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Polarisability correlation function

The total electron density is just the sum of the densities for the two types of electron. The exchange-correlation functional is typically different for the two cases, leading to a set of spin-polarised Kohn-Sham equations ... [Pg.149]

It has been shown that with parallel polarisers. the expression for I involves a third correlation function T2—S2) which multiplies cos lij/ and imparts twofold symmetry to the scattering pattern. [Pg.103]

Although the relation between fluorescence depolarisation and rotational Brownian motion was first identified by Perrin and the development of the theoretical background of the time-resolved fluorescence depolarization experiments was made by Jablonski use of the technique was limited until the advent of improved fluorescence decay time measurements some fifteen years i. An alternative, related technique, involving excitation using a continuous polarised light source, provides only the time average of the correlation function (Eq. 18) and as such, is less useful than the time resolved method. Other disadvantages are that the natural decay time of the chromophore must be determined from a sqrarate experiment and it is necessary to alter the viscosity, and/or temperature of the medium, often withun-... [Pg.143]

Fig. 1.3 The Bhatia-Thornton pair-correlation functions rhu(r) (I, J = N, C) [solid dark (black) curves] where the upper, middle and lower pairs of panels show the NN, CC and NC functions, respectively. For each pair, the upper panel gives the function obtained for a polarisable ion model (PIM) with ax = 20 au [20] and the lower panel gives the measured function for glassy ZnCh [15, 16], Each function is broken down into its contributions from rhxx(r) [broken (n 4) curves], rhuxir) [light solid (green) curves] and rhuMO") [solid (blue) curves]. The abscissa for the simulated functions are scaled by 1.98/2.09 to reflect the relative positions of the principal peak in the simulated and measured (k) partial structure factors... Fig. 1.3 The Bhatia-Thornton pair-correlation functions rhu(r) (I, J = N, C) [solid dark (black) curves] where the upper, middle and lower pairs of panels show the NN, CC and NC functions, respectively. For each pair, the upper panel gives the function obtained for a polarisable ion model (PIM) with ax = 20 au [20] and the lower panel gives the measured function for glassy ZnCh [15, 16], Each function is broken down into its contributions from rhxx(r) [broken (n 4) curves], rhuxir) [light solid (green) curves] and rhuMO") [solid (blue) curves]. The abscissa for the simulated functions are scaled by 1.98/2.09 to reflect the relative positions of the principal peak in the simulated and measured (k) partial structure factors...
This model raises the issue of the effective thickness of the electrochemically active portion of the anode structure. Primdahl and Mogensen [20] found no correlation between polarisation effects and electrode thickness down to 20 pm, and in more recent work [26] a depth of 10 pm for the active zone is sustained. Mathematical modelling [29] is in accord with this experimental evidence (Figure 6.11). Beyond that thickness, the cermet can be regarded as a passive contact layer, and in anode-supported intermediate temperature fuel cells, as also having a structural and mechanical function. It is therefore available as a site for fuel reactions such as reforming. Some studies with this as objective have already been reported, such as the incorporation of ruthenium as catalyst [30],... [Pg.163]

CAS SCF calculations were therefore performed with the split valence basis set incremented by a p polarisation function on the hydrogen atoms. Two different sets of active orbitals were considered. The first one was designed to account for the d - n back donation and was therefore restricted to the n type valence orbitals. The three 3d orbitals, which are strongly occupied, were each correlated by two weakly occupied orbitals, owing to the mixed 4d and tt o character of these weakly occupied orbitals. This 3 + 6 set of active orbitals referred to as CAS SCF-6 is populated by 6 electrons. The second set, hereafter referred as CAS SCF-12, took into account both a and n correlation eficcts. Twelve electrons were correlated and... [Pg.59]

Using the measured CHI data of the model compounds we can set up a correlation equation to express the H-bond acidity (a), H-bond basicity (f) and the polarisability-dipolarity (n) parameters by the CHI values obtained on a particular stationary phase with a particular mobile phase. The plot of the database descriptors as a function of the estimated ones based on the measured CHI values can be seen in Figs. 12.20-12.22. The best equations for the estimation of the descriptors are also shown in the figures. It can be seen that the CHI values obtained on Luna C-18 columns with acetonitrile and trifluoroethanol gradients are used for the fi and the ir calculations. The CHI values... [Pg.586]


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See also in sourсe #XX -- [ Pg.212 ]




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Polarisability

Polarisable

Polarisation

Polarisation function

Polariser

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