Lecture 5: Interactions between macroscopic bodies I What did we cover in the last lecture? Dispersion interactions Dispersion interaction energy Repulsive interactions and the Lennard Jones potential 12 6 A C U ( x) 12 6 4 x x x x repulsive attractive In this lecture… 1. Interactions between extended and macroscopic bodies 2. Why do we need to consider macroscopic bodies? (atomic manipulation, particleparticle interactions and geckos) 3. Interactions between molecules and surfaces 4. Interactions between particles and surfaces Recap: Dispersion interactions between isolated atoms In the last lecture we saw that dispersion interactions is short ~0.3nm Total energy of interaction U (repulsive + dispersion) 12 6 A C U ( x) 12 6 4 x x x x repulsive attractive However, they are strong enough to hold atoms/molecules together and overcome the influence of thermal (brownian) motion! Interactions between extended bodies What happens when many atoms/molecules come together? If central atom/molecule has N nearest neighbours, then total interaction energy Utot~ N U So energy of interaction increases as more atoms/molecules are brought together Explains why dispersion forces are capable of holding together simple organic liquids and solids (which have no other interactions) Dispersion Interactions between macroscopic bodies…geckos feet Geckos feet are covered in small structures called setae Dispersion interactions allow these setae to let the gecko walk up smooth surfaces Dispersion interactions in nanoscience Dispersion interactions are also important in nanoscience As we will see in later lectures, they are often a significant component of the forces which are exerted between nanoparticles and surfaces and in inter-nanoparticle interactions Solid Surface Dispersion forces in AFM Dispersion forces also influence the interaction between an AFM tip and a surface Position sensitive detector More on this in a future lecture! Additivity of interactions The additive nature of short range dispersion interactions means that interactions between individual atoms/molecules and macroscopic bodies (solids) can be significant. Consider… Atom/molecule Semi infinite Solid What is the force between the atom/molecule and a semi-infinite solid? Detailed picture Firstly we consider dispersion interactions between the atom/molecule and a plane within the solid We start with the form of our potential between two atoms/molecules and determine the interaction energy between a thin ring/annulus in the plane and our atom/molecule (See OHP) C U ( x) 6 x Interactions between macroscopic bodies I Problem 1: Derive an expression for the dispersion forces which act between a perfectly flat slab of area S and a semi-infinite solid if the number density of atoms in the solid and slab are n1 and n2 respectively. Summary of key results Dispersion interactions between macroscopic bodies occur over longer ranges than between atoms and simple molecules Dispersion interactions can be large enough to overcome the effects of gravity Dispersion force between a molecule and a semi infinite solid scales as Dispersion force between a slab and a solid (or two parallel surfaces) U ( D) nC 6D 3 n1n2CS U ( D) 12 D 2