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Models mixed kinetics

Substrate and product inhibitions analyses involved considerations of competitive, uncompetitive, non-competitive and mixed inhibition models. The kinetic studies of the enantiomeric hydrolysis reaction in the membrane reactor included inhibition effects by substrate (ibuprofen ester) and product (2-ethoxyethanol) while varying substrate concentration (5-50 mmol-I ). The initial reaction rate obtained from experimental data was used in the primary (Hanes-Woolf plot) and secondary plots (1/Vmax versus inhibitor concentration), which gave estimates of substrate inhibition (K[s) and product inhibition constants (A jp). The inhibitor constant (K[s or K[v) is a measure of enzyme-inhibitor affinity. It is the dissociation constant of the enzyme-inhibitor complex. [Pg.131]

Figure 1.52. Uniformly mixed kinetics model. q volume flow rate (m /s), Cj initial concentration (molal), 1 height (m), r radius (m), C concentration (molal), V volume of the system (m ). Figure 1.52. Uniformly mixed kinetics model. q volume flow rate (m /s), Cj initial concentration (molal), 1 height (m), r radius (m), C concentration (molal), V volume of the system (m ).
Bokkers, G. A., Van Sint Annaland, M., and Kuipers, J. A. M., Comparison of continuum models using kinetic theory of granular flow with discrete particle models and experiments extent of particle mixing induced by bubbles. Proceedings of Fluidization XI, May 9-14, 2004, 187-194, Naples, Italy (2004). [Pg.146]

Here we focus on the issue of how to build computational models of biochemical reaction systems. The two foci of the chapter are on modeling chemical kinetics in well mixed systems using ordinary differential equations and on introducing the basic mathematics of the processes that transport material into and out of (and within) cells and tissues. The tools of chemical kinetics and mass transport are essential components in the toolbox for simulation and analysis of living biochemical systems. [Pg.41]

A more advanced model was suggested very recently by [78] based on the adsorption isotherm for proteins given by Eq. (2.124). In addition to diffusion of the molecules in the bulk, a kinetic process was assumed equivalent to the mechanism used in the mixed kinetic model. The configuration changes, i.e. orientation of a globular protein molecule to the surface, were characterised by one rate constant k. The following Fig. 4.7 shows model calculations where the following parameters were used coi = 2.5-10 m /mol, W2 = 5.010 m /mol (i.e. coj/ ] = 2), a i = 200. These parameters correspond to those for HSA adsorbed at the water/air interface [79]. The diffusion coefficient was taken to be D = lO cmVs and the protein concentration as 10 mol/I. The equilibrium surface pressure of the protein solutions was taken to be 20 mN/m, typical for HSA at this concentration. It should be noted first that the time required for an experimentally observable decrease of the surface tension, say by 0.5 mN/m, is about 3100 s... [Pg.305]

Additional short and long time approximations have been summarised by Fainerman et al. [99] based on diffusion-controlled, barrier-controlled and mixed kinetic models. An analysis of the known long time approximations was given by Makievski et al. [15]. They compared the long time approximations given by Hansen and by Joos. While Hansen s approximation [22, 117] yields... [Pg.321]

Mixed Kinetics Model Overall, the dissolution rate is defined by the kinetics of chemical processes and mass transfer through the Nernst layer. At that, mostly chemical processes within the kinetic zone and physical processes in the diffuse one are tied up with each other and affect each other. A successful attempt to tie these different processes is the mixed kinetics model. [Pg.235]

Various approaches have been adopted for the simulation of mass transport across the HFSLM. These approaches can be classified in two major groups (1) where the ratedetermining step is the diffusion across the boundary layers (diffusional mass transport) and (2) where the rate of interfacial reactions (complexation and decomplexation of metal ion) is comparable to the diffusion processes. The latter approach is also known as mixed kinetic model approach. Both of these approaches will be discussed in the following sections. [Pg.803]

B. W. Madsen and M. E. Wadsworth, A Mixed Kinetics Dump Leaching Model for Ores (Con-... [Pg.538]

Reactions are limited by the slowest step in the overall process. If the reaction flux (/j(, mol/m sec) for a dissolving solid is fast compared to the diffusion flux (Jj) mol/m sec), the dissolution process is limited by the rate of transfer of reactants or products between the solution and the solid s surface. When Jji Jj), the overall rate of dissolution is controlled by mixed kinetics, which is modeled by convolving the models for both the dissolution and transport process. [Pg.140]

This model assumes laminar flow past a flat plate with L = 0.001 m and q = 0.001 m/sec (Table 7.3). Figure 7.7 shows that the rate of gypsum dissolution changes from reaction limited at T < 0°C to transport limited for T > 100° C. The apparent activation energy for the mixed kinetics model ranges from 22 kJ/ mol at 0°C to 5 kJ/mol at 100°C. [Pg.147]

The equilibrium and dynamic aspects of surface tension and adsorption of surfactants at the air-water interface are important factors in foam film stability [82]. Dynamic adsorption models with the diffusion-controlled and mixed-kinetic mechanisms are discussed in some surfactant solution litera-... [Pg.110]

In diffusion-controlled adsorption models, one assumes that there is no activation energy barrier to the transfer of surfactant molecules between the subsurface and the surface [85]. Thus diffusion is the only mechanism needed in establishing adsorption equilibrium. The time required for the molecules to transfer from the bulk to the subsurface is much longer than the time required for equilibration between the surface and the subsurface. On the contrary, if the adsorption or desorption rate at the interface is slow or comparable to the diffusion rate, the adsorption process is significant. This model is called the mixed-kinetic adsorption model. This condition may depend not only on the properties of the system but also on the diffusion length and possibly on convection conditions. The diffusion-controlled model of Eqs. (3) and (4) have been given by Fainerman et al. [86,87]. [Pg.111]

In a continuous-flow chemical reactor, the concern is not only with probabilistic transitions among chemical species but also with probabilistic liansitions of each chemical species between the interior and exterior of the reactor. Pippel and Philipp [8] used Markov chains for simulating the dynamics of a chemical system. In their approach, the kinetics of a chemical reaction are treated deterministically and the flow through the system are treated stochastically by means of a Markov chain. Shinnar et al. [9] superimposed the kinetics of the first order chemical reactions on a stochastically modeled mixing process to characterize the performance of a continuous-flow reactor and compared it with that of the corresponding batch reactor. Most stochastic approaches to analysis and modeling of chemical reactions in a flow system have combined deterministic chemical kinetics and stochastic flows. [Pg.542]

Naturally, Eq. (4) is an approximation and valid only if the supposition of proportionality in Eq. (3) proves to be true. In reality, the time dependence of the degree of homogeneity, i.e. the kinetics of a mixing process is not so simple function of the actual deviation of M from the perfectly mixed state. Generally, it is a more intricate function of the spatial distribution of components, and also depends on the specific mechanism of mixing. Therefore, to elucidate mixing kinetics, careful experiments and more sophisticated description or mathematical models are needed. [Pg.636]


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