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Patchy Colloids, Proteins and Network Forming Liquids: Analogies and new insights from computer simulations Lyon - CECAM - June 26-28 Dynamics in patchy.

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Presentation on theme: "Patchy Colloids, Proteins and Network Forming Liquids: Analogies and new insights from computer simulations Lyon - CECAM - June 26-28 Dynamics in patchy."— Presentation transcript:

1 Patchy Colloids, Proteins and Network Forming Liquids: Analogies and new insights from computer simulations Lyon - CECAM - June 26-28 Dynamics in patchy colloids and network forming liquids: gels and strong glass-forming liquids Francesco Sciortino

2 Motivations The fate of the liquid state…. Gels and phase separation: essential features (Sticky colloids - Proteins, network-forming liquids) Models of patchy particles. Why to revisit them ? Thermodynamic and dynamic behavior of new patchy colloids. Clues in understanding dynamics in network forming liquids (Silica, water….) Essential ingredients of “strong behavior” (A. Angell scheme) in glass-forming liquids.

3 Glass line (D->0) Liquid-Gas Spinodal Binary Mixture LJ particles “Equilibrium” “homogeoues” arrested states only for large packing fraction BMLJ

4 The general (spherical) case (for hard core complemented by attraction)

5 N max =4 phase diagram - Isodiffusivity lines

6 The PMW model J. Kolafa and I. Nezbeda, Mol. Phys. 161 87 (1987) Hard-Sphere + 4 sites (2H, 2LP) Tetrahedral arrangement H-LP interact via a SW Potential, of range  0.15 . V(r) r  (length scale) (energy scale) u0u0 Bonding is properly defined --- Lowest energy state is well defined

7 The PMS Model Ford, Auerbach, Monson, J.Chem.Phys, 8415,121 (2004) Silicon Four sites (tetrahedral) Oxygen Two sites 145.8 o  OO =1.6   SW interaction between Si sites and O sites 

8 Equilibrium phase diagram (PMW)

9 Pagan and Gunton JCP (2005) Pagan-Gunton

10 Equilibrium Phase Diagram PSM

11 Critical Point of PMW GC simulation BOX SIZE=  T C =0.1095  C =0.153

12 Critical Point of PMS GC simulation BOX SIZE=  T C =0.075  C =0.0445 s=0.45 Critical point PSM

13 Potential Energy for the PMW Optimal density !

14 Potential Energy -- Approaching the ground state Progressive increase in packing prevents approach to the GS PMW energy

15 E-E gs vs. 1/T

16 Potential Energy along isotherms Optimal density Hints of a LL CP

17 S(q) in the phase-separation region

18 S(q) in the network region

19 PMS -Potential Energy

20 PMS E vs 1/T

21 PMS Structure (r-space)

22 Structure (q-space)

23 E vs n

24 Summary of static data Optimal Network Region - Arrhenius Approach to Ground State Region of phase separation Packing Region Phase Separation Region Packing Region

25 R2 vs t

26 Diffusion Coefficient

27 D along isotherms Diffusion Anomalies

28 Isodiffusivities …. Isodiffusivities (PMW) ….

29 Si dynamic in PSM

30

31 Comparing different potentials Bonded-triples angle 

32 How to compare these (and other) models for tetra- coordinated liquids ? Focus ONLY on the # of 4-coordinated particles (other particles are “bond-mediators”) (#) Length scale ---- nn-distance among 4-coordinated particles (l 44 ) Scaled Density = # (l 44 ) 3 /V Energy scale ---- Tc

33 Comparing E(n) at low T

34 Comparing isodiffusivity lines

35 Analogies with other network-forming potentials SPC/E ST2 (Poole) BKS silica (Saika-Voivod) Faster on compression Slower on compression

36 Water Phase Diagram  ~ 0.34

37 Comments Directional interaction and limited valency are essential ingredients for offering a new final fate to the liquid state and in particular to arrested states at low  The resulting low T liquid state is (along isochores) a strong liquid. Directional bonding is essential for being strong. Gels and strong liquids are two faces of the same medal.

38 Graphic Summary Two glass lines ? Strong liquids - Gels Arrest line Fragile Liquids - Colloidal Glasses

39 Coworkers: Cristiano De Michele (PMW,PMS) Simone Gabrielli (PMW) Piero Tartaglia Emanuela Zaccarelli

40 http://www.socobim.de/

41 Gelation as a result of phase separation (interrupted by the glass transition) T T  

42 Density Anomalies… (and possible 2’nd CP) Density anomalies

43

44

45 D vs (1-p b )

46 D vs (1-p b ) --- (MC) D ~ f 0 4 ~(Stanley-Teixeira)

47 G. Foffi, E. Zaccarelli, S. V. Buldyrev, F. Sciortino, P. Tartaglia Aging in short range attractive colloids: A numerical study J. Chem. Phys. 120, 1824, 2004 Foffi aging


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