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Average electron number

Figure 4.43. Trends of the isoelectronic curves in the different Mo-Me systems and in their combinations (curves of constant average group number of the atoms involved). The values of the average electron number per atom are indicated. Figure 4.43. Trends of the isoelectronic curves in the different Mo-Me systems and in their combinations (curves of constant average group number of the atoms involved). The values of the average electron number per atom are indicated.
Fig. 1. The JT-p staircase for Jf in the vicinity of the integer N0. The values of the reactivity indices holding on the = N0 tread and the two adjacent risers are indicated. These values are independent of the location of the (p, /F) point on the tread or on the risers. Here, is the ensemble-average electron number and p is the chemical potential... Fig. 1. The JT-p staircase for Jf in the vicinity of the integer N0. The values of the reactivity indices holding on the = N0 tread and the two adjacent risers are indicated. These values are independent of the location of the (p, /F) point on the tread or on the risers. Here, is the ensemble-average electron number and p is the chemical potential...
Specimens were placed in a silica reactor that was equipped with two side tubes for XPS and ESR measurements and connected to a circulation apparatus, described elsewhere [25, 26]. The catalysts, dried at 383 K, were characterized as prepared (a.p.), after heating in dry oxygen at 773 K (s.o.), or after reduction with CO. In some experiments, as specified, samples were exposed to NO, NH3, or various mixtures NO-O2-NH3. Electrons per V atom (e/V) were determined from the CO consumed. The average oxidation number of vanadium was calculated as 5 - eA/. [Pg.692]

Here i/j. ng l 2mK is the fractional occupation number of the 2ma- sp/n-orbitals of Shell K and is a suitably averaged electron interaction matrix (cf. the usual... [Pg.166]

In a fluid model the correct calculation of the source terms of electron impact collisions (e.g. ionization) is important. These source terms depend on the EEDF. In the 2D model described here, the source terms as well as the electron transport coefficients are related to the average electron energy and the composition of the gas by first calculating the EEDF for a number of values of the electric field (by solving the Boltzmann equation in the two-term approximation) and constructing a lookup table. [Pg.59]

Taking the rate limiting step in the electron transport chain to be trans-membrane proton translocation, which occurs about five times per sulfate consumed (Rabus et al., 2006), the average stoichiometric number x (entered into REACT as to = 1/x) for Reaction 18.7 is five. Sulfate reducers conserve about 45 kJ mol-1 of sulfate consumed (Qusheng Jin, unpublished data), so we set AGp to this value and m to one. From equations 18.12 and 18.14, then, we can write... [Pg.265]

An open system with a fluctuating number of particles is described by an ensemble or statistical mixture of pure states and the fractional electron number may arise as a time average. Thus, let No be an integer electron number, and N be an average in the interval Ai> < N < Nt) f 1. In this case Y is an ensemble or statistical mixture of the No -electron pure state with wave function T V 1 and probability 1 — t, and the (A 0 I l)-electron pure state with wave function Tv, i and probability t, where 0 < t < 1. [Pg.10]

On the basis of the Periodic Table, topics of intermetallic systematics will be presented in the next chapter. In the present chapter the Periodic Table will be revisited and its structure and subdivisions summarized. In relation also to some concepts previously presented, such as electronegativity, Mendeleev number, etc. described in Chapter 2, typical property trends along the Table will be shown. Strictly related concepts, such as Periodic Table group number, average group number and valence-electron number will be considered and used in the description and classification of intermetallic phase families. [Pg.219]

Figure 4.39. The phase diagrams of the binary Cu systems with Zn, A1 and Sn are shown. In order to highlight their similarities the phase equilibria have been plotted with dilferent scales of the atomic composition in order to have the same extension for a scale based on the average v.e.c. in the alloys (number eta of electrons per atom). Notice the consequent change of length of the at.% scale. The values 1, 2, 3, 4 have been assumed for the valence electron numbers of the metals Cu, Zn, A1 and Sn. [Pg.300]

A general agreement may be noticed this may highlight the relevance, and the limits, of the role played by the average valence-electron number per atom... [Pg.305]

The maximum frequency of the C-O vibrational band and the overall band shape reflect the average electronic environment of the platinum atoms. Changes in band intensity, frequency and shape depend on the cluster size, exposed crystallographic planes, location (inside versus outside zeolite pores) and oxidation state of the metal. The number of publications for CO adsorption on zeolite supported noble metals are too numerous to list here, but a few examples that illustrate the type of information that can be obtained are included below. [Pg.138]


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Electron number

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