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Zero-point correction

Many semiempirical methods compute energies as heats of formation. The researcher should not add zero-point corrections to these energies because the thermodynamic corrections are implicit in the parameterization. [Pg.32]

Temperature 298.150 Kelvin. Pressure 1.0000 Atm. Zero-point correction= 0.029201... [Pg.69]

Reaction path computations allow you to verify that a given transition structure actually connects the starting and ending structures that you think it does. Once this fact is confirmed, you can then go on to compute an activation energy for the reaction by comparing the (zero-point corrected) energies of the reactants and the transition state. [Pg.173]

Zero-point-corrected energies for formaldehyde, hydrogen molecule, and carbon monoxide. [Pg.175]

The geometry of the transition structure and its zero-point corrected energy. [Pg.175]

The zero-point corrected energy for the trans hydroxycarbene structure is -113.75709 hartrees at the RHF/6-31G(d) level of theory. [Pg.179]

First, we perform an optimization of the transition structure for the reaction, yielding the planar structure at the left. A frequency calculation on the optimized structure confirms that it is a first-order saddle point and hence a transition structure, having a zero-point corrected energy of -113.67941 hartrees. The frequency calculation also prepares for the IRC computation to follow. [Pg.179]

Here are the zero-point corrected energies for the various stationary points ... [Pg.210]

The intermediacy of benzenesilanitrile, the isomeric species with a —Si=NI triple bond, is strongly expected from the starting material, but has not been proved by trapping. Ab initio calculations at the fully optimized MP2/6-31G level including zero-point corrections show that the SiN double bond product is 55 kcal mol-1 more stable than the triple bond product.6... [Pg.161]

The zero-point corrected MP3/6-31G 76-31G value of 174.7 kcal mol-1 for H2C=0 agrees well with the experimental value of 171.7 kcal mol-1. The proton affinities increase in the order 3 (174.7 kcal mol-1) <1 (190.5 kcal mol-1) <2 (208.3 kcal mol-1). This is explained in terms of the predominance of the electrostatic overcharge transfer interactions, because the charge separations in the double bonds increase in the order H2C+0 2-0-a4 < H2Si+0 7-S-0 4 < H2Si+1 0-O-a7 while the frontier n orbital levels rise in the order 3 (—11.8 eV) 2 ( — 1 T9 eV) <1 (—9.8 eV). [Pg.124]

Finally, the zero point vibration corrections (SET V) use to be much larger than the pseudopotential corrections. In the present case, these zero point corrections seems to give rise to unrrealistic values, probably because of the harmonic approximation used in the calculations. The torsion mode as well as its interactions with the remaining modes are indeed very anharmonic. [Pg.411]

Here, A zp is the zero-point energy corrected activation energy defined in Eq. (6.22). At intermediate temperatures, Eq. (6.24) smoothly connects these two limiting cases. In many examples that do not involve H atoms, the difference between the classical and zero-point corrected results is small enough to be unimportant. [Pg.158]

Hydron atoms readily dissolve into bulk Pd, where they can reside in either the sixfold octahedral or fourfold tetrahedral interstitial sites. Determine the classical and zero-point corrected activation energies for H hopping between octahedral and tetrahedral sites in bulk Pd. In calculating the activation energy, you should allow all atoms in the supercell to relax but, to estimate vibrational frequencies, you can constrain all the metal atoms. Estimate the temperature below which tunneling contributions become important in the hopping of H atoms between these two interstitial sites. [Pg.159]

There are now very many DFT calculations for chemical systems in which only regions of the PES around the transition states are explored, especially the barriers V for activated processes, since only this region of the PES is necessary to describe the overall chemical rate within transition state theory (TST) (see the chapter by Bligaard and Nprskov in this book). TST requires zero point corrected adiabatic barriers V (0), but the zero point corrections are generally <0.1 eV for most chemistry at surfaces. Therefore, the distinction between V and V (0) will usually be ignored in this chapter. [Pg.149]

Note E denotes the electronic energy while Eg includes zero-point vibrational effects. Ebm is obtained from calculations with a large basis set and without zero-point correction. [Pg.33]

Finally, the total energy at 0 K is obtained by adding the zero-point correction, obtained from the frequencies of step 2, to the total energy ... [Pg.159]

Computations using CAS(12,12) indicated that 8 dissociates via a transition state of C2 symmetry (9TS) [30], The zero-point corrected activation barrier was shown to be 8.5 kcal/mol at the CAS(12,12)/cc-pVTZ level. [Pg.427]

Figure 6 presents results of binding a variety of potential ligands or solvent molecules to the basal open site of 2. The energies, determined according to Eqs. (3) and (4), include zero-point corrections only. [Pg.13]


See other pages where Zero-point correction is mentioned: [Pg.779]    [Pg.361]    [Pg.96]    [Pg.125]    [Pg.150]    [Pg.276]    [Pg.110]    [Pg.340]    [Pg.167]    [Pg.514]    [Pg.195]    [Pg.130]    [Pg.69]    [Pg.551]    [Pg.280]    [Pg.6]    [Pg.468]    [Pg.176]    [Pg.379]    [Pg.32]    [Pg.154]    [Pg.299]    [Pg.299]    [Pg.300]    [Pg.545]    [Pg.545]    [Pg.425]    [Pg.9]    [Pg.10]    [Pg.282]   
See also in sourсe #XX -- [ Pg.159 ]




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Methods zero point correction

Zero point

Zero-point Energies and Thermodynamic Corrections

Zero-point corrections, electronic structure

Zero-point energy corrections

Zero-point vibrational correction

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