Big Chemical Encyclopedia

Chemical substances, components, reactions, process design ...

Articles Figures Tables About

Typical Behavior of

From Figs. 1 and 2, it can be seen that the transition at point Q (between regions II and III) is very sharp as compared to the transition at point P (between regions I and II). This difference in nature can be attributed to the different terms through which the function becomes negative. It can be seen from Eq. (25) that the numerator in the second term on the RHS is always positive, whereas its denominator can be either negative or positive. When the denominator becomes zero, fi will become discontinuous. The other way in which the function fi can become negative is when the denominator is smaller than the numerator. [Pg.19]

In the case of the transition from region I to region II, which is gradual, the function/i becomes negative as the numerator exceeds the denominator (which remains positive). This generally happens when the inertial terms B and C are small, term A approaches unity, and thus the transition is decided by the comparison between GIF and Vz. It will be shown later [Pg.19]

In the present work, we have analyzed only one transition for all the multiphase systems. For bubble columns, we have considered the transition from region III to region II (point Q). In region I, gas hold-up is typically [Pg.21]


This typical behavior of the very unsymmetrical thiazole ring led to a series of studies from the group of H. Erlenmeyer in Basle be studied the H/D exchange of 2,4-dimethyl-5-carboxythia2ole as well as that of similar methylated nitrogen heterocycles (507). The results are shown in Fig. 1-27. [Pg.144]

Exploration of the region 0 < T < requires numerical calculations using eqs. (2.5)-(2.7). Since the change in /cq is small compared to that in the leading exponential term [cf. (2.14) and (2.18)], the Arrhenius plot k(P) is often drawn simply by setting ko = coo/ln (fig. 5). Typical behavior of the prefactor k and activation energy E versus temperature is presented in fig. 6. The narrow intermediate region between the Arrhenius behavior and the low-temperature limit has width... [Pg.15]

Using a delicate reduction method, the aldehyde group can be converted to a sixth hydroxyl group, giving the substance called sorbitol. This compound shows the typical behavior of an alcohol. For example, it forms esters with acids ... [Pg.423]

Fig. 6. Typical behavior of the function y = F(E) === R — f(E). The Newton-Raphson construction shows that the second-order process based on Eqs. III.51 and III.53 does not always converge towards the eigenvalue lying closest to E(0). Fig. 6. Typical behavior of the function y = F(E) === R — f(E). The Newton-Raphson construction shows that the second-order process based on Eqs. III.51 and III.53 does not always converge towards the eigenvalue lying closest to E(0).
The microphase separation of an amphiphilic polyelectrolyte is clearly reflected in the viscosity behavior of its aqueous solution. As a representative example, Fig. 5 shows the reduced viscosities of ASt-x with different styrene (St) content plotted against the polymer concentration in salt-free aqueous solution [29], The AMPS homopolymer and its copolymers with low St content exhibit negative slopes, which is the typical behavior of polyelectrolytes in the concentration range shown in Fig. 5. With increasing St content, however, the slope systematically decreases and eventually turns to be slightly positive, while reduced viscosity itself markedly decreases. These data indicate that, with increasing St content, the... [Pg.63]

A typical behavior of amplitude dependence of the components of dynamic modulus is shown in Fig. 14. Obviously, even for very small amplitudes A it is difficult to speak firmly about a limiting (for A -> 0) value of G, the more so that the behavior of the G (A) dependence and, respectively, extrapolation method to A = 0 are unknown. Moreover, in a nonlinear region (i.e. when a dynamic modulus depends on deformation amplitude) the concept itself on a dynamic modulus becomes in general not very clear and definite. [Pg.93]

Class 111-type behavior is representative of reactions in which jt bonds have to be broken. It is the typical behavior of reactions in which CO or N2 bond activation is rate limiting. [Pg.21]

In both cases, the half-wave potential shifts by RT/ ziF)vaN per pH unit, and a typical example of such a behavior is given in Fig. 9 for the transfer of two acidic fi-diketones at the water-nitrobenzene interface. These results were unexpected, since a current wave is measured at a pH where the compound of interest is by a very large majority neutral, but they in fact represent the typical behavior of ionizable compounds at the ITIES and prove that the interfacial potential and the transfer of protons plays a key role for the distribution in biphasic systems. [Pg.745]

Figure 8.1 shows the typical behavior of a ceria-based sample. As a rule ... [Pg.236]

Substitution of P-substituents other than halogens has been reported for P-ethoxy-l,3,2-diazaphospholene and l,3,2-diazaphospholene-2-oxide which react with trichlorosilane to yield the corresponding P-chloro-substituted heterocycles [49,50]. This reaction reflects a typical behavior of phosphine derivatives undergoing halogen replacement similar to the previously discussed transformations. [Pg.73]

Fig. 4.7 Typical behavior of a solid detergent product during the first 20 minutes in a commercially available washing machine. Relevant parameters (pH value, conductivity A, surface tension y, peroxide content ) were detected by on-line sensorics. Fig. 4.7 Typical behavior of a solid detergent product during the first 20 minutes in a commercially available washing machine. Relevant parameters (pH value, conductivity A, surface tension y, peroxide content ) were detected by on-line sensorics.
The main result was that regardless of dendrimer generation (i.e. molecular weight) and concentration, all of the examined solutions exhibited characteristic Newtonian flow behavior, as shown in Figure 14.6. This was in striking contrast to the typical behavior of either chain-type polymers of comparable molecular weights [33], or suspensions of spherical particles [34-37], both of which exhibit... [Pg.342]

Figure 1.5 Typical behavior of the dipole function M(r) as a function of r (in atomic units). The results shown are realistic for HF (adapted from Zemke et al., 1991 see also Arunan et al., 1992). Figure 1.5 Typical behavior of the dipole function M(r) as a function of r (in atomic units). The results shown are realistic for HF (adapted from Zemke et al., 1991 see also Arunan et al., 1992).
The typical behavior of M0 v is shown in Figure 1.6. One should note that, for the Morse potential, and in lowest approximation, the radial wave functions and thus v are independent of /. This is no longer the case for more general potentials and for the exact solution of the Morse problem. [Pg.16]

Figure 1.6 Typical behavior of the radial matrix elements M0as a function of v. The results shown are for HC1 and are given in SI units. Adapted from Ogilvie and Tipping (1983). Figure 1.6 Typical behavior of the radial matrix elements M0as a function of v. The results shown are for HC1 and are given in SI units. Adapted from Ogilvie and Tipping (1983).
The typical behavior of intensities in molecules was discussed in Chapter 1. A realistic approximation of this behavior can be obtained in the algebraic framework by considering the operator... [Pg.37]

Thermal degradation prior to ionization can cause decarbonylation or decarboxylation of the analyte. Decarbonylation, for example, is observed from a-ketocarboxylic acids and a-ketocarboxylic acid esters, whereas decarboxylation is typical behavior of P-oxocarboxylic acids such as malonic acid and its derivatives and di-, tri-, or polycarboxylic acids. [Pg.289]

Figures 3 to 5 shows the density, heat capacity, and viscosity as a function of the pressure near the critical pressure of CO2 at 320 K. At lower and higher pressures, the curves exhibit the typical behavior of gas and liquid, respectively. Above the critical pressure, the viscosity follows the ascent of density. Figures 3 to 5 shows the density, heat capacity, and viscosity as a function of the pressure near the critical pressure of CO2 at 320 K. At lower and higher pressures, the curves exhibit the typical behavior of gas and liquid, respectively. Above the critical pressure, the viscosity follows the ascent of density.
The typical behavior of an atomic displacement parameter is represented by the curve plotted in Fig. 2. This trend tells us that below the turn point (0e/2) atomic vibrations are not only smaller but also quite constant. [Pg.38]

Because of the choice of enumeration, the vectors of logarithms of reaction rate constants form a convex cone in which is described by the system of inequalities lnfc2i> lnfc,y, (/,/)t (2,1). For each of the possible auxiliary systems (Figure 4) additional inequalities between constants should be valid, and we get four correspondent cones in These cones form a partitions of the initial one (we neglect intersections of faces which have zero measure). Let us discuss the typical behavior of systems from these cones separately. (Let us remind that if in a cone for some values of coefficients dp then,... [Pg.149]

The simplest one-constant limitation concept cannot be applied to all systems. There is another very simple case based on exclusion of "fast equilibria" A Ay. In this limit, the ratio of reaction constants Kij — kij/kji is bounded, 0equilibrium constant", even if there is no relevant thermodynamics.) Ray (1983) discussed that case systematically for some real examples. Of course, it is possible to create the theory for that case very similarly to the theory presented above. This should be done, but it is worth to mention now that the limitation concept can be applied to any modular structure of reaction network. Let for the reaction network if the set of elementary reactions is partitioned on some modules — U j. We can consider the related multiscale ensemble of reaction constants let the ratio of any two-rate constants inside each module be bounded (and separated from zero, of course), but the ratios between modules form a well-separated ensemble. This can be formalized by multiplication of rate constants of each module on a timescale coefficient fc,. If we assume that In fc, are uniformly and independently distributed on a real line (or fc, are independently and log-uniformly distributed on a sufficiently large interval) then we come to the problem of modular limitation. The problem is quite general describe the typical behavior of multiscale ensembles for systems with given modular structure each module has its own timescale and these time scales are well separated. [Pg.160]

When these properties are examined it is clear that the resolution, although it is the response of interest, is not a response which should be modeled. This is because of the typical behavior of the resolution when spots cross (Figure 6.2). At such situations the resolution is not continuous in its derivative and is therefore difficult to model with standard models. These problems are even more pronounced when minimum resolution is used. It is... [Pg.248]

Salts of very powerful oxidizing acids (eg chromic or permanganic) are unknown, and are unlikely to exist. Hydrazonium iodate may exist in solution at low temp (Ref 27a). Alkali metals, amides and hydrides react with hydrazine to give the corresponding alkali hydrazide. Sodium hydrazide explodes violently in the presence of 02 or when heated above 100°C—a typical behavior of the alkali hydrazides. For other reactions, see Ref 24 Explosive and Combustion Properties... [Pg.192]

In multifunctional monomer polymerizations, the mobility of radicals through segmental diffusion falls well before their mobility through reaction diffusion at very low functional group conversions (as compared to linear polymerizations). From this point in the reaction, the termination and propagation kinetic constants are found to be related, and the termination kinetic constant as a function of conversion may actually exhibit a plateau region. Figure 6 illustrates the typical behavior of kp and k, vs conversion as predicted by a kinetic based model. [Pg.196]

From the dynamic mechanical investigations we have derived a discontinuous jump of G and G" at the phase transformation isotropic to l.c. Additional information about the mechanical properties of the elastomers can be obtained by measurements of the retractive force of a strained sample. In Fig. 40 the retractive force divided by the cross-sectional area of the unstrained sample at the corresponding temperature, a° is measured at constant length of the sample as function of temperature. In the upper temperature range, T > T0 (Tc is indicated by the dashed line), the typical behavior of rubbers is observed, where the (nominal) stress depends linearly on temperature. Because of the small elongation of the sample, however, a decrease of ct° with increasing temperature is observed for X < 1.1. This indicates that the thermal expansion of the material predominates the retractive force due to entropy elasticity. Fork = 1.1 the nominal stress o° is independent on T, which is the so-called thermoelastic inversion point. In contrast to this normal behavior of the l.c. elastomer... [Pg.159]


See other pages where Typical Behavior of is mentioned: [Pg.304]    [Pg.253]    [Pg.440]    [Pg.272]    [Pg.83]    [Pg.204]    [Pg.183]    [Pg.226]    [Pg.72]    [Pg.350]    [Pg.285]    [Pg.179]    [Pg.29]    [Pg.101]    [Pg.335]    [Pg.61]    [Pg.37]    [Pg.161]    [Pg.188]    [Pg.46]    [Pg.10]    [Pg.862]    [Pg.1064]    [Pg.153]    [Pg.21]    [Pg.486]   


SEARCH



Typical behavior

© 2024 chempedia.info