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Model phases solid

The performance of fluidized-bed reactors is not approximated by either the well-stirred or plug-flow idealized models. The solid phase tends to be well-mixed, but the bubbles lead to the gas phase having a poorer performance than well mixed. Overall, the performance of a fluidized-bed reactor often lies somewhere between the well-stirred and plug-flow models. [Pg.58]

One way to model a solid is to use software designed for gas-phase molecular computations. A large enough piece of the solid can be modeled so that the region in the center for practical purposes describes the region at the center of an inhnite crystal. This is called a cluster calculation. [Pg.318]

In equilibrium, this describes the coexistence of two different phases (solid and liquid), just as in the case of the Ising model ( hising) with the up and down magnetization phases. When h 0, one of these two phases has a priority. Therefore, a sign change of h -h induces a first-order phase transition. (Note that for modeling reasons h(T) may be assumed to depend on temperature.)... [Pg.878]

The availability of thermodynamically reliable quantities at liquid interfaces is advantageous as a reference in examining data obtained by other surface specific techniques. The model-independent solid information about thermodynamics of adsorption can be used as a norm in microscopic interpretation and understanding of currently available surface specific experimental techniques and theoretical approaches such as molecular dynamics simulations. This chapter will focus on the adsorption at the polarized liquid-liquid interfaces, which enable us to externally control the phase-boundary potential, providing an additional degree of freedom in studying the adsorption of electrified interfaces. A main emphasis will be on some aspects that have not been fully dealt with in previous reviews and monographs [8-21]. [Pg.120]

Figure 8.47. SRSAXS raw data (open symbols) and model fit (solid line) for a nano structured material using a finite lattice model. The model components are demonstrated absorption factor Asr, density fluctuation background Ipu smooth phase transition/. The solid monotonous line demonstrates the shape of the Porod law in the raw data. At sq the absorption is switching from fully illuminated sample to partial illumination of the sample... Figure 8.47. SRSAXS raw data (open symbols) and model fit (solid line) for a nano structured material using a finite lattice model. The model components are demonstrated absorption factor Asr, density fluctuation background Ipu smooth phase transition/. The solid monotonous line demonstrates the shape of the Porod law in the raw data. At sq the absorption is switching from fully illuminated sample to partial illumination of the sample...
A mathematical model for solid entrainment into a permanent flamelike jet in a fluidized bed was proposed by Yang and Keaims (1982). The model was supplemented by particle velocity data obtained by following movies frame by frame in a motion analyzer. The experiments were performed at three nominal jet velocities (35, 48, and 63 m/s) and with solid loadings ranging from 0 to 2.75. The particle entrainment velocity into the jet was found to increase with increases in distance from the jet nozzle, to increase with increases in jet velocity, and to decrease with increases in solid loading in the gas-solid, two-phase jet. [Pg.308]

In dense systems such as encountered in solids suspension, particle-particle interaction may be important as well. Then, the closure of solid-phase stresses is an important issue for which kinetic theory models and solids phase viscosity may be instrumental (see, e.g., Curtis and Van Wachem, 2004). [Pg.170]

Figure 3. Phase diagrams for different form-factor models Gaussian (solid lines), Lorentzian a = 2 (dashed lines) and NJL (dash-dotted). In /3-equilibrium, the colorsuperconducting phase does not exist for Co Gi. In the inset we show for the Gaussian model the comparison of the numerical result with the modified BCS formula Tf = 0.57 A(T = 0, fiq) g(Hq) for the critical temperature of the superconducting phase transition. Figure 3. Phase diagrams for different form-factor models Gaussian (solid lines), Lorentzian a = 2 (dashed lines) and NJL (dash-dotted). In /3-equilibrium, the colorsuperconducting phase does not exist for Co Gi. In the inset we show for the Gaussian model the comparison of the numerical result with the modified BCS formula Tf = 0.57 A(T = 0, fiq) g(Hq) for the critical temperature of the superconducting phase transition.
But many computations of phase-formation based on the application of pseudo-potential, quantum-mechanical techniques, statistic-thermodynamic theories are carried out now only for comparatively small number of systems, for instance [1-3], A lot of papers dedicated to the phenomenon of isomorphic replacement, arrangement of an adequate model of solids, energy theories of solid solutions, for instance [4-7], But for the majority of actual systems many problems of theoretical and prognostic assessment of phase-formation, solubility and stable phase formation are still unsolved. [Pg.204]

In summary, it can be stated that the characterization of sorption of hydro-phobic compounds to the organic matter of solid phase particles by Koc values is a useful model for solids with a high organic carbon content and negligible... [Pg.301]

The different responses of the NXL and XL bands would not occur if the NXL material were present as defects within tire XL phase. These data support a two-phase model of solid state structure in semicrystalline PTLE. Of course, the precise location of the two phases is difficult to specify, but for the XL phase we have good data on its initial morphology and subsequent changes based upon microscopy and X-ray diffraction. [Pg.20]

Fig. 3.36. Unreacted core model, impermeable solid, showing gas phase reactant... Fig. 3.36. Unreacted core model, impermeable solid, showing gas phase reactant...
Parameter Estimation from Phase Diagram Assessment. The second approach used to determine solid-solution behavior is to estimate solution model parameters from a fit to the measured phase diagram. Many of the solution models used to describe the liquid solution have been used to model the solid mixture. The simple-solution expression and its special cases have been used most extensively. [Pg.166]

On the basis of the DLP model, the solid is expected to be an ideal solution for systems in which both components have similar lattice constants. This case is true for the AlAs-GaAs system (Figure 5), in which the solid-phase composition equals the gas-phase composition. Compounds in which the two components have very different behavior will show highly nonlinear composition variations, and miscibility gaps may occur (90, 91). As an example, Figure 5 also shows that the solid-phase composition of In As Sb is a nonlinear function of the gas-phase composition. [Pg.224]

However, there are numerous theoretical models available in the literature that attempt to derive meaningful values from thermal data. Solution phase reactions are generally easier to model than solid-state or heterogeneous reactions and the discussion that follows will consider the two classes separately. In all cases, it is necessary to know the time at which the reaction was initiated, t0, in order to analyse the data correctly. Note that this does not mean the reaction must be initiated directly in the instrument—this is difficult for ampoules prepared on a bench-top—it means that the time axis on the resulting power-time curve must be corrected for the delay caused by loading. No fitting model requires the reaction to run to completion in order to return the correct reaction parameters—if this were the case it would take up to 10,000 years to model some reactions based on the sensitivity of the instrument ... [Pg.333]

Fig. 8. The thermal conductivity of HMX as a function of temperature. Symbols this work (liquid phase) solid bold line experiment (crystal phase) solid thin line semi-empirical form used in some combustion models. The dashed line is an extrapolation of the experimental data for HMX crystal into liquid region. Fig. 8. The thermal conductivity of HMX as a function of temperature. Symbols this work (liquid phase) solid bold line experiment (crystal phase) solid thin line semi-empirical form used in some combustion models. The dashed line is an extrapolation of the experimental data for HMX crystal into liquid region.
Two specific approximations were developed to solve the problems of surface chemistry the periodic approximation, where quantum-chemical methods employ a periodic structure of the calculated system, and the cluster approximation, where the model of solid phase of finite size is created as a cutoff from the system of solid phase (it produces unsaturated dangling bonds at the border of cluster). The cluster approximation has been widely used for studying the interactions of molecules with all types of solids and their surfaces [24]. This approach is powerful in calculations of systems with deviations from the ideal periodic structure like doping and defects. Clay minerals are typical systems having such properties. [Pg.347]

All ASPEN models allow solids to be in inlet streams. The user does not need to take special precautions. The solids are normally assumed to be non-distributing in the liquid and vapor phases. That is, the phase equilibria is unaffected by the solid phase. However, the system does allow for the case of solids distributing into other phases. Solids are taken into account in the energy balance around each equipment model. [Pg.300]


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Model phases solid solution

Modeling phase

Modeling solid

Solid phase, diffusion models

Solid-phase interaction parameter model

Thermodynamic Modeling of Solid Phases, First Edition. Michel Soustelle

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