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Kinetic severity function

From these studies it appears that the kinetics of polymerization of THF are closely approximated by equation 42. The equation does not always apply from the beginning of the polymerization and frequently cannot be applied before a steady-state of active centers is achieved. The initiator term, / , in this equation is often a function of several components. Only in the case of preformed trialkyloxo nium ions of the form R30+X is the initiation simple. These results suggest that in order to theoretically study the kinetics of polymerization of THF or to compare the kinetics of THF polymerization in the presence of different gegenions, it is desirable to use preformed trialkyl oxonium salts. Ideally... [Pg.566]

Berger and Wolfe (1996) reported a correlation of hydrolysis data for 12 sulfonylurea herbicides. The use of bond strength or Hammett a constants was impossible because of the complex structures of the compounds. The hydrolysis pathways for this class of compounds are also more complex, but the use of quantum mechanical parameters provided the detailed structural information needed to develop a useful correlation. As a result of the many different functional groups, several reaction pathways are available depending on the substituents. Also, there is a complicating pH effect on the pathways and the kinetics of hydrolysis as shown by product studies. The 12 herbicides used in this study are listed in Table 13.4, and the pseudo first-order hydrolysis rate constants are given in Table 13.5. Figure 13.2 shows the basic structure of these compounds. [Pg.346]

The data in Table II pertaining to pyrolysis conditions shows that all four feedstocks were pyrolyzed under substantially similar conditions, namely steam-to-hydrocarbon weight ratios of 0.9 0.1, residence times of 0.3 sec, reactor exit pressures of 2.0 bar absolute, and reactor exit temperatures of 835°C. Care also was taken to maintain identical axial temperature profiles in the reactor for each of these runs. No unambiguous measure of substrate conversion during pyrolysis is possible for distillate feedstocks of the type used in the present experiments in terms of the empirical kinetic severity function of Zdonik et al. (5), all of the present experiments were conducted at a severity of about 2. [Pg.89]

Wall effects, or the adherence of material to the bare silica capillary wall, has been a difficult problem since the early days of HPCE, particularly for large molecules such as proteins. Small molecules can have, at most, one point of attachment to the wall and the kinetics of ad-sorption/desorption are rapid. Large molecules can have multiple points of attachment resulting in slow kinetics. Several solutions have been proposed, including the use of (a) extreme-pH buffers, (b) high-concentration buffers, (c) amine modifiers, (d) dynamically coated capillaries, and (e) treated or functionalized capillaries. [Pg.249]

Process licensors have tried to supplant this overall assessment by a finer analysis of the severity of operation of a pyrolysis furnace operating on a complex feed. Among the values thus determined are the MCP (Molecular Collision Parameter) for the treat ment of naphthas, based on considerations stemming from the kinetic theory of gases and developed by Wall and Witt of the Selas Corporation, and especially the KSF (Kinetic Severity Function) proposed by Zdonik et al of Stone ami Webster Engineering. [Pg.127]

Analysis of Desorption Kinetics. Several features are evident from the kinetics of desorption. Plots of the logarithm of the area are a linear function of the square root of time in agreement with a diffusion controlled process governed by the equation ... [Pg.172]

Another way to avoid the ambiguity of the coefficient A is to use a non-local kinetic energy functional linked to the non-local exchange energy functional introduced several years ago by Alonso and Girifalco [24]. This approximation. [Pg.235]

In the case of chain reactions and especially the polymerisotiena, the values of G for the disappearance of the monomers are function of several parameters temperature, dose rate, monomer concentration, etc. Thus, their utilization under operating conditions other than those of the author is difficult. Therefore, we preferred to replace these yields by the yield in radicals 6(R0. These yields G(R1 were determined either by the interceptor method (in particular DPPH), or were deduced from the polymerisation rate and from the number average molecular weight with the aid of kinetic formulae. Two procedures were utilized in these cases. [Pg.12]

Comes reported structure in the ionization-efficiency curves of Ar2 and Kr2" which was dependent upon pressure and which he interpreted as being characteristic of a superposition of excitation functions of two excited states. Melton and Hamill reported two breaks above the initial onsets in the ionization-efficiency curves of Ar2 and Kr2, and they interpreted these as being due to the participation of several states in the reaction. Further evidence of the inadequacy of the single-excited-state assumption used in the steady-state kinetic treatments " was provided by the work of Becker and Lampe and DeCorpo and Lampe. These authors used a single-source mass spectrometric technique with a pulsed electron beam and a variable time-delay (reaction time) between the electron beam pulse and an ion-withdrawal pulse. It was shown that the ionization-efficiency curves depend upon the duration of the electron pulse and the time-delay (reaction time) in a manner that is consistent with the overall curve being a superposition of the excitation functions of several families of excited states. In the case of helium, comparison of the overall curves with the known excitation functions permitted some conclusions to be drawn concerning the identity of the reacting states. [Pg.264]

Calculation of the overall kinetic severity function and the true residence timeT Differential equation 2 can advantageously be rewritten in the following form, within the integration limits proper [13, 14] ... [Pg.431]

The integral term on the right side of Equation 9 is called the overall kinetic severity function, BKSF ... [Pg.431]

If the degree of decomposition can accurately be measured with sufficiency over the entire conversion range, the value of the overall kinetical severity function can be calculated according to the left hand side of Equation 9. In the special case, where n = 1, the overall kinetic severity function becomes BKSF -In (1-X). [Pg.432]

The purpose of Introducing the overall kinetic severity function, BKSF, Instead of the degree of decomposition, X, is, first of all, that due to the "scale expansion" effect, the yield curves can be more precisely calculated in the X >0.95 range, which Is of great significance In studying and describing commercial reactors. [Pg.432]

The overall kinetic severity function (BKSF), just as the degree of decomposition, X, defined in Equation 1, is dimensionless, thereby allowing the kinetic model and the yield curves to be directly transferred to larger reactors (tube furnaces). [Pg.432]

Because the yield versus degree of decomposition plots lack the requ,ired precision in the X > 0.95 range, detailed analysis of the experimental data, as well as the model applicable to calculate tube furnaces,- where rather based on the use of the overall kinetic severity function (BKSF). [Pg.435]

Previous sections oresented the so-called kinetic model of naphtha feedstock cracking, which allows the calculation of the degree of decomposition, X, the overall kinetic severity function, BKSF, and the true residence time, T, as functions of the relative length of the reactor, z. [Pg.441]

The first term represents the kinetic rotational energy. This equation is amenable to Mathieu s equation and analytical formulae for the eigenstates are known. However, with computer facilities available nowadays, it is faster to calculate numerically both eigenvalues and eigenfunctions [59]. If necessary, these calculations can be performed for potential functions including several Fourier terms. [Pg.287]

The product distribution in steam cracking is determined by the kinetic severity function (KSF) [374] [533], which is the integral of the rate constant and residence time, 9 ... [Pg.230]


See other pages where Kinetic severity function is mentioned: [Pg.200]    [Pg.530]    [Pg.326]    [Pg.430]    [Pg.77]    [Pg.200]    [Pg.49]    [Pg.16]    [Pg.410]    [Pg.127]    [Pg.200]    [Pg.652]    [Pg.123]    [Pg.534]    [Pg.294]    [Pg.2981]    [Pg.81]    [Pg.191]    [Pg.187]    [Pg.1082]    [Pg.813]    [Pg.588]    [Pg.244]    [Pg.176]    [Pg.423]    [Pg.432]    [Pg.231]   
See also in sourсe #XX -- [ Pg.423 ]




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