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Potential energy surface intermediate complex

Potential energy hypersurfaces form the basis for the complete description of a reacting chemical system, if they are throughly researched (see also part 2.2). Due to the fact that when the potential energy surface is known and therefore the geometrical and electronical structure of the educts, activated complexes, reactive intermediates, if available, as well as the products, are also known, the characterizations described in parts 3.1 and 3.2 can be carried out in theory. [Pg.192]

Figure 4. Schematic potential energy surface for the reaction of FeO" " with methane. The sohd line indicates the sextet surface the quartet surface is shown with a dotted line, in each case leading to the production of Fe + CH3OH. The dashed line leads to formation of FeOET + CH3. The pathway leading to the minor FeCH2" + H2O channel is not shown. Schematic structures are shown for the three minima the [OFe CHJ entrance channel complex, [HO—Fe—CH3] insertion intermediate, and Fe" (CH30H) exit channel complex. See text for details on the calculations on which the potential energy surface is based. Figure 4. Schematic potential energy surface for the reaction of FeO" " with methane. The sohd line indicates the sextet surface the quartet surface is shown with a dotted line, in each case leading to the production of Fe + CH3OH. The dashed line leads to formation of FeOET + CH3. The pathway leading to the minor FeCH2" + H2O channel is not shown. Schematic structures are shown for the three minima the [OFe CHJ entrance channel complex, [HO—Fe—CH3] insertion intermediate, and Fe" (CH30H) exit channel complex. See text for details on the calculations on which the potential energy surface is based.
The energy term in the Boltzmann factor may be considered as the size of the barrier along a potential energy surface for a system of reactants going to products, as shown schematically in Fig. 2.1. The state of the reacting species at this activated energy can be regarded as some intermediate complex that... [Pg.45]

The empirical valence bond (EVB) approach introduced by Warshel and co-workers is an effective way to incorporate environmental effects on breaking and making of chemical bonds in solution. It is based on parame-terizations of empirical interactions between reactant states, product states, and, where appropriate, a number of intermediate states. The interaction parameters, corresponding to off-diagonal matrix elements of the classical Hamiltonian, are calibrated by ab initio potential energy surfaces in solu-fion and relevant experimental data. This procedure significantly reduces the computational expenses of molecular level calculations in comparison to direct ab initio calculations. The EVB approach thus provides a powerful avenue for studying chemical reactions and proton transfer events in complex media, with a multitude of applications in catalysis, biochemistry, and PEMs. [Pg.383]

These, and similar data for other systems, demonstrate the tremendous potential that the MICR technique has for the qualitative elucidation of potential energy surfaces of relatively complex organic reactions. Once implementation of the quadrupolar excitation technique has been effected to relax ions to the cell center, the technique will become even more powerful, in that the determination of highly accurate unimolecular decomposition lifetimes of chemically activated intermediates will also become possible. No other technique offers such a powerful array of capabilities for the study of unimolecular dissociation mechanisms and rates. [Pg.70]

The dicarboxonium ions would be useful intermediates for the diacylation of aromatics. The 1,2-dicarboxonium ion (oxalyl dication, 17) has yet to be experimentally obtained. The ionization of the oxalyl fluoride in SbFs presumably forms the donor-acceptor complex, 18, which spontaneously decomposes to CO and COF2. The expected oxalyl dication (OCCO), 17, was not observed although theoretical calculations at MP2/6-31G level indicate 17 to be a minimum on the potential energy surface. [Pg.225]

The reaction with Fe (Fig. 3) is somewhat more complicated as it also involves participation of an intermediate-spin (IS, S = 1) state between the LS (S = 0) and the HS (S = 2) states in the course of the reaction. From the initial complex 4, the reaction proceeds virtually without barriers until the final complex 6 is formed. In the cases of both ]TS3 and 1TS4, the activation energies with respect to x4 and ]5 were found to be 2.9 and 0.5 kcal mol-1, respectively, without zero-point vibrational energy (ZPVE) correction. With ZPVE, both 1TS3 and ]TS4 become lower on the potential energy surface than the corresponding complexes 4 and 5 by 0.3 and 1.3 kcal mol-1, respectively. In some cases, we were unable to locate transition states and local minima at all three levels of theory. [Pg.277]

The energetics of the low-, intermediate-, and high-spin states of the key species on the potential energy surface for oxidation of alkenes by Mn(salen) (and the related chromium species [50]) complexes have received considerable attention, following the suggestion [51] by Linde et al that spin-state changes play an important role in the diastereoselectivity of this... [Pg.173]


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Complex energy

Complex intermediate

Complex potential

Intermediate surface complexes

Intermediates, potential

Intermediates, surface

Surface complex

Surface complexation

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