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The Effect of Geometry

The geometry of the metal complex also affects the rate arid mechanism of reductive elimination, as summarized in Equation 8.5. A cis orientation of the two ligands undergoing reductive elimination is required for this reaction to occur by a three-centered, concerted mechanism. Complexes in which the two ligands undergoing reductive elimination are located trans to each other undergo this reaction by stepwise mechanisms or by prior isomerization of the complex to its cis isomer. [Pg.324]

In addition, complexes whose structures resemble the reduced product tend to undergo reductive elimination faster than those that generate this product in an unstable conformation. For example, complexes that can generate a stable linear LjM(O) fragment (in which M = Pd or Pt) eliminate faster than those that generate a bent (chelate) M(0) fragment. [Pg.324]


Gorin has extended this analysis to include (1) the effects of the finite size of the counterions in the double layer of spherical particles [137], and (2) the effects of geometry, i.e. for cylindrical particles [2]. The former is known as the Debye-Huckel-Henry-Gorin (DHHG) model. Stigter and coworkers [348,369-374] considered the electrophoretic mobility of polyelectrolytes with applications to the determination of the mobility of nucleic acids. [Pg.587]

Leng, Y.S., Dyer, P.J., Krstic, P.S., Harrison, R.J. and Cummings, P.T. (2007) Calibration of chemical bonding between benzenedithiolate and gold the effects of geometry and size of gold dusters. Molecular Physics, 105, 293-300. [Pg.244]

There may, however, be a number of other reasons to pursue a predictive first principles theory of Mossbauer spectroscopy. For example, one may want to elucidate structure/spectroscopy correlations in the cleanest way. To this end one may construct in the computer a number of models with systematic variations in oxidation states, spin states, coordination numbers, and identity of hgands to name only a few chemical degrees of freedom. In such studies it is immaterial whether these molecules have been made or could be made what matters is that one can find out which structural details the Mossbauer parameters are most sensitive to. This can provide insight into the effects of geometry or covalency that are very difficult to obtain by any other means. [Pg.138]

The effects of geometry and boundary conditions are usually interrelated, such as in flow redistribution among parallel channels. With common headers connected to the parallel channels, the flow distribution among channels is determined... [Pg.486]

To illustrate the effect of geometry on the Cl shift. Table IV shows some data for several pairs of high spin tetrahedral and octahedral iron complex ions. In each case the shift of tetrahedral ion is more negative than that of the octahedral ion, and the difference in shift is rather substantial. We feel that in these cases the differences in shifts can be ascribed to differences in 4 covalency six electronegative ligands are more able to draw off 5 electron density than are four. Apparently it makes little difference whether the six ligands belong exclusively to a... [Pg.98]

Sattar. S.A. and Kellogg, D.H. (1969). The effect of geometry on the mode of failure of composites in short beam shear test. In Composite Materials Testing and Design. ASTM STP 460, ASTM, Philadelphia, PA, pp. 62-71. [Pg.91]

Tables 12-23 to 12-26 examine the effect of geometry on dipole moments in a small collection of hydrocarbons and amines. Singlepoint 6-31G, EDF1/6-31G, B3LYP/6-31G and MP2/6-31G dipole moment calculations have been carried out using MMFF, AMI and (except for the Hartree-Fock calculations) 6-3IG geometries, and compared with dipole moments obtained from exact structures. While subtle differences exist, for the most part they are very small. In fact, using mean absolute error as a criterion, there is little to differentiate dipole moments obtained from use of approximate geometries from those calculated using exact geometries. Tables 12-23 to 12-26 examine the effect of geometry on dipole moments in a small collection of hydrocarbons and amines. Singlepoint 6-31G, EDF1/6-31G, B3LYP/6-31G and MP2/6-31G dipole moment calculations have been carried out using MMFF, AMI and (except for the Hartree-Fock calculations) 6-3IG geometries, and compared with dipole moments obtained from exact structures. While subtle differences exist, for the most part they are very small. In fact, using mean absolute error as a criterion, there is little to differentiate dipole moments obtained from use of approximate geometries from those calculated using exact geometries.
A truncated cone of fairly small angle behaves roughly like the cylinder. Briscoe et al4 have quoted relationships for a number of indentor geometries and considered the effect of geometry in detail. [Pg.114]

Now let us discuss shortly the effect of geometry on tf. First, in view of the assumption B/q0 > 1 the third term in parentheses of the right-hand side of Eq. (4.37) will be positive (which is satisfied if (B/2q0) > 3.127 for point runners this normally holds true). Then tf grows together with increasing H, B, ho and decreasing the radius of the runner channel q0. Second, an analysis of Eq. (4.37) shows that there exist such 8 = 8 for which tf is minimal. The expression for 8m is as follows ... [Pg.108]

Ab Initio Calculations of 31P NMR Chemical Shielding Anisotropy Tensors in Phosphates The Effect of Geometry on Shielding... [Pg.320]

Slentz et al. [133] described the effects of geometry (size, shape, and dimensions) on the performance of COMOSS. Vreeland and Barron [134] described the design of functional materials for genomic and proteomic analyses in NCE. The authors discussed different polymer chemistries for micro-channel surface passivation and improved DNA separation. [Pg.45]

The effect of geometry relaxation of chemical bonds in solution is small, but not negligible. On average, as the polarity of the solvent increases C - H bonds become shorter, while the polar O - H and N - H bonds elongate (see Table 4.2), suggesting a flux of electrons H -> O/N which will reinforce the bond dipole. Not surprisingly, C = O bonds... [Pg.502]

More light can be shed on the effect of geometry and symmetry on fullerene anions by studying their 13C NMR chemical shifts that are affected by both charge distribution and ring currents. [Pg.508]

Simulations on P Pd clusters and Pd monolayers on different metal surfaces have provided insight into low-Pt and Pt-free catalysts. Calvo et al performed DFT calculations on finite PhPd clusters (with x + y = 10) focusing on the effects of geometry and local electronic structure on ORR. The PtsPdv cluster is thermodynamically most favorable for the ORR in terms of reaction energies of OOH and water formation. The activity of Pd monolayers deposited on Ru(OOOl), Rh(lll), Ir(lll), Pt(lll), and Au(lll) surfaces were investigated with periodic DFT calculations. From calculated -band center shifts, the following order in the ORR activity was proposed Pd/Ru(0001) < Pd/Ir(lll) < Pd/Rh( 111) < Pd/Au( 111) < Pd/Pt(l 11). [Pg.102]

The effect of geometry and axial orientation of spheroidal particles on the adsorption rate in a granular porous medium... [Pg.745]

Recent efforts have attempted to address quantitatively the complex fluid mechanics on trays, although the effects of geometry, flow rates, and physical properties on interfacial area and transfer rate are not completely understood. Prado and Fair (1990) made the first attempt, using such variables as bubble size distribution, residence times, and vapor/liquid diffusional phenomena. Garcia... [Pg.463]

Both these geometric parameters altered diffusion data measured as Sherwood dimensionless number or as diffusion coefficients maxima and minima in these parameters mirrored nodes and antinodes from the ultrasound. This involved relative motions between the various components of several centimeters since the wavelength of sound at 20 kHz is of this order, depending on the medium. These workers were using electrochemistry as a probe to monitor ultrasonic power, and a fuller account of this work is given in another chapter of this volume, but the effects of geometry upon behavior of the electrochemical probe are noteworthy. [Pg.219]

In spite of the development of new methods of measurements, fewer than 300 molecular electron affinities have been measured in the gas phase [5-7]. With the limited number of experimental Ea it is important to have a simple rigorous quantum mechanical procedure for the calculation of electron affinities of large molecules. Electron correlation is the crucial problem in the calculation of Ea. The correlation energies are significant because Ea represent a small difference between two large quantities. Since an electron is added to the system, the effects of geometry changes and correlation reinforce each other rather than cancel out, as in ionization potentials. [Pg.141]

The effects of the geometry of the impeller, vessel, and its internals are incorporated into the S parameter. Values of S are listed in Table 2 for a variety of impellers. The S value varies with D/T, and C/T. Zwietering provided plots of 5" as a function of D/T and C/r.[ 2] More recently, Armenante and Uehara Nagamine and Armenante, Uehara Nagamine, and Susanto have sought simple mathematical expressions to describe the effects of geometry D/T and C/T) on [25,27] results, reported in Table 3, are yet to... [Pg.1773]


See other pages where The Effect of Geometry is mentioned: [Pg.10]    [Pg.147]    [Pg.198]    [Pg.15]    [Pg.244]    [Pg.283]    [Pg.21]    [Pg.199]    [Pg.266]    [Pg.176]    [Pg.93]    [Pg.148]    [Pg.501]    [Pg.13]    [Pg.145]    [Pg.183]    [Pg.310]    [Pg.543]    [Pg.135]    [Pg.298]    [Pg.196]    [Pg.439]    [Pg.292]    [Pg.393]    [Pg.15]    [Pg.200]    [Pg.680]    [Pg.688]    [Pg.14]    [Pg.177]   


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