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Molecular scattering curve

Fig. 19. Radial distribution functions f(r) and f(r) derived from the molecular scattering curves for gaseous CHJ2 at different delay times between the photodissociating fs laser pulse (at A = 310 nm) and the ps electron pulse (pulse-width 15 ps). The corresponding theoretical f(r) curve for CH2I2 is superimposed on the — 20-ps data set. The changes observed are at r = ca. 2.0 and 3.5 A corresponding to the C—I and I—I internuclear spacings, respectively [reproduced with permission from (96), p. 161],... Fig. 19. Radial distribution functions f(r) and f(r) derived from the molecular scattering curves for gaseous CHJ2 at different delay times between the photodissociating fs laser pulse (at A = 310 nm) and the ps electron pulse (pulse-width 15 ps). The corresponding theoretical f(r) curve for CH2I2 is superimposed on the — 20-ps data set. The changes observed are at r = ca. 2.0 and 3.5 A corresponding to the C—I and I—I internuclear spacings, respectively [reproduced with permission from (96), p. 161],...
FIGURE 7.6 The molecular scattering curves associated with diffraction from closed shells of (CsI) Cs+ clusters. Bragg scattering peaks for bulk Csl are shown at the top of the figure. [Pg.178]

In practice, p is adjusted in the numerical calculations until the calculated Mapp agrees with the measured one. All other quantities, for instance the molecular-weight dependence of (S2)z, or the shape of the scattering curve, and the whole dynamic scattering behaviour, are now fully determined if the effective bond length is known. [Pg.50]

Nearly all theories to date predict that IETS intensities should be proportional to n, the surface density of molecular scatterers. Langan and Hansma (21) used radioactively labeled chemicals to measure a surface concentration vs solution concentration curve ( Fig. 10 ) for benzoic acid on alumina using the liquid doping technique. The dashed line in Fig. 10 is a 2 parameter fit to the data using a simple statistical mechanical model by Cederberg and Kirtley (35). This model matched the free energy of the molecule on the surface with that in solution. The two parameters in this model were the surface density of binding sites ( 10" A )... [Pg.231]

Figure 3. Angular scattering for Latex 42BRD47 at pH 3.64 for excess Wv scattering. Upper curve is from latex particles and lower curve is from residual molecular scattering in excess of the solvent. Figure 3. Angular scattering for Latex 42BRD47 at pH 3.64 for excess Wv scattering. Upper curve is from latex particles and lower curve is from residual molecular scattering in excess of the solvent.
Once the effective atomic number of the scattering species is known, for example using the HETRA method described in Section 2.3.1., it is possible to account for the IAM component of scattering in the diffraction profile, allowing the molecular interference function to be extracted. For this purpose, a universal free atom scattering plot, which can be extrapolated to non-integral values of the effective atomic number, is needed. The IAM total scattering curves for the elements with 6 < Z < 9 normalized to unit l/e... [Pg.212]

Fig. 3. The molecular scattering intensity pattern for the Me3N-GaH3 molecule related by Fourier transformation to the corresponding radial distribution curve. The difference between the observed and calculated radial distribution curves is also shown (adapted from Ref. 51). Fig. 3. The molecular scattering intensity pattern for the Me3N-GaH3 molecule related by Fourier transformation to the corresponding radial distribution curve. The difference between the observed and calculated radial distribution curves is also shown (adapted from Ref. 51).
One way to 3D molecular descriptors is deriving them from molecular transforms, which are generalized scattering functions used to create theoretical scattering curves in electron diffraction studies. A molecular transform serves as the functional basis for deriving the relationship between a known molecular structure and x-ray and electron diffraction data. The general molecular transform is... [Pg.77]

The x-ray approach has few peers as regards nondestructive definition of structure at the secondary level. Although microscopy is more direct, the preparative problems and necessary subjectiveness in the interpretation of photo- and electron micrographs make absolutely necessary the joint use of the two techniques. The work of Preston and his school on the structural polysaccharides of plants is a good example of how the two techniques should be combined. A rough textural model of the molecular architecture of a cell wall of a plant is capable of quantitative and detailed definition by means of the complete, wide and small angle, x-ray scattering curve. This application is, perhaps, one of the potentially more fruitful, areas of future study it is part of the major, solid-state... [Pg.430]


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Molecular scattering

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