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Silica fitting data

Fitting data on 0.049 silica weight fraction compound... [Pg.311]

This also illustrates the use of different wavelengths of light to obtain much more infomration on the nature of the film. Here A and T are plotted versus the wavelength of light ( ) and the line drawn tln-ough these data represents a fit calculated for the various fihns of yttrium oxide deposited on silica as shown at tire bottom of the figure [40],... [Pg.1888]

Well as various samples of nonporous but amorphous silica. They found that the points fitted on to a common curve very closely, which may be plotted from Table 2.14. A corresponding curve, though based on fewer samples, was put forward for y-alumina. The two curves are close to one another, but the divergence between them is greater than that between different samples of the same substance. Standard isotherm data for argon (at 77 K) on silica have been obtained by various workers. ... [Pg.92]

FIGURE 22.11 Uniaxial stress-strain data (up-cycles) of solution-based styrene-butadiene rubber (S-SBR) samples with 60 phr silica at different prestrains s =100%, 150%, 200%, 250%, and 300% (symbols) and fittings (lines) with the stress-softening model Equations 22.19-22.24. The fitting parameters are indicated. The insert shows a magnification of the small-strain data. (From Kliippel, M. and Heinrich, G., Kautschuk, Gummi, Kunststojfe, 58, 217, 2005. With permission.)... [Pg.620]

Figure 4. Cross-sectional bright-field TEM views of Au-implanted silica samples at 3 x lO Au /cm, 190 keV, aimealed for 1 h at (a) 400 °C in air, (b) 700 °C in air, (c) 900 °C in air, and (d) 900 °C in Ar, respectively (e) the histograms of the size distribution of the samples annealed 1 h in air at different temperatures (f) Arrhenius plot of the squared average cluster radius after 1 h annealing in air (filled circles) or argon (empty triangles). Solid lines are linear fit to the experimental data. Figure 4. Cross-sectional bright-field TEM views of Au-implanted silica samples at 3 x lO Au /cm, 190 keV, aimealed for 1 h at (a) 400 °C in air, (b) 700 °C in air, (c) 900 °C in air, and (d) 900 °C in Ar, respectively (e) the histograms of the size distribution of the samples annealed 1 h in air at different temperatures (f) Arrhenius plot of the squared average cluster radius after 1 h annealing in air (filled circles) or argon (empty triangles). Solid lines are linear fit to the experimental data.
Ruland and Smarsly [84] study silica/organic nanocomposite films and elucidate their lamellar nanostructure. Figure 8.47 demonstrates the model fit and the components of the model. The parameters hi and az (inside H ) account for deviations from the ideal two-phase system. Asr is the absorption factor for the experiment carried out in SRSAXS geometry. In the raw data an upturn at. s o is clearly visible. This is no structural feature. Instead, the absorption factor is changing from full to partial illumination of the sample. For materials with much stronger lattice distortions one would mainly observe the Porod law, instead - and observe a sharp bend - which are no structural feature, either. [Pg.202]

Figure 14 Self-diffusivity D versus configurational entropy Sc data (symbols) for the BKS silica model at two different density p values. The lines are fits to the AG form given by Eq. [10] with tr Figure 14 Self-diffusivity D versus configurational entropy Sc data (symbols) for the BKS silica model at two different density p values. The lines are fits to the AG form given by Eq. [10] with tr <x 1/D. Reprinted with permission from Ref. 91.
Also other Type B and C series from Table II are consistent with the above elimination mechanisms. The dehydration rate of the alcohols ROH on an acid clay (series 16) increased with the calculated inductive effect of the group R. For the dehydrochlorination of polychloroethanes on basic catalysts (series 20), the rate could be correlated with a quantum-chemical reactivity index, namely the delocalizability of the hydrogen atoms by a nucleophilic attack similar indices for a radical or electrophilic attack on the chlorine atoms did not fit the data. The rates of alkylbenzene cracking on silica-alumina catalysts have been correlated with the enthalpies of formation of the corresponding alkylcarbonium ions (series 24). Similar correlations have been obtained for the dehydrosulfidation of alkanethiols and dialkyl sulfides on silica-alumina (series 36 and 37) in these cases, correlation by the Taft equation is also possible. The rate of cracking of 1,1-diarylethanes increased with the increasing basicity of the reactants (series 33). [Pg.169]

A decrease in metal-carbon distances when going down a group has also been pointed out. However, if this observation can roughly be applied to Zr and Hf (owing to lanthanide contraction), it does not fit the data obtained for Ti (Table 11.1). In contrast, for tetracoordinated complexes of the third transition row, replacement of just one neopentyl ligand is reported only when silica was pretreated at 700°C [18, 19, 23, 24]. For the tantalum complex [Ta(=CHCMe3)Np3, its... [Pg.421]

FIGURE 6.5 The measured power of the third harmonic power generated in the bulk of solution containing 0.5- xm-diameter fused silica microspheres as a function of microspheres concentration. Circles are experimentally measured data points the dashed line is a linear fit. [Pg.133]

Further work by Cornish and Watt ( ) and Silvernail and Goet-zinger ( ) established the active role played by the presence of water, and these authors concluded that a chemical-mechanical hypothesis would fit the observed data. In the case of ceric oxide polishing of glass, Cornish and Watt suggest the formation of a "CeO-Si" activated complex which permits the rupture of the O-Si-0 bonds by hydrolysis. The complex "CeO-Si" then breaks apart, the hydrated silica is swept away along with alkalis released from the glass surface, and the process repeats. [Pg.97]

Analytical. Samples were chromatographed on a Hewlett-Packard 5880A gas chromatograph which was fitted with a 30M fused silica capillary column (DBS) and an automatic sampler. The GC was interfaced to a Hewlett-Packard 3354 Laboratory Automation System (LAS). Raw data was automatically transferred to the LAS where peaks were selected by retention time, integrated and stored in a processed file. Processed data was then transferred... [Pg.112]

PUF. Each of the three 2.0-mL PUF extracts was subjected to GC-MS analyses. All analyses were conducted with a Finnigan OWA 1020 GC-MS system fitted with an SE-54 fused-silica capillary column. All spectra were collected in the total ion mode. Component spectra, both raw and background subtracted, were manually compared against USEPA-NIH library spectra to permit component identifications. Quantitative data were again provided by using dio-anthracene as the internal standard. [Pg.250]

The ammoxidation of isobutene has not received much attention. The only contribution in this field is by Onsan and Trimm [2.44] for a rather unusual catalyst, a mixture of the oxides of Sn, V and P (ratio 1/9/3) supported on silica. At 520 C, a maximum selectivity to methacrylonitrile + methacrolein of 80% was reached with a Sn—V—P oxide catalyst (ratio 1/9/3), an isobutene/ammonia/oxygen ratio of 1/1.2/2.5 and a contact time of 120 g sec l ]. The kinetics are very similar to those for the pro-pene ammoxidation. Again, the data are initially analysed by means of (parallel) power rate equations, for which the parameters were calculated, while a more detailed analysis proves that a Langmuir—Hinshelwood model with surface reaction as the rate-controlling step provides the best fit with regard to the two main products. At 520° C, the equation which applies for the production of methacrolein plus methacrylonitrile is... [Pg.179]

As appears from the examination of the equations (giving the best fit to the rate data) in Table 21, no relation between the form of the kinetic equation and the type of catalyst can be found. It seems likely that the equations are really semi-empirical expressions and it is risky to draw any conclusion about the actual reaction mechanism from the kinetic model. In spite of the formalism of the reported studies, two observations should be mentioned. Maatman et al. [410] calculated from the rate coefficients for the esterification of acetic acid with 1-propanol on silica gel, the site density of the catalyst using a method reported previously [418]. They found a relatively high site density, which justifies the identification of active sites of silica gel with the surface silanol groups made by Fricke and Alpeter [411]. The same authors [411] also estimated the values of the standard enthalpy and entropy changes on adsorption of propanol from kinetic data from the relatively low values they presume that propanol is weakly adsorbed on the surface, retaining much of the character of the liquid alcohol. [Pg.353]

These mechanisms are in formal agreement with kinetic equations assuming surface reaction between molecularly adsorbed reactants besides the group of catalysts used by Mochida et al. [406], such equations were also found to fit the kinetic data for silica—alumina [405] and bauxite [414] (see Table 21). [Pg.355]


See other pages where Silica fitting data is mentioned: [Pg.157]    [Pg.309]    [Pg.310]    [Pg.310]    [Pg.404]    [Pg.614]    [Pg.17]    [Pg.55]    [Pg.115]    [Pg.115]    [Pg.97]    [Pg.19]    [Pg.176]    [Pg.182]    [Pg.93]    [Pg.607]    [Pg.287]    [Pg.472]    [Pg.112]    [Pg.613]    [Pg.81]    [Pg.143]    [Pg.222]    [Pg.430]    [Pg.432]    [Pg.333]    [Pg.171]    [Pg.522]    [Pg.577]    [Pg.588]    [Pg.608]   
See also in sourсe #XX -- [ Pg.311 ]




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