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Single Instantaneous Reactions

In contrast with the two-film model the reaction plane is not fixed in space since the element at the surface is considered to have a finite capacity, transients have to be considered. In the zone between the interface at y = 0 and the location of the reaction plane at yi(t) a non-steady-state balance on A leads to  [Pg.328]

The solution of these equations is well known. It may be obtained by the Laplace transform as  [Pg.328]

In the reaction plane yi(t) = 2Py/t the stoichiometry requires that Nja = —(Ng/b). Writing the fluxes in terms of Pick s law leads to an additional relation that enables /J to be determined. The result is  [Pg.329]

An example of the evolution of the profiles with time is given in Fig. 6.4.a-l. [Pg.329]

The average rate of absorption at the surface is, with Higbie s uniform age, i  [Pg.330]


To determine the reaction rate at a given instant in the course of the reaction, we should make our two concentration measurements as close together in time as possible. In other words, to determine the rate at a single instant we determine the slope of the tangent to the plot of concentration against time at the time of interest (Fig. 13.4). This slope is called the instantaneous rate of the reaction. The instantaneous reaction rate changes in the course of the reaction (Fig. 13.5). [Pg.653]

Finally, to conclude our discussion on coupling with chemistry, we should note that in principle fairly complex reaction schemes can be used to define the reaction source terms. However, as in single-phase flows, adding many fast chemical reactions can lead to slow convergence in CFD simulations, and the user is advised to attempt to eliminate instantaneous reaction steps whenever possible. The question of determining the rate constants (and their dependence on temperature) is also an important consideration. Ideally, this should be done under laboratory conditions for which the mass/heat-transfer rates are all faster than those likely to occur in the production-scale reactor. Note that it is not necessary to completely eliminate mass/heat-transfer limitations to determine usable rate parameters. Indeed, as long as the rate parameters found in the lab are reliable under well-mixed (vs. perfect-mixed) conditions, the actual mass/ heat-transfer rates in the reactor will be lower, leading to accurate predictions of chemical species under mass/heat-transfer-limited conditions. [Pg.300]

I l urc 6. Combined effect of chemical reaction and mass transport. Single instantaneous inputs of A nd ( are made to ( ) a well-mixed closed system and (b) a continuously stirred tank reactor (CSTR). I ollutant C is conservative tracer its concentration is constant in the closed system, and decreases in i In- ( STR because of the outward flux of water. Chemical A is transformed into product B according In liisl-order kinetics. The sum [A] + [B]) is constant in the closed system, but decreases in the CSTR, Loss of A from the CSTR arises from both chemical reaction and mass transport. [Pg.20]

If only a single fast (or instantaneous) reaction is involved, relatively slow mixing and state of segregation may cause a change in the apparent reaction rate (reduction in plant capacity), but no... [Pg.644]

Figure 1 The <5 N of reactant and product N pools of a single unidirectional reaction as a function of the fraction of the initial reactant supply that is left unconsumed, for two different models of reactant supply and consumption, following the approximate equations given in the text. The Rayleigh model (black lines) applies when a closed pool of reactant N is consumed. The steady-state model (gray lines) applies when reactant N is supplied continuously. The same isotopic parameters, an isotope effect e) of 5%o and a <5 N of 5%o for the initial reactant supply, are used for both the Rayleigh and steady-state models, e is approximately equal to the isotopic difference between reactant N and its product (the instantaneous product in the case of the Rayleigh model). Figure 1 The <5 N of reactant and product N pools of a single unidirectional reaction as a function of the fraction of the initial reactant supply that is left unconsumed, for two different models of reactant supply and consumption, following the approximate equations given in the text. The Rayleigh model (black lines) applies when a closed pool of reactant N is consumed. The steady-state model (gray lines) applies when reactant N is supplied continuously. The same isotopic parameters, an isotope effect e) of 5%o and a <5 N of 5%o for the initial reactant supply, are used for both the Rayleigh and steady-state models, e is approximately equal to the isotopic difference between reactant N and its product (the instantaneous product in the case of the Rayleigh model).
Assigning instantaneous substrate concentration to S, instantaneous reaction time to t, steady-state kinetics of Michaelis-Menten enzyme on single substrate follows Equ.(l). [Pg.159]

Precatalytic Reactions and Xpre. The catalyst precursor must transform under reaction conditions into intermediates to obtain an active system. This transformation may involve, in a small number of cases, only a single elementary step, for example, the dissociation of a ligand from a transition-metal complex. However, a series of elementary reaction steps are usually required to convert the catalyst precursor. Useful examples include (1) the degradation of a polynuclear precursor to mononuclear intermediates, (2) the modification of a precursor with a ligand L which is used to control selectivity, and (3) the transformation of finely divided metal. The characteristic time scale for the precatalytic reaction will be denoted tpre, and the instantaneous reaction rate will be denoted Ppre- Precatalytic phenomena and the associated induction periods have been directly monitored in a number of in situ spectroscopic studies using a variety of mononuclear, dinuclear, polynuclear, and metallic precursors (11). [Pg.2111]

The predictions of this model have to be considered in terms of the assumptions made. In the context of ants fighting off an intruder, it is likely that the chemical signal will be released over a period of time, or several times, or both, whereas the model assumes a single, instantaneous emission. This will result in distorted, overlapping signals, but the principle of different active spaces for the two behavioral reactions will still hold. A more serious problem is presented by local air movements, which will tend to move pockets of air containing high concentrations of the pheromone, away from the source, much faster than if they had been transmitted by molecular diffusion. Under these conditions... [Pg.436]

Thermal methods in kinetic modelling. Methods for the estimation of thermokinetic parameters based on experiments in a reaction calorimeter will be discussed below. As mentioned in section 5.4.4.3, instantaneous heat evolved due to a single reaction is directly proportional to the reaction rate. Assume that the reaction is of first order. Then for isothermal operation ... [Pg.320]

Adsorption and desorption. The user can choose to handle this using either temperature-corrected first order reaction kinetics, in which case the concentrations are always moving towards equilibrium but never quite reach it, or he can use a Freundlich isotherm, in which instantaneous equilibrium is assumed. With the Freundlich method, he can elect either to use a single-valued isotherm or a non-single-valued one. This was included in the model because there is experimental evidence which suggests that pesticides do not always follow the same curve on desorption as they do on adsorption. [Pg.134]

In this situation, transport equations similar to those discussed previously can be applied. For example, by assuming sorption to be essentially instantaneous, the advective-dispersion equation with a reaction term (Saiers and Hornberger 1996) can be considered. Alternatively, CTRW transport equations with a single ti/Ci, t) can be applied or two different time spectra (for the dispersive transport and for the distribution of transfer times between mobile and immobile—diffusion, sorption— states can be treated Berkowitz et al. 2008). [Pg.233]


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