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Atom approach

As an interesting footnote, Ceyer [291] has found that ethylene is hydrogenated by hydrogen absorbed in the bulk region just below a Ni(l 11) surface. In this case, the surface ethylenes are assumed to by lying flat, with the dissolved H atoms approaching the double bond from underneath. [Pg.733]

Conventional associative ionization (AI) occurring at ambient temperature proceeds in two steps excitation of isolated atoms followed by molecular autoionization as the two atoms approach on excited molecular potentials. In sodium for example [44]... [Pg.2475]

Two colliding atoms approach on tire molecular ground-state potential. During tire molasses cycle witli tire optical fields detuned only about one line widtli to tire red of atomic resonance, tire initial excitation occurs at very long range, around a Condon point at 1800 a. A second Condon point at 1000 takes tire population to a 1 doubly excited potential tliat, at shorter intemuclear distance, joins adiabatically to a 3 potential, drought to be die... [Pg.2479]

Dalibard J and Cohen-Tannoudji C 1985 Dressed-atom approach to atomic motion in laser light the dipole force revisited J.Opt.Soc.Am. B 21707-20... [Pg.2479]

In the reactant channel leading up to the transition region, motion along represents the FI atom approaching the molecule, while motion along / is the vibrational motion of the atom. The initial wavepacket is chosen to represent the desired initial conditions. In Figure 2, the FI2 molecule is initially in the ground... [Pg.260]

Figure 2. Wavepacket dynamics of the H + H H2 + H scattering reaction, shown as snapshots of the density (wave packet amplitude squard) at various times, The coordinates, in au, are described in Figure la, and the wavepacket is initially moving to describe the H atom approaching the H2 molecule. The density has been integrated over the angular coordinate, The PES is plotted for the collinear interaction geometry, 0 180, ... Figure 2. Wavepacket dynamics of the H + H H2 + H scattering reaction, shown as snapshots of the density (wave packet amplitude squard) at various times, The coordinates, in au, are described in Figure la, and the wavepacket is initially moving to describe the H atom approaching the H2 molecule. The density has been integrated over the angular coordinate, The PES is plotted for the collinear interaction geometry, 0 180, ...
Output. Upon successful execution, you will obtain an output file from which you can follow the geometry change during iterative minimization,, As the atoms approach their respective potential energy minima, they are moved less and less until the criterion of minimum geometry change is met (see also PART 2, Pile 4-3),... [Pg.155]

Another strategic device applies specifically to polycyclic compounds. In the interests of simplification we want to remove some of the rings and give an intermediate with a famihar ring structure. We can do this by the common atom approach. In TM 329, mark all the carbon atoms which belong to more than one ring - the common atoms . [Pg.107]

Using the common atom approach, design a synthesis of TM 332. [Pg.108]

Asimple example is the formation of the hydrogen molecule from two hydrogen atoms. Here the original atomic energy levels are degenerate (they have equal energy), but as the two atoms approach each other, they interact to form two non degenerate molecular orbitals, the lowest of which is doubly occupied. [Pg.49]

In (a), an ion and a gas atom approach each other with a total kinetic energy of KE, + KEj. After collision (b), the atom and ion follow new trajectories. If the sum of KE, + KEj is equal to KE3 + KE4, the collision is elastic. In an inelastic collision (b), the sums of kinetic energies are not equal, and the difference appears as an excess of internal energy in the ion and gas molecule. If the collision gas is atomic, there can be no rotational and no vibrational energy in the atom, but there is a possibility of electronic excitation. Since most collision gases are helium or argon, almost all of the excess of internal energy appears in the ion. [Pg.374]

When two atoms approach each other so closely that their electron clouds interpenetrate, strong repulsion occurs. Such repulsive van der Waals forces follow an inverse 12th-power dependence on r (1/r ), as shown in Figure 1.13. Between the repulsive and attractive domains lies a low point in the potential curve. This low point defines the distance known as the van der Waals contact distance, which is the interatomic distance that results if only van der Waals forces hold two atoms together. The limit of approach of two atoms is determined by the sum of their van der Waals radii (Table 1.4). [Pg.16]

Some force fields use the so-called united atom approach where (for example) a methyl group is treated as a single pseudo-atom. They arose historically in order to save computer resource when dealing with large systems such as amino-acid chains. [Pg.43]

When two sp-hybridized carbon atoms approach each other, sp hybrid orbitals on each carbon overlap head-on to form a strong sp-sp a bond. In addition, the pz orbitals from each carbon form a pz-pz it bond by sideways overlap and the py orbitals overlap similarly to form a py-py tt bond. The net effect is the sharing of six electrons and formation of a carbon-carbon triple bond. The two remaining sp hybrid orbitals each form a bond with hydrogen to complete the acetylene molecule (Figure 1.16). [Pg.18]

Steric strain—the strain due to repulsive interactions when atoms approach each other too closely... [Pg.114]

The formation of the BeF2 molecule can be explained by assuming that, as two fluorine atoms approach Be, the atomic orbitals of the beryllium atom undergo a significant change. Specifically, the 2s orbital is mixed or hybridized with a 2p orbital to form two new sp hybrid orbitals. (Figure 7.12). [Pg.186]

How large is an atom We cannot answer this question for an isolated atom. We can, however, devise experiments in which we can find how closely the nucleus of one atom can approach the nucleus of another atom. As atoms approach, they are held apart by the repulsion of the positively charged nuclei. The electrons of the two atoms also repel one another but they are attracted by the nuclei. The closeness of approach of two nuclei will depend upon a balance between the repulsive and attractive forces. It also depends upon the energy of motion of the atoms as they approach one another. If we think of atoms as spheres, we find that their diameters vary from 0.000 000 01 to 0.000 000 05 cm (from 1 X 10-8 to 5 X 10 8 cm). Nuclei are much smaller. A typical nuclear diameter is 10, s cm, about 1/100,000 the atom diameter. [Pg.88]

Fig. 16-4. Attractive and repulsive forces when helium atoms approach. Fig. 16-4. Attractive and repulsive forces when helium atoms approach.
Figure 16-3D shows the simplified representation of the interaction of two helium atoms. This time each helium atom is crosshatched before the two atoms approach. This is to indicate there are already two electrons in the Is orbital. Our rule of orbital occupancy tells us that the Is orbital can contain only two electrons. Consequently, when the second helium atom approaches, its valence orbitals cannot overlap significantly. The helium atom valence electrons fill its valence orbitals, preventing it from approaching a second atom close enough to share electrons. The helium atom forms no chemical bonds. ... [Pg.278]

We see that the neutral fluorine atom has seven valence electrons that is, seven electrons occupy the outermost partially filled cluster of energy levels. This cluster of energy levels, the valence orbitals, contains one electron less than its capacity permits. Fluorine, then, has the capacity for sharing one electron with some other atom which has similar capacity. If, for example, another fluorine atom approaches, they might share... [Pg.279]

Suppose a hydrogen atom approaches an oxygen atom in its most stable state, (27). Each... [Pg.282]


See other pages where Atom approach is mentioned: [Pg.703]    [Pg.308]    [Pg.49]    [Pg.170]    [Pg.144]    [Pg.100]    [Pg.115]    [Pg.187]    [Pg.107]    [Pg.28]    [Pg.58]    [Pg.61]    [Pg.170]    [Pg.505]    [Pg.49]    [Pg.226]    [Pg.227]    [Pg.180]    [Pg.125]    [Pg.28]    [Pg.58]    [Pg.61]    [Pg.52]    [Pg.92]    [Pg.41]    [Pg.11]    [Pg.277]    [Pg.56]   
See also in sourсe #XX -- [ Pg.203 ]




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A Computer-Algebraic Approach to the Derivation of Feynman-Goldstone Perturbation Expansions for Open-Shell Atoms and Molecules

Atom Transfer Radical Polymerization (ATRP) Approach to Polymer-grafted CNTs

Atom superposition, electron delocalization molecular orbital approach

Atom-Centered Basis Function Approach

Atom-based approach

Atomic basic experimental approaches

Atomic systems dressed-atom approach

Atoms-in-molecules approach

Common atom approach

Gauge-including atomic orbital approach

Linear combination of atomic orbitals approach

Linear-combination-of-atomic-orbitals LCAO) approach

Many-atom systems partitioning approach

Octanol/water partition coefficients atomic approach

Reactive scattering, atom-diatom approach

United atom approach

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