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Path calculation

In Gaussian, a reaction path calculation is requested with the IRC keyword in the route section. Before you can run one, however, certain requirements must be met. An IRC calculation begins at a transition structure and steps along the reaction path a fixed number of times (the default is 6) in each direction, toward the two minima that it connects. However, in most cases, it will not step all the way to the minimum on either side of the path. [Pg.173]

All the reaction paths calculated with the CD method were determined by stepping forward (from reactant to intermediate state) and backward (from intermediate... [Pg.60]

For both reaction path calculations, it only took two modified NEB cycles to optimize the new images to the MEP. The reason for this very fast convergence is that the initial approximation for the extra images on the path is not too far from the MEP. [Pg.69]

The calculated potential and free energies for the first step of the four paths is presented in Table 3-2. As can be seen, the paths calculated with the combined procedure present activation energies of 17.77 and 16.85 kcal/mol for paths A and B respectively. On the other hand, the calculated potential activation energies are 20.37 kcal/mol for path C and 22.02 for path D. This is in contrast to the calculated... [Pg.72]

Reactions for common minerals fall in both categories, but many important cases tend, except under acidic conditions, to be surface controlled (e.g., Aagaard and Helgeson, 1982 Stumm and Wollast, 1990). For this reason and because of their relative simplicity, we will consider in this chapter rate laws for surface-controlled reactions. The problem of integrating rate laws for transport-controlled reactions into reaction path calculations, nonetheless, is complex and interesting (Steefel and Lasaga, 1994), and warrants further attention. [Pg.233]

Integrating isotope fractionation into the reaction path calculation is a matter of applying the mass balance equations while tracing over the course of the reaction path the system s total isotopic composition. Much of the effort in programming an isotope model consists of devising a careful accounting of the mass of each isotope. [Pg.275]

Fig. 31.2. Masses of species produced by reacting pyrite with a hypothetical groundwater that is held in equilibrium with atmospheric oxygen, according to the reaction path calculation shown in Figure 31.1. Fig. 31.2. Masses of species produced by reacting pyrite with a hypothetical groundwater that is held in equilibrium with atmospheric oxygen, according to the reaction path calculation shown in Figure 31.1.
Perkins, E. H. and T. H. Brown, 1982, Program path, calculation of isothermal and isobaric mass transfer. University of British Columbia, unpublished manuscript. [Pg.527]

Wireless sensor networks are prone to failures. Furthermore, the sensor nodes die due to their limited energy resources. Therefore, the failures of sensor nodes must be modeled and incorporated into the breach path calculations in the future. Simulating the reliability of the network throughout the entire life of the wireless sensor network is also required. Lastly, especially for perimeter surveillance applications, obstacles in the environment play a critical role in terms of sensing and must be incorporated into the field model. [Pg.115]

The process of mutation by tautomerization is similar to the excited-state process described here. If a misprint induced by a tautomer takes place during replication, then an error is recorded. Because reaction path calculations of DNA base pairs show similar potential-energy characteristics to those discussed here, we anticipate being able to explore the relevance of tautomerization dynamics to mutagenesis. In this area, we are currently examining these and other systems, also in solutions. [Pg.40]

These classical path calculations are relatively easy to carry out, and analytic results are available in the straight-line path, perturbation limit (40). Thus when the approximations are... [Pg.62]

For a heavier system, such as N2O + Ar, a calculation of rotational transitions and microwave or infrared line widths would follow the same course through the flow chart, as that followed above in detail for HC1 + Ar. However, at the last stage (low j, small b collisions), the number of coupled states would probably be too large for the non-perturbative, fixed classical path calculation to be practical. Then one should calculate "classical S matrices" including interference between trajectories, to cover these remaining collisions. [Pg.66]

The potential mean force (PMF) calculations by using the QM/MM-MD method has been used to obtain free energy change along the reaction coordinate in solution.138 141 TS optimization and minimum energy path calculations on the PES were carried out for a methyl-transfer reaction in water, and PMF calculations along the path were used to obtain the free energy of activation of... [Pg.214]

Figure 6. From top to bottom action surface Lagrangian manifold (LM) and extreme paths calculated [80] for the system (17) using equations (21). The parameters for the system were A = 0.264 and Figure 6. From top to bottom action surface Lagrangian manifold (LM) and extreme paths calculated [80] for the system (17) using equations (21). The parameters for the system were A = 0.264 and <n —1.2. To clarify interrelations between singularities in the pattern of optimal paths, action surface, and LM surface, they are shown in a single figure, as follows, the action surface has been shifted up by one unit and the LM has been scaled by a factor j and shifted up by 0.4.
Figure 7.43. Predicted reaction path for the meteoric diagenetic system of the Floridan aquifer. These reaction path calculations agree reasonably well with observations, as shown by variousl symbols. Reaction path calculations of this nature can be applied to other modern meteoric diagenetic systems, and perhaps, with modifications to ancient systems now removed from original meteoric water. (After Plummer et al., 1983.)... Figure 7.43. Predicted reaction path for the meteoric diagenetic system of the Floridan aquifer. These reaction path calculations agree reasonably well with observations, as shown by variousl symbols. Reaction path calculations of this nature can be applied to other modern meteoric diagenetic systems, and perhaps, with modifications to ancient systems now removed from original meteoric water. (After Plummer et al., 1983.)...
For a qualitative characterization of the PE surface relevant for the hydrogen transfer reaction, a simplified version of the MEP approach can be adopted. In this so-called coordinate-driven MEP approach one defines one of the 3N— 6 intramolecular degrees of freedom as the reaction coordinate, while the remaining (3N — 7) coordinates are optimized at each step of the reaction path calculation. There are no strict rules for choosing the reaction coordinate. In principle, it can be any of the 3N — 6 degrees of freedom. In practice, it should be the coordinate which changes the most when the reaction proceeds. [Pg.415]

A superior method for the calculation of excited-state PE surfaces is CC2, which is a simplified and computationally efficient variant of coupled-cluster theory with single and double excitations [22], CC2 can be considered as the equivalent of MP2 for excited electronic states. Efficient implementations of CC2 with density fitting [23] and analytic gradients [24] allow reaction path calculations for rather large systems. Being a singlereference method, CC2 fails in the vicinity of conical intersections of excited states with the electronic ground state. [Pg.416]

Nondynamical electron correlation effects are generally important for reaction path calculations, when chemical bonds are broken and new bonds are formed. The multiconfiguration self-consistent field (MCSCF) method provides the appropriate description of these effects [25], In the last decade, the complete active space self-consistent field (CASSCF) method [26] has become the most widely employed MCSCF method. In the CASSCF method, a full configuration interaction (Cl) calculation is performed within a limited orbital space, the so-called active space. Thus all near degeneracy (nondynamical electron correlation) effects and orbital relaxation effects within the active space are treated at the variational level. A full-valence active space CASSCF calculation is expected to yield a qualitatively reliable description of excited-state PE surfaces. For larger systems, however, a full-valence active space CASSCF calculation quickly becomes intractable. [Pg.417]

Example 4. Evaporation and homogeneous redox reactions Example 5.—Irreversible reactions Example 6.--Reaction-path calculations Example 7.--Gas-phase calculations Example 8. Surface complexation... [Pg.111]

The values for mean free path calculated by using Eq. 3.12 represent approximations because measurements of typical molecular diameters are not very accurate. [Pg.229]

Our heatup path calculations assume that there is no transfer of heat between gas and reactor walls or between gas and catalyst. The result is, therefore, an adiabatic heatup path. [Pg.131]

Table 21.1. Bottom half of Table O.l s 3rd catalyst bed heatup path-equilibrium curve intercept worksheet. Input and output gas enthalpies are shown in rows 43 and 44. Note that they are the same. This is because our heatup path calculations assume no convective, conductive or radiative heat loss during catalytic SO2+V2O2 —> SO3 oxidation, Section 11.9. 1st and 2nd catalyst bed enthalpies are calculated similarly - using Tables J.2 and M.2. [Pg.238]


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See also in sourсe #XX -- [ Pg.143 ]




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Enthalpy equations for heatup path calculations

Goal Seek calculations heatup path-equilibrium curve

Heatup Path-Equilibrium Curve Intercept Calculation

Heatup paths balances for calculating

Heatup paths calculations

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Mean free path calculation

Minimum energy paths , potential calculation techniques

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Reaction paths calculation

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