abc # 0, eq 6 represents the linearly forced harmonic oscillator. Pechukas and Child3 showed analytically that the (pf,c@, curve for this system was a circle displaced from the phase space origin. Now, trajectory calculations with c = 0 and abd # 0 yield an elliptical @f,gf),i curve with center at the origin and rotated axes for the quadratically forced harmonic oscillator.% Such a phase space picture is isomorphous to that obtained for the overlap integral between harmonic oscillators with identical equilibrium positions but different force constants, kl = 1 and k2 # 1. The functional form for these overlap integrals is well-known, and the phase space pictures suggest that it may be related to the less tractable expressions for the transition probabilities obtained by Lewis and Riesenfeld% for the harmonic oscillator with time-dependent force constant. Such an oscillator is a possible model for experimentally observed30 non-Landau-Teller behavior in Ar + CsI scattering.Whether used to explain results from sophisticated CID calculations or to suggest links between simple theoretical models, classical S-matrix phase space pictures appear to be an easily employed theoretical tool worthy of continued application and development.
P.M.H. is indebted to the DowThe results of investigations into the association reactions occurring in polar gases by analysis of the pressure and temperature dependence of thermal conductivity are reviewed. The gases studied include water, methanol, ethanol, 2-propanol, 2-methyl-2-propano1, 2,2,2-trifluoroethanol, acetone, acetonitrile, pyridine, acetic acid, trifluoroacetic acid, as well as the binary mixtures methanol-water, trifluoroethanol-water, and acetic acid-water. The prewure and temperature ranges of these studies are 100-2000 torr and 33&440 K, respectively. Expressions for the thermal conductivity of reacting gases derived by Butler and Brokaw, based on the work of Hirschfelder, give calculated thermal conductivities which fit the observed data very well for all the types of observed pressure dependence. The fits yield information on the associated species present (e.g., dimer, trimer, tetramer, etc.), on the concentrations of the species, and on their enthalpies and entropies of association. The thermodynamic results, in conjunction with ab initio molecular orbital calculations, provide information on the strength and structure of hydrogen bonding occurring in the cluster species.