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Molecule formation

The evolution of nitrogen from liquid steel is also dependent on the oxygen content, again because of the blocking of the surface sites which are necessary for Na molecule formation prior to evolution. [Pg.363]

Compared with GD-OES (and -MS, if used for depth profiling) SNMS provides somewhat better depth resolution (1 nm range) HE-plasma SNMS hardly suffers from molecule formation in the plasma gas (Ar), as do the CD techniques, in which ar-gides are formed because of the comparatively high pressure. [Pg.122]

The horizontal axis corresponds to an intemuclear separation running from 1.5 to 2.5 flo and the vertical axis corresponds to an orbital exponent running from 1,0 to 1.4. The potential energy minimum corresponds to an exponent of 1.238, and we note the contraction of the atomic Is orbital on molecule formation. [Pg.81]

There is a second point to note in dementi s paper above where he speaks of 3d and 4f functions. These atomic orbitals play no part in the description of atomic electronic ground states for first- and second-row atoms, but on molecule formation the atomic electron density distorts and such polarization functions are needed to accurately describe the distortion. [Pg.161]

Carbon atoms in free space have spherical symmetry, but a carbon atom in a molecule is a quite different entity because its charge density may well distort from spherical symmetry. To take account of the finer points of this distortion, we very often need to include d, f,. .. atomic orbitals in the basis set. Such atomic orbitals are referred to as polarization functions because their inclusion would allow a free atom to take account of the polarization induced by an external electric field or by molecule formation. 1 mentioned polarization functions briefly in Section 9.3.1. [Pg.170]

This resonance energy leads to molecule formation only if the eigenfunction is symmetric in the two nuclei. The perturbation energy for the antisymmetric eigenfunction is... [Pg.45]

In this case, too, molecule formation results from the symmetric eigenfunction. The corresponding perturbation energy W1 is obtained from an equation of the type of Equation 20 involving I hj and the wave equation 28. It is... [Pg.49]

This, the naive potential function, is also shown in figure 11. It corresponds to a relatively small attraction, so that the conclusion can be drawn that in the hydrogen molecule the interchange energy of the two electrons is the principal cause of the forces leading to molecule formation. [Pg.52]

The Interaction of Simple Atoms.—The discussion of the wave equation for the hydrogen molecule by Heitler and London,2 Sugiura,3 and Wang4 showed that two normal hydrogen atoms can interact in either of two ways, one of which gives rise to repulsion with no molecule formation, the other... [Pg.65]

In the first step bromocriptine 2 is isomerized to 2a, followed by an attack on proline ring in aminocyclol moiety of the molecule (formation of a new double bound on lO -ll, and bromination). This dibromo-compound 5 is brominated additionally on C-2 -propyl group. Tribromo-compound fi is very lipophilic and practically devoid of pharmacological activity. Hydroxy group and amide groups remain intact after all these reactions. [Pg.82]

A thorough consideration of mechanisms of formation of the organometallic products led to the conclusion " that the j5-decay itself must be the cause of the molecule formation. Neither purely mechanical collisiona substitution, nor thermal chemical reactions, nor radical reactions, nor radiation-induced reactions seem to be responsible for the synthesis reactions. [Pg.88]

The only species which apparently cannot lead directly to molecule formation is a highly charged atom with low kinetic energy. (Even these could undergo thermal reactions if they were not scavenged first.) It thus appears that almost anything can under appropriate conditions lead to molecular products of some sort. [Pg.94]

Note Added in Proof. Since this review was completed, two significant experiments have been done whose results bear strongly on the question of the mechanism of molecule formation following nuclear activation. [Pg.104]

An earlier study by Baumgartner and Reichold (11) shows further that even single metal atoms can react with available CO molecules to produce carbonyls. By irradiating a mixture of powdered Cr(CO)j and UjOg, they were able to catch the fission product Mo and isolate it as Mo(CO)g. This clearly indicates that molecule formation is not dependent on previously formed bonds. The yields of Mo(CO)6 (60%) were too high to represent only the primary fission product molybdenum atoms, and indicate that some short-lived precursors of Mo ( Zr, Nb) may also have formed at least tentative metal-CO bonds, and produced Mo(CO)g after )3-decay. [Pg.228]

The mass spectrometric currents follow largely, but not completely the faradaic current signals. The contributions to the respective faradaic currents resulting from complete oxidation to CO2, which are calculated using the calibration constant K (see Section 13.2), are plotted as dashed lines in the top panels in Fig. 13.3. For the calculations of the partial reaction currents, we assumed six electrons per CO2 molecule formation and considered the shift in the potential scale caused by the time... [Pg.427]

The calibrated m/z = 44 and m/z = 60 ion currents were converted into the respective partial reaction faradaic currents as described above, and are plotted in Fig. 13.3c as dashed (m/z = 44) and dash-dotted (m/z = 60) lines, using electron numbers of 6 electrons per CO2 molecule and 4 electrons per formic acid molecule formation. The calculated partial current for complete methanol oxidation to CO2 contributes only about one-half of the measured faradaic current. The partial current of methanol oxidation to formic acid is in the range of a few percent of the total methanol oxidation current. The remaining difference, after subtracting the PtO formation/reduction currents and pseudocapacitive contributions as described above, is plotted in Fig. 13.3c (top panel) as a dotted line. As mentioned above (see the beginning of Section 13.3.2), we attribute this current difference to the partial current of methanol oxidation to formaldehyde. This way, we were able to extract the partial currents of all three major products during methanol oxidation reaction, which are otherwise not accessible. [Pg.433]

VIII. Reactions of OsHCl(CO)(PiPr3)2 with HX Molecules Formation... [Pg.1]

REACTIONS OF OsHCI(CO)(P Pr3)2 WITH HX MOLECULES FORMATION OF DIHYDROGEN DERIVATIVES... [Pg.19]

The radioactive signals of radio-GC show the 1 -methanol derivates and its common derivates with non radioactive methyl iodide (Fig. lb). The nC-methanol derivates take part in new molecule formation with non-radioactive methyl iodide or/and its derivates on catalyst surface. The C-methyl iodide as a newly formed radioactive product was detected while the selectivity to hydrocarbons sharply decreased (Fig. 2b). [Pg.343]

The state of matter within these regions needs to be determined before the balance of energy and chemistry can be understood. Extreme photon fluxes break all chemical bonds, prevent molecule formation and ionise atoms but as the density of species increases the UV and far-UV photons are absorbed and molecules begin to form. Chemical reactions are, however, slow in the gas phase due to the low temperature, and molecules condense out on the surface of dust particles, perhaps forming ice grains. Once on the surface, molecules continue to be photoprocessed by the starlight as well as by the continual bombardment of cosmic rays. [Pg.121]

Fig. 6. Spreading resistance and SIMS profile from deuterated CZ Si containing an initial uniform concentration of 6 x 1016 cm-3 thermal donors. The high, near-surface concentration is due probably to deuterium molecule formation (Pearton et al., 1986). [Pg.91]

For the case of muonium, nonresonant spin precession in a magnetic field provides a copious source of information about its crystallographic sites and the associated unpaired electron distribution around them (see Chapter 15). Here, the concentration of muons is always too low for molecule formation, and migration to impurities and implantation defects can be kept small by the short muon lifetime and use of pure material and low temperature. [Pg.282]

It is clear that the diffusion of H through semiconductors is a very complicated issue not only does the motion itself involve complex interactions between the impurity and the lattice, but the calculation of a diffusion coefficient requires the inclusion of different charge states plus the interaction of H with itself (molecule formation) and with other defects and impurities in the crystal. Chapter 10 of this volume discusses this problem in more detail. [Pg.632]

AH ° enthalpy of molecule formation under standard conditions (298 K, 1 atm) kJ moU1... [Pg.26]


See other pages where Molecule formation is mentioned: [Pg.352]    [Pg.357]    [Pg.66]    [Pg.99]    [Pg.103]    [Pg.169]    [Pg.89]    [Pg.242]    [Pg.212]    [Pg.419]    [Pg.35]    [Pg.81]    [Pg.620]    [Pg.277]    [Pg.27]    [Pg.40]    [Pg.101]    [Pg.367]    [Pg.324]    [Pg.325]    [Pg.326]   
See also in sourсe #XX -- [ Pg.65 , Pg.66 , Pg.66 , Pg.67 , Pg.68 , Pg.69 , Pg.70 , Pg.70 , Pg.71 , Pg.71 , Pg.72 ]




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