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Three-constant model

Figure 3.4. Dependencies of parameters Go (1), AG (2), and0 (3) of a three-constant model on time in polyurethane curing. Figure 3.4. Dependencies of parameters Go (1), AG (2), and0 (3) of a three-constant model on time in polyurethane curing.
The results of calculations of the time dependencies of the constants are presented in Fig. 3.5. In this case the root-mean-square error of approximation also has a maximum at a specific time, although its magnitude is substantially lower than for the three-constant model. This is to be expected with the four-contant model, because it is known that at t the relaxation spectrum of a curing polymeric material changes radically it widens abruptly, and new relaxation modes appear.130 The four-constant model is insufficient to describe a rapid change in relaxation properties furthermore, the behavior of a real material near the gel-point (at the transition of the system to the heterophase state) is a new phenomenon that is not described by a simple model. [Pg.105]

Campanella and Peleg (1987) presented stress growth and decay data on mayonnaise at shear rates of 1.8, 5.4,9.9, and 14.4s with a controlled shear rate viscometer and a concentric cylinder geometry. They modeled the data by a three-constant model that was a modification of Larson s (1985) model that was successfully employed for polyethylene melts with a wide distribution of molecular weights. The model employed by Campanella and Peleg was ... [Pg.247]

Ellis model n. A three-constant model of pseudoplastic flow that merges Newton s law of flow, applicable at very low shear rates, with the power law at high rates and provides a smooth transition between the two. For onedimensional flow the equation is... [Pg.354]

Figure 3.3 gives logarithmic plots of n/r] versus predicted from three models (1) the ZFD model, (2) the Oldroyd three-constant model, and (3) the Spriggs model. It is seen in Figure 3.3 that the predicted viscosities from all three models decrease at a much faster rate than those observed experimentally (see Figure 3.2) with increasing shear rate, and that the viscosities predicted from the Oldroyd three-constant model level off as shear rate is increased, which is seldom observed experimentally. [Pg.68]

Small-amplitude oscillatory analysis can readily be applied to any nonlinear constitutive equation. For instance, applying Eq. (3.79) to the Oldroyd three-constant model, Eq. (3.21), we obtain... [Pg.74]

Figure 3.11 gives plots of n /irjo versus A.jC that are predicted from two constitutive equations (1) the upper convected Maxwell model, and (2) the Oldroyd three-constant model. It is seen in Figure 3.11 that both models predict values of increasing very rapidly without bound as e increases, in contrast to the experimental results given in Figure 3.10. As a matter of fact, all the expressions summarized in Table 3.3 predict similar elongational behavior, which is considered to be physically unrealistic. Figure 3.11 gives plots of n /irjo versus A.jC that are predicted from two constitutive equations (1) the upper convected Maxwell model, and (2) the Oldroyd three-constant model. It is seen in Figure 3.11 that both models predict values of increasing very rapidly without bound as e increases, in contrast to the experimental results given in Figure 3.10. As a matter of fact, all the expressions summarized in Table 3.3 predict similar elongational behavior, which is considered to be physically unrealistic.
Sepn. Purif., 3, 19 (1989)] takes holdup into account and applies to random as well as structured packings. It is somewhat cumbersome to use and requires three constants for each packing type and size. Such constants have been evaluated, however, For a number of commonly used packings. A more recent pressure drop and holdup model, suitable for extension to the flood point, has been pubhshed by Rocha et al. [Jnd. Eng. Chem. Research, 35, 1660 (1996)]. This model takes into account variations in surface texturing of the different brands of packing. [Pg.1390]

With a three-parameter model of the intermolecular potential, the theoretical spall strength is not simply a constant times the bulk modulus. Although the slightly greater accuracy obtained is not critical to the present investigation, an energy balance is revealed in the analysis which is not immediately transparent in the Orowan approach. [Pg.268]

Figures 1 a and 1 b represent the two-phase and the three-phase models respectively in the representative volume element of the composite. In the modified model three concentric spheres were considered with each phase maintaining a constant volume 4). The novel element in this model is the introduction of the third intermediate hybrid phase, lying between the two principal phases. Figures 1 a and 1 b represent the two-phase and the three-phase models respectively in the representative volume element of the composite. In the modified model three concentric spheres were considered with each phase maintaining a constant volume 4). The novel element in this model is the introduction of the third intermediate hybrid phase, lying between the two principal phases.
The difference in the exponents of the two terms in the three-term model (the third term was a constant) and the exponent in the single power term of the two-term model gave a measure of the quality of adhesion between phases and they were called the adhesion coefficients. [Pg.186]

Calculated Rate Constants and Activation Parameters. Calculated results based on the three different models (TST, SCT, and QMT) are displayed in Table II and compared with experimental results (30) extrapolated to zero ionic strength (Tl). [Pg.275]

In terms of liquid wafer safuration and water management in the CCL, the bimodal 5-distribution leads to a three-state model. Effective properties are constant in each of fhese sfates. In the dry state, the porous structure is water-free (S, 0). Gaseous fransport is opfimal. Electrochemical reaction and evaporation rates are poor, however, because g 0 and 0. In the optimal wetting state (S, = X /Xp), primary pores are completely water filled while secondary pores are water free. Cafalysf ufilization and exchange... [Pg.416]

The hardware of the method is a newly constructed experimental PBC system. It is designed according to the three-step model. The object (variable) of the measurement method is the conversion system, which can be varied that is, different conversion systems in small-scale range (<300 kW) can be studied by this method. The method works well on both continuous and batch conversion systems. However, the primary and secondary air flow need to be constant during the test. [Pg.44]

The complete mixing of solids in the emulsion phase is necessary for considering the various parameters, involving the mass or volume of solids constant, throughout the reactor. That is exactly the case in the two-phase model and the Levenspiel-Kunii three-phase model. This is achieved by circulation of the solids through their entrainment by bubbles, as shown in Figure 3.61. As solids fall from the upper portions of the bed, they follow... [Pg.214]

Equation 4 may be viewed as a three-constant extension pf the simpler equations, and the resulting improvement in agreement between the predictions and the experimental values may be attributed to the inclusion of extra arbitrary constants. If so, similar models, such as the Kiselev equation, which has the same number of constants, would be expected to provide the desired predictions. However, neither this nor other models did correlate the experimental data. Therefore, using models that include terms that describe the stipulated prevailing phenomena (heterogeneity, mobility, adsorbate interactions) provides a more realistic model of the actual mechanism and thus enables more accurate predictions. The application of experimental data to the proposed technique requires only slight increase in effort, which is negligible when computers are employed, despite the fact that the equations are more complex than the expressions derived from the simple models. [Pg.379]


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Oldroyd three-constant model

Three-constant

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