1. Forces, Energies, and Timescale in Condensed Matter 2004/10/04 C. T. Shih Special Topics on Soft Condensed Matters

2. Intermolecular Forces (Long range) Attraction → to condense (Hard core) Repulsion → to avoid collapse Isotropic as in the figure? → usually no for soft matters

4. Type of Forces Two types of bonds: permanent (chemical) bonds and temporary (physical) bonds Van der Waals forces: U ~  2 /r 6,  : polarizability, r: distance. Energy scale ~ 10 -20 J ~ 724 K Ionic interactions: Coulomb potential. Energy scale ~ 10 -18 J Covalent bonds: Energy scale ~ 30~100×10 -20 J Metallic bonds: Delocalization of electrons. Energy scale ~ covalent bonds Hydrogen bonds: Energy scale~ 2~6×10 -20 J Hydrophobic interactions: Energy scale~ 10 -20 J

5. Intermolecular Forces and Phase Transition

8. Elasticity: Hookean Solid An ideal elastic solid An applied shear stress （剪力） produces a shear strain in response The shear strain is proportional to shear stress The constant of proportionality is the shear modulus

10. Viscosity: Newtonian Liquid An ideal viscous liquid An applied shear stress produces a flow with a constant shear strain rate in response The strain rate is proportional to the shear stress, and the constant of proportionality is the viscosity

11. Newtonian Liquid (conti.) Imagine some liquid sandwiched between parallel plates of area A separated by a distance y The plates are moved with a relative velocity v The force resisting the relative motion of the plates F=Aηv/y η is the viscosity v/y is just the time derivative of shear strain, or e’, so it can be written as σ=ηe’

12. Real Material: Viscoelastic Hookean solid and Newtonian liquid are two limiting cases of elasticity and viscosity The behavior of real materials is in between – viscoelastic There is a particular timescale to determine which kind of response: elastic or viscous

13. Relaxation Time

14. shear-thinning fluid: faster-moving, less viscous shear-thickening fluid: faster-moving, more viscous