Big Chemical Encyclopedia

Chemical substances, components, reactions, process design ...

Articles Figures Tables About

Crystal field model

We will discuss the crystal field model here. It assumes that the bonding between metal "Crystal field" isn t a very descriptive term,... [Pg.417]

Most coordination compounds are brilliantly colored, a property that can be explained by the crystal field model. [Pg.417]

Two symmetry parameterizations of the angular overlap model of the ligand field. Relation to the crystal field model. C. E. Schaffer, Struct. Bonding (Berlin), 1973,14, 69-110 (33). [Pg.43]

We are concerned with what happens to the (spectral) d electrons of a transition-metal ion surrounded by a group of ligands which, in the crystal-field model, may be represented by point negative charges. The results depend upon the number and spatial arrangements of these charges. For the moment, and because of the very common occurrence of octahedral coordination, we focus exclusively upon an octahedral array of point charges. [Pg.28]

This would not be expected simply on the basis of a crystal-field model, for the d orbitals will contract with increasing positive charge and hence interact less well with the ligand point charges . The modest decreases in bond length as one traverses the series (Eq. 6.9) are unlikely to compensate for, let alone override, the effects of such orbital contraction. Finally, to add to the confusion, we also note from Eq. (6.7) that zio -t values increase as we go down the periodic table (Eq. 6.10). [Pg.101]

Schaffer CE (1968) A Perturbation Representation of Weak Covalent Bonding. 5 68-95 Schaffer CE (1973) Two Symmetry Parameterizations of the Angular-Overlap Model of the Ligand-Field. Relation to the Crystal-Field Model. 14 69-110 Scheldt WR, Lee YJ (1987) Recent Advances in the Stereochemistry of Metallotetrapyrroles. 64 1-70... [Pg.254]

The second row of Table 6 gives the net populations of the 3 and Ap atomic orbitals. They are quite different from those predicted by the crystal field model, given in the first row. [Pg.117]

Atomic orbital populations and resulting QS in a crystal field model. [Pg.118]

Schaffer, C.E. Two Symmetry Parameterizations of the Angular-Overlap Model of the Ligand-Field. Relation to the Crystal-Field Model. Vol. 14, pp. 69-110. [Pg.130]

The general influence of covalency can be qualitatively explained in a very basic MO scheme. For example, we may consider the p-oxo Fe(III) dimers that are encountered in inorganic complexes and nonheme iron proteins, such as ribonucleotide reductase. In spite of a half-filled ferric high-spin ions show quadrupole splittings as large as 2.45 mm s < 0, 5 = 0.53 mm s 4.2-77 K) [61, 62]. This is explained... [Pg.100]

A quantitative consideration on the origin of the EFG should be based on reliable results from molecular orbital or DPT calculations, as pointed out in detail in Chap. 5. For a qualitative discussion, however, it will suffice to use the easy-to-handle one-electron approximation of the crystal field model. In this framework, it is easy to realize that in nickel(II) complexes of Oh and symmetry and in tetragonally distorted octahedral nickel(II) complexes, no valence electron contribution to the EFG should be expected (cf. Fig. 7.7 and Table 4.2). A temperature-dependent valence electron contribution is to be expected in distorted tetrahedral nickel(n) complexes for tetragonal distortion, e.g., Fzz = (4/7)e(r )3 for com-... [Pg.244]

Foyt et al. [137] interpreted the quadrupole-splitting parameters of low-spin ruthenium(II) complexes in terms of a crystal field model in the strong-field approximation with the configuration treated as an equivalent one-electron problem. They have shown that, starting from pure octahedral symmetry with zero quadrupole splitting, A q increases as the ratio of the axial distortion to the spin-orbit coupling increases. [Pg.280]

Both Fe(ll)(TPP) and Fe(II)(OEP) have positive electric quadrupole splitting without significant temperature dependence which, however, cannot be satisfactorily explained within the crystal field model [117]. Spin-restricted and spin-unrestricted Xoi multiple scattering calculations revealed large asymmetry in the population of the valence orbitals and appreciable 4p contributions to the EFG [153] which then was further specified by ab initio and DFT calculations [154,155]. [Pg.427]

Modelling the Magnetic Properties of Lanthanide Single-Ion Magnets The Use of the Crystal Field Model... [Pg.30]

At an early stage in the development of ligand field theory, it was found that A the splitting parameter for tetrahedral MX4, should be equal to (4/9) of A0, the splitting parameter for octahedral MX6, and experimental data are in good agreement with this prediction. However, this takes no account of the fact that the M—X distance in tetrahedral MX4 is usually some 8—10% shorter than in octahedral MX6. In the pointcharge crystal field model, A is proportional to R-5, so that if the difference in R between MX4 and MX6 is taken into account, we predict (At/A0) to be 0.6—0.7, compared with the experimental value of about 0.5. An AOM treatment (131) leads to better results, since here we find ... [Pg.105]

Figure 4. Calculated HAB values as a function of Fe -Fe separation, based on the structural model given in Figure 1 and the diabatic wavefunctions I/a and f/B. Curves 1 and 2 are based on separate models in which the inner-shell ligands are represented, respectively, by a point charge crystal field model [Fe(H20)62 -Fe(HsO)63 ] and by explicit quantum mechanical inclusion of their valence electrons [Fe(HgO)s2 -Fe(H20)s3+] (as defined by the dashed rectangle in Figure 1). The corresponding values of Kei, the electronic transmission factor, are displayed for various Fe-Fe separations of interest. Figure 4. Calculated HAB values as a function of Fe -Fe separation, based on the structural model given in Figure 1 and the diabatic wavefunctions I/a and f/B. Curves 1 and 2 are based on separate models in which the inner-shell ligands are represented, respectively, by a point charge crystal field model [Fe(H20)62 -Fe(HsO)63 ] and by explicit quantum mechanical inclusion of their valence electrons [Fe(HgO)s2 -Fe(H20)s3+] (as defined by the dashed rectangle in Figure 1). The corresponding values of Kei, the electronic transmission factor, are displayed for various Fe-Fe separations of interest.
Vanadium(n) Complexes.—Dehydration of VSO. THjO has been shown to proceed via the formation of VS04,mH20 (where n = 6, 4, or 1) and V(OH)-(SO4), which were characterized by X-ray studies. The polarographic behaviour and the oxidation potential of the V -l,2-cyclohexanediamine-tetra-acetic acid complex, at pH 6—12, have been determined.Formation constants and electronic spectra have been reported for the [Vlphen),] " and [V20(phen)] complexes. The absorption spectrum of V ions doped in cadmium telluride has been presented and interpreted on a crystal-field model. The unpaired spin density in fluorine 2pit-orbitals of [VF ] , arising from covalent transfer and overlap with vanadium orbitals, has been determined by ENDOR spectroscopy and interpreted using a covalent model. " ... [Pg.38]

The crystal field model may also provide a calciflation scheme for the transition probabilities between levels perturbed by the crystal field. It is so called weak crystal field approximation. In this case the crystal field has little effect on the total Hamiltonian and it is regarded as a perturbation of the energy levels of the free ion. Judd and Ofelt, who showed that the odd terms in the crystal field expansion might connect the 4/ configuration with the 5d and 5g configurations, made such calculations. The result of the calculation for the oscillator strength, due to a forced electric dipole transition between the two states makes it possible to calculate the intensities of the lines due to forced electric dipole transitions. [Pg.120]

Some individual compounds have been studied using LCAO-MO theory in the Wolfsberg-Helmholz approximation (5). Although this method is somewhat more realistic and allows one to account for other properties (such as "charge-transfer bands, EPR, and NMR experiments) nevertheless, compared to the crystal field model it is much more laborious, it is only vahd for the individual case, and the choice of parameters in often rather arbitrary. [Pg.53]

The application of the angular overlap method to MXg chromophores of trigonal bipyramidal and square p3u-amidal stereochemistry leads to the patterns of Fig. 2 for the energies of the antibonding "d molecular orbitals (dc). The crystal field model leads to a similar pattern. [Pg.55]

Large numbers of five-coordinate copper(II) complexes in several stereochemistries are known. The spectra which have been most studied with a view to interpretation are those of the trigonal bipyramidal complexes, for which assignments have been proposed on the basis of molecular orbital, angular overlap, and crystal-field models. [Pg.63]


See other pages where Crystal field model is mentioned: [Pg.425]    [Pg.685]    [Pg.23]    [Pg.30]    [Pg.58]    [Pg.101]    [Pg.101]    [Pg.93]    [Pg.100]    [Pg.426]    [Pg.38]    [Pg.111]    [Pg.90]    [Pg.95]    [Pg.106]    [Pg.106]    [Pg.460]    [Pg.53]   
See also in sourсe #XX -- [ Pg.35 , Pg.36 ]




SEARCH



Additive crystal-field model

An Ionic Bonding Model - Introducing Crystal Field Theory

Complex ions crystal field model

Coordinate bond-bonding models crystal field theory

Crystal field

Crystal field model equilibria

Crystal field model isomerism

Crystal field model naming

Crystal field model paramagnetic

Crystal field model, failure

Crystal field parameters angular overlap model

Crystal field parameters point charge electrostatic model

Crystal field parameters simple overlap model

Crystal field theory angular overlap model

Crystallization fields

Electrostatic crystal field model

Field modeling

Jahn-Teller Effect in Crystal-Field Model

Modeling crystallization

Octahedral complexes crystal field model

The Crystal Field Model

© 2024 chempedia.info