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Ordered molecular systems

Considerable information on molecular interactions and molecular structure can be obtained from studies of ordered materials and samples here the degree of averaging between laboratory and molecular frames of reference is either wholly removed or greatly reduced. There is now a net degree of molecular order in the laboratory frame of reference. As in the case of probe fluorescence [see Equation (11.18)], this intrinsic distribution is conveniently expressed as an expansion in spherical harmonics. [Pg.190]

For a cylindrically symmetric molecular array (no net ordering in the X-Y plane) Q = 0, under these circumstances expanding Equation (11.26) and normalizing to the scalar Tbo( ) 4 ) term, the first four terms of the distribution function have the form [Pg.190]

In an analogous manner to single-photon absorption it is possible to detect molecular order (the (aRg) parameters) by the differeuce in the absorption of Z and X (or Y) polarized light. The absorption of Z and X [Pg.190]

This approach has been widely used to study biological systems, notably to detect tilting motions of myosin domains in muscle fibres. Measurement of the (0 20) order parameter alone does not necessarily yield a complete picture of molecular order, and neglect of higher terms in Equation (11.28) can lead to serious errors. Two-photon dichroism measurements are, however, sensitive to (0 20) and the next term in the expansion (0 40). The absorption strengths for Z and X polarized two-photon absorption are given by [Pg.191]

Two photon dichroism measurements have been used to study the structural properties of highly ordered liquid crystal mesophases from measurements of (020) and (040) it is possible [given a realistic model for Flab(, / )] to predict values of higher terms. Knowledge of (0 20) and [Pg.191]


Crystallinity long has been recognized as one of the characteristics of native cellulosic fibers. Indeed, native cellulose was observed to diffract x-rays, in the manner characteristic of three-dimensionally ordered molecular systems, before the hypothesis of polymeric structure had been proposed by Staudinger (1,2). [Pg.168]

An electrode covered with several molecular layers of dye could be made to adsorb all of the visible light, and obviate the need for the multielectrode stack. Very thick dye layers have tended not to be conductive or highly photoconductive so that their photoelectrochemical efficiencies are no better and perhaps worse than those seen on electrodes modified with very thin dye films. Molecular disorder of the dye appears to be the dominant reason for lack of conductivity in thick films of fluorescein-type, cyanine-type, and phthalocyanine-type dyes (12). It has been shown however that ordered molecular systems (mainly conjugated, highly unsaturated hydrocarbons) have considerable potential as conductive media, and that these ordered systems may be used to chemically modify electrode surfaces (12, 15). [Pg.207]

Fluorescence polarization techniques and ordered molecular systems... [Pg.197]

Bain, A.J. (2002). Time resolved polarized fluorescence studies of ordered molecular systems. In An Introduction to Laser Spectroscopy, Andrews, D.L. and Demidov, A., eds. Chapter 6, pp. 171-210. Kluwer Scientific London. [Pg.197]

Liquid crystal is a state of matter where the molecules are so mobile and a certain anisotropy in motion is involved depending on the inter- and intramolecular forces. This is an origin of softness and sometimes of fluidity of materials. As electronic materials such as semiconductors, one has to consider that the efficient charge transport in ordered molecular systems is ascribed to periodical arrangement of molecules giving a certain intermolecular interaction for strongly coupled electronic states. When the transfer integral of HOMO-HOMO and/or... [Pg.258]

The principal idea behind the CSP approach is to use input from Classical Molecular Dynamics simulations, carried out for the process of interest as a first preliminary step, in order to simplify a quantum mechanical calculation, implemented in a subsequent, second step. This takes advantage of the fact that classical dynamics offers a reasonable description of many properties of molecular systems, in particular of average quantities. More specifically, the method uses classical MD simulations in order to determine effective... [Pg.367]

SAMs are ordered molecular assembHes formed by the adsorption (qv) of an active surfactant on a soHd surface (Fig. 6). This simple process makes SAMs inherently manufacturable and thus technologically attractive for building supedattices and for surface engineering. The order in these two-dimensional systems is produced by a spontaneous chemical synthesis at the interface, as the system approaches equiHbrium. Although the area is not limited to long-chain molecules (112), SAMs of functionalized long-chain hydrocarbons are most frequently used as building blocks of supermolecular stmctures. [Pg.536]

Patterns of ordered molecular islands surrounded by disordered molecules are common in Langmuir layers, where even in zero surface pressure molecules self-organize at the air—water interface. The difference between the two systems is that in SAMs of trichlorosilanes the island is comprised of polymerized surfactants, and therefore the mobihty of individual molecules is restricted. This lack of mobihty is probably the principal reason why SAMs of alkyltrichlorosilanes are less ordered than, for example, fatty acids on AgO, or thiols on gold. The coupling of polymerization and surface anchoring is a primary source of the reproducibihty problems. Small differences in water content and in surface Si—OH group concentration may result in a significant difference in monolayer quahty. Alkyl silanes remain, however, ideal materials for surface modification and functionalization apphcations, eg, as adhesion promoters (166—168) and boundary lubricants (169—171). [Pg.538]

Strkcttire inflkence. The specificity of interphase transfer in the micellar-extraction systems is the independent and cooperative influence of the substrate molecular structure - the first-order molecular connectivity indexes) and hydrophobicity (log P - the distribution coefficient value in the water-octanole system) on its distribution between the water and the surfactant-rich phases. The possibility of substrates distribution and their D-values prediction in the cloud point extraction systems using regressions, which consider the log P and values was shown. Here the specificity of the micellar extraction is determined by the appearance of the host-guest phenomenon at molecular level and the high level of stmctural organization of the micellar phase itself. [Pg.268]

On the basis of data obtained the possibility of substrates distribution and their D-values prediction using the regressions which consider the hydrophobicity and stmcture of amines was investigated. The hydrophobicity of amines was estimated by the distribution coefficient value in the water-octanole system (Ig P). The molecular structure of aromatic amines was characterized by the first-order molecular connectivity indexes ( x)- H was shown the independent and cooperative influence of the Ig P and parameters of amines on their distribution. Evidently, this fact demonstrates the host-guest phenomenon which is inherent to the organized media. The obtained in the research data were used for optimization of the conditions of micellar-extraction preconcentrating of metal ions with amines into the NS-rich phase with the following determination by atomic-absorption method. [Pg.276]

Dynamical simulations monitor time-dependent processes in molecular systems in order to smdy their structural, dynamic, and thennodynamic properties by numerically solving an equation of motion, which is the formulation of the rules that govern the motion executed by the molecule. That is, molecular dynamics (MD) provides information about the time dependence and magnitude of fluctuations in both positions and velocities, whereas the Monte Carlo approach provides mainly positional information and gives only little information on time dependence. [Pg.39]

Order 0 minimization methods do not take the slope or the curvature properties of the energy surface into account. As a result, such methods are crude and can be used only with very simple energy surfaces, i.e., surfaces with a small number of local minima and monotonic behavior away from the minima. These methods are rarely used for macro-molecular systems. [Pg.78]

Once the model of a ligand-receptor complex is built, its stability should be evaluated. Simple molecular mechanics optimization of the putative ligand-receptor complex leads only to the identification of the closest local minimum. However, molecular mechanics optimization of molecules lacks two crucial properties of real molecular systems temperature and, consequently, motion. Molecular dynamics studies the time-dependent evolution of coordinates of complex multimolecular systems as a function of inter- and intramolecular interactions (see Chapter 3). Because simulations are usually performed at nonnal temperature (—300 K), relatively low energy barriers, on the order of kT (0.6 kcal), can... [Pg.361]

Now the problem being addressed is to quantify the effect of quantum fluctuation on the orientational ordering in this molecular system. [Pg.112]

Such large calculations wUl take on the order of one to a few days, depending on the exact molecular system and computer system. However, even larger calculations are possible, provided you are willing to allocate the necessary CPU resources to them. What constitutes a practical calculation is ultimately a matter of individual judgement. Well look at how resource requirements vary with molecule size and calculation type at appropriate points in the course of this work. [Pg.6]

The following table summarizes some recommended research-level model chemistries for predicting total energies for molecular systems of various sizes (the details of the reasons behind these choices will unfold along with the chapters in this part of the book), arranged in order of increasing computational cost ... [Pg.96]

The Dirac operator incorporates relativistic effects for the kinetic energy. In order to describe atomic and molecular systems, the potential energy operator must also be modified. In non-relativistic theory the potential energy is given by the Coulomb operator. [Pg.210]

We study three different approximations for removing unlinked diagrams in EOM-CC and show that these models provide second-order properties and transition probabilities that are close to those provided by CCLR in isolated molecular systems, but in a more convenient computational structure. [Pg.151]


See other pages where Ordered molecular systems is mentioned: [Pg.190]    [Pg.162]    [Pg.105]    [Pg.266]    [Pg.190]    [Pg.162]    [Pg.105]    [Pg.266]    [Pg.87]    [Pg.87]    [Pg.40]    [Pg.226]    [Pg.358]    [Pg.71]    [Pg.237]    [Pg.55]    [Pg.212]    [Pg.79]    [Pg.148]    [Pg.41]    [Pg.71]    [Pg.237]    [Pg.265]    [Pg.199]    [Pg.1]    [Pg.415]    [Pg.148]    [Pg.129]    [Pg.146]    [Pg.52]    [Pg.164]   


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