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Plateau Variation with temperature

Therefore, excluding the presence of the / form and considering the values of zf and w, the negative sign of vf/z, the variation with temperature of coefficient B1 and the presence of plateau characteristic of the... [Pg.366]

The primary emphasis in shock tube interferometric studies of the hydrogen-oxygen reaction has been on induction period phenomena. Recently, however, the entire postshock density profiles of a selection of rich, lean and near stoichiometric Ha-Oa-Ar mixtures have been studied by numerical integration of an assumed reaction mechanism. In this manner it was shown that the characteristic features of the profile prior to the end of the density plateau are essentially independent of the recombination kinetics. Thereafter, however, the shape of the profile is largely accounted for by termolecular reactions (e)-(g). Systematic variation of the termolecular rate coefficient values in experimental regimes where recombination is most sensitive to reactions if) or ig)> respectively, has yielded temperature-dependent expressions of the form kf< = AT for kf and kf believed valid over the range 1400-3000 K. The expression of Jacobs et al. was found satisfactory for kf. In all three cases, variation with temperature is small (1-0 m 0-5). Values at 1700 K, kf = 5-9 x 10 (cited above), kf z= 1-9 X 10 , and kf = 3-6 x 10 cm mole sec, are in excellent accord with those listed in Table 2.2. [Pg.149]

The variation of the transition between form I and form II with temperature is shown in Fig. 5.10. The pressure of the transition plateau increases with temperature, and above a temperature of 42 C no solid condensed monolayer (form II) is formed. This temperature is also in good agreement with the temperature of transition from... [Pg.361]

In Figure 1 in addition to isochronal measurements plateau values of a small step armealing treatment (order-order relaxations) are given for a comparison (o). These points reflect a variation of equilibrium state of LRO-parameter with temperature. [Pg.208]

Figure 3.3 Variation of elastic modulus of a polymer with temperature. As the degree of crystallinity increases, the extent of rubbery plateau region decreases. Figure 3.3 Variation of elastic modulus of a polymer with temperature. As the degree of crystallinity increases, the extent of rubbery plateau region decreases.
Table 5 Variation in the partial pressure of hydrogen in the Li-LiH system with temperature in the plateau region... Table 5 Variation in the partial pressure of hydrogen in the Li-LiH system with temperature in the plateau region...
Figure 3 Variation of the plateau compliance JN° of gluten (Olympic x Gabo cross line -// 7 + 18/-) with temperature in water filled symbols) and in deuterium dioxide (empty symbols). J N was obtained from the fit of the Cole-Cole functions to the dynamic measurements data... Figure 3 Variation of the plateau compliance JN° of gluten (Olympic x Gabo cross line -// 7 + 18/-) with temperature in water filled symbols) and in deuterium dioxide (empty symbols). J N was obtained from the fit of the Cole-Cole functions to the dynamic measurements data...
The study of pH effect has been accomplished by some investigators. Some of them find a linear variation with pH, while others reported a plateau at some pH values [30]. Therefore we studied zeta potential of polymers at constant pH, only for isoelectric point determination we provided pH dependence. Also the effect of temperature should not be neglected, e.g. the -potential of silica increases approximately 1.75% per 1°C [30]. It is therefore important to preserve the constant temperature during zeta potential determination. [Pg.206]

The values obtained for the CMC were closer to NaTDC than NaTC. The variations of CMC with temperature were also more like that of the dihydroxy bile salt. At each NaCl concentration a slight fall or plateau occurs in the CMC at lower temperatures. The CMC does not begin to rise much until 50 °C and then does so gradually in water and all salt concentrations. [Pg.310]

The dynamic properties of filled rubbers are widely studied by many researchers in this field of which the contribution made by Payne is the most significant. The dependence of strain amplitude on the storage modulus in filled mbbers is known as the Payne effect [27]. At a strain more than 0.1 %, the storage modulus of filled rubber collapses from a plateau value of G O to a minimum value Goo and this decrease is accompanied by a maximum of the loss modulus, G". The variation in this storage modulus value with respect to the minimum value is called amplitude of the Payne effect, and this increases with the filler content, specific surface and properties of the filler and its dispersion within the matrix. The amplitude inversely changes with temperature. A lot of investigations were performed in order to explain the Payne effect and reasons behind it. Payne neglected the contribution... [Pg.9]

Conversely, the process cannot be described by a two-state approximation when (1) the transition curve displays one, or more than one, well delineated plateau, or even a shoulder, (2) the different observables do not coincide, (3) AH variations display a maximum, (4) AH, measured from the variations of Kp with temperature, is smaller than true calorimetric AH, and (5) when kinetics are multiphasic. When even only one of these conditions is fulfilled, the transition cannot be described by a two-state process. [Pg.311]

Pectins were incubated in buffered medium in mild alkaline conditions (pH 8.5 to 11.2) at room temperature, leading to both demethylation and P-elimination. At higher pHs p-elimination had increased initial speed but soon plateaued. Demethylation was slower but proceeded until completion. It followed a (pseudo)-first order kinetics with respect to concentration of methylesterified carboxyl groups. A rate constant of 27.2 9.0 moT 1 min was calculated after correction for the pH variation during the course of the reaction. [Pg.603]

Figure 6.16 displays the temperature profile and liquid-phase molar fractions for cumene and DIPB. It may be observed that the temperature is practically constant over the reactive sections with a first plateau at 200 °C and a second one at 210 °C. The top temperature is at 198 °C while the bottom temperature climbs to 242 °C. The explanation may be found in the variation of concentrations for cumene and DIPB in the liquid phase. The maximum reaction rate takes place on the stages where propylene is injected. The cumene concentration increases rapidly and reaches a flat trend corresponding to the exhaustion of the propylene in liquid phase. It may be seen that the amount of DIPB increases considerably in the second reaction zone. This variation is very different from that with a cocurrent PFR. The above variations suggest that the productivity could be improved by providing several side-stream injections and/or optimizing the distribution of catalyst activity. [Pg.198]


See other pages where Plateau Variation with temperature is mentioned: [Pg.443]    [Pg.26]    [Pg.135]    [Pg.351]    [Pg.238]    [Pg.43]    [Pg.58]    [Pg.268]    [Pg.286]    [Pg.372]    [Pg.47]    [Pg.4404]    [Pg.543]    [Pg.266]    [Pg.191]    [Pg.125]    [Pg.169]    [Pg.130]    [Pg.328]    [Pg.5]    [Pg.662]    [Pg.393]    [Pg.308]    [Pg.57]    [Pg.201]    [Pg.440]    [Pg.76]    [Pg.185]    [Pg.5]    [Pg.94]    [Pg.119]    [Pg.122]    [Pg.192]    [Pg.57]    [Pg.442]    [Pg.222]   
See also in sourсe #XX -- [ Pg.121 ]




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