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Neutralization curves

The usefulness of Eq. (3.41) depends crucially on whether or not the sensitivity factor rjA depends on the presence of other elements in the surface ( matrix effects ). It is an experimental finding that in general neutralization depends only on the atomic number of the scattering center, and matrix effects occur rarely. An instructive example is the neutralization of He by A1 in the pure metal and in alumina. The slopes of the neutralization curves turn out to be the same for both materials, i. e. matrix effects are absent [3.143]. This is a strong indication that in the neutralization process not only the valence/conduction electrons, but also atomic levels below the valence/ conduction band are involved. [Pg.156]

Figure 12.18 Neutralization curve for aqueous orthophosphoric acid. For technical reasons the curve shown refers to 10 cm of 0.1 M NaH2P04 titrated (to the left) with 0.1 m aqueous HCl and (to the right) with 0.1m NaOH solutions. Extrapolations to points corresponding to 0.1m H3PO4 (pH 1.5) and 0.1m Na3P04 (pH 12.0) are also shown. Figure 12.18 Neutralization curve for aqueous orthophosphoric acid. For technical reasons the curve shown refers to 10 cm of 0.1 M NaH2P04 titrated (to the left) with 0.1 m aqueous HCl and (to the right) with 0.1m NaOH solutions. Extrapolations to points corresponding to 0.1m H3PO4 (pH 1.5) and 0.1m Na3P04 (pH 12.0) are also shown.
The neutral curves are therefore characteristic of non-associated substances, a conjecture which is in accord with the results of independent branches of investigation. [Pg.402]

Wittwer and Zollinger (1954) determined the neutralization curves of aqueous solutions of diazonium salts under standard conditions of ionic strength, etc., and found that the acidity depended on the degree of neutralization in a manner different to that expected for a dibasic acid. The curve obtained did not exhibit two steps with an intermediate region of a few pH units in which the monobasic acid is stable, as is the case, for instance, with oxalic acid (Fig. 5-1). On the contrary, there was only one step, but it extended over two equivalents of base per diazonium ion. [Pg.90]

Fig. 3 shows a hypothetical case similar to the NH" situation but for which the anion and neutral curves approach closely at longer bond lengths. In this case, one would expect larger rates of detachment than in NH because... [Pg.293]

The anion and neutral curves approach one another at R values that are accessible to the vibrational wavefimctions of the two states shown in Fig. 3, thus allowing strong modulation of the HOMO. [Pg.293]

The slope of the tangent to the curve at the inflection point where oc = is thus inversely proportional to the number of electrons n. The E-oc curves are similar to the titration curves of weak acids or bases (pH-or). For neutralization curves, the slope dpH/doc characterizes the buffering capacity of the solution for redox potential curves, the differential dE/da characterizes the redox capacity of the system. If oc — for a buffer, then changes in pH produced by changes in a are the smallest possible. If a = in a redox system, then the potential changes produced by changes in oc are also minimal (the system is well poised ). [Pg.190]

The oxidation-neutralization curve (Fig. 3) gives a long term prediction of AMD generation (see Benzaazoua et al. 2001 for more details). Assuming steady-state geochemical behaviour, the oxidation products (sulfates) would disappear before theneutralizing elements (Ca, Mg, and Mn). [Pg.329]

Fig. 3. Extrapolated oxidation-neutralization curve for the long-term prediction of acid mine drainage of the tree samples (Benzaazoua Al 2001)... Fig. 3. Extrapolated oxidation-neutralization curve for the long-term prediction of acid mine drainage of the tree samples (Benzaazoua Al 2001)...
FIGURE 13.4. Neutralization curve of a palladium nitrate solution [Pd] = 5 g/L by addition of soda [NaOH] = 0.1 N. [Pg.260]

We note that the a anion lies 3.80 eV above the imnimum of the neutral species in our calculations, which is somewhat higher than the experimentally determined 3.25 eV value in the DEA yield spectrum [7] (although this peak is 0.5 eV broad). We also note that the anion and neutral curves cross ca. 1.63 eV above the neutral s minimum. This amount of energy seems to be too high for vibrational excitation of the C-S bond to access at room temperature and thus accessing this crossing point remains unrealizable except at considerably elevated temperatures. [Pg.246]

A measurement of the ability of a buffer system to limit the change in pH of a solution upon the addition of an increment of strong base. ft is the reciprocal of the slope of the pH-neutralization curve. Consider the simple equilibrium, HA H+ -h A where K = [H+][A ]/ [HA] in which K is a practical dissociation constant determined under conditions of constant ionic strength. In such systems the practical pK is equal to the pH of solution when there are equal concentrations of the two buffer species. Since the total concentration of the two... [Pg.102]

Legeza, O., Roder, J., Hess, B.A. Qc-DMRG study of the ionic-neutral curve crossing of life. Mol. Phys. 2003, 101(13), 2019. [Pg.162]

The search for a possible oscillatory instability is slightly different from the procedure used in the stationary case. The solvability condition of the linearized set of equations determines both the neutral curve and the frequency along this curve. When searching for such a solution we scanned approximately the same parameter space as used for Figs. 5-7. Since the frequency tends to zero when the oscillatory neutral curve gets close to the stationary one, we concentrated on the frequency range 0 < co < 2 and checked in some cases for higher frequencies. [Pg.126]

Fig. 12 In most parts of the scanned parameter space no possibility for an oscillatory instability was found. If the director field is only very weakly coupled to the layering (in this plot we used Bo = 200 and V = 0.4) a neutral curve for an oscillatory instability ( Fig. 12 In most parts of the scanned parameter space no possibility for an oscillatory instability was found. If the director field is only very weakly coupled to the layering (in this plot we used Bo = 200 and V = 0.4) a neutral curve for an oscillatory instability (<dashed line) appears above the stationary neutral curve solid line ). Note that the critical wave vectors are close to each other for both oscillatory and stationary instability. The inset shows the frequency along the neutral curve...
The solvability condition of (85) and (86) defines the neutral curve 9o(q) and its minimum directly gives the critical values 6C and qc (within the approximations of this section) ... [Pg.141]

The 6-molybdoiodates or 6-tungstoiodates are prepared similarly. The free acid is made directly from periodate and molybdenum trioxide. It may also be prepared by reaction between barium molybdate, periodic acid, and sulfuric acid. Its neutralization curve has been reported147. The yellow free acid evolves gaseous products upon isolation27 and, therefore, probably undergoes some decomposition. [Pg.38]

Fig. 3. Neutralization curves of the polyhydrochlorides of different PTN, namely poly[thio-l-... Fig. 3. Neutralization curves of the polyhydrochlorides of different PTN, namely poly[thio-l-...
The Interest In the chemical interrelationships of phytate Initially centered around Its complexatlon with calcium and subsequent effect on the availability of calcium (33). This led to the classical studies by Hoff-Jorgenson (34). He determined eight of the twelve dissociation constants of phytic acid and using these data calculated thj solubilij products of penta-calclum phytate as between 10 and 10. A decade later with the use of neutralization curves and conductivity measurements it was concluded that phytic acid contained 6 strong acid groups which were completely dissociated in solution (pk = 1.84), 2 weak acid functions (pk = 6.3) and 4 very weak acid protons (pk = 9.7) (M). [Pg.149]

Along with the constant-Oj contours, the constant-Or contours can be plotted in the Re — wo)-plane, as shown in Fig. 2.3. The neutral curve is included in this figure to provide a reference. From this figure, it is noted... [Pg.45]

Consider the application of spatial theory for a wall-bounded external flow. On the top panel of Fig. 2.5, we once again show the neutral curve... [Pg.48]

The amplification rate suffered by the disturbances within the neutral curve is shown in the middle panel of Fig. 2.5. Note the sign of the plotted rate, with negative values plotted along the positive ordinate direction. For two-dimensional disturbances in two-dimensional mean flow, the amplification rate can be expressed as. [Pg.50]

In Fig. 2.8, the neutral curves for the above four velocity profiles of Fig. 2.7 are compared. The deciding trend is that as H increases, Rccr decreases. And for flows with > 0, the critical Reynolds numbers are significantly lower. [Pg.52]

Figure 2.8 Neutral curves of some shear layer velocity profiles... Figure 2.8 Neutral curves of some shear layer velocity profiles...
To understand the spatio-temporal growth of waves, few cases were considered in Sengupta et al. (2006), marked as A, B, C and D in Fig. 4.2, with respect to the neutral curve shown in the Re — wo)-plane for the leading eigenmode. [Pg.166]

Figure 4.2 Neutral curve for the Blasius boundary layer identifying stable and unstable regions. The marked points are further investigated. Figure 4.2 Neutral curve for the Blasius boundary layer identifying stable and unstable regions. The marked points are further investigated.

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See also in sourсe #XX -- [ Pg.158 ]

See also in sourсe #XX -- [ Pg.52 , Pg.275 , Pg.277 ]




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