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Single first

The autocatalator model is in many ways closely related to the FONT system, which has a single first-order exothennic reaction step obeying an Arrhenius temperature dependence and for which the role of the autocatalyst is taken by the temperature of the system. An extension of this is tlie Sal nikov model which supports tliennokinetic oscillations in combustion-like systems [48]. This has the fonn ... [Pg.1115]

To illustrate the development of a physical model, a simplified treatment of the reactor, shown in Fig. 8-2 is used. It is assumed that the reac tor is operating isothermaUy and that the inlet and exit volumetric flows and densities are the same. There are two components, A and B, in the reactor, and a single first order reaction of A B takes place. The inlet concentration of A, which we shall call Cj, varies with time. A dynamic mass balance for the concentration of A (c ) can be written as follows ... [Pg.719]

L(f(c)) = e-tDS Hence for a single first-order lag with time delay... [Pg.85]

Figure 23.9 illustrates the model and kinetics scheme for these conditions. We confine our analysis to a single first-order reaction, based on the development of Kunii and Levenspiel (1990 1991, pp. 300-302). However, extension to other reaction orders is straightforward. [Pg.592]

The reaction of a mixture of species A and Aj which interconvert rapidly compared with the reaction under study, can also lead to a single first-order process. In order to resolve the kinetic data, information on the A Aj equilibrium is essential. When the relative amounts of A and A are pH-controlled however (Sec. 1.10.1) or when the products of reaction of A and Ai differ and do not interconvert readily, resolution is also in principle possible. [Pg.9]

Oxidation of 8-Fe(rr) to 8-Fe(oo) by a number of one-electron oxidants gives a single first-order process. After ruling out the more obvious reasons for this observation, it is concluded that condition (1.91) holds, one often referred to as statistical kinetics . For other examples, see Refs. 87 and 88. Even if (1.91) is not strictly satisfied, linear plots may still be obtained. [Pg.22]

In contrast, diols 2a-2g and 3a-3g are not LC materials. Diols 2a-2g were shown to be crystalline by microscopy and by the existence of single first order transitions in the DSC. Diols 3a-3g appeared amorphous in the micrographs and had no first order transitions in the DSC. [Pg.327]

A derivation similar to that for single first-order reactions can be developed for the Denbigh reaction system... [Pg.463]

The first two equations are functions of Ca and Cg only, but now the first equation is coupled to the second because it contains Cg and the second contains Ca. Thus we must solve the two equations simultaneously. This is generally a more complicated problem than for a single first-order differential equation. However, note that both of these equations are linear in Ca and Cg-... [Pg.160]

In this chapter and in Chapter 6 we will usually solve these equations assuming a single first-order irreversible reaction, r = k T)C/. Other orders and multiple reactions could of course be considered, but the equations are much more difficult to solve mathematically, and the solutions are qualitatively the same. We will see that the solutions with these simple kinetics are sufficiently complicated that we do not want to consider more complicated kinetics and energy balances at the same time. [Pg.214]

For the adiabatic reactor we have a unique relation between T and conversion. We can therefore solve for T and eliminate it from the mass-balance equation. For the CSTR the mass-balance equation for a single first-order irreversible reaction... [Pg.221]

To introduce the appropriate features and concepts of reaction in flow systems, we start by considering the simplest irreversible examples—a single first-order step and then two consecutive first-order steps. [Pg.142]

Equations (7.16a) and (7.16b) correspond to our single first-order exothermic reaction occurring in 9 CSTR fed by reactants at the oven temperature, with the exponential approximation made to the Arrhenius temperature dependence of the reaction rate constant. Stationary-state solutions cor-repond to values of the dimensionless concentration a and temperature rise 9 for which da/dr and dO/dt are simultaneously equal to zero, i.e. [Pg.186]

The species boundary condition at the stagnation surface follows from the fact that the diffusive mass flux in the fluid is balanced by a heterogeneous chemical reaction rate on the surface. In general, this can involve multiple and complex surface reactions and complex descriptions of the molecular diffusion. Here, however, we restrict attention to a single species that is dilute in a carrier gas and a single first-order surface reaction. Under these circumstances the surface reaction rate (mass of Y consumed per unit surface area) is given... [Pg.292]

We shall now proceed to compare the three basic types of reactor—batch, tubular and stirred tank—in terms of their performance in carrying out a single first order irreversible reaction ... [Pg.51]

Derive the material and energy balance equations for a nonadiabatic CSTR where a single first-order reaction A —> B takes place. [Pg.132]

In a dynamic experiment, the temperature and the conversion vary with time. Since the temperature is forced to follow the imposed scan rate, by varying the scan rate, the peak appears at different times, that is, at different temperatures (Figure 11.10). This allows for kinetic analysis of the thermograms. The principles of such evaluations can be demonstrated on a single first-order reaction, as an example. The temperature varies linearly with time ... [Pg.296]

The factor P is called the autocatalytic factor for P = 0, the reaction becomes a single first-order reaction. With increasing P, the autocatalytic character becomes more important. [Pg.317]

Sparks and Jardine (1984) studied the kinetics of potassium adsorption on kaolinite, montmorillonite, and vermiculite (Fig. 2.1) and found that a single first-order reaction described the data well for kaolinite and smectite while two first-order reactions described adsorption on vermiculite. One will note deviations from first-order kinetics at longer time periods, particularly for montmorillonite and vermiculite, because a quasi-equilibrium state is reached. These deviations result because first-order equations are only applicable far from equilibrium (Skopp, 1986) back reactions could be occurring at longer reaction times. [Pg.14]

The model fit variances are given in Table IV and calculated rate parameters for the two reactions in Table V. In nearly all cases an improvement in model fit was observed. This is typified by the comparison between the fit gg a single first-order and double first-order (DFO) model to the 0 Co data, as shown in Figure 5. Although the DFO model shows considerable improvement over single-site models, residual plots indicate a small systematic deviation at higher concentrations. This is discussed further in the following section. [Pg.58]

Figure 5. Comparison of single first-order and double first-order models to 0co mixing-cell data. Figure 5. Comparison of single first-order and double first-order models to 0co mixing-cell data.
Side effects. Because clobazam has been widely used as an anxiolytic, its side effects are well known and essentially similar to those of the other benzodiazepines. Thus sedation, dizziness, ataxia, blurred vision and diplopia are the most commonly reported in epileptic patients. One of the most problematic features of clobazam is its tendency to produce tolerance, an effect which may occur more frequently with clobazam than with the other widely used benzodiazepine, clonazepam. It has been estimated that at least 50% of patients develop tolerance. Tolerance to the sedative effects of the drug develop more rapidly than those to the antiepileptic effect. Clobazam should be considered as adjunctive therapy whenever treatment with a single first-line drug has proven to be ineffective. [Pg.311]

This feature is illustrated in Fig. 9, which compares the solution of the ideal PFR, ideal CSTR, and the Danckwerts model [Eqs. (146)—(147)] with the twomode convection model [Eqs. (140) (141)] for the case of steady-state and single first-order homogeneous reaction of the form A —> B. The solution of the steady-state Danckwerts model is given by... [Pg.243]

Emig, Hofmann, Hoffmann and Fiand [14] proved experimentally that the criteria of Earkelew, of Agnew and Potter and of McGreavy and Adderley all predict runaway remarkedly well for a single first order reaction in a cooled catalytic tubular reactor. [Pg.318]

Fig. 8. Acceleration of the oxidative refolding of RNase T1 by PPI and PDI. The increase in fluorescence at 320 nm is shown as a function of the time of reoxidation. The final conditions were 2.5 fiM RNase T1 in 0.1 Af Tris-HCl, 0.2 M GdmCl, 2 mM EDTA, 3 mAf glycine, 0.4 mAf oxidized glutathione, and 4 mAf reduced glutathione at pH 7.8 and 25°C. Reoxidation ( ) in the absence of PPI and PDI, (O) in the presence of 1.4 tiM PPI, (A) in the presence of 1.6 fiM PDI, and (A) in the presence of both 1.6 fiM PDI and 1.4 /uAf PPI. In all experiments more than 90% of the observed kinetics were well approximated by single first-order processes, as indicated by the continuous lines. The respective time constants (t) are ( ) t = 4300 sec, (O) r = 2270 sec, (A) t = 1500 sec, (A) T = 650 sec. In all cases the initial fluorescence signal was about 10% of the final emission of the native protein. From Schonbrunner and Schmid (1992). Fig. 8. Acceleration of the oxidative refolding of RNase T1 by PPI and PDI. The increase in fluorescence at 320 nm is shown as a function of the time of reoxidation. The final conditions were 2.5 fiM RNase T1 in 0.1 Af Tris-HCl, 0.2 M GdmCl, 2 mM EDTA, 3 mAf glycine, 0.4 mAf oxidized glutathione, and 4 mAf reduced glutathione at pH 7.8 and 25°C. Reoxidation ( ) in the absence of PPI and PDI, (O) in the presence of 1.4 tiM PPI, (A) in the presence of 1.6 fiM PDI, and (A) in the presence of both 1.6 fiM PDI and 1.4 /uAf PPI. In all experiments more than 90% of the observed kinetics were well approximated by single first-order processes, as indicated by the continuous lines. The respective time constants (t) are ( ) t = 4300 sec, (O) r = 2270 sec, (A) t = 1500 sec, (A) T = 650 sec. In all cases the initial fluorescence signal was about 10% of the final emission of the native protein. From Schonbrunner and Schmid (1992).

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