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Equation, Arrhenius mass-energy

The information flow diagram, for a non-isothermal, continuous-flow reactor, in Fig. 1.19, shown previously in Sec. 1.2.5, illustrates the close interlinking and highly interactive nature of the total mass balance, component mass balance, energy balance, rate equation, Arrhenius equation and flow effects F. This close interrelationship often brings about highly complex dynamic behaviour in chemical reactors. [Pg.132]

In the case of both gas and liquid, assuming that the mass-transfer coefficient follows an Arrhenius-type equation, compute the energy of activation" of mass transfer. Are these high or low in comparison with the energy of activation of typical chemical reactions Note that, for dilute solutions, the identity of the diffusing solute need not have been specified in order to obtain the energy of activation" of mass transfer. What other method might be used to determine whether reaction rate or mass-transfer rate controls ... [Pg.87]

Sampling rates at different temperatures have been determined by Huckins et al. (1999) for PAHs at 10,18, and 26 °C, by Rantalainen et al. (2000) for PCDDs, PCDFs, and non-ortho chlorine substituted PCBs at 11 and 19 °C, and by Booij et al. (2003a) for chlorobenzenes, PCBs, and PAHs at 2,13 and 30 °C. The effect of temperature on the sampling rates can be quantified in terms of activation energies (A a) for mass transfer, as modeled by the Arrhenius equation... [Pg.55]

Thus ((Ax)2) becomes independent of the starting configuration of the cluster. The same equation is obtained if one averages over all configurations in a large number of events. The activation energy of diffusion of the center of mass of the cluster, A cm, as derived from an Arrhenius plot, is related to AE+ and AE by... [Pg.255]

Concentration of A Arrhenius constants Arrhenius constant Constant in equation 5.82 Surface area per unit volume Parameter in equation 5.218 Cross-sectional area Concentration of B Stoichiometric constants Parameter in equation 5.218 Concentration of gas in liquid phase Saturation concentration of gas in liquid Concentration of G-mass Concentration of D-mass Dilution rate DamkOhler number Critical dilution rate for wash-out Effective diffusion coefficient Dilution rate for maximum biomass production Dilution rate for CSTF 1 Dilution rate for CSTF 2 Activation energy Enzyme concentration Concentration of active enzyme Active enzyme concentration at time t Initial active enzyme concentration Concentration of inactive enzyme Total enzyme concentration Concentration of enzyme-substrate complex with substance A... [Pg.433]

A pure gas is absorbed into a liquid with which it reacts. The concentration in the liquid is sufficiently low for the mass transfer to be governed by Fick s law and the reaction is first order with respect to the solute gas. It may be assumed that the film theory may be applied to the liquid and that the concentration of solute gas falls from the saturation value to zero across the film. Obtain an expression for the mass transfer rate across the gas-liquid interface in terms of the molecular diffusivity, D, the first-order reaction rate constant ft, the film thickness L and the concentration Cas of solute in a saturated solution. The reaction is initially carried out at 293 K. By what factor will the mass transfer rate across the interface change, if the temperature is raised to 313 K Reaction rate constant at 293 K = 2.5 x 10 6 s 1. Energy of activation for reaction (in Arrhenius equation) = 26430 kJ/kmol. Universal gas constant R = 8.314 kJ/kmol K. Molecular diffusivity D = 10-9 m2/s. Film thickness, L = 10 mm. Solubility of gas at 313 K is 80% of solubility at 293 K. [Pg.248]

Chemical Kinetics Reactor models include chemical kinetics in the mass and energy conservation equations. The two basic laws of kinetics are the law of mass action for the rate of a reaction and the Arrhenius equation for its dependence on temperature. Both of these strictly apply to elementary reactions. More often, laboratory data are... [Pg.9]

Equation (8.8) also shows that (a) a cc no 2, and (b) the apparent activation energy obtained from the slope of the Arrhenius plot of logo- against 1 jT is AW/2es. The square-root dependence of a on n0 and the occurrence of the factor Vz in the activation energy both stem from the control of the ionic dissociation equilibrium by the Law of Mass Action. [Pg.253]

Mathematically, the combustion process has been modelled for the most general three-dimensional case. It is described by a sum of differential equations accounting for the heat and mass transfer in the reacting system under the assumption of energy and mass conservation laws At present, it is impossible to obtain an analytical solution for the three-dimensional form. Therefore, all the available condensed system combustion theories are based on simplified models with one-dimensional or, at best, two-dimensional heat and mass transfer schemes. In these models, the kinetics of the chemical processes taking place in the phases or at the interface is described by an Arrhenius equation (exponential relationship between the reaction rate constant and temperature), and a corresponding reaction order with respect to reactant concentrations. [Pg.188]

Temperature Dependence of Fast Reactions It is to be noted that rate constants for fast (diffusion-controlled) steps are also temperature dependent, since the diffusion coefficient depends on temperature. The usual experimental procedure, suggested by the Arrhenius equation, of plotting In k versus /T will indicate apparent activation energies for diffusion control of approximately 12-15 kJ moP. For fast heterogeneous chemical reactions in which intrinsic chemical and mass transfer rates are of comparable magnitude, care needs to be taken in interpretation of apparent activation energies for the overall process. [Pg.75]

Ionic reactions in the gas phase are usually carried out in mass spectrometers, often at rather low pressures, for example, 10-5 torr. Under these circumstances, reactive complexes that may be formed do not undergo collisions prior to decomposition. Thus, their energy distributions are not Boltzmann, and the reactions cannot be treated in terms of the Arrhenius equation. We have discussed this problem previously (9, JO), and appropriate recipes are well documented (11, 12),... [Pg.30]

The position of the isotope labels is indicated by. A is the Arrhenius preexponential factor in the rate equation E is the experimental activation energy k is the rate coefficient for elimination from the isotopically labelled substrate. Values calculated from the infrared stretching frequencies of the C-H and C-D bonds in the substrates and derived for C-T by assuming harmonicity and using the reduced mass relationship. [Pg.196]

We have made a distinction between an overall reaction and its elementary steps in discussing the law of mass action and the Arrhenius equation. Similarly, the basic kinetic laws treated in this section can be thought of as applying primarily to elementary steps. What relationships exist between these elementary steps and the overall reaction In Table 1.1 we gave as illustrations the rate laws that have been established on the basis of experimental observations for several typical reactions. A close look, for example, at the ammonia synthesis result is enough to convince one that there may be real difficulties with mass action law correlations. This situation can extend even to those cases in which there is apparent agreement with the mass action correlation but other factors, such as unreasonable values of the activation energy, appear. Let us consider another example from Table 1.1, the decomposition of diethyl ether ... [Pg.12]


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See also in sourсe #XX -- [ Pg.76 ]




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