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Oxygen molecules, probability distribution

Figure 8. The structure of hydrated Na and CP ions at the water/Pt(IOO) interface (dotted lines) compared with the structure in bulk water (solid lines). In the two top panels are the oxygen ion radial distribution functions, and in the two bottom panels are the probability distribution functions for the angle between the water dipole and the oxygen-ion vector for water molecules in the first hydration shell. (Data adapted from Ref. 100.)... Figure 8. The structure of hydrated Na and CP ions at the water/Pt(IOO) interface (dotted lines) compared with the structure in bulk water (solid lines). In the two top panels are the oxygen ion radial distribution functions, and in the two bottom panels are the probability distribution functions for the angle between the water dipole and the oxygen-ion vector for water molecules in the first hydration shell. (Data adapted from Ref. 100.)...
Figure 10.7 Probability density of die centrifuged oxygen gas as a function of the molecular angle and the free propagation time, that is, die time elapsed since die molecules have been released from die centrifuge. The white dashed line (around 1.5 ps) marks the calculated trajectory of a dumbbell distribution rotating widi die classical rotational frequency of an oxygen molecule with an angular momentum of 39ft. Part of Fig. 4 in Ref. 39. Figure 10.7 Probability density of die centrifuged oxygen gas as a function of the molecular angle and the free propagation time, that is, die time elapsed since die molecules have been released from die centrifuge. The white dashed line (around 1.5 ps) marks the calculated trajectory of a dumbbell distribution rotating widi die classical rotational frequency of an oxygen molecule with an angular momentum of 39ft. Part of Fig. 4 in Ref. 39.
However, the fact that the acid product from oxidation of paraffin wax averaging 24C atoms per molecule consists of a variety of acids of varying chain length makes it seem more probable that the oxygen attack is distributed and that rupture may occur at various points in the molecules. ... [Pg.546]

When an oxygen molecule is approaching the surface of an n-type semiconducting oxide, the probability of trapping a conduction electron from the semiconductor is the occupation probability of the band gap acceptor level Ea=%-W, where % is the electron affinity of the gas molecule and is the semiconductor work function. The probability is given by the Fermi-Dirac distribution function (Kireev 1978) ... [Pg.248]

Figures. The Probability Distribution for a Velocity Component of Oxygen Molecules at 298 K. Figures. The Probability Distribution for a Velocity Component of Oxygen Molecules at 298 K.
We have derived this distribution for particles without rotation or vibration, but we now assert that rotation, vibration, and electtonic motion occur independently of translation (the only motion of structureless particles) so that we can use this distribution for the translational motion of any molecules in a dilute gas. The normalized probability distribution is represented in Figure 9.7 for a velocity component of oxygen molecules at 298 K. The most probable value of the velocity component is zero, and most of the oxygen molecules have values of the velocity component between —400ms and 400ms ... [Pg.399]

Figure 9.12 shows this probability distribution of speeds for oxygen molecules at 298 K. The most probable speed, the mean speed, and the root-mean-square speed are labeled on the speed axis. Compare this figure with Figure 9.7. The most probable value of a velocity component is zero, while the most probable speed is nonzero and the probability of zero speed is zero. This difference is due to the fact that the speed probability density is equal to the area of the spherical shell in velocity space (equal to 4nxP-) times the probability density of the velocities lying in the spherical shell. Zero speed is improbable not because the velocity probability density is zero (it is at its maximum value), but because the area of the spherical shell vanishes at n = 0. Figure 9.12 shows this probability distribution of speeds for oxygen molecules at 298 K. The most probable speed, the mean speed, and the root-mean-square speed are labeled on the speed axis. Compare this figure with Figure 9.7. The most probable value of a velocity component is zero, while the most probable speed is nonzero and the probability of zero speed is zero. This difference is due to the fact that the speed probability density is equal to the area of the spherical shell in velocity space (equal to 4nxP-) times the probability density of the velocities lying in the spherical shell. Zero speed is improbable not because the velocity probability density is zero (it is at its maximum value), but because the area of the spherical shell vanishes at n = 0.
The probability of cavity formation in bulk water, able to accommodate a solute molecule, by exclusion of a given number of solvent molecules, was inferred from easily available information about the solvent, such as the density of bulk water and the oxygen-oxygen radial distribution function [65,79]. [Pg.707]

This function is the integrally normalized probability for each water molecule being oriented such that it makes an angle B between its OH bond vectors and the vector from the water oxygen to the carbon atom. This function is calculated for those molecules within 4.9 A of the carbon atom (nearest neighbors), as this distance marks the first minimum in the pair distribution function for that atom. The curve in Figure 10 is typical for hydrophobic hydration (22). [Pg.84]

NH3 is similar to H2O in that they both possess large dipole moments and are both small molecules. The presence of NH3 in a zeolite is chemically similar to the presence of H2O in a zeolite. Therefore, the hydrated cation distribution in zeolites is probably more typical of NH3 adsorption in zeolites than the dehydrated cation distribution. According to Breck (18), for hydrated zeolite X, cations are found in sites SI, SI, SII, and SIV. Of these sites, SI, SII, and SIV would all be adsorption lattice solution sites. The cationic and anionic lattice solution sites (in the supercavity of NaX) are illustrated in Figure 8. For NH3, the subscript J1 will refer to SII sites, the subscript J2 will refer to SI sites, and J3 will refer to SIV sites. The anionic sites are two and are (l) in the center U-membered ring of the connecting frame and (2) near the center of the 0(2)—0(1)—0(l) triad of oxygen atoms. For NH3, the subscript il will refer to the first anionic site the subscript i2 will refer to the second anionic site. [Pg.20]

The solvation structure around a molecule is commonly described by a pair correlation function (PCF) or radial distribution function g(r). This function represents the probability of finding a specific particle (atom) at a distance r from the atom being studied. Figure 4.32 shows the PCF of oxygen-oxygen and hydrogen-oxygen in liquid water. [Pg.593]

Extensive information concerning distribution of the promoters, penetration below the promoters of adsorbed atoms, and chemical behavior of the promoters was obtained by Brunauer and Emmett (25,26). They used chemisorption of carbon monoxide, carbon dioxide, nitrogen, hydrogen, and oxygen, individually and successively measuring the influence of one type of chemisorption upon another type. It was concluded that CO and C02 were chemisorbed as molecules, H2 and N2 as atoms, and 02 probably as ions. C02 is chemisorbed on the alkali molecules located at the surface, whereas H2, N 2, CO, and 02 are chemisorbed on the iron atoms. From the effect of presorbed CO upon the chemisorption of C02 and vice versa it was concluded that the promoters are concentrated on the surface and are distributed so effectively that most surface iron atoms are near to a promoter atom. Strong indication... [Pg.16]


See other pages where Oxygen molecules, probability distribution is mentioned: [Pg.128]    [Pg.361]    [Pg.368]    [Pg.121]    [Pg.238]    [Pg.147]    [Pg.91]    [Pg.11]    [Pg.161]    [Pg.164]    [Pg.209]    [Pg.269]    [Pg.23]    [Pg.177]    [Pg.134]    [Pg.184]    [Pg.145]    [Pg.372]    [Pg.124]    [Pg.2502]    [Pg.15]    [Pg.336]    [Pg.87]    [Pg.131]    [Pg.38]    [Pg.81]    [Pg.137]    [Pg.61]    [Pg.858]    [Pg.110]    [Pg.221]    [Pg.31]    [Pg.343]    [Pg.304]    [Pg.345]    [Pg.156]    [Pg.325]   


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