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Structure discrete molecular

In addition to constitution and configuration, there is a third important level of structure, that of conformation. Conformations are discrete molecular arrangements that differ in spatial arrangement as a result of facile rotations about single bonds. Usually, conformers are in thermal equilibrium and cannot be separated. The subject of conformational interconversion will be discussed in detail in Chapter 3. A special case of stereoisomerism arises when rotation about single bonds is sufficiently restricted by steric or other factors that- the different conformations can be separated. The term atropisomer is applied to stereoisomers that result fk m restricted bond rotation. ... [Pg.76]

Over the years there have been many attempts to simulate the behaviour of viscoelastic materials. This has been aimed at (i) facilitating analysis of the behaviour of plastic products, (ii) assisting with extrapolation and interpolation of experimental data and (iii) reducing the need for extensive, time-consuming creep tests. The most successful of the mathematical models have been based on spring and dashpot elements to represent, respectively, the elastic and viscous responses of plastic materials. Although there are no discrete molecular structures which behave like the individual elements of the models, nevertheless... [Pg.84]

Structural classifications of oxides recognize discrete molecular species and structures which are polymeric in one or more dimensions leading to chains, layers, and ultimately, to three-dimensional networks. Some typical examples are in Table 14.14 structural details are given elsewhere under each individual element. The type of structure adopted in any particular case depends (obviously) not only on the... [Pg.641]

MD simulations also provide an opportunity to detect the structure of molecularly thin films. The most commonly known ordering structure induced by the confinement, the layering, has been revealed that the molecules are packed layer by layer within the film and the atoms would concentrate on several discrete positions. This has been confirmed in the simulations of liquid decane [29]. The density profile of unite atoms obtained from the simulations is given in Fig. 12 where two sharp density peaks appear at the locations near the walls, as a result of adsorption, while in the middle of the film smaller but obvious peaks can be observed on the density profile. The distance between the layers is largely identical to the thickness of the linear chain of decane molecules, which manifests the layered packing of molecules. [Pg.86]

In this chapter, we briefly discuss the theoretical background of polarized x-ray absorption spectroscopy (PXAS). Many of the recent applications of synchrotron radiation to polarized absorption edge structure and to EXAFS are discussed, with particular emphasis being given to the study of discrete molecular systems. We present here some indication of the potential applications of PXAS to systems of chemical and biological interest. [Pg.413]

The Gouy-Chapman theory treats the electrolyte as consisting of point ions in a dielectric continuum. This is reasonable when the concentration of the ions is low, and the space charge is so far from the metal surface that the discrete molecular nature of the solution is not important. This is not true at higher electrolyte concentrations, and better models must be used in this case. Improvements on the Gouy-Chapman theory should explain the origin of the Helmholtz capacity. In the last section we have seen that the metal makes a contribution to the Helmholtz capacity other contributions are expected to arise from the molecular structure of the solution. [Pg.238]

The level of accuracy that can be achieved by these different methods may be viewed as somewhat remarkable, given the approximations that are involved. For relatively small organic molecules, for instance, the calculated AGsoivation is now usually within less than 1 kcal/mole of the experimental value, often considerably less. Appropriate parametrization is of key importance. Applications to biological systems pose greater problems, due to the size and complexity of the molecules,66 156 159 161 and require the use of semiempirical rather than ab initio quantum-mechanical methods. In terms of computational expense, continuum models have the advantage over discrete molecular ones, but the latter are better able to describe solvent structure and handle first-solvation-shell effects. [Pg.59]

For ionic as for molecular solutes (Section III.3), some studies have applied the discrete molecular model to the solvent in the immediate environment of the solute, and treated the remainder as a continuum. This can in principle help to deal with the problem of inner-shell structure as well as that of long-range effects. Thus Straatsma and Berendsen used the Bom equation to correct simulation-obtained free energies of hydration for six monatomic ions.174 This helped in some instances but not in others. [Pg.67]

As already pointed out, recent advances in the synthesis and structural characterisation of discrete molecular alumoxanes have lately been the subject of review [8]. While developments in the crystallisation and structural... [Pg.69]

Control of Permeability through Intramolecular Channels. Control of membrane permeability is effected in a most sophisticated and efficient manner in ligand-gated ion channels having discrete molecular entities with well-defined channel structures. Cyclodextrin derivatives of type 41 and 53 are interesting... [Pg.242]

When an atom or molecule is adsorbed on a surface new electronic states are formed due to the bonding to the surface. The nature of the surface chemical bond will determine the properties and reactivity of the adsorbed molecule. In the case of physisorption, the bond is rather weak, of the order of 0.3 eV. The overlap of the wave functions of the molecule and the substrate is rather small and no major change in the electronic structure is usually observed. On the contrary, when the interaction energy is substantially higher, there are rearrangements of the valence levels of the molecule, a process often denoted chemisorption. The discrete molecular orbitals interact with the substrate to produce a new set of electronic levels, which are usually broadened and shifted with respect to the gas phase species. In some cases completely new electronic levels emerge which have no resemblance to the original orbitals of the free molecule. [Pg.57]

The ylide complex Pt[Au CH2P(S)Ph2 2]2 380 exhibits a structure similar to that of the analogous Pb derivative (see Section 2.4.4), with a linear Au-Pt-Au skeleton, transannular d8-d10 Au-Pt interaction of3.034(1) A, and extended one-dimensional chain polymer formation through weak intermolecular d10-d10 interactions [Au-Au 3.246 A] [34]. Oxidation of 380 or adduct formation resulted in discrete molecular... [Pg.257]

For the above reasons, organolithium compounds and complexes have been termed supramolecules [ complex molecules held together by noncovalent bonds (4) ]. What we have here are ionically bonded (at least as far as the central metal-organic anion linkages are concerned) yet often discrete molecular species. Most of their physical properties reflect their limited aggregation and their organic peripheries. These points are stressed in Fig. 3, a schematic presentation of the major structural types of uncomplexed organic lithium compounds. [Pg.53]

The terms molecular and non-molecular describe geometrical structure, namely the presence or absence of discrete polyatomic units separated by non-bonding boundaries. The infinite linkages characteristic of structural non-molecularity can be classified as one-, two- or three-dimensional the first two types correspond to chain and layer structures, respectively. Structurally molecular complexes may have any charge or size. [Pg.138]

In the Cu-ncyanate complexes the cyanate ligand can be bonded in the terminal N mode321 as well as in the 1,1-ft bridging form.227 The structure of Ag(NCO)305 consists of an infinite —N—Ag— N—Ag— chain as a result of 1,1-ft N-bonding. In contrast [NBudJAgfNCC) ]306 has a discrete molecular structure containing discrete OCN—Ag—NCO units. [Pg.234]


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