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Model Modified

The introduction of the kinetics of the formation of CO and CO2 into the model modifies the temperature equation (31) and the oxygen equation (33). The slow and fast coke burning equations are unchanged except for a change in the effectiveness factor tjt of Eq. (29) to tjtc given by Eq. (73). A new equation for the conversion of CO is introduced. [Pg.49]

As noted in the Introduction, one of the defining characteristics of any fuel-cell model is how it treats transport. Thus, these equations vary depending on the model and are discussed in the appropriate subsections below. Similarly, the auxiliary equations and equilibrium relationships depend on the modeling approach and equations and are introduced and discussed where appropriate. The reactions for a fuel cell are well-known and were introduced in section 3.2.2. Of course, models modify the reaction expressions by including such effects as mass transfer and porous electrodes, as discussed later. Finally, unlike the other equations, the conservation equations are uniformly valid for all models. These equations are summarized below and not really discussed further. [Pg.451]

Trace the evolution of a mechanistic model that started out as an empirical model. How was the original empirical model modified during the development of the model Did experimental observations or theoretical reasoning force adjustments to the model ... [Pg.22]

Rewrite the model, modifying the structure so as to reduce the number of variables that are highly correlated with one another. [Pg.170]

Venkataraman, C., and S. K. Friedlander, Source Resolution of Fine Particulate Polycyclic Aromatic Hydrocarbons Using a Receptor Model Modified for Reactivity, J. Air Waste Manage. Assoc., 44, 1103-1108 (1994c). [Pg.545]

Probably the first major publication of a process model for the autoclave curing process is one by Springer and Loos [14]. Their model is still the basis, in structure if not in detail, for many autoclave cure models. There is little information about results obtained by the use of this model only instructions on how to use it for trial and error cure cycle development. Lee [16], however, used a very similar model, modified to run on a personal computer, to do a parametric study on variables affecting the autoclave cure. A cure model developed by Pursley was used by Kays in parametric studies for thick graphite epoxy laminates [18]. Quantitative data on the reduction in cure cycle time obtained by Kays was not available, but he did achieve about a 25 percent reduction in cycle time for thick laminates based on historical experience. A model developed by Dave et al. [17] was used to do parametric studies and develop general rules for the prevention of voids in composites. Although the value of this sort of information is difficult to assess, especially without production trials, there is a potential impact on rejection rates. [Pg.455]

Correlation of Structure with Source. Allochthonous-derived DOM (8) was isolated from the Suwannee River at its origin in the Okefe-nokee Swamp in southern Georgia. The fiilvic acid fraction, which is responsible for the black coloration of the water, was extensively characterized (9). Several average molecular models based on quantitative analytical data were presented in that report (10) to denote the mixture characteristics of fiilvic acid. One model, modified to depict biochemical sources and based on quantitative analytical data (10), is presented in Structure 1. Other models of Suwannee River fulvic acid (based on lignins, terpenoids, tannins, and flavonoid sources) were previously proposed (II). [Pg.200]

In Equation (9.6), x is the direction of flux, nt [mol m-3 s 1 ] is the total molar density, X [1] is the mole fraction, Nd [mol m-2 s 1] is the mole flux due to molecular diffusion, D k [m2 s 1] is the effective Knudsen diffusion coefficient, D [m2 s 1] is the effective bimolecular diffusion coefficient (D = Aye/r), e is the porosity of the electrode, r is the tortuosity of the electrode, and J is the total number of gas species. Here, a subscript denotes the index value to a specific specie. The first term on the right of Equation (9.6) accounts for Knudsen diffusion, and the following term accounts for multicomponent bulk molecular diffusion. Further, to account for the porous media, along with induced convection, the Dusty Gas Model is required (Mason and Malinauskas, 1983 Warren, 1969). This model modifies Equation (9.6) as ... [Pg.284]

The main purpose of this section is consideration of the FIR spectra due to the second dipole-moment component, p(f). However, for comparison with the experimental spectra [17, 42, 51] we should also calculate the effect of a total dipole moment ptot. In Refs. 6 and 8 the modified hybrid model44 was used, where reorientation of the dipoles in the rectangular potential well was considered. In this section the effect of the p(f) electric moment will be found for the hat-curved, potential, which is more adequate than the rectangular potential pertinent to the hybrid model. In Section VI.B we present the formula for the spectral function of the hat-curved model modified by taking into account the p(f) term (derivation of the relevant formula is given in Section VI.E). The results of the calculations and discussion are presented, respectively, in Sections VI.C and VI.D. [Pg.206]

Fig. 6. (a) Layout of a theoretically modeled modified Cgo electromechanical transis-... [Pg.378]

Fig. 3.3. Roller bottle machines. This photograph shows three different models. The one at the rear is the Luckham 6-tier model modified by the manufacturer by provision of a more powerful motor. It is very heavy to manoeuvre and only three standard (4 ) Winchester bottles can be accommodated on each tier. In the foreground are two tiers of a stackable model mad by Voss Instruments. Each tier has a separate motor. On the left is a model made by Mr. Harvey, Department, of Biochemistry, University of Glasgow. A motor drives a rubber belt which rotates the bottles as they rest on small pulley wheels. Each motor drives 40 bottles. Fig. 3.3. Roller bottle machines. This photograph shows three different models. The one at the rear is the Luckham 6-tier model modified by the manufacturer by provision of a more powerful motor. It is very heavy to manoeuvre and only three standard (4 ) Winchester bottles can be accommodated on each tier. In the foreground are two tiers of a stackable model mad by Voss Instruments. Each tier has a separate motor. On the left is a model made by Mr. Harvey, Department, of Biochemistry, University of Glasgow. A motor drives a rubber belt which rotates the bottles as they rest on small pulley wheels. Each motor drives 40 bottles.
Figure 8.10 Humic substance formation depicted by the early biopolymer degradation and abiotic condensation models. (Modified from Hedges, 1988.)... Figure 8.10 Humic substance formation depicted by the early biopolymer degradation and abiotic condensation models. (Modified from Hedges, 1988.)...
Figure 13.15 Comparison of A14C versus <513C for bacterial nucleic acids and potential sources for the (a) entire York River estuary, (b) the freshwater, (c) mid-salinity, and (d) high-salinity (river mouth) regions in the estuary. Boxes are the 95% confidence intervals for the potential end-members in the York. Dotted lines represent the solution space from one run of a model. (Modified from McCallister et ah, 2004.)... Figure 13.15 Comparison of A14C versus <513C for bacterial nucleic acids and potential sources for the (a) entire York River estuary, (b) the freshwater, (c) mid-salinity, and (d) high-salinity (river mouth) regions in the estuary. Boxes are the 95% confidence intervals for the potential end-members in the York. Dotted lines represent the solution space from one run of a model. (Modified from McCallister et ah, 2004.)...
Figure 15.4 Schematic of the biotic ligand model. (Modified from Di Toro et al., 2001.)... Figure 15.4 Schematic of the biotic ligand model. (Modified from Di Toro et al., 2001.)...
The magnitude and nature of the primary effect will be examined in terms of eq. (11) however, the present remarks are not limited to systems in which active rotations are absent. The discussion is based on calculations using the C2 model for the light molecule and the C2 model, modified to correspond to the measured frequencies for ethane- (Table VI) for the C2-di model. The complex for H rupture, is the semirigid complex 4, specified in II,B2 and Table I. The D-rupture complex (Table VI) was constructed in the same way and fits the Teller-Redlich product rule. The difference in critical energies for the two prototype reactions is Aeo = 1.38 keal. mole-1. The density of states for the molecules and the sum of states for the complexes are shown in Figures 3 and 4, respectively. [Pg.31]

The above discussion demonstrates that high field effects included in the FDTO model modify the OFET characteristics very significantly. The FDTO model is in very good agreement with the experimental results. The model has been compared with two sets of experiments [158], The experimental data for -6T [157] is compared with the FDTO... [Pg.140]

Since the transverse shear wave may penetrate the damping surface layer and the viscous liquid, additivity of the equivalent electrical elements in the BVD circuit is only valid under certain particular conditions. Martin and Frye [53] studied the impedance near resonance of polymer film coated resonators in air with a lumped-element BVD model, modified to account for the viscoelastic properties of the film. In addition to the elements shown in Fig. 12.3 to describe the quartz crystal and the liquid, L/ and Rf were added to describe the viscoelastic film overlayer. For a small... [Pg.476]

The Stern model modifies the Gouy-Chapman model and divides ions present in the solution into two groups a part of the ions is placed near the solid surface, forming the so-called Stern layer (similar to the Helmholtz layer), and the other part having a diffuse distribution (Gouy-Chapman layer). It implies that the surface potential is linear in the Stern layer, and the exponential in the Gouy-Chapman layer. [Pg.31]

Fig. 5. Detailed TRAF2-receptor interactions. (A) Interactions seen in the m or TRAF2-binding motif. (B) Interactions seen in the minor TRAF2-binding motif. TRAF2 structures are shown as magenta worms and white stick models. The bound receptors are shown as yellow stick models. Modified from Ye et al. (1999). (See Color Insert.)... Fig. 5. Detailed TRAF2-receptor interactions. (A) Interactions seen in the m or TRAF2-binding motif. (B) Interactions seen in the minor TRAF2-binding motif. TRAF2 structures are shown as magenta worms and white stick models. The bound receptors are shown as yellow stick models. Modified from Ye et al. (1999). (See Color Insert.)...
The conductor-like continuum solvation model, modified for ab initio in the quantum-chemistry program GAMESS, implemented at the Meller-Plesset order 2 (MP2) level of theory, has been applied to a group of push-pull thiophene systems to illustrate the effects of donor/acceptor and solvation on the stability and energetics of such systems. The most accurate theoretical gas- and solution-phase data to date have been presented for the parent thiophene-2-carbaldehyde system <2000JCP(113)7519>. [Pg.706]

These considerations and the set of equations for transport of the solute through the HF modules are modified and simplified in comparison to the HFCLM [91] theoretical considerations. The models presented in Sections 13.2.1 and 13.2.2 consider more detailed diffusion parameters at the F/LM and LM/R interfaces, more detailed kinetics of chemical reactions. So, they are more identical to the real transport processes, therefore, these models, modified for a hollow-fiber permeator, may be used for the hoUow-fiber transport also. [Pg.386]

Used the advancing front model and three reversible reaction models Bunge and Noble [16] model, Lin and Lxtng [23] model, modified Bunge and Noble model. [Pg.713]

Comparison of data range on the confidence intervals of a regression model. (Modified from Moore, D.R.J. and P.-Y. Caux. 1997. Estimating low toxic effects. Environ. Toxicol. Chem. 16 794—801. With permission.)... [Pg.59]

Figure 14.4. Binding conformation of inverse agonist RY80 (29)in the GABAa/BzR pharmacophore/ receptor model. (Modified from Ref 189.)... Figure 14.4. Binding conformation of inverse agonist RY80 (29)in the GABAa/BzR pharmacophore/ receptor model. (Modified from Ref 189.)...
This simple model was later extended by Guth and Gold to include interparticular disturbances. One form of this model is given by Eq 7.6. This model modified by Thomas fits some experimental data ... [Pg.384]

Is C related to the size of the counterions, than it should be different on the both sides of the PZC for amphoteric surfaces. An analogous modification of the constant capacitance model was discussed above (Figs. 5.35-5.38). The Stern model modified by allowing different C values for positive and negative branch of the... [Pg.631]

FIGURE 16.6 Molecular structure of the paint Araldit 488 and infinite dilution activity coefficients (Qf) with various models for Araldit 488-solvent systems. Results are shown with the Entropic-FV and UNIFAC-FV activity coefficient models and the GC-Flory equation of state. The calculations with the two activity coefficient models are shown for two different values of the density of the polymer, predicted by the GC-VOL and van Krevelen models. (Modified from Lindvig et al., AIChE J., 47(11), 2573-2584, 2001.)... [Pg.713]

A theoretical model was developed to correlate molecular weight distribution of this system. This was compared to the experimental gel permeation chromatography trace with the theoretical model modified to Include the effect of the PEG central block, the spreading of the trace as it went through the columns and the slope of the log MW versus retention volume line. A good fit was found with kl/kp = 0.0070. When methyl tosylate was used to polymerize 2-lsobutyl oxazollne, a similar treatment of the data showed kl/kp = 0.22. The effect of the PEG Is explained as due to solvation of the Initial adduct by the neighboring ether group. [Pg.231]


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Difference model, modified Bloch

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Dipole-proton coupling model, modified strong

Ellis model modified

Exponentially modified Gaussian model

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General Rheological model modified

Genetically Modified Mouse Models

Genetically modified animal models

Group contribution models modified

Kinetic modelling at electrodes modified by films

Localization-modified model

Mathematical Model with Actual Conventional and Modified Composite Boards

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Model modifying existing

Modeling of toxicokinetics and modifying factors

Models Modified Redlich-Kwong

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Modified Campbell-Dontula Model

Modified Cross model

Modified Fick model

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Modified Ising model

Modified NDDO Models

Modified Neglect of Differential Overlap MNDO) model

Modified Penetration Model for Rotary Kiln Wall-to-Bed Heat Transfer

Modified Poisson-Boltzmann models

Modified Poisson-Boltzmann models electrolyte solutions

Modified Quasichemical Model

Modified Random Network model

Modified Verwey-Niessen model

Modified cell model

Modified field effect model, electrical

Modified free-volume model

Modified intermediate neglect differential overlap model

Modified switching device model

Modified thermal model

Rheological models modified

Rheological models modified Carreau

Solubility parameter modified models

Surface-modified Polystyrene Particles as Model Carriers

The Modified Embedded-Atom Model

The modified UNIFAC model (Dortmund)

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