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Molecular orientation at the

Molecular orientation at the surface may also be important. A molecule orients planarly when deposited on a solid surface. Molecular strands prefer to be parallel to the surface their probability of being oriented normal to the surface is very low. Several mechanisms can cause this orientation (1) Surface-active sites may favor entire chain segments to interact with the surface. (2) The... [Pg.227]

L. M. Folan and S. Arnold, Determination of molecular orientation at the surface of an aerosol particle by morphology-dependent photoselection, Opt. Lett. 13, 1-3 (1988). [Pg.384]

Figure 10.5. Adsorbate molecular orientation at the electrode surface d) nicotinic acid (Z ) benzoic acid (c) 2,6-pyridinedicarboxylic acid. (From Ref. 12, with permission from the American Chemical Society.)... Figure 10.5. Adsorbate molecular orientation at the electrode surface d) nicotinic acid (Z ) benzoic acid (c) 2,6-pyridinedicarboxylic acid. (From Ref. 12, with permission from the American Chemical Society.)...
Figure 11.42 (Top) Structures of spider web dendritic amphiphiles. (Bottom) Schematic representation of the molecular orientation at the water-air interface. Reprinted from Ariga et al. (2004). Copyright 2004 American Chemical Society. Figure 11.42 (Top) Structures of spider web dendritic amphiphiles. (Bottom) Schematic representation of the molecular orientation at the water-air interface. Reprinted from Ariga et al. (2004). Copyright 2004 American Chemical Society.
In the Langmuir derivation the adsorbed molecules are allowed to interact with the adsorbent but not with each other The adsorbed layer is assumed to be ideal. This necessarily limits adsorption to a monolayer. Once the surface is covered with adsorbed molecules, it has no further influence on the system. The assumption that adsorption is limited to monolayer formation was explicitly made in writing Equations (72) and (73) for the saturation value of the ordinate. Ii is an experimental fact, however, that adsorption frequently proceeds to an extent that exceeds the monolayer capacity of the surface for any plausible molecular orientation at the surface. That is, if monolayer coverage is postulated, the apparent area per molecule is only a small fraction of any likely projected area of the actual molecules. In this case the assumption that adsorption is limited to the monolayer fails to apply. A model based on multilayer adsorption is indicated in this situation. This is easier to handle in the case of gas adsorption, so we defer until Chapter 9 a discussion of multilayer adsorption. [Pg.337]

The bimolecular lipid membrane (BLM) produced in aqueous solution described in this paper is of considerable interest for two main reasons. First, the BLM is a new type of interfacial film of ultrathinness. The limiting thickness of BLM is 40-130 A. as estimated from various measurements. The values obtained by optical methods are probably most reliable, indicating that the thickness of the BLM is equal to about twice the length of the lipid molecules. The environment in which the BLM is formed and the molecular orientation at the biface lends itself as a promising tool in understanding some outstanding problems in colloid and interfacial chemistry such as Van der Waals attraction and... [Pg.120]

Figure 9 Probabilities for rotational-vibrational interconversion in the scattering of H2 as a function of the molecular orientation at the classical turning point [71]. Figure 9 Probabilities for rotational-vibrational interconversion in the scattering of H2 as a function of the molecular orientation at the classical turning point [71].
Since the scope of this article is purely theoretical, we just outline below the state of the experimental situation. The ideal experiment in Chemical Dynamics would be that in which starting with reactants in definite intramolecular quantum-states and running towards each other in a definite way (relative velocity and orbital angular momentum) the distribution of the products over the various intramolecular quantum-states and the state of the relative motion (direction and velocity) would be measured. Such an experiment would show whether there is a preferential molecular orientation at the heart of the collision, what the lifetime of the intermediate complex is, how the excess energy is distributed over the various degrees of freedom of... [Pg.4]

The electromagnetic field enhancement provided by nanostructure plasmonics is the key factor to manipulate the quantum efficiency. However, as it is illustrated in the unified theory of enhancement, since both the radiative and non-radiative rates of the molecular systems are affected by proximity of the nanostructure, the tuning has to be done on a case by case basis. In addition, there are factors due to molecule-metal interactions and molecular orientation at the surface causing effects that are much more molecule dependent and as are much more difficult to predict. Given the fact that fluorescence cross sections are the one of the highest in optical spectroscopy the analytical horizon of SEF or MEF is enormous, in particular in the expanding field of nano-bio science. [Pg.86]

In centrosymmetric molecules, HRS gains intensity via Herzberg-Teller term (the first vibronic B-term), indicating that IR-active modes and silent modes are enhanced. In the case of non-centrosymmetric molecules, however, Franck-Condon mechanism (A-term) dominantly contributes to the enhancement. Moreover, the mutual exclusive rules between HRS and RS are broken, and hence, some of RS-active modes selectively appear in the spectra. In the case of plasmonic enhancement, the spectral appearance is more sensitive to molecular orientations at the metal surface because of the surface selection rules [25]. [Pg.103]

The magnitude of surface tension, y, has also been calculated from statistical theory and molecular orientations at the free surface in nematic liquid crystals. ... [Pg.96]

As we stated at the beginning of this section, most of the work in this area has focused upon the study of molecular orientation at the liquid-vapor interface and how this is affected by details of the intermolecular forces. Thompson and Gubbins have carried out molecular dynamics simulations of the vapor-liquid interface for homonuclear 12-6 diatomic molecules and for such molecules with point-charge quadrupoles. They find that in the case of the nonpolar molecules, there is a tendency for molecules in the liquid to align perpendicular to the surface and those in the vapor to align parallel to the surface. The addition of a quadrupole to the 12-6 diatomic " reverses this effect. A study of the vapor-liquid interface for an interaction site model of -octance leads to similar conclusions as for the nonpolar diatomic. These effects are reproduced qualitatively by all the theoretical approximations, with the exception of the influence of the quadrupole, which can only be predicted at first order within the context of the perturbation theory based upon division of the Mayer function Eq. (3.5.2). [Pg.537]

A type of angle-dependent x-ray photoemission spectroscopy was used to investigate the molecular orientation at the surface of sulfonated polystyrene as a function of reaction depth. A model based on these measurements indicates that at a critical sulfonation depth the aliphatic hydrocarbon backbone becomes exposed preferentially at the surface. These results are consistent with surface energy and tribo-electric charging measurements, which also reveal the effects of associative interactions in the form of conversion dependencies. [Pg.289]

In summary, through the use of a simple type of XPS(0), the molecular orientation at the surface of sulfonated PS films has been determined. In the more sulfonated films the sulfur and oxygen atoms reside preferentially below the surface, as their respective XPS(6) core-level signals decrease with increasing 0 faster than the matrix C(l ) signal. These results are corroborated by surface energy measurements that also indicate that the accessibility of the sulfonate groups depends on associative interactions in the solid. In particular, it appears that a preferential... [Pg.300]

Molecular orientation at the surface of biomaterials has received increased attention in recent years. Again, as for surface contamination, the driving force for the surface reorientation observed often can be explained in thermodynamic terms as a mechanism for reducing the interfacial energy. [Pg.17]

The spectrum of CO on Pt(poly) is shown in Fig. 5.9 [2]. This spectrum is significant as it demonstrated the possibility of obtaining SFG from electrochemical interfaces with very good S/N ratio. Further, the results are comparable to those obtained using infrared spectroscopy. In the same report, Tadjeddine and coworkers also presented potential-dependent SFG spectra of CN" on a Pt electrode. Since the SFG process is coherent, the phase of each resonance is present in the spectra. As noted earlier, phase information can be used to determine molecular orientation at the surface. For example, the phase information can determine whether CN is surface coordinated through the nitrogen or the carbon atom [24]. [Pg.177]

The solubility parameter of the polymer is calculated from bond energies. The sensitivity to ESC is affected by the polymer molecular weight and by molecular orientation at the surface of injection mouldings. [Pg.317]

The area occupied on the water surface by a single alkanoic acid molecule within the monolayer is about 0.2 nm. This value corresponds closely to the cross-sectional area of the carboxyl end of the molecule as shown in Figure 12.10c. This implies that the floating film is indeed monomolecular in dimension. Snch measurements have been made for a huge number of different materials, providing insight into the relationships between the detailed molecular structure and the molecular orientation at the air-water interface. [Pg.383]

FIGURE 8.2. Dynamic smface tension in pure liquids (a) for a liquid of isotropic molecular shape, dynamic surface tension effects are controlled by the rate of diffusion of molecules from the bulk to the new surface (b) in polar or anisotropic liquids, the situation may be further complicated by the question of molecular orientation at the surface. [Pg.145]

An additional comphcation in evaluating dynamic surface tensions may arise in terms of molecular orientation at the surface. For a symmetric molecule, orientation will not be a problem however, for many systems, especially... [Pg.146]

The strength of weld lines in injection-molded articles is generally weaker than that of the bulk. This is due to the incomplete entanglement of polymer chains at the two impinging fountain flow fronts in the mold cavity. When the two flow fronts meet in the cold cavity, the molecular orientation at the interface remains parallel to the weld line as evidenced by the frozen-in molecular orientation found in the molded article under proper injection-molding conditions... [Pg.256]

Structure of thermotropic liquid crystals is rather well understood. There are three main structural types nematic, cholesteric, and smectic. In nematic liquid crystals molecules are aligned approximately in the same direction, but positionally molecules are disordered. An axis of preferable molecular orientation is called a director. More precisely, the director is defined as a unit vector n(r) that is parallel to the molecular orientation at the point r. If we use the long axis of the molecules as a reference and denote it as k, the microscopic scalar order parameter 5 is defined [16,17] as follow ... [Pg.142]

Hi) Detection of surface chemical composition and reactivity due to the unique molecular orientation at the interface. [Pg.444]


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Molecular orientation

Molecular orientation at the interface

Molecular orientation at the solid-liquid interface

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