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Non-Equilibrium Computer Experiments of Soft Matter Systems Arash Nikoubashman Institute of Theoretical Physics Vienna University of Technology [email protected]

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Page 1: Non-Equilibrium Computer Experiments of Soft Matter Systems Arash Nikoubashman Institute of Theoretical Physics Vienna University of Technology arash.nikoubashman@tuwien.ac.at

Non-Equilibrium Computer Experiments of Soft Matter Systems

Arash Nikoubashman

Institute of Theoretical PhysicsVienna University of Technology

[email protected]

Page 2: Non-Equilibrium Computer Experiments of Soft Matter Systems Arash Nikoubashman Institute of Theoretical Physics Vienna University of Technology arash.nikoubashman@tuwien.ac.at

Table of Contents

• Introduction• Simulation Technique• Flow Properties of Cluster Crystals• Cluster Crystals under Shear Flow• Cluster Crystals under Poiseuille Flow• Conclusions & Outlook• Appendix

Page 3: Non-Equilibrium Computer Experiments of Soft Matter Systems Arash Nikoubashman Institute of Theoretical Physics Vienna University of Technology arash.nikoubashman@tuwien.ac.at

Introduction

What is Soft matter?• Mesoscopic particles (1nm – 1mm) dispersed in

an atomic solvent

Page 4: Non-Equilibrium Computer Experiments of Soft Matter Systems Arash Nikoubashman Institute of Theoretical Physics Vienna University of Technology arash.nikoubashman@tuwien.ac.at

Introduction

What is Soft matter?• Mesoscopic particles (1nm – 1mm) dispersed in

an atomic solvent

• Everyday soft materials:• Blood

Page 5: Non-Equilibrium Computer Experiments of Soft Matter Systems Arash Nikoubashman Institute of Theoretical Physics Vienna University of Technology arash.nikoubashman@tuwien.ac.at

Introduction

What is Soft matter?• Mesoscopic particles (1nm – 1mm) dispersed in

an atomic solvent

• Everyday soft materials:• Blood• Paint

Page 6: Non-Equilibrium Computer Experiments of Soft Matter Systems Arash Nikoubashman Institute of Theoretical Physics Vienna University of Technology arash.nikoubashman@tuwien.ac.at

Introduction

What is Soft matter?• Mesoscopic particles (1nm – 1mm) dispersed in

an atomic solvent

• Everyday soft materials:• Blood• Paint• Milk

Page 7: Non-Equilibrium Computer Experiments of Soft Matter Systems Arash Nikoubashman Institute of Theoretical Physics Vienna University of Technology arash.nikoubashman@tuwien.ac.at

Introduction

What is Soft matter?• Mesoscopic particles (1nm – 1mm) dispersed in

an atomic solvent

• Everyday soft materials:• Blood• Paint• Milk• Ice Cream

Page 8: Non-Equilibrium Computer Experiments of Soft Matter Systems Arash Nikoubashman Institute of Theoretical Physics Vienna University of Technology arash.nikoubashman@tuwien.ac.at

Introduction

…and why are these substances soft?• Elastic constant G for a simple cubic crystal1:

G = 1/v eF’’(r=a)

[1] C. N. Likos, Phys. Rep. 348, 267 (2001)

Atomic Crystal Colloidal Crystal

e 10-1 – 10 eV kBT ≃ 1/40 eV

F Irrelevant Irrelevant

v Å3 = 10-30 m3 10-18 – 10-21 m3

Gcolloidal/Gatomic = 10-12 – 10-9

Page 9: Non-Equilibrium Computer Experiments of Soft Matter Systems Arash Nikoubashman Institute of Theoretical Physics Vienna University of Technology arash.nikoubashman@tuwien.ac.at

Introduction

Why is soft matter out of equilibrium interesting?

Page 10: Non-Equilibrium Computer Experiments of Soft Matter Systems Arash Nikoubashman Institute of Theoretical Physics Vienna University of Technology arash.nikoubashman@tuwien.ac.at

Introduction

It is omnipresent in our daily lives!

Page 11: Non-Equilibrium Computer Experiments of Soft Matter Systems Arash Nikoubashman Institute of Theoretical Physics Vienna University of Technology arash.nikoubashman@tuwien.ac.at

Introduction

It is omnipresent in our daily lives!• Cellular transport2

[2] Medalia et al., Science 298, 1209 (2002)

Page 12: Non-Equilibrium Computer Experiments of Soft Matter Systems Arash Nikoubashman Institute of Theoretical Physics Vienna University of Technology arash.nikoubashman@tuwien.ac.at

Introduction

It is omnipresent in our daily lives!• Cellular transport• DNA sequencing3

[3] M. Zwolak and M. Di Ventra, Rev. Mod. Phys. 80, 141 (2008)

Page 13: Non-Equilibrium Computer Experiments of Soft Matter Systems Arash Nikoubashman Institute of Theoretical Physics Vienna University of Technology arash.nikoubashman@tuwien.ac.at

Introduction

It is omnipresent in our daily lives!• Cellular transport• DNA sequencing• Blood flow4

[4] Pan et al., Microvasc. Res. 82, 163 (2011)

Page 14: Non-Equilibrium Computer Experiments of Soft Matter Systems Arash Nikoubashman Institute of Theoretical Physics Vienna University of Technology arash.nikoubashman@tuwien.ac.at

Introduction

It is omnipresent in our daily lives!• Cellular transport• DNA sequencing• Blood flow• Microfluidics5

[5] T. M. Squires and S. R. Quake, Rev. Mod. Phys. 77, 977 (2005)

Page 15: Non-Equilibrium Computer Experiments of Soft Matter Systems Arash Nikoubashman Institute of Theoretical Physics Vienna University of Technology arash.nikoubashman@tuwien.ac.at

Introduction

It is omnipresent in our daily lives!• Cellular transport• DNA sequencing• Blood flow• Microfluidics• Paint

Page 16: Non-Equilibrium Computer Experiments of Soft Matter Systems Arash Nikoubashman Institute of Theoretical Physics Vienna University of Technology arash.nikoubashman@tuwien.ac.at

Introduction

It is omnipresent in our daily lives!• Cellular transport• DNA sequencing• Blood flow• Microfluidics• Paint• Oil recovery

Page 17: Non-Equilibrium Computer Experiments of Soft Matter Systems Arash Nikoubashman Institute of Theoretical Physics Vienna University of Technology arash.nikoubashman@tuwien.ac.at

Introduction

Interesting flow properties!• Shear thickening6

[6] http://www.youtube.com/watch?v=KL8--cmew3k

Page 18: Non-Equilibrium Computer Experiments of Soft Matter Systems Arash Nikoubashman Institute of Theoretical Physics Vienna University of Technology arash.nikoubashman@tuwien.ac.at

Introduction

Interesting flow properties!• Shear thickening• Shear thinning7

[7] http://www.youtube.com/watch?v=pes1Ju1Cl8o

Page 19: Non-Equilibrium Computer Experiments of Soft Matter Systems Arash Nikoubashman Institute of Theoretical Physics Vienna University of Technology arash.nikoubashman@tuwien.ac.at

Introduction

Interesting flow properties!• Shear thickening• Shear thinning• Ferrofluidics8

[8] http://www.kodama.hc.uec.ac.jp/spiral/

… and much more

Page 20: Non-Equilibrium Computer Experiments of Soft Matter Systems Arash Nikoubashman Institute of Theoretical Physics Vienna University of Technology arash.nikoubashman@tuwien.ac.at

Table of Contents

• Introduction• Simulation Technique• Flow Properties of Cluster Crystals• Cluster Crystals under Shear Flow• Cluster Crystals under Poiseuille Flow• Conclusions & Outlook• Appendix

Page 21: Non-Equilibrium Computer Experiments of Soft Matter Systems Arash Nikoubashman Institute of Theoretical Physics Vienna University of Technology arash.nikoubashman@tuwien.ac.at

Simulation Technique

Computational task• Simulation of complex

fluids in and out of equilibrium• Take hydrodynamic

interactions (HI) of solvent into account9

[9] http://iffwww.kfa-juelich.de/www/Applets/iMPC/

Page 22: Non-Equilibrium Computer Experiments of Soft Matter Systems Arash Nikoubashman Institute of Theoretical Physics Vienna University of Technology arash.nikoubashman@tuwien.ac.at

Simulation Technique

“Naïve” approach: pure MD simulations • Pro:• Straight-forward implementation• Atomistic simulations• Contra:• Large disparity in length- and timescales between

solute and solvent particlesComputationally expensive, O(N2)

Page 23: Non-Equilibrium Computer Experiments of Soft Matter Systems Arash Nikoubashman Institute of Theoretical Physics Vienna University of Technology arash.nikoubashman@tuwien.ac.at

Simulation Technique

“Our” approach: Multi-Particle Collision Dynamics10 • Pro:• Hydrodynamics fully resolved• Thermal fluctuations preserved• Many different flow fields possible• Can be easily integrated into existing MD codes• Very fast and scalable algorithm, O(N)• Contra:• Coarse grained fluid

[10] A. Malevanets & R. Kapral, J. Chem. Phys. 110, 8605 (1999)

Page 24: Non-Equilibrium Computer Experiments of Soft Matter Systems Arash Nikoubashman Institute of Theoretical Physics Vienna University of Technology arash.nikoubashman@tuwien.ac.at

Shear flow Poiseuille flow

Simulation Technique

• Flow profile not superimposed, but self-emerging (through the appropriate boundary conditions)• Thus, we can induce:• Wall-Slip• Nonlinear velocity profiles• …

Page 25: Non-Equilibrium Computer Experiments of Soft Matter Systems Arash Nikoubashman Institute of Theoretical Physics Vienna University of Technology arash.nikoubashman@tuwien.ac.at

Table of Contents

• Introduction• Simulation Technique• Flow Properties of Cluster Crystals• Cluster Crystals under Shear Flow• Cluster Crystals under Poiseuille Flow• Conclusions & Outlook• Appendix

Page 26: Non-Equilibrium Computer Experiments of Soft Matter Systems Arash Nikoubashman Institute of Theoretical Physics Vienna University of Technology arash.nikoubashman@tuwien.ac.at

Flow Properties of Cluster Crystals

• We study particles interacting via GEM potential:

• Potential is:• Purely repulsive• Bounded

Partial and full particle overlap is possible

Page 27: Non-Equilibrium Computer Experiments of Soft Matter Systems Arash Nikoubashman Institute of Theoretical Physics Vienna University of Technology arash.nikoubashman@tuwien.ac.at

Flow Properties of Cluster Crystals

GEM crystals have peculiar equilibrium properties• Clustering• Density independent lattice constant• Activated hopping

Page 28: Non-Equilibrium Computer Experiments of Soft Matter Systems Arash Nikoubashman Institute of Theoretical Physics Vienna University of Technology arash.nikoubashman@tuwien.ac.at

Cluster Crystals under Shear Flow

• What happens out of equilibrium?• Let’s shear the system11!

soft

hard ?

[11] A. Nikoubashman, G. Kahl and C. N. Likos, Phys Rev. Lett. 107, 068302 (2011)

Page 29: Non-Equilibrium Computer Experiments of Soft Matter Systems Arash Nikoubashman Institute of Theoretical Physics Vienna University of Technology arash.nikoubashman@tuwien.ac.at

Cluster Crystals under Shear Flow

Page 30: Non-Equilibrium Computer Experiments of Soft Matter Systems Arash Nikoubashman Institute of Theoretical Physics Vienna University of Technology arash.nikoubashman@tuwien.ac.at

Cluster Crystals under Shear Flow

• Shear destroys crystalline order• System melts and array of strings emerges!

soft

hard

Page 31: Non-Equilibrium Computer Experiments of Soft Matter Systems Arash Nikoubashman Institute of Theoretical Physics Vienna University of Technology arash.nikoubashman@tuwien.ac.at

Cluster Crystals under Shear Flow

• What if we shear even stronger?

soft

hard ?

Page 32: Non-Equilibrium Computer Experiments of Soft Matter Systems Arash Nikoubashman Institute of Theoretical Physics Vienna University of Technology arash.nikoubashman@tuwien.ac.at

Cluster Crystals under Shear Flow

• Particles can escape from their string• System destabilizes and melts completely

soft

hard

Page 33: Non-Equilibrium Computer Experiments of Soft Matter Systems Arash Nikoubashman Institute of Theoretical Physics Vienna University of Technology arash.nikoubashman@tuwien.ac.at

Cluster Crystals under Shear Flow

• Potential exerted by a string of GEM particles

Page 34: Non-Equilibrium Computer Experiments of Soft Matter Systems Arash Nikoubashman Institute of Theoretical Physics Vienna University of Technology arash.nikoubashman@tuwien.ac.at

Cluster Crystals under Shear Flow

• Free volume decreases rapidly• Fluid resistance grows, viscosity increases

Free volume of the system as a function of shear-rate

Page 35: Non-Equilibrium Computer Experiments of Soft Matter Systems Arash Nikoubashman Institute of Theoretical Physics Vienna University of Technology arash.nikoubashman@tuwien.ac.at

Cluster Crystals under Shear Flow

• Free volume decreases rapidly• Fluid resistance grows, viscosity increases

Shear-stress as a function of shear-rate

Page 36: Non-Equilibrium Computer Experiments of Soft Matter Systems Arash Nikoubashman Institute of Theoretical Physics Vienna University of Technology arash.nikoubashman@tuwien.ac.at

Table of Contents

• Introduction• Simulation Technique• Flow Properties of Cluster Crystals• Cluster Crystals under Shear Flow• Cluster Crystals under Poiseuille Flow• Conclusions & Outlook• Appendix

Page 37: Non-Equilibrium Computer Experiments of Soft Matter Systems Arash Nikoubashman Institute of Theoretical Physics Vienna University of Technology arash.nikoubashman@tuwien.ac.at

Cluster Crystals under Poiseuille Flow

Expose cluster crystal to Poiseuille flow12

• Velocity profile of pure solvent:

• Local shear rate:

How does the crystal react?

[12] A. Nikoubashman, G. Kahl and C. N. Likos, Soft Matter, DOI:10.10139/c1sm06899g (2012)

Page 38: Non-Equilibrium Computer Experiments of Soft Matter Systems Arash Nikoubashman Institute of Theoretical Physics Vienna University of Technology arash.nikoubashman@tuwien.ac.at

Cluster Crystals under Poiseuille Flow

Scenario I• String-formation close to

the walls• Crystalline layer(s) at the

center of the channel

Scenario II• String phase is global, no

microphase separation!

Crystalline layers act on strings as external potential

Strings break up into clumps

Thick crystalline slab flows

Presence of crystal flattens velocity profile

Page 39: Non-Equilibrium Computer Experiments of Soft Matter Systems Arash Nikoubashman Institute of Theoretical Physics Vienna University of Technology arash.nikoubashman@tuwien.ac.at

Cluster Crystals under Poiseuille Flow

Page 40: Non-Equilibrium Computer Experiments of Soft Matter Systems Arash Nikoubashman Institute of Theoretical Physics Vienna University of Technology arash.nikoubashman@tuwien.ac.at

Cluster Crystals under Poiseuille Flow

Flow strongly affected by GEM crystal

Velocity profile of the liquid in the presence of the GEM crystal

Particle flux of solute particles. Arrows indicate when the first layer melts

Page 41: Non-Equilibrium Computer Experiments of Soft Matter Systems Arash Nikoubashman Institute of Theoretical Physics Vienna University of Technology arash.nikoubashman@tuwien.ac.at

Cluster Crystals under Poiseuille Flow

Flow quantization

Plateau height of the plug flow pattern Width of the flat part of the velocity profile

Page 42: Non-Equilibrium Computer Experiments of Soft Matter Systems Arash Nikoubashman Institute of Theoretical Physics Vienna University of Technology arash.nikoubashman@tuwien.ac.at

Table of Contents

• Introduction• Simulation Technique• Flow Properties of Cluster Crystals• Cluster Crystals under Shear Flow• Cluster Crystals under Poiseuille Flow• Conclusions & Outlook• Appendix

Page 43: Non-Equilibrium Computer Experiments of Soft Matter Systems Arash Nikoubashman Institute of Theoretical Physics Vienna University of Technology arash.nikoubashman@tuwien.ac.at

Conclusions & Outlook

Conclusions•Soft matter in and out of equilibrium is ubiquitous in our daily lives•MPCD technique is a suitable means for studying it

Outlook•Monomer resolved simulations of cluster crystals•Polymeric networks under flow

Page 44: Non-Equilibrium Computer Experiments of Soft Matter Systems Arash Nikoubashman Institute of Theoretical Physics Vienna University of Technology arash.nikoubashman@tuwien.ac.at

Thank you for your attention!

The End

Page 45: Non-Equilibrium Computer Experiments of Soft Matter Systems Arash Nikoubashman Institute of Theoretical Physics Vienna University of Technology arash.nikoubashman@tuwien.ac.at

Table of Contents

• Introduction• Simulation Technique• Flow Properties of Cluster Crystals• Cluster Crystals under Shear Flow• Cluster Crystals under Poiseuille Flow• Conclusions & Outlook• Appendix

Page 46: Non-Equilibrium Computer Experiments of Soft Matter Systems Arash Nikoubashman Institute of Theoretical Physics Vienna University of Technology arash.nikoubashman@tuwien.ac.at

Appendix

Flow dynamics: two step process1. Streaming step:

Page 47: Non-Equilibrium Computer Experiments of Soft Matter Systems Arash Nikoubashman Institute of Theoretical Physics Vienna University of Technology arash.nikoubashman@tuwien.ac.at

Appendix

Flow dynamics: two step process1. Streaming step:2. Collision step:

Page 48: Non-Equilibrium Computer Experiments of Soft Matter Systems Arash Nikoubashman Institute of Theoretical Physics Vienna University of Technology arash.nikoubashman@tuwien.ac.at

Appendix

• String-formation independent of initial configuration• Can we exploit this to accelerate crystallization?

Page 49: Non-Equilibrium Computer Experiments of Soft Matter Systems Arash Nikoubashman Institute of Theoretical Physics Vienna University of Technology arash.nikoubashman@tuwien.ac.at

Appendix

Yes, shear facilitates the crystallization process10!

Color coded density profiles. Top half: unsheared system, lower half: presheared system

[10] A. Nikoubashman, G. Kahl and C. N. Likos, Soft Matter, DOI:10.10139/c1sm06899g (2012)

Page 50: Non-Equilibrium Computer Experiments of Soft Matter Systems Arash Nikoubashman Institute of Theoretical Physics Vienna University of Technology arash.nikoubashman@tuwien.ac.at

Appendix

Page 51: Non-Equilibrium Computer Experiments of Soft Matter Systems Arash Nikoubashman Institute of Theoretical Physics Vienna University of Technology arash.nikoubashman@tuwien.ac.at

Appendix

Page 52: Non-Equilibrium Computer Experiments of Soft Matter Systems Arash Nikoubashman Institute of Theoretical Physics Vienna University of Technology arash.nikoubashman@tuwien.ac.at

Appendix