Surface energy study

1. Surface energy study γS : surface free energy of solid γL : surface free energy of liquid γSL : interfacial free energy between solid and liquid θ: solid/liquid contact angle Young‘s equation γSL = γS - γL cosθ (1) γSL = γS + γL - 2(γSγL) ½ (2) from (1) (2) γS =γL(1+cosθ)2/4 (3)

2. LW AB γS = γS + γS (4) γS =2 (γS+γS-) ½ (5) γS = γS + 2 (γS+γS-) ½ (6) γS : apolar component, accounting for Liftshitz/van der Waals type interactions γS : polar component, accounting for acid-base or donor- acceptor type interactions γS+ : Lewis-acid component, electron acceptor γS- : Lewis-base component, electron donor AB LW LW AB Fowkes first suggest that surface tension could resolved into component due to dispersion force, the induction and dipole-dipole forces, and hydrogen bonding

3. Hydrogen bonding We may compare the surface tension data of CHCl3 and CCl4 and interfacial tension vs. water and free energy of adhesion to water. -ΔGaij = γi + γj - γij (7) -ΔGaij : free energy of adhesion surface interfacial tension free energy of adhesion Substance tension (mN/m) vs. water (mN/m)to water(mJ/m2) CHCl3 27.13 31.6 -68.3 CCl4 26.95 45.0 -54.7

4. ΔGaSL = (ΔGaSL)LW + (ΔGaSL)AB (8) For liquid on solid, contact angle follow the Young-Dupré equation : γL(1 + cosθ) = -ΔGaSL (9) The acid-base component of the free energy of adhesion is given by (ΔGaSL)AB = -2(γS+γL-) ½ -2(γS–γL+) ½ (10) (ΔGaSL)LW = -2(γS γL ) ½ (11) γL(1 + cosθ) = 2(γS γL ) ½ + 2(γS+γL-) ½ + 2(γS -γL+) ½ (12) LW LW LW LW

5. apolar monopolar bipolar γS =γL(1+cosθ)2/4 γS =γL (1+cosθ)2/4 = γL ( apolar liquid )(1+cosθ)2/4 (13) LW LW LW LW γL(1 + cosθ) = 2(γS γL ) ½ + 2(γS+γL-) ½ + 2(γS–γL+) ½ LW γS = γS + 2 (γS+γS-) ½

6. γij : interfacial free energy between i and j γij = γij + γij = [ (γi ) ½ - (γj ) ½ ]2 + [ (γi ) ½ - (γj ) ½ ]2 (14) = [ (γi ) ½ - (γj ) ½ ] 2 + 2[ (γi+) ½ - (γj-) ½ ] [ (γi-) ½ - (γj+) ½ ] (15) LW AB LW LW LW LW AB AB An important, practical restriction on the use of Eqs. (12) and (13) Is the fact that the liquid must have a surface tension larger than the critical surface tension of the solid. The γS values for a large number of important polymer are in the neighborhood of 40 mJ/m2. LW

7. Low surface energy finishes are important in many practical application. γ,surface free energy of polymer poly(tetrafluoroethylene), PTFE, Teflon γ= 21mJ/m2 polystyrene, PS, γ= 42mJ/m2 poly(methyl methacrylate), PMMA, γ= 39 to 43 mJ/m2 It is now established that the surface energy of constituent groups decreases in the order CH2 (36 dyn cm-1) > CH3 (30 dyn cm-1) > CF2 (23 dyn cm-1) > CF3 (15 dyn cm-1).

8. Amorphous materials exhibit lower surface energy values than crystalline counterparts. As a general rule, amorphous, comb like polymers possessing a flexible linear backbone onto which side-chains with low intermolecular interactions are attached, exhibit low γ values.

9. poly(tetrafluoroethylene) PTFE Fluoropolymers and Silicones The low intermolecular forces present in fluorinated polymers have been recognized to account for the relatively low surface free energy. poly(dimethylsiloxane)PDMS polyethylene PE

10. General Rules for Low Surface Free Energy Polymers As a general rule, amorphous, comb like polymers possessing a flexible linear backbone onto which side-chains with low intermolecular interactions are attached, exhibit low γ values. poly(perfluoroalkylacrylate) PFA Adv. Mater. 2003, 15, 647

11. The Influence of Intra- and Intermolecular Interactions on Surface Free Energy Poly(N-isopropylacrylamide) (PNIPAAm) Hydrophilic Hydrophobic < LCST > LCST intermolecular hydrogen bonding between the PNIPAAm main chains and water molecules intramolecular hydrogen bonding between the C=O and N－H higher surface free energy lower water contact angles lowsurface free energy high contact angles for water Angew. Chem. Int. Ed.2004, 43, 357

12. The Influence of Intermolecular Hydrogen Bonding on Surface Free Energy ANA 6F acid AAA HQAT J. Phys. Chem. B, 2001,105, 4145