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Crystal facets

Interesting pattern formations also occur in surfactants spreading on water due to a hydrodynamic instability [52]. The spreading velocity from a crystal may vary with direction, depending on the contour and crystal facet. There may be sufficient imbalance to cause the solid particle to move around rapidly, as does camphor when placed on a clean water surface. The many such effects have been reviewed by Stemling and Scriven [53]. [Pg.112]

As with any system, there are complications in the details. The CO sticking probability is high and constant until a 0 of about 0.5, but then drops rapidly [306a]. Practical catalysts often consist of nanometer size particles supported on an oxide such as alumina or silica. Different crystal facets behave differently and RAIRS spectroscopy reveals that CO may adsorb with various kinds of bonding and on various kinds of sites (three-fold hollow, bridging, linear) [307]. See Ref 309 for a discussion of some debates on the matter. In the case of Pd crystallites on a-Al203, it is proposed that CO impinging on the support... [Pg.736]

The most characteristic and unique property of crystalline solids is however, neither the shape of their crystals nor the relative size of the crystal faces, but the angle between any pair of crystal facets. For any substance, the angle between the crystal facets is constant and invariable, regardless of the overall shape or size of the crystals. Under some circumstances a substance may form short, wide crystals, while under others, the... [Pg.103]

What information can be obtained from NMR about the interfaces or surfaces in such systems, including crystal facets/surface planes How do NMR parameters vary as a function of distance from the surface ... [Pg.290]

Here /, is the surface energy of the crystal surface i. The equilibrium shape of a crystal is thus a polyhedron where the area of the crystal facets is inversely proportional to their surface energy. Hence the largest facets are those with the lowest surface energy. [Pg.167]

Figure 7.10 The principle of field ionization. Left the potential for a helium atom near a metal without field, and (right) in the presence of an electric field of strength F (V/cm). Field ionization by electron tunneling becomes possible when the He Is level (ionization potential /) is above the Fermi level of the metal. Tunneling increases when the He atom is closer to the surface. This, however, requires high local fields, which are present at the edges of crystal facets or at adsorbed atoms. Figure 7.10 The principle of field ionization. Left the potential for a helium atom near a metal without field, and (right) in the presence of an electric field of strength F (V/cm). Field ionization by electron tunneling becomes possible when the He Is level (ionization potential /) is above the Fermi level of the metal. Tunneling increases when the He atom is closer to the surface. This, however, requires high local fields, which are present at the edges of crystal facets or at adsorbed atoms.
To test this hypothesis beyond CO adsorption on Pt(l 11), Weaver et al. compared CO and NO stretching frequencies on multiple crystal facets of Pt, Rh, Pd, and Ir in UHV and electrochemical environments.58 With the exception of NO and CO on Pt(l 11), in which both unsolvated and D20 solvated environments were examined, only unsolvated UHV environments were considered. In this comparison, the same... [Pg.320]

When working with metal electrodes, the energy of the electrons in the metal is lower than the vacuum level by the work function of the metal, which tends to be 3-5 eV. Work functions of some materials relevant to LED devices are collected in Table 10.2 [11]. The work function can vary depending upon the crystal facet from which emission is measured (or if the metal is amorphous), and sample preparation details. The photoelectric (PE) effect is exploited in XPS (ESCA) or UPS to measure the work function. It is very critical to realize that, in these experiments, what is measured is the energy required to remove an electron to a point just outside the surface of the solid, not to infinity. At this range, the dipolar forces at the surface are still active, and one can learn about surface dipoles in the material. [Pg.630]

Work Functions of Some Materials Relevant to LED Devices. The Work Function Can Vary Depending upon the Crystal Facet from Which Emission Is Measured, and Sample Preparation Details... [Pg.631]

The problem of the variation in the surface energies of various crystal facets can be attacked from several points of view. Bravais first noted that those planes of a crystal which were most densely packed and were also separated most distantly from the neighbouring parallel plane were those which appeared most frequently in crystals he noted also that a closely packed surface was usually associated with a wide interplanar distance and vice versa. Later Willard Gibbs indicated that the most stable planes on a growing crystal were those possessing the least interfacial surface energy. [Pg.124]

Not only must we consider the crystal facets themselves from this point of view as differentiated in their respective surface energies but if we consider the comers and edges common to two crystal surfaces we note again that the cohesion of atoms so situated in respect to the mother crystal is far weaker than that for atoms actually in one of the surfaces and we should anticipate that the adhesional energy of such atoms, or the external field, will be greater for these edges and comers than for the planes. A crystal... [Pg.126]

FIGURE 5.2 (a) Experimental (filled circles) wavelength tuning curve and accessible Raman freqnencies as a fnnction of the crystal temperatnre. The solid curves are a result of the calculations. (b) OPO output power versus pump power at the crystal facet (c) and (d) show the typical signal pulse spectrum and autocorrelation trace at the OPO cavity detuning of minus 36 (xm, respectively. [Pg.105]

Couple reaction, 1169 Cryostat, cooling by. 1121 Crystal facets... [Pg.33]

Even isopropanol and other secondary alcohols cannot superimpose on the surface during dehydrogenation (Fig. 2). Since the difference in the dehydrogenation of the secondary and primary alcohols is only a quantitative one, the latter should also react on the elevations in the form of Taylor s peaks (<5) or Volkenshtein s biographical active centers (6). But the author (7) believes, moreover, these elevations to be carriers of crystal facets. Such islets are metastable and, depending on their differences in heights and surface areas and consequently in the deformations caused by the neighboring lattice atoms, are subject to statistical treatment. If their distribution bears an exponential character, then this can explain the appearance of parameter h in Equation (1) 8-11). [Pg.96]


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See also in sourсe #XX -- [ Pg.120 , Pg.241 , Pg.244 , Pg.315 , Pg.377 , Pg.412 ]

See also in sourсe #XX -- [ Pg.138 , Pg.139 ]




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