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Stacking mode

The optimised interlayer distance of a concentric bilayered CNT by density-functional theory treatment was calculated to be 3.39 A [23] compared with the experimental value of 3.4 A [24]. Modification of the electronic structure (especially metallic state) due to the inner tube has been examined for two kinds of models of concentric bilayered CNT, (5, 5)-(10, 10) and (9, 0)-(18, 0), in the framework of the Huckel-type treatment [25]. The stacked layer patterns considered are illustrated in Fig. 8. It has been predicted that metallic property would not change within this stacking mode due to symmetry reason, which is almost similar to the case in the interlayer interaction of two graphene sheets [26]. Moreover, in the three-dimensional graphite, the interlayer distance of which is 3.35 A [27], there is only a slight overlapping (0.03-0.04 eV) of the HO and the LU bands at the Fermi level of a sheet of graphite plane [28,29],... [Pg.47]

They form adducts with Lewis bases in which the phenanthroline is monodentate, PtX2(dimphen)L (L = Me2S, Me2SO, PhNO) [87], c/s-Pt(bipy)Cl2 exists in yellow and red forms, the difference in colour results from different stacking modes in the solid state, with respective Pt-Pt distances of 4.435 and 3.45 A [88]. [Pg.207]

Taken from the three spontaneous symmetry-breaking events leading to this layer structure [formation of layers with long-range orientational order of the director (Sm), tilt of the director from the layer normal (C), and polar orientation of the molecular arrows (P)], we term phases of this type SmCP. All of the complex textures and EO behavior of NOBOW in the B 2 phase can be understood in terms of various stacking modes of SmCP layers as shown in Figure 8.23. [Pg.496]

Fig. 20 Idealized stacking modes of two diphenylcarbene molecules. Two benzene rings, one each from the two carbenes, are always in a superimposable disposition. Fig. 20 Idealized stacking modes of two diphenylcarbene molecules. Two benzene rings, one each from the two carbenes, are always in a superimposable disposition.
Stacked mode Displays the data set in a stacked plot form. Local functional... [Pg.126]

Density mode. Manual, Grid, Cutting Level with the Stacked mode and... [Pg.128]

Particulates packed in reactor beds are subjected to the static pressures of the bed height and thus must be sufficiently strong to resist crushing. Monoliths, particularly when used in a stacked mode, for example, in stationary pollution abatement, must resist crushing axially. For vehicular use, for example, auto exhaust and ozone... [Pg.109]

Quirino JP, Terabe S. On-line concentration of neutral analytes for micellar elec-trokinetic chromatography I. Normal stacking mode. J Chromatogr A 1997 781 119. [Pg.41]

Table I shows examples of the steady-state and time-resolved emission characteristics of [Ru(phen)2(dppz)]2+ upon binding to various DNAs. The time-resolved luminescence of DNA-bound Ru(II) is characterized by a biexponential decay, consistent with the presence of at least two binding modes for the complex (47, 48). Previous photophysical studies conducted with tris(phenanthroline)ruthenium(II) also showed biexponential decays in emission and led to the proposal of two non-covalent binding modes for the complex (i) a surface-bound mode in which the ancillary ligands of the metal complex rest against the minor groove of DNA and (ii) an intercalative stacking mode in which one of the ligands inserts partially between adjacent base pairs in the double helix (36, 37). In contrast, quenching studies using both cationic quenchers such as [Ru(NH3)6]3+ and anionic quenchers such as [Fe(CN)6]4 have indicated that for the dppz complex both binding modes... Table I shows examples of the steady-state and time-resolved emission characteristics of [Ru(phen)2(dppz)]2+ upon binding to various DNAs. The time-resolved luminescence of DNA-bound Ru(II) is characterized by a biexponential decay, consistent with the presence of at least two binding modes for the complex (47, 48). Previous photophysical studies conducted with tris(phenanthroline)ruthenium(II) also showed biexponential decays in emission and led to the proposal of two non-covalent binding modes for the complex (i) a surface-bound mode in which the ancillary ligands of the metal complex rest against the minor groove of DNA and (ii) an intercalative stacking mode in which one of the ligands inserts partially between adjacent base pairs in the double helix (36, 37). In contrast, quenching studies using both cationic quenchers such as [Ru(NH3)6]3+ and anionic quenchers such as [Fe(CN)6]4 have indicated that for the dppz complex both binding modes...
As mentioned earlier, the tendency of the plane of the donor moieties to be nearly perpendicular to the TCNQ plane prohibits formation of the desired stacking mode. A series of naphtho-1,4-dioxin derivatives (75) has been synthesized to obtain more planar molecules of this type (benzene ring as a donor) [123]. These compounds appeared to be strong acceptors and give rise to conducting salts (e.g., Cu derivatives) (J. Y. Becker, M. Hanack, J. Bernstein, and L. Kaufman-Orenstein, unpublished results). [Pg.108]

This finding demonstrated that the presence of segregated stacks is a necessary condition for electrical conductivity. Reflecting the relative stabilities for the two stacking modes noted above, crystals of the red semiconductor form are obtained from a thermodynamic or equilibrium crystallization equimolar solutions of the donor and acceptor in accetonitrile are mixed and allowed to evaporate slowly. On the other hand, crystals of the black form are obtained from a kinetic or non-equilibrium crystallization hot equimolar solutions of the donor and acceptor in (the same) acetonitrile solvent are mixed and cooled rapidly. Some microcrystals of the resulting black powder are then used as seeds to obtain larger crystals of the segregated stack black form. [Pg.190]

The samrated-unsaturated mixed-acid TAGs involving fra r-unsaturated acids have recently been examined with and without the effects of surfactant additives (67, 68). It is notable that p is most stable in PEP (l,3-dipalmitoyl-2-elaidoyl-5M-glycerol). On the other hand, SES (l,3-distearoyl-2-elaidoyl-5 -glycerol) has the most stable form of p. In contrast to the stabilization of p in ESS and SEE, the most stable form of EPP and PEE is p. The mechanisms for the stabilization of the p in PEP, EPP, and PEE remain unknown. It seems that the methyl end stacking mode may be a key factor, although further clarification is needed. [Pg.143]

The dehydration of copper(Il) formate tetrahydrate is a topotactic process [145]. The anhydrous crystalline product of dehydration retains two-dimensional features of the reactant structure but the stacking mode is changed. This structure is different from that obtained by the direct preparation of anhydrous Cu(HCOO)2. [Pg.249]

Most functions such as 2 and /2 have the same functionality as in ID WIN-NMR and have been explained already whilst some are specifically for the manipulation of 2D data. The utmost right column of four buttons can be used to toggle between the different 2D representation modes contour plot, density mode, stacked mode and 3D mode (from top to bottom). The button measures distances in the spectrum window the first point is fixed using a left mouse button click and as the crosshair is moved the distance is displayed in the information bar at the bottom of the window. A right mouse button click releases the fixed point for a new distance measurement. The buttons marked with a frequency scale and f 1 or f2 can be used to toggle the chemical shift scales between ppm, Hz or data points. [Pg.103]

In real structures, the. -symmetry of the M layer with a given pattern of cation ordering may be lower than the ideal one described by the trigonal model as a function of the concrete stacking mode in a polytype this phenomenon is known as desymmetrization (Durovic 1979). A primitive P lattice for the layer occurs in the unique example of anandite-20 (space group Pnmn, Giuseppetti and Tadini 1972, Filut et al. [Pg.126]


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Normal Mode Stacking Coefficients

Shear Mode Stacking Coefficients

Stacking of material phases with respect to normal modes

Stacking of material phases with respect to shear modes

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