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Atomization kinetics

Nucleophilic reactivity of the sulfur atom has received most attention. When neutral or very acidic medium is used, the nucleophilic reactivity occurs through the exocyclic sulfur atom. Kinetic studies (110) measure this nucleophilicity- towards methyl iodide for various 3-methyl-A-4-thiazoline-2-thiones. Rate constants are 200 times greater for these compounds than for the isomeric 2-(methylthio)thiazole. Thus 3-(2-pyridyl)-A-4-thiazoline-2-thione reacts at sulfur with methyl iodide (111). Methyl substitution on the ring doubles the rate constant. This high reactivity at sulfur means that, even when an amino (112, 113) or imino group (114) occupies the 5-position of the ring, alkylation takes place on sulfiu. For the same reason, 2-acetonyi derivatives are sometimes observed as by-products in the heterocyclization reaction of dithiocarba-mates with a-haloketones (115, 116). [Pg.391]

Baechler and coworkers204, have also studied the kinetics of the thermal isomerization of allylic sulfoxides and suggested a dissociative free radical mechanism. This process, depicted in equation 58, would account for the positive activation entropy, dramatic rate acceleration upon substitution at the a-allylic position, and relative insensitivity to changes in solvent polarity. Such a homolytic dissociative recombination process is also compatible with a similar study by Kwart and Benko204b employing heavy-atom kinetic isotope effects. [Pg.745]

The structure of the Z-isomer was determined (Figure 21) indicating considerable pyramidal distortion at the germanium, reflected in the large dihedral angle (36°) at these atoms. Kinetic investigations H-NMR) of the Z-E isomerization in CgDg indicated that the equilibrium is shifted to the Z-isomer [(E)/(Z) values are 0.490 at 40.1 °C and 0.368 at 17.0 °C],... [Pg.559]

Film topography as a function of the metal atom kinetic energy will be measured. [Pg.469]

P. K. Acharya, L. J. Bartolotti, S. B. Sears, and R. G. Parr, An atomic kinetic energy functional with full Weizsacker correction. Proc. Natl. Acad. Sci. USA 77, 6978-6982 (1980). [Pg.480]

Accdg to the late W.H. Rinkenbach (Ref 51) "Pressure is described as a thermodynamic coordinate , and this is correct. Basically, it is an increase in the number of molecular or atomic kinetic impacts per unit area of a container. This may be caused by increase in temperature or by increase in the number of molecules or atoms per unit volume... [Pg.483]

The production of species i (number of moles per unit volume and time) is the velocity of reaction,. In the same sense, one understands the molar flux, jh of particles / per unit cross section and unit time. In a linear theory, the rate and the deviation from equilibrium are proportional to each other. The factors of proportionality are called reaction rate constants and transport coefficients respectively. They are state properties and thus depend only on the (local) thermodynamic state variables and not on their derivatives. They can be rationalized by crystal dynamics and atomic kinetics with the help of statistical theories. Irreversible thermodynamics is the theory of the rates of chemical processes in both spatially homogeneous systems (homogeneous reactions) and inhomogeneous systems (transport processes). If transport processes occur in multiphase systems, one is dealing with heterogeneous reactions. Heterogeneous systems stop reacting once one or more of the reactants are consumed and the systems became nonvariant. [Pg.3]

Let us now consider the atomic kinetic equation (4.70). There are also two contributions to the collision integral I (Pt), the first one leaves the incident atom unchanged. The relevant processes are... [Pg.246]

The experimental results were analyzed using an integrated approach. To obtain the temporal evolution of the temperature and the density profiles of the bulk plasma, the experimental hot-electron temperature was used as an initial condition for the 1D-FP code [26]. The number of hot electrons in the distribution function were adjusted according to the assumed laser absorption. The FP code is coupled to the 1-D radiation hydrodynamic simulation ILESTA [27]. The electron (or ion) heating rate from hot electrons is first calculated by the Fokker-Planck transport model and is then added to the energy equation for the electrons (or ions) in ILESTA-1D. Results were then used to drive an atomic kinetics package [28] to obtain the temporal evolution of the Ka lines from partially ionized Cl ions. [Pg.204]

Fig. 10.4. Comparison of experimental results with steady state solutions from the atomic kinetics code for a C2H3CI and b Al plasmas. Time- and space-averaged temperatures of 120 and 70 eV are obtained, respectively... Fig. 10.4. Comparison of experimental results with steady state solutions from the atomic kinetics code for a C2H3CI and b Al plasmas. Time- and space-averaged temperatures of 120 and 70 eV are obtained, respectively...
Fig. 10.6. Time dependences of K lines from partially ionized Cl ions, calculated by the atomic kinetics code. Temperature and density were given by the Fokker-Planck calculations shown in Fig. 10.5... Fig. 10.6. Time dependences of K lines from partially ionized Cl ions, calculated by the atomic kinetics code. Temperature and density were given by the Fokker-Planck calculations shown in Fig. 10.5...
Fig. 10.7. Comparison of the time-integrated Cl Ka line intensities with the atomic kinetics code. Normalization was performed for the Ka Cl9+ line... Fig. 10.7. Comparison of the time-integrated Cl Ka line intensities with the atomic kinetics code. Normalization was performed for the Ka Cl9+ line...
Figure 4 Quasi-classical opacity function P(p), defined as the fraction of reactive trajectories for a given impact parameter, p (solid line). Also plotted is Krei, the component of the relative incident-target H atom kinetic energy parallel to the surface, following a non-reactive collision (dotted line). The results correspond to H-on-D for the flat-surface potential described in the text. Figure 4 Quasi-classical opacity function P(p), defined as the fraction of reactive trajectories for a given impact parameter, p (solid line). Also plotted is Krei, the component of the relative incident-target H atom kinetic energy parallel to the surface, following a non-reactive collision (dotted line). The results correspond to H-on-D for the flat-surface potential described in the text.
A wide variety of plasma diagnostic applications is available from the measurement of the relatively simple X-ray spectra of He-like ions [1] and references therein. The n = 2 and n = 3 X-ray spectra from many mid- and high-Z He-like ions have been studied in tokamak plasmas [2-4] and in solar flares [5,6]. The high n Rydberg series of medium Z helium-like ions have been observed from Z-pinches [7,8], laser-produced plasmas [9], exploding wires [8], the solar corona [10], tokamaks [11-13] and ion traps [14]. Always associated with X-ray emission from these two electron systems are satellite lines from lithium-like ions. Comparison of observed X-ray spectra with calculated transitions can provide tests of atomic kinetics models and structure calculations for helium- and lithium-like ions. From wavelength measurements, a systematic study of the n and Z dependence of atomic potentials may be undertaken. From the satellite line intensities, the dynamics of level population by dielectronic recombination and inner-shell excitation may be addressed. [Pg.163]


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See also in sourсe #XX -- [ Pg.34 ]




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