Experiment
•Thrombus growing on a blood vessel wall in vivo
•Accumulation of platelets in a thrombus
•Exponential thrombus growth rate coefficients -- effects of pulsation (right)
Effects of Red Blood Cells
•DPD simulations show exponential growth rate of thrombus
• RBCs increase diffusivity
Future Plans
•Effects of red blood cells (Experiment I, in vitro results)
•Deformation of cells (effect on aggregation rates)
•Model plasma adhesive proteins (vWf, fibrinogen, …)
•Simulate diffusion of chemicals (ADP, …)
•Validation against available experimental results
•Gorog’s hemostatometer (in-vitro)
•Begent & Born (in-vivo)
References on Dissipative Particle Dynamics
•E. Keaveny, I. Pivkin, M.R. Maxey and G.E. Karniadakis, “A comparative study between dissipative
particle dynamics and molecular dynamics for simple- and complex-geometry flows”, J. Chemical Physics,
vol. 123, p. 104107, 2005.
•I. Pivkin and G.E. Karniadakis, “A new method to impose no-slip boundary conditions in dissipative particle
dynamics”, J. Computational Phys., vol. 207, pp. 114-128, 2005.
•V. Symeonidis, G.E. Karniadakis and B. Caswell, “A seamless approach to multiscale complex fluid simulation”,
Computing in Science & Engineering, pp. 39-46, May/June 2005.
•V. Symeonidis, G.E. Karniadakis and B. Caswell, “Dissipative particle dynamics simulations of polymer chains:
Scaling laws and shearing response compared to DNA experiments”, Phys. Rev. Lett., vol 95, 076001, 2005.
•V. Symeonidis & G.E. Karniadakis, “A family of time-staggered schemes for integrating hybrid DPD models for
polymers: Algorithms and applications”, J. Computational Phys., available on line, 2006.
•I. Pivkin and G.E. Karniadakis, “Coarse-graining limits in open and wall-bounded DPD systems”, J. Chemical
Physics, vol 124, 184101, 2006.
•I. Pivkin and G.E. Karniadakis, “ Controlling density fluctuations in wall-bounded DPD systems, Phys. Rev. Lett.,
vol 96 (20), 206001, 2006