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Fox s equation

It 1s useful to compare the T values obtained for the amorphous M-M-23/25-51 and 24-M-B-23/25-48 series to predictions for random homo-geneous systems. Using for instance Fox s equation (27) ... [Pg.47]

This equation fits fiber moisture-content data over a wider range than does Fox s equation. [Pg.526]

Figure 5. Tg values determined by (— —) DMTA and calculated from the Fox s equation (—) for the PCN/PTMG compositions. Figure 5. Tg values determined by (— —) DMTA and calculated from the Fox s equation (—) for the PCN/PTMG compositions.
Figure 19. Tg values determined by DSC, DMT A, DRS, and TSEXD versus LPU content. The dotted line is a fit of Fox s equation (eq. 2) to the DMTA data and the dashed line is a fit of the Couchman-Karasz equation (eq. 3) to the DSC data. Figure 19. Tg values determined by DSC, DMT A, DRS, and TSEXD versus LPU content. The dotted line is a fit of Fox s equation (eq. 2) to the DMTA data and the dashed line is a fit of the Couchman-Karasz equation (eq. 3) to the DSC data.
Table 9. DSC data and the parameters of the microphase-separated structure of the polyurethane ionomers W2 is the HS weight fraction, the melting temperature of the SS-rich phase, Tg s the glass transition temperature of the SS-rich phase, AT the width of the glass transition temperature of the SS-rich phase, T the calculated glass transition temperature of the sample using Fox s equation, A the specific heat capacity jump at Tg, Wi the overall weight fraction of the SS-rich phase, Wj the weight fraction of the SS component in the SS-rich phase, and Wj j, the weight fraction of the HS component in the SS-rich phase 65 ... Table 9. DSC data and the parameters of the microphase-separated structure of the polyurethane ionomers W2 is the HS weight fraction, the melting temperature of the SS-rich phase, Tg s the glass transition temperature of the SS-rich phase, AT the width of the glass transition temperature of the SS-rich phase, T the calculated glass transition temperature of the sample using Fox s equation, A the specific heat capacity jump at Tg, Wi the overall weight fraction of the SS-rich phase, Wj the weight fraction of the SS component in the SS-rich phase, and Wj j, the weight fraction of the HS component in the SS-rich phase 65 ...
Disappearance of predators may also imbalance the equilibrium, and the problem scales up, such as the disappearance of foxes, predators of the deer mouse, which has allowed spreading of the hantavirus in the US, carried by mice (Levins 1993). Similarly, Sabia virus has emerged in Brazil, Guaranito virus in Venezuela (Lisieux 1994), machupo virus in Bolivia, and Junin fever in Argentine (Garrett 1994). In contrast, in a robust ecosystem, elimination of a predator provides space for another predator, such as in the disappearance of the coyote, which has opened the control of field mice to snakes and owls. When both predator and prey are endangered, it may occur that the prey develops resistance. This is taken into account in Volterra s equation (Ehrlich 1986). [Pg.276]

Let us remark that Di Marzio s equation reduces to the Fox-Loshaek equation at low crosslink densities ... [Pg.313]

Several methods have been proposed in the literature for this purpose. The first method, which may be called the Flory-Fox-Schaefgen method, is based on the combination of Flory and Fox s viscosity equation (4) and Flory s excluded volume equation (8) [see, Flory and Fox (103)]. The substitution of Eqs. (5) and (6) into Eq. (8) yields... [Pg.201]

Non-linear two point boundary value differential equations arise in fixed bed catalytic reactors mainly in connection with the diffusion and reaction in porous catalyst pellets. It may also arise in the modelling of axial and radial dispersion in the catalyst bed. In addition they also arise in cases of counter-current cooling or heating of the reactor. For this last case, the use of a shooting technique with an iterative procedure similar to the Newton method (Fox s method) seems to be the easiest and most straightforward technique (Kubicek and Hlavacek, 1983). [Pg.231]

Figure 7.72 illustrates a large number of glass transition data of polymer solutions with comparisons to the Gibbs-DiMarzio (DM), Fox (F), and Schneider (S) equations described in Fig. 7.69 [30]. The upper left displays two sets of literature data on poly(vinylidene fluoride)-poly(methyl methacrylate) solutions (B,A). The glass transition shows a positive deviation from simple additivity of the properties of the pure components, which can only be represented with the help of the indicated interaction parameters of the Schneider equation. The lower left set of data illustrates poly(oxyethylene)-poly (methyl methacrylate) solutions (, o). They are well described by all three of the equations, indicating rather small specific interactions and great similarity between volume and entropy descriptions. Figure 7.72 illustrates a large number of glass transition data of polymer solutions with comparisons to the Gibbs-DiMarzio (DM), Fox (F), and Schneider (S) equations described in Fig. 7.69 [30]. The upper left displays two sets of literature data on poly(vinylidene fluoride)-poly(methyl methacrylate) solutions (B,A). The glass transition shows a positive deviation from simple additivity of the properties of the pure components, which can only be represented with the help of the indicated interaction parameters of the Schneider equation. The lower left set of data illustrates poly(oxyethylene)-poly (methyl methacrylate) solutions (, o). They are well described by all three of the equations, indicating rather small specific interactions and great similarity between volume and entropy descriptions.
In this solved example, we present the development of the isothermal model and its boundary conditions for a case where the equation is linear and can be solved analytically. Also presented is another case, where the model is nonlinear and we describe its numerical solution using Fox s iterative method. [Pg.307]

B. If the reaction is second order and the numerical value of Da (Damkohler number) is the same as in part 1 (although its definition is slightly different), find the exit conversion using the Fox s iterative method (explain your formulation of adjoint equations for the iterative solution of the nonlinear two-point boundary-value differential equation). [Pg.308]

B. For the Second-Order Reaction and Fox s Iterative Method for Nonlinear Two-Point Boundary-Value Differential Equation... [Pg.316]

For both cases of limited Sh and Sh oo, we get a two-point boundary-value dilferential equation. For the nonlinear cases, it has to be solved iteratively (we can use Fox s method, as explained for the axial dispersion model in Chapter 4 or orthogonal collocation techniques as explained in Appendix E). [Pg.489]

A proposal based on Onsager s theory was made by Landau and Lifshitz [27] for the fluctuations that should be added to the Navier-Stokes hydrodynamic equations. Fluctuating stress tensor and heat flux temis were postulated in analogy with the Onsager theory. Flowever, since this is a case where the variables are of mixed time reversal character, tlie derivation was not fiilly rigorous. This situation was remedied by tlie derivation by Fox and Ulilenbeck [13, H, 18] based on general stationary Gaussian-Markov processes [12]. The precise fomi of the Landau proposal is confimied by this approach [14]. [Pg.705]

Much has been made about methylene glycol being the cause for formaldehyde s slow rate of fixation, succinctly expressed by Fox et al.7 Equilibrium between formaldehyde as carbonyl formaldehyde and methylene glycol explains most of the mystery of why formaldehyde penetrates rapidly (as methylene glycol) and fixes slowly (as carbonyl formaldehyde). Flowever, the equilibrium equation indicates the proportional amounts of carbonyl formaldehyde and methylene glycol, not the rate of conversion between the two... [Pg.202]

Glass transition data for copolymers and terpolymers of controlled and uncontrolled composition are shown in Figures 6 and 7. The Tg s calculated using the equations 7 and 8 of Fox (12) and Woods (13) have been used with the following hompolymer Tg s methyl methacrylate, 108°C tributyltin methacrylate, 0°C 2-ethylhexyl acrylate, -50"C (14-16) are also shown. [Pg.332]

Differential Scanning Calorimetry. Thermal analysis of PVME/PS blends and IPNs by DSC indicates only one glass transition temperature, which is located between the homopolymer T s. The position of Tg is dependent upon composition although it does not follow the prediction of the Fox equation (21), Table II. The breadth of the transition also increases significantly with increased PS content for the blends and IPNs. The broad transition might result from either the clustering of like mers near... [Pg.423]

Pl-lSx (a) There are initially 500 rabbits (x) and 200 foxes (y) on Farmer Oat s property, Use POLYMATH or MATLAB to plot the concentration of foxes and rabbits as a function of time for a period of up to 500 days. The predator-prey relationships are given by the following set of coupled ordinary differential equations ... [Pg.32]

Earlier literature sometimes equated Zc with (2Z,) on the basis of a pseudogelation theory. Anote byMARKOvrcz, Fox and Ferry (147) suggested this reasoning was not valid, and that the symbol A be used to denote alternatively Zg dete-mined from jj (Z) curves, or Z as deduced from certain mechanical measurements and usually identified directly with Z,. It is now believed that the two parameters Zj and Z are distinct, perhaps related through Eq. (3.11). In this case, a gle symbol for both is inappropriate. In the present nomenclature, Zl =Z, Z s=a (ZJ2). [Pg.310]

Before becoming too optimistic about the possibility of evaluatii unperturbed macroion dimensions from the procedure outlined above, we must recall two serious objections advancal by Flory 49), First of all. extrapolations of intrinsic viscosity data for the graphical evaluation of K, as required by equations (2) and (3), as well as by the equation of Flory and Fox [50), are extrapolations into a region in which approximate theories of pol5nner solutions are no longer tenable. Secondly, Flory indicates that there is at least one case which clearly shows that the application of equation (3) leads to physically irrational conclusions, namely the case of hydroxyethylcellulose in aqueous solution. Flory s original paper must be consulted for a clearer appreciation of the two important objections indicated above. The first objection is of basic importance and it is perhaps worthwhile to digress briefly and to try... [Pg.378]

Glass transition temperatures, Tg. as represented by the temperatures for the maxima in the E curves, are plotted against composition in Figure 4. As expected, the values varies with composition. However, the Tg s for the prepolyraer procedure are always lower than those for the one-shot procedure, which fell between the predictions of Fox (33) and Pochan equations (34) (Figure 3), i.e.. [Pg.314]


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