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Crystals rotational disorder

Because of the orientational freedom, plastic crystals usually crystallize in cubic structures (Table 4.2). It is significant that cubic structures are adopted even when the molecular symmetry is incompatible with the cubic crystal symmetry. For example, t-butyl chloride in the plastic crystalline state has a fee structure even though the isolated molecule has a three-fold rotation axis which is incompatible with the cubic structure. Such apparent discrepancies between the lattice symmetry and molecular symmetry provide clear indications of the rotational disorder in the plastic crystalline state. It should, however, be remarked that molecular rotation in plastic crystals is rarely free rather it appears that there is more than one minimum potential energy configuration which allows the molecules to tumble rapidly from one orientation to another, the different orientations being random in the plastic crystal. [Pg.207]

Benzene forms a rotationally disordered structure on the reconstructed (100) platinum surface. However, the work function changes with increasing surface coverage are similar to that of benzene on the (111) crystal face. [Pg.104]

Obviously, if R is large enough to affect the packing of tbe molecule in the crystal then tbe possibility of rotational disorder does not exist. [Pg.52]

There are four independent molecules in the crystal of205 at 138 K two of them show rotational disorder about their central bonds3 8. Another phase formed on cooling consists of twinned crystals, which cannot be used for a structure determination318. Approximate Z)3h sysmmetry and bond lengths of about 1.60 and 1.53 A (corrected for the large thermal motion) in the ordered molecules at 138 K correspond to those in the gas phase. [Pg.204]

Polyoxybenzoate is a stiff chain, lyotropic liquid crystalline material, as was discussed on the basis of its copolymers with ethylene terephthalate (see Sect. 5.1.4). The crystal structure of the homopolymer polyoxybenzoate was shown by Lieser 157) to have a high temperature phase III, described as liquid crystalline. X-ray and electron diffraction data on single crystals suggested that reversible conformational disorder is introduced, i.e. a condis crystal exists. Phase III, which is stable above about 560 K, has hexagonal symmetry and shows an 11 % lower density than the low temperature phases I and II. It is also possible to find sometimes the rotational disorder at low temperature in crystals grown during polymerization (CD-glass). [Pg.47]

This intermolecular potential for ADN ionic crystal has further been developed to describe the lowest phase of ammonium nitrate (phase V) [150]. The intermolecular potential contains similar potential terms as for the ADN crystal. This potential was extended to include intramolecular potential terms for bond stretches, bond bending and torsional motions. The corresponding set of force constants used in the intramolecular part of the potential was parameterized based on the ab initio calculated vibrational frequencies of the isolated ammonium and nitrate ions. The temperature dependence of the structural parameters indicate that experimental unit cell dimensions can be well reproduced, with little translational and rotational disorder of the ions in the crystal over the temperature range 4.2-250 K. Moreover, the anisotropic expansion of the lattice dimensions, predominantly along a and b axes were also found in agreement with experimental data. These were interpreted as being due to the out-of-plane motions of the nitrate ions which are positions perpendicular on both these axes. [Pg.165]

Crystals of most polar lipids can swell in the presence of water. The corresponding phases, gel-phases, with lamellarly packed lipid, and water layers, are sometimes thermodynamically stable (Larsson, 1994, p. 41). Also, the hydrocarbon chain packing of gel-phases usually show some axial rotational disorder. The alkyl chain cross-sectional area is close to 20 A2 in a plane perpendicular... [Pg.34]

Filamentous viruses have been studied mostly by fiber diffraction (Namba et al., 1989). Fibers can be considered to be crystals in which there is rotational disorder about the helical axis. This has the effect of smearing the discrete spots of crystalline diffraction into layer lines. There is a resulting loss of information, but sufficient experimental observations can be made for highly symmetric virus structures so that a unique high-resolution structure is obtainable (Makowski, 1991). [Pg.128]

The NOWF7 complex is simple cubic and must be a plastic crystal, the WF7 being rotationally disordered. The (NO)2WFs salt is isomorphous with (NOljReFs... [Pg.239]

Calamitic phases are essentially defined as a set of mesophases that occur between the breakdown of the long-range periodic, translational ordering of the crystal and the loss of long range orientational order at the transition to the isotropic liquid. In this context six mesophases exist the nematic phase and five smectic phases labelled A, B, C, F and I. Other closely related soft crystal phases, in which the molecules have long-range periodic order but are themselves rotationally disordered, also exist in concert with liquid crystal phases. This second set of mesophases are labelled E, J, G, H, and K, and are essentially the crystal versions of the... [Pg.472]


See other pages where Crystals rotational disorder is mentioned: [Pg.2549]    [Pg.4]    [Pg.35]    [Pg.120]    [Pg.96]    [Pg.84]    [Pg.183]    [Pg.62]    [Pg.1074]    [Pg.797]    [Pg.296]    [Pg.301]    [Pg.88]    [Pg.18]    [Pg.93]    [Pg.88]    [Pg.165]    [Pg.34]    [Pg.309]    [Pg.653]    [Pg.149]    [Pg.151]    [Pg.289]    [Pg.290]    [Pg.293]    [Pg.797]    [Pg.90]    [Pg.93]    [Pg.652]    [Pg.663]    [Pg.664]    [Pg.667]    [Pg.787]    [Pg.203]    [Pg.212]    [Pg.1031]    [Pg.591]    [Pg.202]   
See also in sourсe #XX -- [ Pg.466 ]




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Crystal disorder

Rotational disorder

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