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Energy population

Molecular descriptors must then be computed. Any numerical value that describes the molecule could be used. Many descriptors are obtained from molecular mechanics or semiempirical calculations. Energies, population analysis, and vibrational frequency analysis with its associated thermodynamic quantities are often obtained this way. Ah initio results can be used reliably, but are often avoided due to the large amount of computation necessary. The largest percentage of descriptors are easily determined values, such as molecular weights, topological indexes, moments of inertia, and so on. Table 30.1 lists some of the descriptors that have been found to be useful in previous studies. These are discussed in more detail in the review articles listed in the bibliography. [Pg.244]

Some results are shown (47) in Fig. 21. The left-hand column of Fig. 21 is a reminder of how VER occurs in ACN with only the C-H stretch fundamental C-3000 cm-1) pumped. The C-H stretch decays in 5 ps, and only 2% of this energy populates the 2153 cm-1 C=N stretch, which has an 80 ps lifetime. The 918 cm-1 C-C stretch rises in 30 ps because it is populated by the pathway C-H stretch -> C-H bend C-C stretch. Subsequent C-C stretch decay occurs with an 45 ps time constant. With combination band pumping (right-hand column of Fig. 21), the C-H stretch... [Pg.590]

States of different energy populated according to a Boltzmann distribution where n, and w2 are the populations of states having energies and E2, respectively. [Pg.92]

Bartlett, A.A. 2004. Thoughts on long-term energy supplies Scientists and the silent lie The world s population continues to grow—shouldn t physicists care Physics Today, 57(7) 53-55. http //fire.pppl.gov/energy population pt 0704.pdf (accessed August 29, 2009). [Pg.124]

The recommended approach to modeling is to create models based on fundamental balances (of mass, species, energy, population) and basic kinetics and use them to build a complete model of the precipitator, as shown in earlier sections. Such a set of equations is known as a physical or a mechanistic model. Complete physical models are difficult to create and solve because they require identification in advance of all physical and chemical subprocesses, properties, and parameters. That is why the semiempirical models of a form similar to the complete physical models (but usually simpler) and with fewer equations are often used for scaling up. Parameters of such models are often given in lumped form, some of them fitted to available experimental data obtained from the small-scale system. Such a model can be useful for scaling up, but one cannot be sure that the scale-up will be completely correct because there is no guarantee that the model contains the complete mechanism (88). However, scale-up errors should be smaller than in the case of purely empirical models. CFD codes that are based on reasonable simplifications (closures) regarding their accuracy can be placed between the physical and semiempirical models their application was demonstrated earlier. [Pg.149]

Fig. 9. Rotational energy population of NO(A II) in o=0,1,2 plotted vs internal energy for each rotational level individually. Open circles and dots refer to the two spinstates, II, 2 and II3/2, respectively. Fig. 9. Rotational energy population of NO(A II) in o=0,1,2 plotted vs internal energy for each rotational level individually. Open circles and dots refer to the two spinstates, II, 2 and II3/2, respectively.
As the OH-aromatlc adducts were deactivated to an essentially thermal energy population at the total pressures used In the studies of Ferry, Atkinson, and Ferry (264, 265), the rate constant k was given by... [Pg.454]

Hydrogen infrastructure build-up is much more relevant for mobile applications than for stationary ones. How hydrogen supply infrastructure would develop and what this would look like depends heavily on country-specific conditions such as the available feedstocks (such as renewable energies), population density and geographic factors, and must therefore be assessed on a country-by-country basis. Nevertheless, it is possible to derive some robust strategies and cross-national communalities. [Pg.245]

EATING PATTERNS WHICH LEAD TO DIETARY DEFICIENCIES. Although hunger due to a lack of a sufficient quantity of food often causes a deficiency disease(s), the factors which lead to this problem are discussed elsewhere. (See HUNGER, WORLD MALNUTRITION, PROTEIN-ENERGY POPULATION, WORLD and WORLD POOD.) Herein, the dietary patterns which may cause deficiency diseases even though sufficient quantity of food is available are identified as follows ... [Pg.254]

Also see MALNUTRITION, PROTEIN-ENERGY POPULATION, WORLD PROTEIN, WORLD PER CAPITA and WORLD FOOD.)... [Pg.563]

Figure 3.33 Overlay of the apparent velocity distributions derived on the assumption that the sputtered neutral population follows the Sigmund-Thompson distributions (Relation 3.4) for Cu" and Cn secondary ions emanating from a polycrystalline surface under 17.5 KeV Ar" " impact, 14.0 KeV Cs" " impact, 17.5 KeV02 impact, and7.5 KeV0 impact. The same calculations were applied to all data sets and with all plots arbitrarily normalized to unity at zero 1 jv. The lines represent the trends relayed by Relation 3.10(a) or (b) fitted to the lower 1 (higher emission energy) populations. Reproduced with permission from van der Heide and Karpusov (2000) Cop)night 2000 Elsevier. Figure 3.33 Overlay of the apparent velocity distributions derived on the assumption that the sputtered neutral population follows the Sigmund-Thompson distributions (Relation 3.4) for Cu" and Cn secondary ions emanating from a polycrystalline surface under 17.5 KeV Ar" " impact, 14.0 KeV Cs" " impact, 17.5 KeV02 impact, and7.5 KeV0 impact. The same calculations were applied to all data sets and with all plots arbitrarily normalized to unity at zero 1 jv. The lines represent the trends relayed by Relation 3.10(a) or (b) fitted to the lower 1 (higher emission energy) populations. Reproduced with permission from van der Heide and Karpusov (2000) Cop)night 2000 Elsevier.
The basic information required to rationalize a photoinduced phenomenon is the energy levels of the excited solutions and the probability of energy (population) transfer from one state to the other. In the semiclassical treatment of the interaction radiation-matter, whereas we treat the molecule quantum-mechanically, the radiation field is seen as a classical wave obeying Maxwell s equations. [Pg.488]


See other pages where Energy population is mentioned: [Pg.3047]    [Pg.22]    [Pg.443]    [Pg.630]    [Pg.126]    [Pg.70]    [Pg.205]    [Pg.58]    [Pg.32]    [Pg.179]    [Pg.122]    [Pg.314]    [Pg.25]    [Pg.122]    [Pg.122]    [Pg.122]    [Pg.3047]    [Pg.147]    [Pg.160]    [Pg.258]    [Pg.53]    [Pg.201]    [Pg.190]    [Pg.314]    [Pg.590]   
See also in sourсe #XX -- [ Pg.36 , Pg.64 , Pg.78 , Pg.105 ]




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