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Experimental external transfer

This type of plot has been used widely to correlate experimental mass-transfer data. De Acetis and Thodos have summarized the data available up to 1960 in a single rve of vs Reynolds number, as shown in Fig. 10-2. For spherical pellets /)sis the diameter for other shapes dp can be taken as the diameter of a sphere with the same external area. Other investigations and correlations of mass-transfer datg include those of Carberry, Yeh, Bradshaw and Bennett, and Thoenes and Kramers. ... [Pg.363]

Here t. is the intrinsic lifetime of tire excitation residing on molecule (i.e. tire fluorescence lifetime one would observe for tire isolated molecule), is tire pairwise energy transfer rate and F. is tire rate of excitation of tire molecule by the external source (tire photon flux multiplied by tire absorjDtion cross section). The master equation system (C3.4.4) allows one to calculate tire complete dynamics of energy migration between all molecules in an ensemble, but tire computation can become quite complicated if tire number of molecules is large. Moreover, it is commonly tire case that tire ensemble contains molecules of two, tliree or more spectral types, and experimentally it is practically impossible to distinguish tire contributions of individual molecules from each spectral pool. [Pg.3020]

Stoicescu and Dimonie103 studied the polymerization of 2-vinylfuran with iodine in methylene chloride between 20 and 50 °C. The time-conversion curves were not analysed for internal orders but external orders with respect to catalyst and monomer were both unity. Together with an overall activation energy of 2.5 kcal/mole for the polymerization process, these were the only data obtained. Observations about the low DP s of the products, their dark colour, their lack of bound iodine and the presence of furan rings in the oligomers, inferred by infrared spectra (not reported), completed the experimental evidence. The authors proposed a linear, vinylic structure for the polymer, and a true cationic mechanism for its formation and discussed the occurrence of an initial charge-transfer complex on the... [Pg.72]

Thus the key experimental observation Equation (7.11), is satisfied in presence of spillover. When an external overpotential AUWR is applied, with a concomitant current, I, and O2 flux I/2F, although UWR is not fixed anymore by the Nemst equation but by the extremally applied potential, still the work function Ow will be modified and Equations (7.11) and (7.12), will remain valid as long as ion spillover is fast relative to the electrochemical charge transfer rate I/2F.21 This is the usual case in solid state electrochemistry (Figs. 7.3b, 7.3d) as experimentally observed (Figs. 5.35, 5.23, 7.4, 7.6-7.9). [Pg.350]

Although some workers suggest that exchange interactions are dominant in determining the effects of external heavy atoms/1455 experimental evidence at this point tends to favor charge transfer as the mechanism for external... [Pg.436]

Equations 12.4.22 and 12.4.24 indicate that the observed reaction order will differ from the intrinsic reaction order in the presence of intraparticle and/or external mass transfer limitations. To avoid drawing erroneous conclusions about intrinsic reaction kinetics, we must be careful to either eliminate these limitations by proper choice of experimental conditions or to properly take them into account in our data analysis. [Pg.479]

In the conventional vision, product quality is mainly based on external, nutritive and sensory properties and is strongly directed by traders and trends. Besides tastiness and ripeness, organic consumers expect products to have properties such as vitality and coherence , which are not easy to define and thus to explain and transfer. In the past, experimental parameters have been proposed to estimate vitality and coherence , but they were neither scientifically validated nor related to a validated quality concept with relation to human health. [Pg.53]

A given electrode reaction may correspond to any of these situations depending on the experimental conditions, in particular on the external control of mass transfer. [Pg.5]

The results reviewed above suggest that gas-phase diffusion can contribute significantly to polarization as O2 concentrations as high as a few percent and are not necessarily identifiable as a separate feature in the impedance. Workers studying the P02 -dependence of the electrode kinetics are therefore urged to eliminate as much external mass-transfer resistance in their experiments as possible and verify experimentally (using variations in balance gas or total pressure) that gas-phase effects are not obscuring their results. [Pg.596]

First experimental results on dye-loaded zeolite L systems modified with commercial stopcock molecules on the external surface show that electronic excitation energy can be transferred from molecules inside the channels to the stopcocks and vice versa and that the stopcocks prefer to adsorb on the cylinder base instead of the coat [42]. [Pg.337]

Consideration of the spin-orbit interaction and the effect of an external magnetic field on the electronic ground state of an ion in a CF allows evaluation of the various terms in the spin-Hamiltonian of Equation (31). In addition, the interaction of the nucleus of the paramagnetic ion and ligand nuclei with the d-electron cloud must be considered. In this way the experimentally determined terms of the spin-Hamiltonian may be related to such parameters as the energy differences between levels of the ion in the CF and amount of charge transfer between d-electrons and ligands. [Pg.89]

The effects of non-uniform distribution of the catalytic material within the support in the performance of catalyst pellets started receiving attention in the late 60 s (cf 1-4). These, as well as later studies, both theoretical and experimental, demonstrated that non-uniformly distributed catalysts can offer superior conversion, selectivity, durability, and thermal sensitivity characteristics over those wherein the activity is uniform. Work in this area has been reviewed by Gavriilidis et al. (5). Recently, Wu et al. (6) showed that for any catalyst performance index (i.e. conversion, selectivity or yield) and for the most general case of an arbitrary number of reactions, following arbitrary kinetics, occurring in a non-isothermal pellet, with finite external mass and heat transfer resistances, the optimal catalyst distribution remains a Dirac-delta function. [Pg.410]


See other pages where Experimental external transfer is mentioned: [Pg.69]    [Pg.127]    [Pg.272]    [Pg.1933]    [Pg.464]    [Pg.728]    [Pg.34]    [Pg.50]    [Pg.206]    [Pg.107]    [Pg.24]    [Pg.108]    [Pg.344]    [Pg.146]    [Pg.191]    [Pg.46]    [Pg.439]    [Pg.454]    [Pg.475]    [Pg.139]    [Pg.32]    [Pg.86]    [Pg.36]    [Pg.49]    [Pg.283]    [Pg.241]    [Pg.58]    [Pg.415]    [Pg.345]    [Pg.141]    [Pg.299]    [Pg.42]    [Pg.51]    [Pg.396]    [Pg.1137]    [Pg.60]    [Pg.367]    [Pg.224]    [Pg.486]   
See also in sourсe #XX -- [ Pg.294 ]




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External transfer

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