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Solid local

Internal boundaries in a crystal, when disordered, form extended defects. However, if the boundaries become ordered, they simply extend the unit cell of the structure and hence are no longer regarded either as boundaries or defects (Fig. 3.20c). In addition, some boundaries can change the composition of a solid locally and, if present in large numbers, can change the macroscopic composition noticeably. When these are ordered, new series of compounds form. Boundaries that do cause significant composition changes are described in Chapter 4. [Pg.107]

In solids, local fields are often relatively large and thus cause very short decays. In order to observe the FID, the spectrometer must recover from the preceding rf pulse before M decays to zero. In most cases, this condition can be satisfied, and FID signals are normally observed. However, in the case of our Pt-cfjtalyst samples, the distribution of local fields is very large. M decays to zero long before the spectrometer can recover from the rf pulse, and no FID signal can be observed. [Pg.380]

The principal conclusion from the previous studies was that ICP-AES was the most rugged and flexible approach, but also that LA-ICP-MS was uniquely suitable for direct solid local analyses [120]. [Pg.457]

Liquid/Solids Localized sweating, nausea, vomiting, involuntary urina-... [Pg.24]

Phonon Induced Delocalization in disordered solids, localization can result when a wavefunction interferes with itself due to elastic scattering and forms a standing wave. Phonon scattering can destroy this interference effect and cause the wavefunctions to be more extended. [Pg.751]

J. W, Perry and A. H, Zewail, Observation of high-energy vibrational overtones of molecules in solids Local modes and intramolecular relaxations, J. Chem. Phys. 70 582 (1979). [Pg.35]

However, before extrapolating the arguments from the gross patterns through the reactor for homogeneous reactions to solid-catalyzed reactions, it must be recognized that in catalytic reactions the fluid in the interior of catalyst pellets may diSer from the main body of fluid. The local inhomogeneities caused by lowered reactant concentration within the catalyst pellets result in a product distribution different from that which would otherwise be observed. [Pg.48]

Generally speaking, temperature control in fixed beds is difficult because heat loads vary through the bed. Also, in exothermic reactors, the temperature in the catalyst can become locally excessive. Such hot spots can cause the onset of undesired reactions or catalyst degradation. In tubular devices such as shown in Fig. 2.6a and b, the smaller the diameter of tube, the better is the temperature control. Temperature-control problems also can be overcome by using a mixture of catalyst and inert solid to effectively dilute the catalyst. Varying this mixture allows the rate of reaction in different parts of the bed to be controlled more easily. [Pg.56]

The microscopic contour of a meniscus or a drop is a matter that presents some mathematical problems even with the simplifying assumption of a uniform, rigid solid. Since bulk liquid is present, the system must be in equilibrium with the local vapor pressure so that an equilibrium adsorbed film must also be present. The likely picture for the case of a nonwetting drop on a flat surface is... [Pg.378]

The coefficient of friction between two unlubricated solids is generally in the range of 0.5-1.0, and it has therefore been a matter of considerable interest that very low values, around 0.03, pertain to objects sliding on ice or snow. The first explanation, proposed by Reynolds in 1901, was that the local pressure caused melting, so that a thin film of water was present. Qualitatively, this explanation is supported by the observation that the coefficient of friction rises rapidly as the remperarure falls, especially below about -10°C, if the sliding speed is small. Moreover, there is little doubt that formation of a water film is actually involved [3,4]. [Pg.438]

Before entering the detailed discussion of physical and chemical adsorption in the next two chapters, it is worthwhile to consider briefly and in relatively general terms what type of information can be obtained about the chemical and structural state of the solid-adsorbate complex. The term complex is used to avoid the common practice of discussing adsorption as though it occurred on an inert surface. Three types of effects are actually involved (1) the effect of the adsorbent on the molecular structure of the adsorbate, (2) the effect of the adsorbate on the structure of the adsorbent, and (3) the character of the direct bond or local interaction between an adsorption site and the adsorbate. [Pg.582]

Gas A, by itself, adsorbs to a of 0.02 at P = 200 mm Hg, and gas B, by itself, adsorbs tod = 0.02 at P = 20 mm Hg Tisll K in both cases, (a) Calculate the difference between (2a and (2b> the two heats of adsorption. Explain briefly any assumptions or approximations made, ib) Calculate the value for 6 when the solid, at 77 K, is equilibrated with a mixture of A and B such that the final pressures are 200 mm Hg each, (c) Explain whether the answer in b would be raised, lowered, or affected in an unpredictable way if all of the preceding data were the same but the surface was known to be heterogeneous. The local isotherm function can still be assumed to be the Langmuir equation. [Pg.672]

The three-dimensional synnnetry that is present in the bulk of a crystalline solid is abruptly lost at the surface. In order to minimize the surface energy, the themiodynamically stable surface atomic structures of many materials differ considerably from the structure of the bulk. These materials are still crystalline at the surface, in that one can define a two-dimensional surface unit cell parallel to the surface, but the atomic positions in the unit cell differ from those of the bulk structure. Such a change in the local structure at the surface is called a reconstruction. [Pg.289]

Heinz K 1994 Diffuse LEED and local surface structure Phys. Status. Solid A 146 195-204... [Pg.1777]

One of the most important advances in electrochemistry in the last decade was tlie application of STM and AFM to structural problems at the electrified solid/liquid interface [108. 109]. Sonnenfield and Hansma [110] were the first to use STM to study a surface innnersed in a liquid, thus extending STM beyond the gas/solid interfaces without a significant loss in resolution. In situ local-probe investigations at solid/liquid interfaces can be perfomied under electrochemical conditions if both phases are electronic and ionic conducting and this... [Pg.1948]

The take-home lesson is that the vast majority of high-pressure studies are on solids or other rigid media and are not done under hydrostatic conditions. The stresses and stress-related properties may vary throughout the sample. Unless the probes are very local and focus on a small region of the sample, measurements are averages over a range of, often uncharacterized, conditions. [Pg.1956]


See other pages where Solid local is mentioned: [Pg.335]    [Pg.236]    [Pg.236]    [Pg.78]    [Pg.18]    [Pg.297]    [Pg.1127]    [Pg.179]    [Pg.468]    [Pg.28]    [Pg.339]    [Pg.237]    [Pg.136]    [Pg.289]    [Pg.443]    [Pg.335]    [Pg.236]    [Pg.236]    [Pg.78]    [Pg.18]    [Pg.297]    [Pg.1127]    [Pg.179]    [Pg.468]    [Pg.28]    [Pg.339]    [Pg.237]    [Pg.136]    [Pg.289]    [Pg.443]    [Pg.49]    [Pg.241]    [Pg.372]    [Pg.588]    [Pg.112]    [Pg.123]    [Pg.124]    [Pg.133]    [Pg.1098]    [Pg.1253]    [Pg.1278]    [Pg.1324]    [Pg.1497]    [Pg.1786]    [Pg.1787]    [Pg.1791]    [Pg.1957]    [Pg.2202]   
See also in sourсe #XX -- [ Pg.343 , Pg.348 ]




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