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B* axis

In a molecule such as the asymmetric rotor formaldehyde, shown in Figure 5.1(f), the a, b and c inertial axes, of lowest, medium and highest moments of inertia, respectively, are defined by symmetry, the a axis being the C2 axis, the b axis being in the yz plane and the c axis being perpendicular to the yz plane. Vibrational transition moments are confined to the a, b or c axis and the rotational selection mles are characteristic. We call them... [Pg.181]

FIGURE 14.20 Random, single-displacement bisnbstrate mechanism where A does not affect B binding, and vice versa. Note that the lines intersect at the 1/[A] axis. (If [B] were varied in an experiment with several fixed concentrations of A, the lines would intersect at the 1/[B] axis in a 1/u versus 1/[B] plot.)... [Pg.450]

Small needle-shaped single crystals were examined by transmission electron microscopy (TEM) and electron diffraction (ED) (see Fig. 16-17). The results show that the crystals are elongated along the b-axis, which is the direction of weak intermolecular n-n interactions, and have a well-developed (ab) top surface. It corresponds to the surface of aliphatic tails (direction of weak intermolecular interactions). There are indications of displacement of successive ( / )-laycrs along the fl-axis, in line with the other signs of disorder in the aliphatic layer. [Pg.303]

Figure 14-16. Low temperature (LT) and high temperature (IHT) polymorphs ol qualenhiophcnc. Top view along the unique b axis botiom view along the molecular axis (note the herringbone packing) (Adapted from Refs. 791 and 82 ). Figure 14-16. Low temperature (LT) and high temperature (IHT) polymorphs ol qualenhiophcnc. Top view along the unique b axis botiom view along the molecular axis (note the herringbone packing) (Adapted from Refs. 791 and 82 ).
Since the first structure determination by Wadsley [56] in 1952 there has been confusion about the correct cell dimensions and symmetry of natural as well of synthetic lithiophorite. Wadsley determined a monoclinic cell (for details see Table 3) with a disordered distribution of the lithium and aluminium atoms at their respective sites. Giovanoli et al. [75] found, in a sample of synthetic lithiophorite, that the unique monoclinic b-axis of Wadsley s cell setting has to tripled for correct indexing of the electron diffraction patterns. Additionally, they concluded that the lithium and aluminum atoms occupy different sites and show an ordered arrangement within the layers. Thus, the resulting formula given by Giovanelli et al. [Pg.101]

All the modifications of the a form would present, perpendicular to the b axis, macromolecular bilayers including all isoclined chains. A regular succession of bilayers with anticlined helices would correspond to the limiting ordered modification (a2), while a statistical succession of bilayers would correspond to the limiting disordered modification (a ) [40]. [Pg.195]

The approach discussed above can provide a qualitative description of the effect of external fields on bond-breaking processes. For example, consider the H2 molecule (HA — HB) in the presence of an Li+ ion 3 A away from HB on the A-B axis. To study this problem, we assume that there is no charge migration to the Li location (so that Pc = 0) and that fiAC = pBC = 0 since the Li+ ion is sufficiently far from HA and HB. In this case, we can write the H matrix as... [Pg.12]

The first example with concrete short T1—Au bonds is AuTl[Ph2P(CH2)S]2. The complex is formed by reacting Tl with [(Ph3P)2N] tAuPh2P(CH2)S] . It forms a one-dimensional polymer along the unique crystallographic b-axis of the lattice ... [Pg.49]

In the latter type, the direction of the unique axis (b-axis) of the polymer coincides with that of the monomer while the directions of the other two axes do not. In the case of 3 OMe none of the directions of the axes of the polymer coincide with those of the monomer. However, the temperature effect on the reaction behaviour (see Section 3) and the continuous change of the X-ray diffraction pattern indicate a typical diffusionless crystal-lattice controlled mechanism (Hasegawa et al., 1981). [Pg.130]

Figure 5. ORTEP [7] drawing of hydrogen bonded network showing two ribbons in neighboring layers. The structure is viewed along the c-axis with the u-axis vertical and the b-axis horizontal. [Pg.329]

Fig. 30. Schematic illustration of the 2 1 clathrate between N-tritylurea and dimethyl-formamide, showing the self-association of the host molecules along the b axis of the crystal (crystal data a — 29.614, b = 8.906, c = 16.127 A, p — 121.04°, space group Cc)23)... Fig. 30. Schematic illustration of the 2 1 clathrate between N-tritylurea and dimethyl-formamide, showing the self-association of the host molecules along the b axis of the crystal (crystal data a — 29.614, b = 8.906, c = 16.127 A, p — 121.04°, space group Cc)23)...
Fig. 7. Projection of thieno 3,4-<7]thiepin 3,3-dioxide (128) along the b axis showing bond lengths and angles... Fig. 7. Projection of thieno 3,4-<7]thiepin 3,3-dioxide (128) along the b axis showing bond lengths and angles...
Each point in the phase diagram in Fig. 8.8 corresponds to a certain value of a and b, i.e., it represents the possible chemical composition of a molecular population. Variable a forms the horizontal axis, (1 +a) being the number of monomer types. The b axis represents the quality factor of the polymer catalysis. The transition region contains those populations which can have both ordered and disordered... [Pg.233]


See other pages where B* axis is mentioned: [Pg.456]    [Pg.1550]    [Pg.103]    [Pg.398]    [Pg.308]    [Pg.360]    [Pg.254]    [Pg.857]    [Pg.604]    [Pg.90]    [Pg.68]    [Pg.146]    [Pg.309]    [Pg.382]    [Pg.619]    [Pg.89]    [Pg.94]    [Pg.95]    [Pg.96]    [Pg.409]    [Pg.353]    [Pg.107]    [Pg.346]    [Pg.392]    [Pg.408]    [Pg.27]    [Pg.163]    [Pg.158]    [Pg.145]    [Pg.170]    [Pg.250]    [Pg.40]    [Pg.46]    [Pg.46]    [Pg.50]    [Pg.722]    [Pg.188]    [Pg.659]   
See also in sourсe #XX -- [ Pg.359 ]




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