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Distribution supported

Fig. 9. Incidence energy dependence of the vibrational state population distribution resulting when NO(u = 12) is scattered from LiF(OOl) at a surface temperature of (a) 480 K, and (b) 290 K. Relaxation of large amplitude vibrational motion to phonons is weak compared to what is possible on metals. Increased relaxation at the lowest incidence energies and surface temperatures are indicators of a trapping/desorption mechanism for vibrational energy transfer. Angular and rotational population distributions support this conclusion. Estimations of the residence times suggest that coupling to phonons is significant when residence times are only as long as ps. (See Ref. 58.)... Fig. 9. Incidence energy dependence of the vibrational state population distribution resulting when NO(u = 12) is scattered from LiF(OOl) at a surface temperature of (a) 480 K, and (b) 290 K. Relaxation of large amplitude vibrational motion to phonons is weak compared to what is possible on metals. Increased relaxation at the lowest incidence energies and surface temperatures are indicators of a trapping/desorption mechanism for vibrational energy transfer. Angular and rotational population distributions support this conclusion. Estimations of the residence times suggest that coupling to phonons is significant when residence times are only as long as ps. (See Ref. 58.)...
Distribution supported by documentation that the procedure has been reviewed by all testing personnel. [Pg.406]

Investigation of simulated natural copolymers having holes in the distribution supports this view as shown in Figure 8. If the ranges... [Pg.194]

The fragment excited-state NO(A2S+) is a molecular 3r Rydberg state, and we shall refer to this as NO(A, 3s). The observed NO(A, 3.v) product state distributions supported the notion of a planar dissociation involving restricted intramolecular vibrational energy redistribution (IVR) [176]. A scheme for studying NO dimer photodissociation dynamics via TRPES is depicted in Fig. 25. The NO(A, 3.v) + NO(X) product elimination channel, its scalar and vector properties, and its evolution on the femtosecond time scale have been discussed in a number of recent publications (see Ref. [175] and references cited therein). [Pg.560]

Structure-sensitive reactions are extensively discussed in the catalytic literature, but careful examination of the published work reveals that on the atomic scale the catalytic materials used in these studies are in general poorly characterized with respect to particle size and structure. Extended X-ray absorption fine structure (EXAFS) has been successfully applied to the study of small particles on supportsand small metal molecules in matrices subject to the caveat that samples of these materials consist of a distribution of particle sizes. Information thus obtained is an average over the entire distribution. Supported, monosized clusters have not yet been used in catalytic studies. However, Woste and coworkers demonstrated in the first experiment where monosized clusters were deposited that Ag4 is the critical cluster... [Pg.212]

The examples presented above showed that size-selected clusters on surfaces reveal remarkable size-effects, however, they have been studied so far only by one-cycle experiments. Thus an experimental proof that these systems are active for catalytic processes, e.g. several cycles of a catalytic reaction are promoted without destruction of the catalyst, is still missing. In the following we present an experimental scheme to study catalytic processes of clusters on surfaces with high sensitivity and we report turn-over frequencies TOFs for the oxidation of CO on size-distributed supported Pd clusters. [Pg.578]

Product distribution/ supporting electrolyte NaOAc Me4NN03... [Pg.60]

Some of these results are in marked contrast to other observations that indicate an increase in MRR value with increased conditioner downforce.12 13 In this study the MRR was examined against variations in conditioner down-force, slurry abrasive type (fumed or colloidal), conditioning approach (in situ or ex situ), and pad slurry distribution support geometry (perforated or grooved). Results indicated a strong positive correlation in nearly all cases between conditioner downforce and MRR (Figure 7.15). [Pg.155]

Figure 3.10 Vapor-distributing support. (From F. Moore and F. Rukovena, Chemical Plant and Processing, Europe edition, August 1987. Reprinted courtesy of Chemical Plant and Processing.)... Figure 3.10 Vapor-distributing support. (From F. Moore and F. Rukovena, Chemical Plant and Processing, Europe edition, August 1987. Reprinted courtesy of Chemical Plant and Processing.)...
A vapor-distributing support (Fig. 3.10) is a flat perforated plate containing perforated vapor risers. Liquid descends through the floor perforations, while vapor rises through the riser perforations. The bottom portion of the vapor risers is unperforated, so that vapor is injected above the liquid pool on the plate. Sumps are optional and recommended (289) where liquid inventory is to be reduced. The vapor-distributing support combines two internals (a vapor distributor and a support plate) into one. Compared to a vapor distributor, this saves both vertical space and internals costs. On the other hand, obstruction of perforations by pieces of packing and possible liquid overflow into risers may make its vapor distribution quality somewhat lower. [Pg.80]

Pressure drop through the vapor distributor or a vapor-distributing support should be at least equal to the velocity head at the column inlet nozzle (386). T3rpically, a pressure drop of 1 to 8 in of water (289) is used for these devices. In one typical specific example (346), it was 4 ins. [Pg.81]

A vapor distributor with insufficient pressure drop may be ineffective. A case has been reported (75) where poor column efficiency resulted from specifying a vapor distributor with lower pressure drop than recommended by the manufacturer. The vapor distributor (or vapor-distributing support) pressure drop can be minimized by entering the feed via a sparger pipe with the bottom quadrant removed (rather than perforated). Although such a sparger pipe will not be an effective vapor distributor, it will serve to break the incoming vapor jet and reduce its velocity head. [Pg.81]

Vapor-distributing supports should not be used with foaming systems (289). [Pg.81]

As well as the RAMOs, the spin density distribution is delocalized on the directly coordinating N and Sy atoms of the His and Met residues in the CTu state, respectively, while it is almost localized over only the CU2S2 diamond core in the ttu oxidized state. As listed in Table 30.1, the Mulliken atomic spin densities are found on the Hisl61, His204, and Met207 parts in the CTu oxidized Cua models, whereas most of the Mulliken atomic spin densities are found on only the core part in the ttu oxidized ones. The RAMOs and spin density distribution supports the advantage of the CTu state in the electron transfer compared with the Ku state. [Pg.520]

Process product design architecture—documents the design architecture for the life cycle process products related to development (systems engineering and integration), manufacturing, verification, distribution, support, training, and disposal. Products include equipment, software, people, facilities, processes, and services integral to a specific life cycle process. [Pg.13]

The enterprise should initiate development of applicable downstream life cycle processes for development, production, test, distribution, support, training, and disposal to provide life cycle support to products and their subsystems, and for assemblies and their components. If system elements are being procured from suppliers or subcontractors, then consideration for life cycle support of the system elements should be addressed. Each life cycle process goes through the same development events and activities as described for products in 5.1 through 5.5, including technical reviews. [Pg.34]

Femtosecond photoelectron spectroscopy was employed to study the excitation of trons-stilbene above the isomerization reaction barrier [82]. Apart from the contribution, evidence of a second electronic state was found on the basis of two different transients measured across the photoelectron spectrum. Time-dependent density functional theory calculations on So, Si, S2, and Do, tt ether with simulations of the electron energy distribution, supported the experimental findings for selective photoelectron energies of the So, Si,... electronic states. The photoelectron spectra of trans-stilbene following the excitation with 266 nm laser pulses consisting of a pronounced three-peak structure were subjected to a substantia] broadening, due to the large number of closely spaced vibrational states involved in the excitation scheme. [Pg.121]

Implementation ease. Tlie small number of tools makes them easier to purchase, distribute, support and learn to use. Because these tools are available for all computers, one is fre from the need to support one family of hardware. [Pg.157]


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See also in sourсe #XX -- [ Pg.99 ]




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