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Diffusion modeling

For homogeneous solutions, two different models are usually employed to determine the reencounter probability. The simplest, and most often employed, is the [Pg.173]

/r is a phenomenological rate constant. The great advantage of this model is its computational simplicity, allowing rapid calculations even for real RPs with multiple nondegenerate HFCs. A more realistic model of diffusion in free solution developed by [Pg.173]

spin-state mixing is possible only at distances beyond Rq, and is the separation at which the radicals can recombine. D is the mutual diffusion coefficient for the radicals in the given solvent. [Pg.173]

Notably, recent studies have used some modern mathematical deconvolutions to try to extract reencounter probabilities from experimental MARY curves. It is signihcant that experiments employing time-insensitive measurements can be used to deliver time-resolved information on rapid diffusional processes. [Pg.173]


Using the analytical data and parts of the model, diffusion coefficients, reaction rate constants, etc. have been estimated. [Pg.230]

The diffusion of solutes in water is an important event in many biological processes. The influences of water temperature and hydropathic states of the solute are expected to be of importance in this process. A study modeling diffusion using CA was reported by Kier et al. [6]. The study revealed increases in diffusion rates with higher temperatures and higher solute hydrophobicity. More recent studies indicate that the diffusion rate may be maximum at an intermediate level of hydrophobicity and temperature [7]. [Pg.66]

The Chemkin package deals with problems that can be stated in terms of equation of state, thermodynamic properties, and chemical kinetics, but it does not consider the effects of fluid transport. Once fluid transport is introduced it is usually necessary to model diffusive fluxes of mass, momentum, and energy, which requires knowledge of transport coefficients such as viscosity, thermal conductivity, species diffusion coefficients, and thermal diffusion coefficients. Therefore, in a software package analogous to Chemkin, we provide the capabilities for evaluating these coefficients. ... [Pg.350]

These effects, specialized for the geometries and materials properties of the collagen-rich stroma and sclera, have been calculated in a paper by Edwards and Prausnitz [197], They also modeled diffusion across the corneal endothelium assuming that the major path was... [Pg.439]

The equations used in these models are primarily those described above. Mainly, the diffusion equation with reaction is used (e.g., eq 56). For the flooded-agglomerate models, diffusion across the electrolyte film is included, along with the use of equilibrium for the dissolved gas concentration in the electrolyte. These models were able to match the experimental findings such as the doubling of the Tafel slope due to mass-transport limitations. The equations are amenable to analytic solution mainly because of the assumption of first-order reaction with Tafel kinetics, which means that eq 13 and not eq 15 must be used for the kinetic expression. The different equations and limiting cases are described in the literature models as well as elsewhere. [Pg.464]

Figure 3. Step 1 in the modified MacFarland bioactivity model Diffusion or carriage by plasma protein from the entry point to the anterior membrane surface (ams) transfer from the first aqueous phase (0 ) to the ams passage through the membrane by diffusion or by lipid soluble membrane carrier molecule bound to the posterior membrane surface (pms) transfer from the pms to the second aqueous phase (02). Figure 3. Step 1 in the modified MacFarland bioactivity model Diffusion or carriage by plasma protein from the entry point to the anterior membrane surface (ams) transfer from the first aqueous phase (0 ) to the ams passage through the membrane by diffusion or by lipid soluble membrane carrier molecule bound to the posterior membrane surface (pms) transfer from the pms to the second aqueous phase (02).
This solution is shown in Figure 1-9. It is a widely used solution in experiments and in modeling diffusion behavior in nature. [Pg.198]

DDI DISSOL DLM DLVO DOC DOE DTA DU Distilled, deionized water Thermodynamic simulation model Diffuse layer model named after Derjaguin, Landau, Vervey, Overbeek Dissolved organic carbon Department of Energy Differential thermal analysis Depleted uranium... [Pg.682]

Modeling diffusive transport requires appropriate constitutive relationships, such as Fourier s law for heat conduction or Fick s law for species diffusion. It is important to... [Pg.668]

The DI model (diffuse incident model, Figure 25c) is thought to take into account the abovementioned inadequacies. The model in which profiles of radiant power or of irradiance are independent of the radius of the cylindrical reactor was originally proposed by Huff and Walker [114] and has been tested by Jacob and Dranoff [111] using sensor equipment. Their results show that radius-independent radiant power or irradiance distribution can only be found for radii of less than 0.5 in. in their particular equipment (Figure 27). [Pg.285]

Bifurcations of a model diffusion-reaction system (with C.R. Kennedy). In P. Holmes (ed.),... [Pg.461]

Second, the definition of DM, the model diffusion coefficient, relates Ax, At, and AD ... [Pg.584]

This result is generally applicable to any situation in which a fixed-width diffusion medium is partitioned into (Jmax - 1) volume elements. In this case, the selection of Jmax fixes the magnitude of the model diffusion coefficient DM. The constraints of Equation 20.12 still apply, however. Therefore, one must resist the temptation to increase the size of Jmax (without limit) to reduce the size of Ax. The maximum value of Jmax selected must be such that DM is still less than /2. [Pg.591]

INPUT "ENTER THE MODEL DIFFUSION COEFFICIENT OF A [UP TO 0.5] DMA 160 PRINT... [Pg.594]

Modeling diffusion-coupled vaporization processes associated with non-stoichiometric carbides requires the use of the chemical diffusion coefficient, D, for the calculation of temporal C concentrations. Clearly D will have a strong concentration dependence. In principle, the concentration dependence should be calculable from measured D (NC,T) and ac(Nc,T) values. However, our attempts and those of Wakelkamp31 to verify the correlation have been unsuccessful for TiC, ZrC, VC, and TaC. The disparity is probably based in the approximations used to derive these equations. For example, Howard and Lidiard32 have shown that the right hand sides of equations 3.10 and 3.11 are approximate and proposed that additional terms are needed. [Pg.43]

The simplifying assumptions that permit us to consider only specular reflections are no longer met when the wall surfaces contain features that are comparable in size to the wavelength of the sound. In this case, the reflected sound will be scattered in various directions, a phenomenon referred to as difjusion. The source image model cannot be easily extended to handle diffusion. Most auralization systems use another geometrical model, called ray tracing [Krokstad et al., 1968], to model diffuse reflections. A discussion of these techniques is beyond the scope of this paper. [Pg.62]

Table 1.4 Mass transport coefficients m,, for different experimental conditions. The values of m, correspond to the application of a constant potential. The expressions corresponding to the Rotating Disc Electrode (convective mass transport) under stationary conditions and to Dropping Mercury Electrode with the expanding plane model (diffusive-convective mass transport) have also been included... Table 1.4 Mass transport coefficients m,, for different experimental conditions. The values of m, correspond to the application of a constant potential. The expressions corresponding to the Rotating Disc Electrode (convective mass transport) under stationary conditions and to Dropping Mercury Electrode with the expanding plane model (diffusive-convective mass transport) have also been included...
Keywords Cahn-Hilliard model Diffusion Nonlinear dynamics Pattern selection Polymer blends Soret effect Spinodal decomposition Thermal diffusion... [Pg.146]

Moldrup, P., Olesen, T Rolston, D. E and Yamaguchi, T. (1997). Modeling diffusion and reaction in soils VII. Predicting gas and ion diffusivity in undisturbed and sieved soils. Soil Sci. 162,632-640. [Pg.48]

If transport through a membrane involving both surface reaction (dissociation) and diffusion was limited by surface reactions, then n = 1. If transport was diffusion-limited, then n = 0.5. Intermediate values of n (0.5proton transport membranes was modeled with the same form of the equations used to model diffusion membranes, Eqns. 3 and 4. Values of k H2 and n were determined from Eqn. 3. The concentration of hydrogen on the permeate-side was insignificant relative to the concentration on the retentate-side. Therefore was equated to... [Pg.99]

In this section we will present briefly some relevant aspects of the classical approach to model diffusion in polymers along with representative features and results of the most often cited of these models. [Pg.126]

In approaching the problem of modelling diffusion in polymers, regardless if in a classical or computational manner, an important feature must be highlighted, namely that markedly different diffusion mechanisms operate at temperatures above and below the glass transition temperature, Tg, of the polymer. This is due in principal to the fact that polymers at temperatures T > Tg, so-called rubbery polymers, respond rapidly to changes in their physical condition. Therefore, the penetrant polymer system adjusts immediately to a new equilibrium when a penetrant species is... [Pg.126]

As a conclusion from the Hildebrand/Trouton Rule, the definition of a standard vapor phase in a standard state with a well known amount of disorder can be made. This definition can be used as a starting point for modeling diffusion coefficients of gases and liquids. [Pg.166]

In all aggregate states in this model, diffusion is considered to be a consequence of interactions between the particles that are in conformity with the first assumption of the model. This means the diffusion coefficient can be described as an exponential function of a relative density of interaction energy qr. [Pg.168]

At constant temperature the ratio DG2IDGI of the diffusion coefficients in a gas at two states 1 and 2 equals the ratio V2 Vt of the system volumes at the two states. Then together with the first assumption a starting point for modeling diffusion coefficients will be the relation DG2 = (V2IV,)Due p(qr) with the unit value Du = lm2/s and qr = iv/ for a perfect gas. By selecting V,- 105 V at pu = 1 Pa as a reference volume the following equation results for a self-diffusion coefficient, Do, in a perfect gas ... [Pg.168]

Figure 9.8 Structured Markovian model. Diffusion is expressed by means of h+, h, and compartments 1 to is. Erlang-type elimination is represented by means of ho and compartments is to m. The drug is given in compartment is and cleared from compartment m. Figure 9.8 Structured Markovian model. Diffusion is expressed by means of h+, h, and compartments 1 to is. Erlang-type elimination is represented by means of ho and compartments is to m. The drug is given in compartment is and cleared from compartment m.
Modelling diffusion coefficients The Wilke-Chang model is... [Pg.554]

In physics, the random walk method has already been in use for decades to understand and model diffusion processes. Prickett et al. (1981) developed a simple model for groundwater transport to calculate the migration of contamination. An essential advantage of the methods of random walk and particle tracking is that they are free of numeric dispersion and oszillations (Abbot 1966). [Pg.65]


See other pages where Diffusion modeling is mentioned: [Pg.1]    [Pg.363]    [Pg.296]    [Pg.536]    [Pg.234]    [Pg.292]    [Pg.289]    [Pg.755]    [Pg.143]    [Pg.162]    [Pg.2]    [Pg.134]    [Pg.249]    [Pg.586]    [Pg.351]    [Pg.410]    [Pg.310]    [Pg.325]    [Pg.229]    [Pg.584]   
See also in sourсe #XX -- [ Pg.330 ]

See also in sourсe #XX -- [ Pg.211 , Pg.217 ]




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