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Lewis structure natural

For hydrogen fluoride, which is well described by a single Lewis structure (cf. Example 1.6), the localized natural Lewis-structure model wavefunction gives... [Pg.29]

In this case the energy of the natural Lewis-structure model... [Pg.30]

Figure 2.4 Components of the Li-F potential-energy curve E R) = E (R) + E(NL>(R), showing the localized natural-Lewis-structure model energy E(L> (circles, left-hand scale) and delocalized non-Lewis correction ,(NL) (squares, right-hand scale). The classical electrostatic estimate E (dotted line) is shown for comparison. Figure 2.4 Components of the Li-F potential-energy curve E R) = E (R) + E(NL>(R), showing the localized natural-Lewis-structure model energy E(L> (circles, left-hand scale) and delocalized non-Lewis correction ,(NL) (squares, right-hand scale). The classical electrostatic estimate E (dotted line) is shown for comparison.
Table 3.1 compares key bonding and ionicity descriptors for the NBO Lewis-structure representations of the five AF diatomic fluorides in this series. From this table it can be seen that the single-term natural Lewis-structure description is practically exact for all species (with %p 99.9% for A = F, Cl, Br, H, and only a... [Pg.101]

As described in Sections 1.4 and 1.5, a general fia— 2b donor-acceptor interaction between Lewis ( 2a) and non-Lewis (fib ) NBOs leads to perturbative corrections to the zeroth-order natural Lewis-structure wavefunction... [Pg.183]

Let us first inquire whether basic criteria for the validity of low-order perturbation theory are actually satisfied in the present case. As described in Section 1.4, the perturbative starting point is an idealized natural Lewis-structure wavefunction (t//,l )) of doubly occupied NBOs. The accuracy of this Lewis-type starting point may be assessed in terms of the percentage accuracy of the variational energy (E) or density (p(l ). as shown for each molecule in Table 3.20. [Pg.185]

It must be emphasized that the formulation of three-center T-bonds provides a qualitative (not merely incremental) improvement in the accuracy of the natural Lewis-structure description of diborane. Because a three-center orbital is intrinsically more mathematically flexible than a two-center orbital, the description of any molecule is seemingly improved by employing three-center in place of two-center NBOs. However, for most non-boron molecules this improvement would be quite negligible (e.g., less than 0.1% for ethane, whose two-center Lewis-structure... [Pg.309]

Figure 4.23 Variations of metal-metal bond length with nominal formal bond order (the number of bonds in the natural Lewis structure) in duodectet-rule-conforming dinuclear hydrides H MMH (see Table 4.15). Figure 4.23 Variations of metal-metal bond length with nominal formal bond order (the number of bonds in the natural Lewis structure) in duodectet-rule-conforming dinuclear hydrides H MMH (see Table 4.15).
Table 4.36. The NBO descriptors o/ M2H2 species (see Fig. 4.57) namely the accuracy of the natural Lewis structure (%/+). metal charge (Qu), metal hybrid (hM), percentage polarization toward metal (%m), and occupancies (Occ.) of two-center bonds and antibonds... Table 4.36. The NBO descriptors o/ M2H2 species (see Fig. 4.57) namely the accuracy of the natural Lewis structure (%/+). metal charge (Qu), metal hybrid (hM), percentage polarization toward metal (%m), and occupancies (Occ.) of two-center bonds and antibonds...
Since Lewis-type NBOs typically have (slightly) less than double occupancy, they are not yet true molecular orbitals in the Hartree-Fock sense. Equivalently, one may say that a determinant of doubly-occupied NBOs, the natural Lewis structure wavefunction "Pl = det (cTAB) (crcD) I must have higher energy than the Hartree-Fock MO wavefunction... [Pg.1800]

What would the world be like if the Lewis structure picture were exact, and resonance effects were absent Such a world without resonance is the essential defining characteristic of the Natural Lewis Structure wavefunction a well-defined starting point for the systematic NBO-based exploration of chemical behavior. [Pg.92]

Figure 8.6 Torsional variations of non-Lewis error (pnl) for single-bonded (dashed line) versus double-bonded (solid line) natural Lewis structures of CH2CH2 (circles) and BH2NH2 (crosses), showing the NLS crossing point for each species (marked by a box) with crossing angles 66° and 75° for BH2NH2 and CH2CH2, respectively. Figure 8.6 Torsional variations of non-Lewis error (pnl) for single-bonded (dashed line) versus double-bonded (solid line) natural Lewis structures of CH2CH2 (circles) and BH2NH2 (crosses), showing the NLS crossing point for each species (marked by a box) with crossing angles 66° and 75° for BH2NH2 and CH2CH2, respectively.
Table 11.2 Calculated bond length (Re), NRT bond order ( no) atomic charge at N (2n) and a/p natural lewis structure (NLS) representations (and percentage accuracy) for low-lying states of nitric oxide (CIS/6-311 +G level) (cf. Fig. 11.1a for state labels). Table 11.2 Calculated bond length (Re), NRT bond order ( no) atomic charge at N (2n) and a/p natural lewis structure (NLS) representations (and percentage accuracy) for low-lying states of nitric oxide (CIS/6-311 +G level) (cf. Fig. 11.1a for state labels).

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