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Potential interaction energy

We have two interaction potential energies between uncharged molecules that vary with distance to the minus sixth power as found in the Lennard-Jones potential. Thus far, none of these interactions accounts for the general attraction between atoms and molecules that are neither charged nor possess a dipole moment. After all, CO and Nj are similarly sized, and have roughly comparable heats of vaporization and hence molecular attraction, although only the former has a dipole moment. [Pg.228]

Fig. VI-5. The effect of electrolyte concentration on the interaction potential energy between two spheres where K is k in cm". (From Ref. 44.)... Fig. VI-5. The effect of electrolyte concentration on the interaction potential energy between two spheres where K is k in cm". (From Ref. 44.)...
From the data in Problem 13, calculate the interaction potential energy between... [Pg.250]

Here the transition state is approximated by the lowest crossing pomt on the seam intersecting the diabatic (non-interacting) potential energy surfaces of the reactant and product. The method was originally developed... [Pg.2350]

The essence of this analysis involves being able to write each wavefunction as a combination of determinants each of which involves occupancy of particular spin-orbitals. Because different spin-orbitals interact differently with, for example, a colliding molecule, the various determinants will interact differently. These differences thus give rise to different interaction potential energy surfaces. [Pg.274]

Equations (2) and (3) relate intermolecular interactions to measurable solution thermodynamic properties. Several features of these two relations are worth noting. The first is the test-particle method, an implementation of the potential distribution theorem now widely used in molecular simulations (Frenkel and Smit, 1996). In the test-particle method, the excess chemical potential of a solute is evaluated by generating an ensemble of microscopic configurations for the solvent molecules alone. The solute is then superposed onto each configuration and the solute-solvent interaction potential energy calculated to give the probability distribution, Po(AU/kT), illustrated in Figure 3. The excess... [Pg.310]

The mean value of the interaction potential energy should provide some guidance on the value of the first of the terms on the right it helps that those interaction energies will have a lower bound. The second term then primarily addresses entropic contributions to jLt x that integral accumulates the weight of the favorable configurations, well-bound to the solute, that the solvent host offers the solute without coercion. [Pg.331]

As it will be explained in section 6, the usual way to evaluate the potential energy of a system simulated by Monte Carlo techniques, makes use of the pair potential approximation (although, as it will also be reviewed, several works have already appeared where nonadditivity corrections to the interaction potential have been included). In the pair potential approximation only two body interactions are taken into account. We will briefly explain here how to apply this approximation for the calculation of the potential energy, to the periodic system just described. The interaction potential energy under the pair potential approximation can be written as ... [Pg.132]

A rigourous way to evaluate the total interaction potential energy, U(q(N- ), would be the formulation and resolution of the Schrodinger equation for the whole system at each configuration. However, given the size of the samples where the statistical simulations are performed, this method is impracticable. [Pg.152]

In most MC (11,12) and MD (12,13) studies, a small number (N) of particles are placed in a cell of fixed volume (V) and the total interaction potential energy (U ) from all pairwise interaction potentials (U j) between particles i and j is calculated ... [Pg.21]

To determine the movement of molecules, the following algorithm (15) is often used. The force acting on the ith atom in a molecule (Fj) is determined from the spatial derivative of the total interaction potential energy of that particle ... [Pg.23]

Green S. H. and Gordon R. G. (1974). POTLSVRF A program to compute the interaction potential energy surface between a closed-shell molecule and an atom. Quantum Chemistry Program Exchange No. 251, Indiana University. [Pg.832]

The predicted adiabatic exponent increases with increase in volume, until the volume corresponding to the minimum in the interaction potential energy is reached. These predictions were borne out by the experimental data reported by J.W. Kury et al (Ref 15, pp 3-12)... [Pg.289]

The potential at the inner limit of the diffuse part of the double layer enters Equation (1) through T0, defined by Equation (11.65) with p0 in place of ip. For large values of ip0, T0 1, so sensitivity to the value of p0 decreases as ip0 increases. Figure 13.7 shows the effect of variations in the value of ip0 on the total interaction potential energy with k (109 m -l or 0.093 M for a 1 1 electrolyte) and A (2 10 19 J) constant. The height of the potential energy barrier is seen to increase with increasing values of ip0, as would be expected in view of the... [Pg.585]

In actuality, molecules in a gas interact via long-ranged attractions and short-range repulsive forces. An interaction potential energy function is used to describe these forces as a function of intermolecular distance and orientation. This section introduces two commonly used interaction potential energy functions. [Pg.492]

The results of the last section showed that, for any macroscopic container at normal pressures, it is not reasonable to conclude that the molecules proceed from wall to wall without interruption. However, if the interaction potential energy between molecules at their mean separation is small compared to the kinetic energy, the speed distribution and the average concentration of gas molecules is about the same everywhere in the container. In this limit, the only real effect of collisions is the excluded volume occupied by the molecule, which effectively shrinks the size of the container. At 1 atm, only about 1/1000 of the space is occupied (remember the density ratio between gas and liquid), so each additional molecule sees only 99.9% of the container as free space. On the other hand, if the attractive part of the interaction potential cannot be totally neglected, the molecules which are very near the wall will be pulled slightly away from the wall by the other molecules. This tends to decrease the pressure. [Pg.168]

The motion in the reaction coordinate Q is, like in gas-phase transition-state theory, described as a free translational motion in a very narrow range of the reaction coordinate at the transition state, that is, for Q = 0 hence the subscript trans on the Hamiltonian. The potential may be considered to be constant and with zero slope in the direction of the reaction coordinate (that is, zero force in that direction) at the transition state. The central assumption in the theory is now that the flow about the transition state is given solely by the free motion at the transition state with no recrossings. So when we associate a free translational motion with that coordinate, it does not mean that the interaction potential energy is independent of the reaction coordinate, but rather that it has been set to its value at the transition state, Q j = 0, because we only consider the motion at that point. The Hamiltonian HXlans accordingly only depends on Px, as for a free translational motion, so... [Pg.251]

By contrast, if the dipole moments are antiparallel to one another (see Fig. 4C), the interaction potential energy is reduced to... [Pg.138]

Adsorption occurs when the interaction potential energy is equal to the work done to bring a gas molecule to the adsorbed state. As a first approximation, the adsorbed state is assumed to be at the saturated vapor pressure. [Pg.81]

Fig. 4. All-electron, effective potential, and average relativistic effective core potential configuration-interaction potential-energy curves of Xe2 and Xe2+. Dashed curves are from allelectron calculations and AREP curves are less repulsive than EP. Fig. 4. All-electron, effective potential, and average relativistic effective core potential configuration-interaction potential-energy curves of Xe2 and Xe2+. Dashed curves are from allelectron calculations and AREP curves are less repulsive than EP.

See other pages where Potential interaction energy is mentioned: [Pg.61]    [Pg.181]    [Pg.227]    [Pg.227]    [Pg.231]    [Pg.235]    [Pg.2241]    [Pg.663]    [Pg.120]    [Pg.7]    [Pg.59]    [Pg.343]    [Pg.467]    [Pg.794]    [Pg.147]    [Pg.78]    [Pg.34]    [Pg.237]    [Pg.173]    [Pg.9]    [Pg.289]    [Pg.871]    [Pg.374]    [Pg.251]    [Pg.383]    [Pg.20]    [Pg.41]    [Pg.133]   
See also in sourсe #XX -- [ Pg.204 , Pg.210 , Pg.252 , Pg.307 ]




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