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Reactivity distribution function

Using these distribution functions, we can write the reactive flux correlation function in the compact form... [Pg.206]

To generate the necessary distribution functions, the ratio of is used to approximate the true molecular weight distribution by a Schulz-Zimm distribution. It is also assumed that the reactive functional groups are distributed randomly on the polymer chain. The Schulz-Zimm parameters used to calculate distribution functions and probability generating functions (see below) are defined as follows ... [Pg.195]

Filming of atomic motions in liquids was thus accomplished. More specifically, the above experiment provides atom-atom distribution functions gpv(F, t) as they change during a chemical reaction. It also permits one to monitor temporal variations in the mean density of laser-heated solutions. Finally, it shows that motions of reactive and solvent molecules are strongly correlated the solvent is not an inert medium hosting the reaction [58]. [Pg.275]

The above method enables us to calculate the transition probability at various initial nonequilibrium conditions. As an example, we will consider the transition from the state in which the initial values of the coordinate and velocity of the reactive oscillator are equal to zero.85 In this case, the normalized distribution function has the form... [Pg.167]

Rhodes, P. R. 1975. A probability distribution function for turbulent flows. In Turbulent mixing in nonreactive and reactive mixing. Ed. S. N. B. Murthy. New York, NY Plenum Press. 235-41. [Pg.153]

The kinetics data of the geminate ion recombination in irradiated liquid hydrocarbons obtained by the subpicosecond pulse radiolysis was analyzed by Monte Carlo simulation based on the diffusion in an electric field [77,81,82], The simulation data were convoluted by the response function and fitted to the experimental data. By transforming the time-dependent behavior of cation radicals to the distribution function of cation radical-electron distance, the time-dependent distribution was obtained. Subsequently, the relationship between the space resolution and the space distribution of ionic species was discussed. The space distribution of reactive intermediates produced by radiation is very important for advanced science and technology using ionizing radiation such as nanolithography and nanotechnology [77,82]. [Pg.288]

The degree of conversion inside this volume is constant, but the MWD function qw(n, r), where n is the degree of polymerization, depends on r. This is a reflection of different reaction time in the various layers of the polymer. The residence time distribution function f(r) for the reactive mass in a reactor is determined from rheokinetic considerations, while the MWD for each microvolume qw(n,t) is found for various times t from purely kinetic arguments. The values t and r in the expressions for qw are related to each other via the radial distribution of axial velocity. [Pg.154]

N number of particles, a range of inter-particle forces). If the collision process is binary and non-reactive (post-collision species i, j remain the same as pre-collision species i and j), these indices do not appear in the collision integral, and we can adopt the standard notations of a binary collision turning the two velocities v, v into v, v, with the corresponding abbreviations for the distribution functions /, /i and /, /, respectively. Let W(v, vi —> v, v ) denote the probability for such a transition, then... [Pg.42]

A generalization to reactive and chemical processes is straight forward and indicated by the brackets in the previous two statements. The collision integrals remain bi-linear in the two distribution functions of the two particles entering the collision. We must introduce appropriate Kronecker-Delta s and allow for more than two post-collision particles. We obtain, e.g., for three post-collision particles (in processes such as e + H2 —> e I II I II, dissociation, or e + H —> e + IT1 + e, ionization) for the gain term in the equation for species j ... [Pg.43]

Another proof against inhomogeneous cure in simple epoxy-amine and other systems has been supplied by gel point measurements. The critical conversion at the gel point (cf. Sect. 4) is a sensitive function of any inhomogeneity. For epoxy-amine systems, the gel point conversion has been found to agree well with the prediction of the theory assuming uniform distribution of reactive groups throughout the volume The deviation does not exceed 1 %. In contrast, for free-radical... [Pg.8]

We have in the present chapter shown results from theoretical model system studies of the catalytic reaction mechanisms of three radical enzymes Galatose oxidase. Pyruvate formate-lyase and Ribonucleotide reductase. It is concluded that small models of the key parts of the active sites in combination with the DPT hybrid functional B3LYP and large basis sets provides a good description of the catalytic machineries, with low barriers for the rate determining steps and moderate overall exothermicity. The models employed are furthermore able to reproduce all the observed features in terms of spin distributions and reactive intermediates. [Pg.177]

In collision theory we postulate that not all collisions are reactive only those collisions with energy E or greater will react. Assume that the fraction of collisions which have enough energy to result in reaction is given by Maxwell s distribution function. [Pg.943]

Where Cf is a structural parameter that counts available reactive carbon sites and c, is a coefficient that account for distribution of reactive carbon sites types and catalytic effects and thus a variation in c, may change kinetic parameters. The gas composition vector (F) in J X) may beside the CO2 partial pressure also include such gas partial pressures as KOH since the likelihood that a catalytic site is activated is a function of the partial pressure of the catalyst, the site-catalyst attraction forces and the temperature. Since from Eq. (2) the structural profile invariance SPI assumption is by no means obvious we suggest that a temperature and partial pressure range are always given for the validity of the structural profile invariance assumption. Only if the invariant structural profile assumption is approximately valid a reference profile (/ /) can be used to eliminate the structural profile to form a normalised reactivity (R ) and to determine kinetics up to a constant... [Pg.63]

Confinement may occur via a bonding connectivity between the reactive sjjecies, as in the case of cyclization reactions of polymer chains. The segment-segment distribution function is used to define the one-dimensional effective potential, and the vibrational modes of the polymer backbone are used to... [Pg.364]

However, there is another typ>e of confinement that can be imposed on a reactive system, namely, by a reduction in the effective dimensionality. The simplest examples are those in which the motions of the reactive species are confined to a flat surface or a one-dimensional chain. However, in many systems the connectivity of the configuration space is such that it has effectively a fractal dimension d. The Hausdorf dimension is defined from the behavior of the pair distribution function at sufficiently large R, which varies as that is, the probability of finding the pair with a separation between R and R + dR is proportional to dR. The reduction of the encounter problem from d dimensions to the one dimension R is studied in Section VII A. The important case of reactions on surfaces is considered separately in Section VIIB. [Pg.446]

The steady-state molecular distribution near the saddle point may be written explicitly by invoking two assumptions valid in that region. First, because the reactive and nonreactive modes are nearly uncoupled, the molecular distribution is written as a product of both. Second because near the barrier the reactive flux is directed along the reactive mode coordinate, the distribution function of the n — 1 nonreactive mode system is approximated by its... [Pg.517]

Closure models for terms like the second term in the bracket of the right-hand side are vital to the modeling of turbulent reactive flow processes. It must be noted that as the chemistry becomes more complicated, several such terms will appear, which will make the task of modeling more difficult. Various methods have been used to develop such closure models. These methods are classified into two groups, namely conventional closure models with or without using probability distribution functions... [Pg.136]


See other pages where Reactivity distribution function is mentioned: [Pg.161]    [Pg.156]    [Pg.166]    [Pg.169]    [Pg.255]    [Pg.413]    [Pg.139]    [Pg.39]    [Pg.258]    [Pg.92]    [Pg.567]    [Pg.154]    [Pg.114]    [Pg.496]    [Pg.167]    [Pg.209]    [Pg.200]    [Pg.296]    [Pg.32]    [Pg.148]    [Pg.98]    [Pg.6]    [Pg.741]    [Pg.103]    [Pg.48]    [Pg.117]    [Pg.48]    [Pg.4434]   
See also in sourсe #XX -- [ Pg.220 ]




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