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Regimes of control

It will be noted that E can change from a high positive value (for chemical control) to a negligible value for external diffusion control. There can also be a region of negative activation energy corresponding to surface diffusion control, but this is almost never observed and is not considered [Pg.212]


We have shown that known reaction of luminol with peroxydisulphate at low luminol concentrations takes place in the regime of controlled generation of SO ion-radicals at spontaneous destruction of peroxydisulphate. The detection limit for various types of antioxidants in water using this reaction is varied from 10 to 10 M. It is possible also to determine some polluting admixtures present in the atmosphere. The reagent used is the mixture of the luminol, base and K S O, which, once prepai ed, could be used during a working day. [Pg.403]

One can identify at least live major controlling regimes in an MASR gas-liquid mass transfer, liquid-solid mass transfer of A, liquid-solid mass transfer of B, pore diffusion, and surface reaction. Table 17.4 lists the effects of different variables on the reaction for all of these regimes of control. These effects have been classified as major and minor effects. [Pg.536]

Chapter 7 Catalysis by Solids, 2 The Catalyst and Its Microenvironment, 171 Modeling of Solid Catalyzed Reactions, 171 Role of Diffusion in Pellets Catalyst Effectiveness, 183 Effect of External Mass and Heat Transfer, 201 Combined Effects of Internal and External Diffusion, 204 Relative Roles of Mass and Heat Transfer in Internal and External Diffusion, 205 Regimes of Control, 206... [Pg.928]

Figure 6.8 Effectiveness factor as a function of Weisz (observable) modulus 0a and also Thiele modulus 0i. The regimes of control are also shown. Figure 6.8 Effectiveness factor as a function of Weisz (observable) modulus 0a and also Thiele modulus 0i. The regimes of control are also shown.
Figure 4.5.25 Arrhenius plot of effective rate constant for the three regimes of control by reaction, interplay of reaction and pore diffusion, and control by external diffusion. Figure 4.5.25 Arrhenius plot of effective rate constant for the three regimes of control by reaction, interplay of reaction and pore diffusion, and control by external diffusion.
The Pollution Prevention and Control Act 1999 introduced a new regime of control for certain industries, who were required to develop Integrated Pollution Prevention and Control (IPPC). Regulations to implement the provisions of the Act were implemented in August 2000. [Pg.315]

As it has appeared in recent years that many hmdamental aspects of elementary chemical reactions in solution can be understood on the basis of the dependence of reaction rate coefficients on solvent density [2, 3, 4 and 5], increasing attention is paid to reaction kinetics in the gas-to-liquid transition range and supercritical fluids under varying pressure. In this way, the essential differences between the regime of binary collisions in the low-pressure gas phase and tliat of a dense enviromnent with typical many-body interactions become apparent. An extremely useful approach in this respect is the investigation of rate coefficients, reaction yields and concentration-time profiles of some typical model reactions over as wide a pressure range as possible, which pemiits the continuous and well controlled variation of the physical properties of the solvent. Among these the most important are density, polarity and viscosity in a contimiiim description or collision frequency. [Pg.831]

In tlie polarization curve of figure C2.8.4 (solid line), tlie two regimes, activation control and diffusion control, are schematically shown. The anodic and catliodic plateau regions at high anodic and catliodic voltages, respectively, indicate diffusion control tlie current is independent of tlie applied voltage and7 is reached. [Pg.2721]

Over 25 years ago the coking factor of the radiant coil was empirically correlated to operating conditions (48). It has been assumed that the mass transfer of coke precursors from the bulk of the gas to the walls was controlling the rate of deposition (39). Kinetic models (24,49,50) were developed based on the chemical reaction at the wall as a controlling step. Bench-scale data (51—53) appear to indicate that a chemical reaction controls. However, flow regimes of bench-scale reactors are so different from the commercial furnaces that scale-up of bench-scale results caimot be confidently appHed to commercial furnaces. For example. Figure 3 shows the coke deposited on a controlled cylindrical specimen in a continuous stirred tank reactor (CSTR) and the rate of coke deposition. The deposition rate decreases with time and attains a pseudo steady value. Though this is achieved in a matter of rninutes in bench-scale reactors, it takes a few days in a commercial furnace. [Pg.438]

Figure 10.38 shows an input window with three triangular fuzzy sets NB, Z and PB. Each set is positioned in its regime of operation by the centre parameter c so that, for example, NB can only operate on the negative side of the universe of discourse. The width of each set is controlled by parameter ri . [Pg.372]

Depending on the dose and temperature regime, the screening effect azomopine is observed after intoxication by chlorophos. The survival of white rats injected with this preparation is 50% higher than that of control rats. When toxic doses of copper sulfate were injected for 7 days, 70 and 36% of the rats survived. After the simultaneous injection of azomopine, their survival increased to 100 and 70% (74MI1). [Pg.83]

Another important point to consider is that of control. As Fig. 2.17 shows, when the enzymes are almost saturated the rate hardly changes with the concentration of the substrate, implying that the rate of product formation cannot be controlled by [S]. Of course, control is optimally possible in the low substrate concentration regime. Hence, in cases where substrate control of the rate is important, the reaction should ideally proceed in the region of [S] between 5 and IOKm. [Pg.76]

Noteworthy that all the above formulated results can be applied to calculate the statistical characteristics of the products of polycondensation of an arbitrary mixture of monomers with kinetically independent groups under any regime of this process. To determine the values of the elements of the probability transition matrix of corresponding Markov chains it will suffice to calculate only the concentrations Q()- of chemical bonds (ij) at different conversions of functional groups. In the case of equilibrium polycondensation the concentrations Qy are controlled by the thermodynamic parameters, whereas under the nonequilibrium regime of this process they depend on kinetic parameters. [Pg.189]


See other pages where Regimes of control is mentioned: [Pg.157]    [Pg.196]    [Pg.206]    [Pg.431]    [Pg.688]    [Pg.238]    [Pg.212]    [Pg.348]    [Pg.1707]    [Pg.203]    [Pg.69]    [Pg.157]    [Pg.196]    [Pg.206]    [Pg.431]    [Pg.688]    [Pg.238]    [Pg.212]    [Pg.348]    [Pg.1707]    [Pg.203]    [Pg.69]    [Pg.542]    [Pg.830]    [Pg.207]    [Pg.393]    [Pg.216]    [Pg.1346]    [Pg.1883]    [Pg.2564]    [Pg.418]    [Pg.547]    [Pg.169]    [Pg.168]    [Pg.61]    [Pg.50]    [Pg.247]    [Pg.179]    [Pg.250]    [Pg.186]    [Pg.133]    [Pg.18]    [Pg.310]    [Pg.552]    [Pg.708]    [Pg.113]   
See also in sourсe #XX -- [ Pg.190 ]




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