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Diffusional steady-state

THE DIFFUSIONAL STEADY-STATE (dSS) APPROACH 2.4.1 The Essence of the dSS Approach... [Pg.170]

Uniqueness of electro-diffusional steady states is expected and should be proved for one-dimensional systems with less than three alterations of sign N. [Pg.157]

Such progresses have obviously opened new frontiers to electrochemistry. Yet, several other areas have also become accessible to the discipline because of the unique properties of ultramicroelectrodes. Among these, and besides the two above examples, we wish to restrict our presentation to electrochemistry in the nanosecond time scale, in the one hand, and to diffusional steady state voltanunetry in the other hand. These topics will be discussed based on examples taken from our research in organic or organometallic reactivity. [Pg.626]

Finally, to conclude this introduction, and to avoid any possible confusion in the terminology, we wish to define briefly what is an ultramicroelectrode (at least in our sense ). When their interfacial properties are to be considered identical with those of any other electrode of a larger dimension, ultramicroelectrodes must remain much larger than the double layer thickness. This sets a lower dimension of a few tens of A for ultramicroelectrodes.On the other hand, if diffusional steady state voltammetry has to be observed without significant interference of convection, they must be smaller than convective layers, which sets an upper limit of a few tens of /im. Between these limits, all ultramicroelectrodes possess identical intrinsic physico-chemical properties. However, their behavior (viz. ohmic drop, steady state or transient currents, etc) obviously depends on the medium and the time-scale considered. ... [Pg.626]

Use of Operating Curve Frequently, it is not possible to assume that = 0 as in Example 2, owing to diffusional resistance in the liquid phase or to the accumulation of solute in the hquid stream. When the back pressure cannot be neglected, it is necessary to supplement the equations with a material balance representing the operating line or curve. In view of the countercurrent flows into and from the differential section of packing shown in Fig. 14-3, a steady-state material balance leads to the fohowing equivalent relations ... [Pg.1354]

The partial pressures in the rate equations are those in the vicinity of the catalyst surface. In the presence of diffusional resistance, in the steady state the rate of diffusion through the stagnant film equals the rate of chemical reaction. For the reaction A -1- B C -1-. . . , with rate of diffusion of A limited. [Pg.2095]

The estimation of the diffusional flux to a clean surface of a single spherical bubble moving with a constant velocity relative to a liquid medium requires the solution of the equation for convective diffusion for the component that dissolves in the continuous phase. For steady-state incompressible axisym-metric flow, the equation for convective diffusion in spherical coordinates is approximated by... [Pg.347]

The anions, which are not involved in the reaction v = 0, should not move in the steady state [i.e., in Eq. (4.17), J = 0]. This implies that the diffusional component of their flux to the surface should be fully compensated by a migration component away from the surface (Fig. 4.3). [Pg.59]

The following example, taken from Welty et al. ( 1976), illustrates the solution approach to a steady-state, one-dimensional, diffusional or heat conduction problem. [Pg.227]

For the diffusional monitor the steady state mass transport... [Pg.935]

Figure 4 Diffusion across a membrane with aqueous diffusional layers. cbI and cb2 are the concentrations of bulk solutions 1 and 2, respectively. The thicknesses of the aqueous diffusion layers are /i, and h2. The membrane has a thickness of hm. Equilibrium is assumed at the interfaces of the membrane and the aqueous diffusion layers. At steady state, the concentrations remain constant at all points in the membrane and in the aqueous diffusion layers. The concentration profiles inside the membrane and aqueous diffusion layers are linear, and the flux is constant. Figure 4 Diffusion across a membrane with aqueous diffusional layers. cbI and cb2 are the concentrations of bulk solutions 1 and 2, respectively. The thicknesses of the aqueous diffusion layers are /i, and h2. The membrane has a thickness of hm. Equilibrium is assumed at the interfaces of the membrane and the aqueous diffusion layers. At steady state, the concentrations remain constant at all points in the membrane and in the aqueous diffusion layers. The concentration profiles inside the membrane and aqueous diffusion layers are linear, and the flux is constant.
At steady state, changes in the concentrations of drug and metabolite with distance involving diffusional and concurrent bioconversion kinetics are given by... [Pg.305]

In many situations of practical interest, an appreciable drop in concentration arises between a fluid phase and the external surface of the catalyst because of diffusional resistance. In the steady state, the rate of diffusion to the external surface equals the rate of input to the pore mouth, rd = kga(Cg-Cs) = D(dC/dr)r=R>c=Cs (7.37)... [Pg.736]

When diffusional resistance occurs at the external surface of nonporous catalyst, the rate relations at steady state are... [Pg.763]

At steady state the diffusional and surface reaction rates are equal,... [Pg.764]

A reactant diffuses into a stagnant liquid film where the concentration of excess reactant B remains essentially constant at Cb0. At the inlet face the concentration is Cal, Making the material balance over a differential dz of the distance leads to the second order diffusional equation. In the steady state and for unit cross section,... [Pg.839]

In the steady state the diffusional rates through the gas and liquid films equal the rate of surface reaction. The concentration in the gas phase is Ag, at the interface At and at the surface As. A is the equilibrium value in the liquid.For a reaction of order m,... [Pg.849]

This problem illustrates the solution approach to a one-dimensional, non-steady-state, diffusional problem, as demonstrated in the simulation examples, DRY and BNZDYN. The system is represented in Fig. 4.2. Water diffuses through a porous solid, to the surface, where it evaporates into the atmosphere. [Pg.175]

This may be partly the result of increased steric crowding in the transition state of transalkylation. Another contributory factor to the increased selectivity in ZSM-5 is the higher diffusion rate of ethylbenzene vs m-/o-xylene in ZSM-5 and hence a higher steady state concentration ratio [EB]/[xyl] in the zeolite interior than in the outside phase. Diffusional restriction for xylenes vs ethylbenzene may also be indicated by the better selectivity of synthetic mordenite vs ZSM-4, since the former had a larger crystal size. [Pg.280]

Contents Introduction. - Basic Equations. -Diffusional Transport - Digitally. - Handling of Boundary Problems. - Implicit Techniques and Other Complications. - Accuracy and Choice. -Non-Diffusional Concentration Changes. - The Laplace Equation and Other Steady-State Systems. - Programming Examples. - Index. [Pg.120]

If Da = 1 is defined as the transition between diffusionally controlled and kinetically controlled regimes, an inverse relationship is observed between the particle diameter and the system pressure and temperature for a fixed Da. Thus, for a system to be kinetically controlled, combustion temperatures need to be low (or the particle size has to be very small, so that the diffusive time scales are short relative to the kinetic time scale). Often for small particle diameters, the particle loses so much heat, so rapidly, that extinction occurs. Thus, the particle temperature is nearly the same as the gas temperature and to maintain a steady-state burning rate in the kinetically controlled regime, the ambient temperatures need to be high enough to sustain reaction. The above equation also shows that large particles at high pressure likely experience diffusion-controlled combustion, and small particles at low pressures often lead to kinetically controlled combustion. [Pg.528]

This equation holds at the steady state. In a diffusional regime and in absence of rigid interfacial films, Ri is generally negligible relative to R and R . [Pg.241]


See other pages where Diffusional steady-state is mentioned: [Pg.148]    [Pg.171]    [Pg.262]    [Pg.43]    [Pg.148]    [Pg.171]    [Pg.262]    [Pg.43]    [Pg.395]    [Pg.145]    [Pg.577]    [Pg.59]    [Pg.511]    [Pg.31]    [Pg.305]    [Pg.251]    [Pg.438]    [Pg.287]    [Pg.385]    [Pg.352]    [Pg.27]    [Pg.141]    [Pg.522]    [Pg.238]    [Pg.100]    [Pg.24]    [Pg.204]   


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Diffusional steady-state approach

Diffusionism

Non-steady state diffusional flow

Phenomenological treatment of non-steady state diffusional processes in binary systems

Phenomenological treatment of steady state diffusional processes

Steady state diffusional flow

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