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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 colloids and network forming liquids: gels and strong glass-forming liquids Francesco Sciortino
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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.
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Glass line (D->0) Liquid-Gas Spinodal Binary Mixture LJ particles “Equilibrium” “homogeoues” arrested states only for large packing fraction BMLJ
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The general (spherical) case (for hard core complemented by attraction)
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N max =4 phase diagram - Isodiffusivity lines
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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
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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
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Equilibrium phase diagram (PMW)
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Pagan and Gunton JCP (2005) Pagan-Gunton
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Equilibrium Phase Diagram PSM
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Critical Point of PMW GC simulation BOX SIZE= T C =0.1095 C =0.153
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Critical Point of PMS GC simulation BOX SIZE= T C =0.075 C =0.0445 s=0.45 Critical point PSM
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Potential Energy for the PMW Optimal density !
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Potential Energy -- Approaching the ground state Progressive increase in packing prevents approach to the GS PMW energy
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E-E gs vs. 1/T
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Potential Energy along isotherms Optimal density Hints of a LL CP
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S(q) in the phase-separation region
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S(q) in the network region
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PMS -Potential Energy
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PMS E vs 1/T
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PMS Structure (r-space)
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Structure (q-space)
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E vs n
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Summary of static data Optimal Network Region - Arrhenius Approach to Ground State Region of phase separation Packing Region Phase Separation Region Packing Region
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R2 vs t
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Diffusion Coefficient
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D along isotherms Diffusion Anomalies
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Isodiffusivities …. Isodiffusivities (PMW) ….
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Si dynamic in PSM
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Comparing different potentials Bonded-triples angle
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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
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Comparing E(n) at low T
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Comparing isodiffusivity lines
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Analogies with other network-forming potentials SPC/E ST2 (Poole) BKS silica (Saika-Voivod) Faster on compression Slower on compression
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Water Phase Diagram ~ 0.34
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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.
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Graphic Summary Two glass lines ? Strong liquids - Gels Arrest line Fragile Liquids - Colloidal Glasses
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Coworkers: Cristiano De Michele (PMW,PMS) Simone Gabrielli (PMW) Piero Tartaglia Emanuela Zaccarelli
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http://www.socobim.de/
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Gelation as a result of phase separation (interrupted by the glass transition) T T
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Density Anomalies… (and possible 2’nd CP) Density anomalies
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D vs (1-p b )
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D vs (1-p b ) --- (MC) D ~ f 0 4 ~(Stanley-Teixeira)
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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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