Intermolecular Forces and Potentials Flashcards
Van der Waals
non-covalent interactions
force
vector
Positive Q
attractive
Negative Q
repulsive
Multipole moment of heterodiatomic
quadrupole, accumulation of e- density between the nuclei
monopole
point charge
dipole
superposition of 2 monopoles with opposite charges
quadrupole
superposition of 2 oppositely oriented dipoles
Components of intermolecular potential
dipole A - dipole B, dipole A - quad B, quad A - dipole B, quad A - quad B
Distance dependence of monopole-monopole
r-1
Distance dependence of monopole-dipole
r-2
Distance dependence of monopole-quadrupole
r-3
Distance dependence of dipole-dipole
r-3
Distance dependence of dipole-quadrupole
r-4
Distance dependence of quadrupole-quadrupole
r-5
Orientation of multipoles
orientations sampled with probability that reflects their energy ie. use boltzmann
Dipole-dipole interactions
also called Keesom, attractive or repulsive depending on orientation, molecules don’t rotate freely at finite temp, attractive orientations more favoured than repulsive interactions
Induction interactions
always attractive, permanent multipole of A induces permanent multipole on B, magnitude depends on magnitude of multipole of A and polarisability of B, not frustrated by thermal motion
Dispersion interactions
also called London Dispersion, always attractive, instantaneous multipole of A correlate with instantaneous multipole of B, not frustrated by thermal motion
Origin of dispersion interactions
electrons in constant motion so can have instantaneous dipole moment, this induces another dipole in adjacent atom giving an attractive potential
Magnitude of polarisability volumes
similar in magnitude to actual molecular volumes, correlates with HOMO-LUMO separation in atoms/molecules, electron distribution distorted easily if LUMO and HOMO are close in energy
Dipoles at low AC frequency
dipoles have time to re-orient themselves with oscillating electric field, can contribute to dielectric constant, use Debye equation to interpret temp dependence of molar polarisation
Dipoles at high AC frequency
dipoles can’t keep up with oscillating freq, can’t contribute to dielectric const, molar polarisation independent of temp and use mossotti to determine polarisability
Stark deceleration
molecule with permanent dipole approaches dipole and slows due to increasing field, reaches position at top of energy hill, fields switched to prevent molecule continuing down hill, voltage of first and second electrode swapped, molecule instantaneously arrives at bottom of hill and continues climbing but slower, repeated until desired velocity reached