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Inverse bond valence

As the most notable contribution of ab initio studies, it was revealed that the different modes of molecular deformation (i.e. bond stretching, valence angle bending and internal rotation) are excited simultaneously and not sequentially at different levels of stress. Intuitive arguments, implied by molecular mechanics and other semi-empirical procedures, lead to the erroneous assumption that the relative extent of deformation under stress of covalent bonds, valence angles and internal rotation angles (Ar A0 AO) should be inversely proportional to the relative stiffness of the deformation modes which, for a typical polyolefin, are 100 10 1 [15]. A completly different picture emerged from the Hartree-Fock calculations where the determined values of Ar A0 AO actually vary in the ratio of 1 2.4 9 [91]. [Pg.108]

The numerous transformations of cyclooctatetraene 189 and its derivatives include three types of structural changes, viz. ring inversion, bond shift and valence isomerizations (for reviews, see References 83-85). One of the major transformations is the interconversion of the cyclooctatetraene and bicyclo[4.2.0]octa-2,4,7-triene. However, the rearrangement of cyclooctatetraene into the semibullvalene system is little known. For example, the thermolysis of l,2,3,4-tetra(trifluoromethyl)cyclooctatetraene 221 in pentane solution at 170-180 °C for 6 days gave three isomers which were separated by preparative GLC. They were identified as l,2,7,8-tetrakis(trifluoromethyl)bicyclo[4.2.0]octa-2,4,7-triene 222 and tetrakis(trifluoromethyl)semibullvalenes 223 and 224 (equation 71)86. It was shown that a thermal equilibrium exists between the precursor 221 and its bond-shift isomer 225 which undergoes a rapid cyclization to form the triene 222. The cyclooctatetraenes 221 and 225 are in equilibrium with diene 223, followed by irreversible rearrangement to the most stable isomer 224 (equation 72)86. [Pg.773]

The inverse spinel structure (Zn)[TiZn]04 has Znl placed in octahedral sites, Zn2 placed in tetrahedral sites and Ti placed in octahedral sites. The normal spinel structure, (Ti)[Zn2]04, exchanges the Ti in octahedral sites with Zn2 in tetrahedral sites. The bond valence sums for the two alternative structures are given in Table 7.1. The cation valences for the inverse structure, Znl = 2.13, 7,n2 = 1.88, Ti = 3.85, are reasonably close to those expected, viz. Znl = 2.0,... [Pg.165]

Because the X-ray scattering factors of Mg and A1 are similar, it is not easy to assign the cations in the mineral spinel, MgAl204 to either octahedral or tetrahedral sites (see Section 7.8 for more information). The bond lengths around the tetrahedral and octahedral positions are given in the table. Use the bond valence method to determine whether the spinel is normal or inverse. The values of r0 are r0 (Mg2+) = 0.1693 m, r0 (Al3+)= 0.1651 nm, B = 0.037 nm, from... [Pg.183]

The energy of valence interactions accounts for bond stretching (bond), valence angle bending (angle), dihedral angle torsion (torsion), and inversion, also called out of plane interactions (oop) ... [Pg.225]

Table 2. Bond valences in oxide olivine and inverse spinel structures. The numbers in the first three columns are the valences of the atoms A, B, C respectively (C is the tetrahedrally-coordinated cation). 6 is the difference in valence for the M-O(l) and Af-0(2) bonds... Table 2. Bond valences in oxide olivine and inverse spinel structures. The numbers in the first three columns are the valences of the atoms A, B, C respectively (C is the tetrahedrally-coordinated cation). 6 is the difference in valence for the M-O(l) and Af-0(2) bonds...
The solution for this case is readily obtained as a special case (with Vx = Vy = 2) of the solution of the inverse spinel structure given above and is given in Table 2. [Note that, in the table, I write [0(1), 0(2)] for olivine as 0(1) and 0(3) of olivine as 0(2).] It may be verified that if further, Va = Vb = 2 then a = P = Y = 6 = l/3 and e = g = 1, so that in (e.g.) Mg2Si04 all Mg-0 and all Si-O bonds are found to have the same valence -one must therefore attribute the variations in bond lengths actually observed to factors other than bond valence constraints. The olivine structure is further discussed below. [Pg.178]

In this paper, I have outlined how the bond valence method may be used to predict bond lengths in crystal structures, particularly in cases where use of radius sums fails. I have also indicated some of its limitations. My feeling is that to go much beyond the present level of treatment would require the introduction of too many empirical parameters to be generally useful. On the other hand the inverse procedure of using observed bond lengths to calculate apparent valences promises to be very fruitful and capable of considerable further development. [Pg.186]

Still it should have become obvious from the above discussion that there is a close functional relationship between bond valence and electron density at the bond critical point (and in the same way between bond valence and the Laplacian of V Pbcp) and that this correlation involves a scaling based on the principal quantum number (row number) of the atoms involved or a closely correlated quantity, and at least for the case of the Laplacian to a measure of atomic polarizability (such as the atomic hardness or its inverse the atomic sofmess). This fundamental correlation should thus be taken into account when fine-tuning approaches to determine bond valence parameters and BV-related forcefields. [Pg.107]

Ionova I V and Carter E A 1995 Crbital-based direct inversion in the iterative subspace for the generalized valence bond method J. Chem. Phys. 102 1251... [Pg.2356]

Terms in the energy expression that describe a single aspect of the molecular shape, such as bond stretching, angle bending, ring inversion, or torsional motion, are called valence terms. All force fields have at least one valence term and most have three or more. [Pg.50]

Electronegativity x is the relative attraction of an atom for the valence electrons in a covalent bond. It is proportional to the effective nuclear charge and inversely proportional to the covalent radius ... [Pg.303]

The Diels-Alder reaction of cyclopropenes with 1,2,4,5-tetrazines (see Vol.E9c, p 904), a reaction with inverse electron demand, gives isolable 3,4-diazanorcaradienes 1, which are converted into 4H-1,2-diazepines 2 on heating. The transformation involves a symmetry allowed [1,5] sigmatropic shift of one of the bonds of the three-membered ring, a so-called walk rearrangement , followed by valence isomerization.106,107... [Pg.348]

According to the transition state theory, the pre-exponential factor A is related to the frequency at which the reactants arrange into an adequate configuration for reaction to occur. For an homolytic bond scission, A is the vibrational frequency of the reacting bond along the reaction coordinates, which is of the order of 1013 to 1014 s 1. In reaction theory, this frequency is diffusion dependent, and therefore, should be inversely proportional to the medium viscosity. Also, since the applied stress deforms the valence geometry and changes the force constants, it is expected... [Pg.110]

In this book the discussion has been restricted to the structure of the normal states of molecules, with little reference to the great part of chemistry dealing with the mechanisms and rates of chemical reactions. It seems probable that the concept of resonance can be applied very effectively in this field. The activated complexes which represent intermediate stages in chemical reactions are, almost without exception, unstable molecules which resonate among several valence-bond structures. Thus, according to the theory of Lewis, Olson, and Polanyi, Walden inversion occurs in the hydrolysis of an alkyl halide by the following mechanism ... [Pg.253]

For the valence bond orbitals themselves, it is generally natural to specify a starting guess in the AO basis. Such a guess might, of course, not lie entirely inside the space spanned by the active space, and it must therefore be projected onto the space of the active MOs. This is achieved trivially in CASVB, by multiplication by the inverse of the matrix of MO coefficients. [Pg.315]

Computation of the overlap matrix between valence bond stmctures, as required for w I) or w l), then requires Vvb applications of T(s), after which diagonalization of SvB easily yields both its inverse and square root. [Pg.317]


See other pages where Inverse bond valence is mentioned: [Pg.182]    [Pg.182]    [Pg.200]    [Pg.165]    [Pg.121]    [Pg.180]    [Pg.532]    [Pg.335]    [Pg.251]    [Pg.951]    [Pg.91]    [Pg.99]    [Pg.88]    [Pg.39]    [Pg.51]    [Pg.237]    [Pg.27]    [Pg.331]    [Pg.5]    [Pg.94]    [Pg.72]    [Pg.604]    [Pg.70]    [Pg.39]    [Pg.57]    [Pg.134]    [Pg.165]   
See also in sourсe #XX -- [ Pg.199 ]




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Bonding inversion

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