Observed value

Range of values observed over the acidity range. Isotope effect at H = -2.0. 

The maximum oxidation state observed for the elements first increases and then decreases as we go across the transition row. Thus we have 4-3 for scandium, 4-4 for titanium, 4-5 for vanadium, 4-6 for chromium, and 4-7 for manganese. The 4-7 represents the highest value observed for this transition row. After manganese, the maximum value diminishes as we continue toward the end of the transition row. 

Because the sulfonic acid melts with decomposition, the value observed for the melting point is highly dependent on the rate of heating of the sample.9-12 

The emf depends on the concentrations of the ions, as we explore later here we have reported the value observed when the two solutions have equal cation concentrations.) In this case, the electrons can be thought of as tending to travel 

Fig. 2. Observed vs. calculated rates of hydrolysis of enamines at 24.8°. Drawn lines calculated log k values. Observed values o for 4-(2-methylpropenyl)morpholine A for l-(2-methylpropenyl)piperidine for l-(2-methylpropenyl)pyrrolidine. Values are corrected for buffer contributions (23).

The trans,trans-dmnylene group has a Pr value of 57, somewhat greater than the pr values observed for p-phenylene, rrans-vinylene, and ethynylene. 

The values for PuBr3+ and PuBr deduced by Shiloh and Marcus (100) from absorption spectra of concentrated LiBr solutions are one order of magnitude lower than the values observed by the same authors for the chloride complexes in LiCl solutions at 

Ruths and Granick [95] have studied the self-adhesion of several monolayers and adsorbed polymers onto mica. For loose-packed monolayers, the adhesion, in excess of a constant value observed at low rate, increased as a power law with the square root of the separation rate. In the case of adsorbed diblocks, the excess adhesion increased linearly with logarithmic separation rate. The time effects were ascribed to interdigitation and interdiffusion between the contacting layers. 

The S S distance in the dimer of the thiatrazinyl radical 4.16 (E = S) is 2.67 similar to the values observed for the intramolecular S S interactions in 4.12 (R = NMc2) and 4.1. Indeed this dimerization involves a interaction analogous to those depicted in Eigure 4.8 

Figure 4.14 shows the first few iteration steps in the evolution of the spatial measure block-entropy of rule R122 for blocks with size B < 5. Although the irreversibility of this rule predictably leads to a decrease of entropy with time, there nonetheless appears to be a relaxation to equilibrium values. Observe also 

By way of comparison, for natural grass playing fields in late autumn ranges from about 75 for wet fields to 280 for fro2en turf (8). The intermediate values observed depend on soil type, moisture, condition, and other variables. 

The first empirical and qualitative approach to the electronic structure of thiazole appeared in 1931 in a paper entitled Aspects of the chemistry of the thiazole group (115). In this historical review. Hunter showed the technical importance of the group, especially of the benzothiazole derivatives, and correlated the observed reactivity with the mobility of the electronic system. In 1943, Jensen et al. (116) explained the low value observed for the dipole moment of thiazole (1.64D in benzene) by the small contribution of the polar-limiting structures and thus by an essentially dienic character of the v system of thiazole. The first theoretical calculation of the electronic structure of thiazole. benzothiazole, and their methyl derivatives was performed by Pullman and Metzger using the Huckel method (5, 6, 8). 

When the pressures to induce shock-induced transformations are compared to those of static high pressure, the values are sufficiently close to indicate that they are the same events. In spite of this first-order agreement, differences between the values observed between static and shock compression are usually significant and reveal effects controlled by the physical and chemical nature of the imposed deformation. Improved time resolution of wave profile measurements has not led to more accurate shock values rather. 

The scope of Wessling route has been extended by Mullen and co-workers to develop a soluble precursor route to poly(anthrylene vinyiene)s (PAVs) [51]. It was anticipated that the energy differences between the quinoid and aromatic resonance structures would be diminished in PAV relative to PPV itself. An optical band gap of 2.12 eV was determined for 1,4-PAV 29, some 0.3 eV lower than the value observed in PPV. Interestingly, the 9, lO-b/.v-sulfonium salt does not polymerize, possibly due to stcric effects (Scheme 1-9). 

In TFE the secondary isotope effect for solvolysis ( h/ d3)s is found to have the value 1.46 and that for Na,Np-rearrangement (kH/kD3)r has the value 1.42 (Szele and Zollinger, 1981). The two isotope effects are similar to the largest values observed in nucleophilic aliphatic substitutions following the DN + AN mechanism (Shiner, 

While pressure melting may be important for snow and ice near 0°C, it is possible that even here an alternative explanation will prove important. Ice is a substance of unusual structural complexity, and it has been speculated that a liquidlike surface layer is present near the melting point [17,18] if this is correct, the low /t values observed at low sliding speeds near 0°C may be due to a peculiarity of the surface nature of ice rather than to pressure melting. 

The Eo values for 2-substituted 1,4-benzoquinones (sets 45-4 through 45-7, 45-10) show an average value of pr of 59. Thus the resonance effect predominates. For most of these sets, the Op constants are not the best parameters for correlation. By contrast, the electron reduction potentials (set 45-8) show a Pr value of 39, which indicates predominance of the localized effect. The 2,5-disubstituted 1,4-benzoquinones differ distinctly in their behavior from the 2-substituted 1,4-benzoquinones in that they show an average Pr value of 53. The one-electron reduction potentials of these compounds show about the same composition of the electrical effect, with a value of Pr of 50. The only set of Eq values available for the 2,6-disubstituted 1,4-benzoquinones pve a Pr value of 51, comparable to the values observed for the 2,5-disubsti-tuted 1,4-benzoquinones. The 2,3,5,6-tetrasubstituted 1,4-benzoquinones have 

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