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Diffraction patterns, generation

The Malvern particle sizer is one of the most widely used, most effective, simple, and reliable methods commercially available for rapid measurements of ensemble characteristics of a spray. It is able to handle high droplet concentrations. It is easy to use and does not require comprehensive knowledge of its basic principles for operation. The primary advantage of the system is the speed of data acquisition and analysis. In addition, measurements of droplet size distributions can be made at any droplet velocities due to the fact that the diffraction patterns generated by droplets are independent of the... [Pg.427]

Fig. 16. Photographs of the surface plasmon field-enhanced diffraction patterns generated by various PS patterns on Au surfaces (A) parallel lines 40 pm wide, separated by 62.5 pm (B) parallel lines 28 pm wide, separated by 83 pm (C) square grid pattern, bar width 28 pm, grid width 83 pm, [D] hexagonal grid pattern, bar width 8 pm, hexagonal grid width 48 pm. Fig. 16. Photographs of the surface plasmon field-enhanced diffraction patterns generated by various PS patterns on Au surfaces (A) parallel lines 40 pm wide, separated by 62.5 pm (B) parallel lines 28 pm wide, separated by 83 pm (C) square grid pattern, bar width 28 pm, grid width 83 pm, [D] hexagonal grid pattern, bar width 8 pm, hexagonal grid width 48 pm.
For example, the surface self-diffusion coefficient can be measured by etching a periodic surface profile (e.g., sinusoidal) into a single-crystal surface. The amplitude of the profile is measured as a function of time via the intensity distribution of a laser diffraction pattern generated by the profile itself [52]. The self-diffusion coefficient can be evaluated from the change of the profile amplitude A (/) with time as the surface relaxes into its equilibrium surface structure upon heating ... [Pg.342]

XRD (x-ray diffiaction)—a reciprocal-space method of structural analysis that measures the structure of a lattice based on the diffraction pattern generated when x-ray radiation passes through a regular crystal lattice. [Pg.723]

Figure 10.15 Diffraction pattern generated by narrow apertures. Top circular aperture (iris diaphragm) of diameter h bottom slit aperture of width h... Figure 10.15 Diffraction pattern generated by narrow apertures. Top circular aperture (iris diaphragm) of diameter h bottom slit aperture of width h...
At present, SR sources have become so powerful that it has become feasible not only to perform real-time experiments on conventional polymeric systems, but also to perform much more sophisticated experiments on extremely small samples. This includes experiments on a single silk fiber spun by a spider or the changes in the fiber diffraction pattern generated by the fibers in the muscles from a live drosophila fly, which was persuaded to flap its wings in an x-ray beam. [Pg.8101]

In all cases, broad diffuse reflections are observed in the high interface distance range of X-ray powder diffraction patterns. The presence of such diffuse reflection is related to a high-order distortion in the crystal structure. The intensity of the diffuse reflections drops, the closer the valencies of the cations contained in the compound are. Such compounds characterizing by similar type of crystal structure also have approximately the same type of IR absorption spectra [261]. Compounds with rock-salt-type structures with disordered ion distributions display a practically continuous absorption in the range of 900-400 cm 1 (see Fig. 44, curves 1 - 4). However, the transition into a tetragonal phase or cubic modification, characterized by the entry of the ions into certain positions in the compound, generates discrete bands in the IR absorption spectra (see Fig. 44, curves 5 - 8). [Pg.115]

The X-ray powder diffraction pattern of sodium valproate was determined by visual observation of a film obtained with a 143 2 mm Debye-Scherrer Powder Camera (Table IV). An Enraf-Nonius Difractis 601 Generator 38 KV and 18 MA with nikel filtered copper radiation A = 1.5418, was employed (4). [Pg.544]

An example of monotropic behavior consists of the system formed by anhydrous ibuprofen lysinate [41,42], Figure 4.12 shows the DSC thermogram of this compound over the temperature range of 20-200°C, where two different endothermic transitions were noted for the substance (one at 63.7°C and the other at 180.1°C). A second cyclical DSC scan from 25 to 75°C demonstrated that the 64°C endotherm, generated on heating, had a complementary 62°C exotherm, formed on cooling (see Fig. 4.13). The superimposable character of the traces in the thermograms demonstrates that both these processes were reversible, and indicates that the observed transition is associated with an enantiotropic phase interconversion [41]. X-ray powder (XRPD) diffraction patterns acquired at room temperature, 70°C, and... [Pg.91]


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Diffraction patterns

Pattern generators

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