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Substrate symmetry

The growth direction of MgCl2 is independent of the substrate symmetry [93]. Growth on a cubic crystal, namely Pd(lOO), leads to hexagonal LEED pattern. However, the structure of the films is much more complex due to the... [Pg.132]

Alworth, W. L. Stereochemistry and its Application in Biochemistry. The Relation between Substrate Symmetry and Biological Stereospecificity. Wiley-Interscience New York, London, Sydney, Toronto (1972). [Pg.618]

Substrates Symmetry Lattice parameters (A) mol/ sub Grain orientation (rotation angle)... [Pg.302]

The situation is different if the substrate is a prochiral or meso compound. Since these molecules have a center or plane of symmetry the binding of pro-S or pro-R forms is equivalent. The chirahty appears only as a result of the transformation. Hence, at least theoretically, the compound can be converted to one enantiomer quantitatively. [Pg.332]

The 27T-electrons of the carbon-nitrogen double bond of 1-azirines can participate in thermal symmetry-allowed [4 + 2] cycloadditions with a variety of substrates such as cyclo-pentadienones, isobenzofurans, triazines and tetrazines 71AHC(13)45). Cycloadditions also occur with heterocumulenes such as ketenes, ketenimines, isocyanates and carbon disulfide. It is also possible for the 27r-electrons of 1-azirines to participate in ene reactions 73HCA1351). [Pg.59]

This concerted model assumes furthermore that the symmetry of the molecule is conserved so that the activity of all its subunits is either equally low or equally high, that is, all structural changes are concerted. Subsequently Daniel Koshland, University of California, Berkeley, postulated a sequential model in which each subunit is allowed independently to change its tertiary structure on substrate binding. In this model tertiary structural changes in the subunit with bound ligand alter the interactions of this... [Pg.113]

Figure 2 Examples of overlayer structures with appropriate notation, (a) fee (100) p(2X2) (b) fee (100) c(2X2) (c) fee (111) p(73 X 73>R30< (d) bee (110 ) p(2 X 1) and bee (110) p(1 X 2). The two orientations for the unit mesh in (d) are both possible because of the symmetry of the substrate they have the same free energy and are called degenerate. Figure 2 Examples of overlayer structures with appropriate notation, (a) fee (100) p(2X2) (b) fee (100) c(2X2) (c) fee (111) p(73 X 73>R30< (d) bee (110 ) p(2 X 1) and bee (110) p(1 X 2). The two orientations for the unit mesh in (d) are both possible because of the symmetry of the substrate they have the same free energy and are called degenerate.
The lack of a well-defined specular direction for polycrystalline metal samples decreases the signal levels by 10 —10, and restricts the symmetry information on adsorbates, but many studies using these substrates have proven useful for identifying adsorbates. Charging, beam broadening, and the high probability for excitation of phonon modes of the substrate relative to modes of the adsorbate make it more difficult to carry out adsorption studies on nonmetallic materials. But, this has been done previously for a number of metal oxides and compounds, and also semicon-... [Pg.449]

Fig. 10. Unpolarized Raman spectra (T = 300 K) for solid Ceo, KaCeo, RbsCeo, NaeCeo, KaCco, RbeCeo and CseCeo [92, 93], The tangential and radial modes of Ag symmetry are identified, as are the features associated with the Si substrates. From the insensitivity of these spectra to crystal structure and specific alkali metal dopant, it is concluded that the interactions between the Cao molecules are weak, as are also the interactions between the Cao anions and the alkali metal cations. Fig. 10. Unpolarized Raman spectra (T = 300 K) for solid Ceo, KaCeo, RbsCeo, NaeCeo, KaCco, RbeCeo and CseCeo [92, 93], The tangential and radial modes of Ag symmetry are identified, as are the features associated with the Si substrates. From the insensitivity of these spectra to crystal structure and specific alkali metal dopant, it is concluded that the interactions between the Cao molecules are weak, as are also the interactions between the Cao anions and the alkali metal cations.
An important issue in the thermodynamics of confined fluids concerns their symmetry which is lower than that of a corresponding homogeneous bulk phase because of the presence of the substrate and its inherent atomic structure [52]. The substrate may also be nonplanar (see Sec. IV C) or may consist of more than one chemical species so that it is heterogeneous on a nanoscopic length scale (see Sec. VB 3). The reduced symmetry of the confined phase led us to replace the usual compressional-work term —Pbuik F in the bulk analogue of Eq. (2) by individual stresses and strains. The appearance of shear contributions also reflects the reduced symmetry of confined phases. [Pg.11]

While the smooth substrate considered in the preceding section is sufficiently reahstic for many applications, the crystallographic structure of the substrate needs to be taken into account for more realistic models. The essential complications due to lack of transverse symmetry can be dehneated by the following two-dimensional structured-wall model an ideal gas confined in a periodic square-well potential field (see Fig. 3). The two-dimensional lamella remains rectangular with variable dimensions Sy. and Sy and is therefore not subject to shear stresses. The boundaries of the lamella coinciding with the x and y axes are anchored. From Eqs. (2) and (10) one has... [Pg.12]

FIGURE 15.9 Monod-Wyman-Changeux (MWC) model for allosteric transitions. Consider a dimeric protein that can exist in either of two conformational states, R or T. Each subunit in the dimer has a binding site for substrate S and an allosteric effector site, F. The promoters are symmetrically related to one another in the protein, and symmetry is conserved regardless of the conformational state of the protein. The different states of the protein, with or without bound ligand, are linked to one another through the various equilibria. Thus, the relative population of protein molecules in the R or T state is a function of these equilibria and the concentration of the various ligands, substrate (S), and effectors (which bind at f- or Fj ). As [S] is increased, the T/R equilibrium shifts in favor of an increased proportion of R-conformers in the total population (that is, more protein molecules in the R conformational state). [Pg.470]

The reactivity of cyanuric chloride (2,4,6-trichloro-s-triazine) as an indication of s-triazine activation is misleadingly high because of mutual activation of the chlorines meta activation > ortho or para activation) and its symmetry (cf. Section III,A, 1), However, the greatest variety of nucleophilic substitutions have been investigated with this substrate. [Pg.301]

We describe the situation by saying that the receptor provides a chiral environment for the substrate. In the absence of a chiral environment, the two red substituents are chemically identical, but in the presence of the chiral environment, they are chemically distinctive (Figure 9.18a). The situation is similar to what happens when you pick up a coffee mug. By itself, the mug has a plane of symmetry and is achiral. You could, if you wanted, drink from on either side of the handle. When you pick up the mug, however, your hand provides a chiral environment so one side becomes much more accessible and easier to drink from than the other (Figure 9.18b). [Pg.320]


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See also in sourсe #XX -- [ Pg.189 ]




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