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Molecules in the gas phase

Shelton D P and Rice J E 1994 Measurements and calculations of the hyperpolarizabilities of atoms and small molecules in the gas phase Chem. Rev. 94 3... [Pg.211]

As the temperature of the liquid phase is increased, the system ultimately reaches a phase boundary, the bubble point at which the gas phase (vapour) begins to appear, with the composition shown at the left end of the horizontal two-phase tie-line . As the temperature rises more gas appears and the relative amounts of the two phases are detemiined by applying a lever-ami principle to the tie-line the ratio of the fractionof molecules in the gas phase to that hn the liquid phase is given by the inverse of the ratio of the distances from the phase boundary to the position of the overall mole fraction Xq of the system. [Pg.613]

It is often the case that the solvent acts as a bulk medium, which affects the solute mainly by its dielectric properties. Therefore, as in the case of electrostatic shielding presented above, explicitly defined solvent molecules do not have to be present. In fact, the bulk can be considered as perturbing the molecule in the gas phase , leading to so-called continuum solvent models [14, 15]. To represent the electrostatic contribution to the free energy of solvation, the generalized Bom (GB) method is widely used. Wilhin the GB equation, AG equals the difference between and the vacuum Coulomb energy (Eq. (38)) ... [Pg.364]

Example For a mediiim-sl/eti molecule in the gas phase, with vibration s larger th an 50 cm, a trajectory of on ly 10 ps should be adequate to explore motion s due to vibration s. [Pg.88]

TIk experimentally determined dipole moment of a water molecule in the gas phase is 1.85 D. The dipole moment of an individual water molecule calculated with any of thv se simple models is significantly higher for example, the SPC dipole moment is 2.27 D and that for TIP4P is 2.18 D. These values are much closer to the effective dipole moment of liquid water, which is approximately 2.6 D. These models are thus all effective pairwise models. The simple water models are usually parametrised by calculating various pmperties using molecular dynamics or Monte Carlo simulations and then modifying the... [Pg.235]

The number of collisions z that a molecule in the gas phase makes per unit time, when only one species is present, is given by... [Pg.38]

The kinetics of this reaction, which can also be regarded as an erosion reaction, shows die effects of adsorption of the reaction product in retarding the reaction rate. The path of this reaction involves the adsorption of an oxygen atom donated by a carbon dioxide molecule on die surface of the coke to leave a carbon monoxide molecule in the gas phase. [Pg.272]

In the present case, each endpoint involves—in addition to the fully interacting solute—an intact side chain fragment without any interactions with its environment. This fragment is equivalent to a molecule in the gas phase (acetamide or acetate) and contributes an additional term to the overall free energy that is easily calculated from ideal gas statistical mechanics [18]. This contribution is similar but not identical at the two endpoints. However, the corresponding contributions are the same for the transfonnation in solution and in complex with the protein therefore, they cancel exactly when the upper and lower legs of the thermodynamic cycle are subtracted (Fig. 3a). [Pg.179]

A type of molecular resonance scattering can also occur from the formation of short-lived negative ions due to electron capture by molecules on surfrices. While this is frequently observed for molecules in the gas phase, it is not so important for chemisorbed molecules on metal surfaces because of extremely rapid quenching (electron transfer to the substrate) of the negative ion. Observations have been made for this scattering mechanism in several chemisorbed systems and in phys-isorbed layers, with the effects usually observed as smaU deviations of the cross section for inelastic scattering from that predicted from dipole scattering theory. [Pg.445]

Energy Distribution Profile of Solute Molecules in the Gas Phase... [Pg.11]

The molecular mechanics calculations discussed so far have been concerned with predictions of the possible equilibrium geometries of molecules in vacuo and at OK. Because of the classical treatment, there is no zero-point energy (which is a pure quantum-mechanical effect), and so the molecules are completely at rest at 0 K. There are therefore two problems that I have carefully avoided. First of all, I have not treated dynamical processes. Neither have I mentioned the effect of temperature, and for that matter, how do molecules know the temperature Secondly, very few scientists are interested in isolated molecules in the gas phase. Chemical reactions usually take place in solution and so we should ask how to tackle the solvent. We will pick up these problems in future chapters. [Pg.57]

Chemical reactions generally take place in condensed media. I have had very little to say so far about the presence or otherwise of a solvent, and many of our calculations refer to isolated molecules in the gas phase at 0 K. [Pg.252]

There is an evolution with time the older calculations correspond to isolated molecules in the gas phase without any corrections, the more recent ones include solvent effects, with different approximations, and also some corrections, like ZPE (zero-point energy correction). The contributions of some authors to the understanding of tautomerism have been significant. Some of their contributions are collected in Table II. [Pg.11]

Henry s law arises because increasing the pressure raises the concentration of molecules in the gas phase. To balance this change and maintain equilibrium, more gas molecules enter the solution, increasing their concentration in the liquid phase. [Pg.266]

Raoulfs law. Adding a solute lowers the concentration of solvent molecules in the liquid phase. To maintain equilibrium, the concentration of solvent molecules in the gas phase must decrease, thereby lowering the solvent vapor pressure. [Pg.268]

Kinetic-molecular theory provides an explanation on a molecular level for this equilibrium. Evaporation from the liquid occurs as fast moving molecules on the surface escape from the liquid. In turn, molecules in the gas phase strike the liquid and condense, As the concentration (pressure) of gas molecules builds up in the gas phase, the rate of condensation increases. Eventually, a pressure is reached where the rate of condensation and rate of evaporation just balance, and equilibrium is achieved. The equilibrium pressure is denoted by p and is known as the vapor pressure. The magnitude ofp depends upon the substance, composition of the liquid, and any two of our thermodynamic variables such as temperature and total pressure. The criteria for equilibrium that we will now derive provide the thermodynamic relationships that will help... [Pg.225]

Elementary reactions are generally unimolecular or bimolecular, depending on whether they entail the reaction of one species or two. Occasionally a termolecular step occurs, particularly between atoms or small molecules in the gas phase. Solution reactions that might appear to be termolecular usually prove really to be a succession of two simpler ones. [Pg.4]

Values of and Qb can be calculated for molecules in the gas phase, given structural and spectroscopic data. The transition state differs from ordinary molecules, however, in one regard. Its motion along the reaction coordinate transforms it into product. This event is irreversible, and as such occurs without restoring force. Therefore, one of the components of Q can be thought of as a vibrational partition function with an extremely low-frequency vibration. The expression for a vibrational partition function in the limit of very low frequency is... [Pg.170]


See other pages where Molecules in the gas phase is mentioned: [Pg.883]    [Pg.1307]    [Pg.326]    [Pg.353]    [Pg.361]    [Pg.290]    [Pg.164]    [Pg.366]    [Pg.16]    [Pg.14]    [Pg.300]    [Pg.20]    [Pg.26]    [Pg.130]    [Pg.31]    [Pg.50]    [Pg.74]    [Pg.387]    [Pg.274]    [Pg.276]    [Pg.278]    [Pg.280]    [Pg.284]    [Pg.286]    [Pg.288]    [Pg.290]    [Pg.292]    [Pg.294]    [Pg.296]    [Pg.298]    [Pg.40]   


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Formation of Diatomic Molecules and Radicals in the Gas Phase

Gas phase in the

In gas phase

Large molecules in the gas phase

Molecule Reactions in the Gas Phase

Molecules gases)

Molecules in gases

Phase molecules

The gas phase

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