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3 Dicembre 2007Firenze
Francesco Sciortino Universita’ di Roma La Sapienza
“Patchy Colloidal Particles:The role of the valence
in gel formation
Introduzione
Main Messages
• Strongly interacting particles (u<<1)---with simple spherical potentials -- at small and intermediate densities ALWAYS phase-separate (in a dense and dilute phase)
• Strongly interacting particles with LIMITED valence ---patchy particles, highly directional interactions, dipolar, quadrupolar --- form equilibrium open structures (GELS, network forming liquids). Empty liquids
• Self-assembly as an equilibrium liquid-state problem
Outline• The fate of the liquid state (neglecting crystallization): phase
diagram of spherical and patchy attractive potentials • A theory-of-liquid approach to self-assembly in
equilibrium polymerization (linear and branched)
• The role of valence: Universality classes for the liquid-gas transition (analogies between network forming (strong) liquids and gels.
• Physical and chemical gels
Phase diagram of spherical potentials*0.13<c<0.27
*One component, “Hard-Core” *One component, “Hard-Core” plus attractionplus attraction
(From van der Waals to Baxter)
Phase diagram of spherical potentials*0.13<c<0.27 [if the attractive range
is very small ( <10%)]
*One component, “Hard-Core” *One component, “Hard-Core” plus attractionplus attraction
(From van der Waals to Baxter)
For this class of potentials arrest at low (gelation) is the result of a phase
separation process interrupted by the glass transition
T T
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(in preparation)
How to go to low T at low (in metastable equilibrium)
reducing “valence”
How to suppress phase separation ?
Patchy particles
Hard-Core (gray spheres) Short-range Square-Well (gold patchy sites)
No dispersion forces The essence of bonding !!!
maximum number of “bonds”, (different from fraction of bonding surface)
It enforces the one bond per patch condition
Pine’s particles
Self-Organization of Bidisperse Colloids in Water DropletsYoung-Sang Cho, Gi-Ra Yi, Jong-Min Lim, Shin-Hyun Kim, Vinothan N. Manoharan,, David J. Pine, and Seung-Man Yang J. Am. Chem. Soc.; 2005; 127(45) pp 15968 - 15975;
DNA functionalized particles
Wertheim TPT for associated liquids(particles with M identical sticky sites )
At low densities and low T (for SW)…..Vb
M=2
FS et al J. Chem.Phys.126, 194903, 2007
M=2 (Chains)
Symbols = Simulation
Lines = Wertheim Theory
<L>
FS et al J. Chem.Phys.126, 194903, 2007
Average chain length
Chain length distributions
What happens with branching ?
A snapshot of
<M>=2.025
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N3=330
N2=5670
T=0.05, =0.01
<M>=2.055
Wertheim theory predicts pb extremely well (in this model) !
(ground state accessed in equilibrium)
Connectivity properties and cluster size distributions: Flory and Wertheim
Connectivity properties and cluster size distributions: Flory and Wertheim
Connectivity properties and cluster size distributions: Flory and Wertheim
No bond-loops in finite clusters !
Generic features of the phase diagram
Cvmax line
Percolation line
unstable
Wertheim Theory (TPT): predictions
E. Bianchi et al, PRL 97, 168301, 2006
Mixtures of particles with 2 and 3 bonds
Empty liquids !Cooling the liquids without phase separating!
Phase Diagram - Theory and Simulations
theorysimulation
Conclusions (I)• Directional interaction and limited valency are essential ingredients for offering a DIFFERENT final fate to the liquid state and in particular to arrested states at low
• In the newly available density region, at low T the system forms a “equilibrium” gel. Arrest driven by bonding (not by caging).
Functionality 4
One Component(water-like)
Binary mixture
(silica-like)
DNA gel model (F. Starr and FS, JPCM, 2006J. Largo et al Langmuir 2007 )
BondSelectivity
StericIncompatibilities
Isodiffusivities ….Isodiffusivities (PMW) ….
DNA-Tetramers phase diagram
How to compare these (and other) models for tetra-coordinated liquids ?
Focus on the 4-coordinated particles (other particles are “bond-mediators”)
Energy scale ---- Tc
Length scale --- nn-distance among 4-coordinated particles
A collection of phase diagramsof four-coordinated liquids
Physical Gels <===> Network forming liquids
Quanto di questo che abbiamo imparato sulla valenza puo’ servirci a capire la gelazione chimica ?
Fino a che punto la gelazione chimica puo’ essere vista come un quench a U/kT --> oo ?
Irreversible aggregation in the absence of bond loops
(Smoluchowski)
Irreversible aggregation in the absence of loops
Smoluchowski coagulation works !
Equilibrium dynamics:
The Flory-Stokmayer distributions are also the equilibrium one !!!
Chemical and physical gelation (in the absence of loops)
t <---->T
Conclusions• Directional interaction and limited valency are essential ingredients for offering a DIFFERENT final fate to the liquid state and in particular to arrested states at low
• In the newly available density region, at low T the system forms a “equilibrium” gel (or a network glass).
• Equilibrium Gels and network forming liquids: two faces of the same medal.
• In the absence of bond-loops, chemical gelation proceeds via a sequence of quasi-equilibrium states (possibility of using phase-coexistence concepts)
Coworkers:
Emanuela Bianchi (Patchy Colloids)Cristiano De Michele (PMW, PMS)Julio Largo (DNA, Patchy Colloids)Francis Starr (DNA)Jack Douglas (NIST) (M=2)
Piero TartagliaEmanuela Zaccarelli