Adsorption versus Depletion of polymer solutions Self-Similar Adsorption profile Tails and Loops Adsorption Kinetics Summary. Polymer Adsorption
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1 Polymer Adsorption J.F. Joanny Physico-Chimie Curie Institut Curie APS March meeting/ PGG Symposium
2 Outline 1 Adsorption versus Depletion of polymer solutions Single Chain Adsorption Adsorption and Depletion of Semi-dilute solutions
3 Outline 1 Adsorption versus Depletion of polymer solutions Single Chain Adsorption Adsorption and Depletion of Semi-dilute solutions 2 Self-Similar Adsorption profile Scaling theory of an adsorbed polymer layer Colloid stabilization
4 Outline 1 Adsorption versus Depletion of polymer solutions Single Chain Adsorption Adsorption and Depletion of Semi-dilute solutions 2 Self-Similar Adsorption profile Scaling theory of an adsorbed polymer layer Colloid stabilization 3 Tails and Loops Adsorption Kinetics
5 Outline 1 Adsorption versus Depletion of polymer solutions Single Chain Adsorption Adsorption and Depletion of Semi-dilute solutions 2 Self-Similar Adsorption profile Scaling theory of an adsorbed polymer layer Colloid stabilization 3 Tails and Loops Adsorption Kinetics
6 Flory Theory of Single Chain Adsorption Loop Tail D Train Flory Theory PGG Confinement Energy F conf N(a/D) 1/ν Attraction Energy F ads = Nɛ(a/D) Equilibrium Thickness D aɛ ν ν 1 Adsorption thickness independent of molecular weight Proximal effects Eisenriegler et al. Diverging concentration profile. Only change in exponent. Connection to special transition
7 Mean Field Theory Propagator Equation PGG 1969 Diffusion Equation G N N = a2 6 2 G N + UG N Boundary condition 1 G N G N z = κ = 1 D Ground state dominance approximation G N (z, z ) = n exp ɛ n N ψ n (z)ψ n (z ) Sum dominated by the first term, exponential concentration profile
8 Outline 1 Adsorption versus Depletion of polymer solutions Single Chain Adsorption Adsorption and Depletion of Semi-dilute solutions 2 Self-Similar Adsorption profile Scaling theory of an adsorbed polymer layer Colloid stabilization 3 Tails and Loops Adsorption Kinetics
9 Semidilute solutions close to a wall ξ Free energy Ground state dominance approximation, c(z) = ψ 2 (z) Excluded volume interaction v, Free energy F/kT = ( a 2 dz 6 (dψ dz )2 + 1 ) 2 vc2 + ɛc Lagrange multiplier ɛ = vcc b insures the imposed bulk concentration c b Bulk correlation length ξ = a/(12vc b ) 1/2 Boundary condition 1 ψ ψ z = κ = 1 D
10 Adsorption and depletion Polymer depletion κ < 0 Leibler, JF, PGG 1978 Polymer adsorption κ > Concentration profile c = c b tanh 2 z+d 2ξ Positive Interfacial tension γ ktc 3/2 b Concentration Profile 2 z+d c = c b tanh 2ξ Adorbed amount Γ = κa 2 /(3v) Adsorbed layer thickness ξ Dilute solutions
11 Outline 1 Adsorption versus Depletion of polymer solutions Single Chain Adsorption Adsorption and Depletion of Semi-dilute solutions 2 Self-Similar Adsorption profile Scaling theory of an adsorbed polymer layer Colloid stabilization 3 Tails and Loops Adsorption Kinetics
12 Self-similar concentration profile PGG 1981 ξ Concentration profile Central Region: local structure of a semidilute solution, ξ z ξ c 3/4 c 1/z 4/3 Proximal region: z < D single chain behavior. Distal region: exponential decay over correlation length (or the radius)
13 Properties of polymer layers adsorbed from dilute solution Self-similar grid with largest size R N 3/5. Adsorbed amount weakly dependent on N: Γ = Γ 0 (1 N 1/5 ). Hydrodynamic thickness R Ellipsometric thickness R dzc(z)zdz N 2/5 Takahashi Neutron scattering Auvray Power law decay of structure factor S(q) q 8/3 Many experiments lead to exponential decay Cosgrove Separation of length scales
14 Outline 1 Adsorption versus Depletion of polymer solutions Single Chain Adsorption Adsorption and Depletion of Semi-dilute solutions 2 Self-Similar Adsorption profile Scaling theory of an adsorbed polymer layer Colloid stabilization 3 Tails and Loops Adsorption Kinetics
15 Interaction between polymer layers Interactions between surfaces R Excluded volume: repulsive Bridging: attractive h R Mean Field theory Equilibrium interaction attractive (h < R) W kt /h 3 Exponentially decaying tail Interaction between irreversibly adsorbed layers W = 0
16 Interaction between polymer layers Scaling theory PGG 1981 Interaction energy W ±kt /h 2 Free energy description Widom Equilibrium interaction : attractive Non equilibrium interaction between saturated layers repulsive Experimental results Surface forces apparatus Klein Non saturated Layers Other techniques Bibette
17 Colloid Stabilization Klein, Pincus Polymer adsorption Good solvent Irreversible adsorption (Glassy Layers) Saturated layers Depends on History
18 Distributions of tails and loops sizes Tails and Loops partition function Semenov, JF Loops Obtained by reconstructing the self similar profile with loops Partition function Z l (n) n (2ν+1) Dominated by short loops (trains) Tails Obtained by cutting a loop into two tails Partition function Z t n (γ ν)/2 1 Dominated by long tails Loops in the inside of the layer, tails on the outside Crossover length z N 1/2
19 Dynamics of adsorbed layers Penetration in a adsorbed layer PGG 1985 End point penetration (no hairpin entrance) Analogy with a quantum tunneling problem Very weak (logarithmic) energy barrier Reptation of an entering chain through the self-similar layer Penetration time T = T 0 N x, x = 0.3 Desorption and exchange Second order chemical Kinetics dγ dt = kγc b no desorption (Saturation condition) Exchange between labelled and non-labelled chains
20 Summary Scaling theory of Polymer adsorption Applications to colloidal stablization Non-Equilibrium adsorption kinetics Guizelin layers Other applications to technological problems Friction Adhesion
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