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Framework, polarity

In this framework, polarization of an ion leads to movement of the center of charge as charge density is redistributed. In some applications, it may be advantageous to work in an ion-fixed coordinate system and track the dipole moment as an indicator of the extent of polarization, as has been done [182]. But an increase in the dipole moment in such a fixed coordinate system does not make the ion more polar , it is simply an artifact of the choice of coordinate. [Pg.103]

An, H., Xiao, D., Wang, E. et al. (2005) Open-framework polar compounds synthesis and characterization of rare-earth polyoxometalates (C6NO2H5)2[Ln(H2O)5(CrMo6H6O24)] 0.5H2O (Ln = Ce and La). European Journal of Inorganic Chemistry, 854-859. [Pg.226]

The binding of T1 and Pb to framework oxygen may be partially covalent and should become more energetic as framework polarity increases (chab-azite < Y < X < A). The ratios in column 4 of Table V increase in this order. The effect considered is present in the other heats—e.g., qo, qn— as seen in Table III. [Pg.117]

Alternatively, in the gas phase one may be able to tell the direction of polarization in the molecular framework by looking at the intensity distribution among the rotational lines in a high-resolution spectrum. [Pg.1136]

Calculations within tire framework of a reaction coordinate degrees of freedom coupled to a batli of oscillators (solvent) suggest tliat coherent oscillations in the electronic-state populations of an electron-transfer reaction in a polar solvent can be induced by subjecting tire system to a sequence of monocliromatic laser pulses on tire picosecond time scale. The ability to tailor electron transfer by such light fields is an ongoing area of interest [511 (figure C3.2.14). [Pg.2987]

It has to be emphasized that in this framework J is the angular momentum operatoi in ordinary coordinate space (i.e., configuration space) and 0 is a (differential) ordinary angular polar coordinate. [Pg.685]

The contribution Op is due to the polarization of the molecules by electric fields on the adsorbent surface, eg, electric fields between positively charged cations and the negatively charged framework of a zeoflte adsorbent. The attractive iateraction between the iaduced dipole and the electric field is called the polarization contribution. Its magnitude is dependent upon the polarizabiUty d of the molecule and the strength of the electric field F of the adsorbent (4) 4>p =... [Pg.270]

The separation of fmctose from glucose illustrates the interaction between the framework stmcture and the cation (Fig. 5) (50). Ca " is known to form complexes with sugar molecules such as fmctose. Thus, Ca—Y shows a high selectivity for fmctose over glucose. However, Ca—X does not exhibit high selectivity. On the other hand, K—X shows selectivity for glucose over fmctose. This polar nature of faujasites and their unique shape-selective properties, more than the molecular-sieving properties, make them most useful as practical adsorbents. [Pg.293]

The diffusion, location and interactions of guests in zeolite frameworks has been studied by in-situ Raman spectroscopy and Raman microscopy. For example, the location and orientation of crown ethers used as templates in the synthesis of faujasite polymorphs has been studied in the framework they helped to form [4.297]. Polarized Raman spectra of p-nitroaniline molecules adsorbed in the channels of AIPO4-5 molecular sieves revealed their physical state and orientation - molecules within the channels formed either a phase of head-to-tail chains similar to that in the solid crystalline substance, with a characteristic 0J3 band at 1282 cm , or a second phase, which is characterized by a similarly strong band around 1295 cm . This second phase consisted of weakly interacting molecules in a pseudo-quinonoid state similar to that of molten p-nitroaniline [4.298]. [Pg.262]

A five-membered heterocyclic ring packs a relatively large number of polarized bonds into a relatively small molecular space. This provides a convenient framework to which to attach necessary side chains. In some cases, the framework itself is believed to be part of the pharmacophore. [Pg.127]

AF Cr at 118/f, manifests itself in the fact that the longitudinal polarization of the SDW changes to the transversal one. From the standpoint of electronic structure, the nature of such SF transition in chromium is still unclear. Moreover, this transition is unlikely to be explained within the framework of non relativistic treatment, the nonrelativistic electron spectrum being identical for the longitudinal and transversal SDW. [Pg.149]

The muffin-tin potential around each atom in the unit cell has been calculated in the framework of the Local-Spin-Density-Approximation using the ASW method. The ASW method uses the atomic sphere approximation (ASA), i.e. for each atom a sphere radius is chosen such that the sum of the volumes of all the overlapping spheres equals the unit cell volume. The calculation yields the expected ferromagnetic coupling between Cr and Ni. From the self-consistent spin polarized DOS, partial and total magnetic moment per formula unit can be computed. The calculated total magnetic moment is 5.2 pg in agreement with the experimental value (5.3 0.1 e calculations presented here have been performed... [Pg.463]

The general idea of using different orbitals for different spins" seems thus to render an important extension of the entire framework of the independent-particle model. There seem to be essential physical reasons for a comparatively large orbital splitting depending on correlation, since electrons with opposite spins try to avoid each other because of their mutual Coulomb repulsion, and, in systems with unbalanced spins, there may further exist an extra exchange polarization of the type emphasized by Slater. [Pg.313]

Abstract This tutorial shows how fundamental is the role plaid by interferences in many of the physical processes involved in astrophysical signal formating and consequently instmmentation. It is obvious in interferometry. Grating spectroscopy is explained within the same framework as Young experiment, and Fabry-Perot filters are explained as Michelson interferometers.Polarization interferences, used in Lyot filters, are discussed, emphasizing the analogy with echelle gratings. [Pg.11]

The susceptibility or mixing coefficients, pj and pj , depend upon the position of the substituent (indicated by the index, /) with respect to the reaction (or detector) center, the nature of the measurement at this center, and the conditions of solvent and temperature. It has been held that the p/scale of polar effects has wide general applicability (4), holding for substituents bonded to an sp or sp carbon atom (5) and, perhaps, to other elements (6). The or scale, however, has been thought to be more narrowly defined (7), holding with precision only for systems of analogous pi electronic frameworks (i.e., having a dependence on reaction type and conditions, as well as on position of substitution). [Pg.15]

A recent discovery shows that the lone pair electrons of the chlorine atom can also facilitate the formation of NCS frameworks. A novel family of salt-containing, mixed-metal sihcates (CU-14), Ba6Mii4Sii2034Cl3 and Ba6Fe5Sin034Cl3, was synthesized via the BaCl2 salt-inclusion reaction [6 a]. These compounds crystallize in the NCS space group Pmcli (No. 26), adopting one of the 10 polar, non-... [Pg.245]

In order to overcome the optimization process of the (hyper) polarizabilities calculations, we have been led to deeply study the perturbational and variational methods and in particular the variation-perturbation treatment introduced by Hylleras (20) since 1930. We will not develop here the theoretical framework of the recent study of N. El Bakali Kassimi (21). We propose criteria for generating adequate sets of polarization functions necessary to calculate (hyper) polarizabilities. [Pg.270]

The theoretical framework developed above is valid in the electric dipole approximation. In this context, it is assumed that the nonlinear polarization Ps 2a)) is reduced to the electric dipole contribution as given in Eq. (1). This assumption is only valid if the surface susceptibility tensor co, m) is large enough to dwarf the contribution from higher... [Pg.139]


See other pages where Framework, polarity is mentioned: [Pg.53]    [Pg.237]    [Pg.411]    [Pg.106]    [Pg.53]    [Pg.237]    [Pg.411]    [Pg.106]    [Pg.72]    [Pg.252]    [Pg.73]    [Pg.449]    [Pg.57]    [Pg.295]    [Pg.457]    [Pg.462]    [Pg.43]    [Pg.29]    [Pg.29]    [Pg.99]    [Pg.200]    [Pg.44]    [Pg.141]    [Pg.162]    [Pg.244]    [Pg.245]    [Pg.246]    [Pg.168]    [Pg.44]    [Pg.379]    [Pg.439]    [Pg.298]    [Pg.498]    [Pg.129]   
See also in sourсe #XX -- [ Pg.114 ]




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