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Solid point

Fig. XVI-7. Dielectric isotherms of water vapor at 15°C adsorbed on a-FeiOa (solid points indicate desorption). A complete monolayer was present at P/P = 0.1, and by P/P = 0.8 several layers of adsorbed water were present. (From Ref. 110.)... Fig. XVI-7. Dielectric isotherms of water vapor at 15°C adsorbed on a-FeiOa (solid points indicate desorption). A complete monolayer was present at P/P = 0.1, and by P/P = 0.8 several layers of adsorbed water were present. (From Ref. 110.)...
Fig. 5.20 Adsorption isotherms for water vapour on x-Fe,Oj at 15°C for various outgassing temperatures. Solid points indicate second isotherm after 25°C evacuation of physically adsorbed water. (Courtesy Zettlemoyer.) Outgassing temperature,<, 25°C , I00°C O, 250°C ... Fig. 5.20 Adsorption isotherms for water vapour on x-Fe,Oj at 15°C for various outgassing temperatures. Solid points indicate second isotherm after 25°C evacuation of physically adsorbed water. (Courtesy Zettlemoyer.) Outgassing temperature,<, 25°C , I00°C O, 250°C ...
Solid points Measured in oxidation Rhines and Connel 1 (1977 ) AAtkinson et al (1982 )... [Pg.1040]

Figure 8. Charge-discharge Curves for Li Sn (x=0.8 to 2.5) at ambient temperature. Solid points are at a current density of 0.24 mAcm 2, and open points at a current density of 0.5 rnAcrn-2. The equilibrium potential is also shown [41 ]. Figure 8. Charge-discharge Curves for Li Sn (x=0.8 to 2.5) at ambient temperature. Solid points are at a current density of 0.24 mAcm 2, and open points at a current density of 0.5 rnAcrn-2. The equilibrium potential is also shown [41 ].
FIG. 35 The phase behavior of dodecane sulfonic acid with water. O, Doubly refracting material appears as the isotropic solution is cooled. <3, Isotropic solution appears as the liquid crystal is heated. CD, Crystalline solid disappears on heating. Pairs of solid points connected with the vertical dashed lines mark the appearance and disappearance of pseudoisotropy as samples are heated. The area ABC, within which the intermediate mesophase exists alone, is not precisely determined. [Pg.192]

Fig. 4. Schematic representation of the smectic layering along with their characteristic diffraction patterns for the monolayer (Ai), the partially bilayer (Aj), the bilayer (A2) and the two-dimensional (A) phases. The arrows indicate permanent dipoles, the solid points are Bragg reflections... Fig. 4. Schematic representation of the smectic layering along with their characteristic diffraction patterns for the monolayer (Ai), the partially bilayer (Aj), the bilayer (A2) and the two-dimensional (A) phases. The arrows indicate permanent dipoles, the solid points are Bragg reflections...
It is significant that in the absence of O2 (solid points in Figure 4) almost no radicals were formed the amount reported is close to the detection limit of the instrument. In one sense, this observation provides an explanation for the positive effect that O, has on the rate of reaction between NO and CH4 [3,4] i.c., O2 enhances CH,- radical formation. However, the results also indicate that NO itself is not very effective in generating active sites which are responsible for CH,- radical production. This means that the reaction of NO with CH4, in the absence of added O, may occur via a nonradical pathway. [Pg.715]

The solid points show the experimental result, the long dashed line the calculation of a g(< )-modified Lindhard response function according to Equation (6), using g(q) after Utsumi and Ichimaru [5]. The solid line gives the result of a calculation that also takes into account self-energy effects on-shell, that is, introducing the lifetime of the involved states into the calculation according to Equation (14). One can clearly see that the latter reproduces the experimental result quite nicely. [Pg.196]

Fig. 25. Comparison between the experimental abstraction reaction H + H2O(00)(0) cross-section (solid point with error bars), and the 5D QM calculations (solid line). The 6D QM cross-sections with the CS approximation (dotted line), and the QCT data using normal (o) and Gaussian (A) binning procedures are shown. Fig. 25. Comparison between the experimental abstraction reaction H + H2O(00)(0) cross-section (solid point with error bars), and the 5D QM calculations (solid line). The 6D QM cross-sections with the CS approximation (dotted line), and the QCT data using normal (o) and Gaussian (A) binning procedures are shown.
Figure 1. Phase diagram showing the three distinct regions discussed in the text. Key n, diblock copolymers O, homopolymer blends pip up, heterogeneous pip down, homogeneous solid points, 12B/1,4B open points, l,4l/l,4B half-open point, 1,4I/1,2B with the abscissa representing the weight fraction of 1,2B. Figure 1. Phase diagram showing the three distinct regions discussed in the text. Key n, diblock copolymers O, homopolymer blends pip up, heterogeneous pip down, homogeneous solid points, 12B/1,4B open points, l,4l/l,4B half-open point, 1,4I/1,2B with the abscissa representing the weight fraction of 1,2B.
Figure 3. Detail of the plane at 50 weight percent diblock content in Fig. 2 including various data points from previous studies (1, 4, 26J. Key > 1,41/1,4B O, 1,2B/1,4B solid points, homogeneous materials open points, heterogeneous materials half solid point, a blend for which contradictory results were obtained in various experimental modes (26). Figure 3. Detail of the plane at 50 weight percent diblock content in Fig. 2 including various data points from previous studies (1, 4, 26J. Key > 1,41/1,4B O, 1,2B/1,4B solid points, homogeneous materials open points, heterogeneous materials half solid point, a blend for which contradictory results were obtained in various experimental modes (26).
The muonium centers observed in the curpous halides (see Table II) are unusual in several respects compared with Mu in other semiconductors and insulators. Figure 12 shows the reduced hyperfine parameters for Mu in semiconductors and ionic insulators plotted as a function of the ionicity (Philips, 1970). The positive correlation is especially apparent for compounds composed of elements on the same row of the periodic table where the lattice constants and valence orbitals are similar (see solid points in Fig. 12). Note however that the Mu hyperfine parameters in cuprous halides lie well below the line and in fact are smaller than in any other semiconductor or insulator (Kiefl et al., 1986b). The reason for this unusual behaviour is still uncertain but may be related to other unusual properties of the cuprous halides. For example the upper valence band is believed... [Pg.590]

Figure 9.3. Characterization of mesoporous Ti02 films templated by Pluronics block copolymers using diverse characterization techniques XRD pattern (a), transmission electron microscope (TEM) image (b), dark-field TEM image (c), and isotherms of Kr adsorption (d).The Pluronic-templated Ti02 films were calcined at 400°C (solid points) and 600°C (open points). The films were prepared according to Alberius et al. (Ref. 14). Figure 9.3. Characterization of mesoporous Ti02 films templated by Pluronics block copolymers using diverse characterization techniques XRD pattern (a), transmission electron microscope (TEM) image (b), dark-field TEM image (c), and isotherms of Kr adsorption (d).The Pluronic-templated Ti02 films were calcined at 400°C (solid points) and 600°C (open points). The films were prepared according to Alberius et al. (Ref. 14).
Figure 12.3. Benchmark of peer-reviewed academic reports of organic semiconductor device field-effect mobility versus time of report. All data points are for spin-coated organic semiconducting transistors. Solid points are derived from the benchmark study completed in 2002 by Brazis and Dyrc at Motorola (unpublished). The curve is a calculated estimation, based on these data, of what the expected mobility values will be in the future. The open points are data derived in 2005 from the public journals for verification of the 2002 prediction.6 38... [Pg.382]

Fig. 1 Micellar effects upon reaction of p-nitrophenyl diphenyl phosphate with benzimidazolide ion (solid points) open points are for reaction in the absence of benzimidazole , 10 4 M benzimidazole, pH 10.7 , 1.2 x 10-4 M benzimidazole, pH 11 O, pH 10.7, and 11 respectively. The solid lines are theoretical. (Reprinted by permission of the American Chemical Society)... Fig. 1 Micellar effects upon reaction of p-nitrophenyl diphenyl phosphate with benzimidazolide ion (solid points) open points are for reaction in the absence of benzimidazole , 10 4 M benzimidazole, pH 10.7 , 1.2 x 10-4 M benzimidazole, pH 11 O, pH 10.7, and 11 respectively. The solid lines are theoretical. (Reprinted by permission of the American Chemical Society)...
Fig. 8 Effect of NaOH upon reaction of 2,4-dinitrochlorobenzene with the hydro-phobic ammonium salts, (C H17)3NCH2CH2OH.X. Solid points in 80 vol% H2Oj open points in 70 vol% H20. Ammonium salt concentrations , 0.008 M, X = Br O, 0.05 M, X = Br , 0.05 M, X = OMs V, 0.1 M, X = OMs. The lines are theoretical. (Reprinted with permission of the American Chemical Society)... Fig. 8 Effect of NaOH upon reaction of 2,4-dinitrochlorobenzene with the hydro-phobic ammonium salts, (C H17)3NCH2CH2OH.X. Solid points in 80 vol% H2Oj open points in 70 vol% H20. Ammonium salt concentrations , 0.008 M, X = Br O, 0.05 M, X = Br , 0.05 M, X = OMs V, 0.1 M, X = OMs. The lines are theoretical. (Reprinted with permission of the American Chemical Society)...
Figure 3 Dependence of C37 on + Sj) obtained at [Si] = 037 mol dm Ref. 32 open points Ref. 31 solid points. Figure 3 Dependence of C37 on + Sj) obtained at [Si] = 037 mol dm Ref. 32 open points Ref. 31 solid points.
Figure 3.19. Variation of the energy transfer into the surface in scattering of NO from Ag(l 11) as a function of Ee = f ccsO,-. Solid lines and solid points are for rotationally elastic scattering. /, = Jj = 0.5 and the open points are for non-state-resolved scattering experiments (and therefore also contains a contribution from rotationally inelastic scattering). From Ref. [181]. Figure 3.19. Variation of the energy transfer into the surface in scattering of NO from Ag(l 11) as a function of Ee = f ccsO,-. Solid lines and solid points are for rotationally elastic scattering. /, = Jj = 0.5 and the open points are for non-state-resolved scattering experiments (and therefore also contains a contribution from rotationally inelastic scattering). From Ref. [181].
Figure 3.21. Rotational temperature 7 rot (defined as T in this chapter) in trapping-desorption scattering of NO from Pt(l 11) and covered Pt(lll) as a function of the surface temperature Ts. Open points are for Et = 80 meV and solid points are for Et = 220 meV. The straight line is for 7rot = Ts. From Ref. [206]. Figure 3.21. Rotational temperature 7 rot (defined as T in this chapter) in trapping-desorption scattering of NO from Pt(l 11) and covered Pt(lll) as a function of the surface temperature Ts. Open points are for Et = 80 meV and solid points are for Et = 220 meV. The straight line is for 7rot = Ts. From Ref. [206].
Figure 3.26. (a) The experimental dissociation probability S for N2 on Ru(0001) plotted logarithmically vs. the incident normal energy E = En for three different N2 vibrational temperatures as noted in the legend. The squares varied both En and Tv simultaneously. From Ref. [244]. (b) First principles predictions of the logarithim of the dissociation probability at two vibrational temperatures as noted in the legend. The solid points are from 3D (Z, R, q) quasi-classical dynamics and the open points are from 6D quasi-classical dynamics. The latter are from Ref. [27]. [Pg.205]

Figure 8.5. Outliers in calibration (a) near the center of the data causing a shift in intercept and (b) at the extreme of the data (a point with high leverage), causing change in slope. The solid lines are fits to the data without outliers (solid points). The dashed lines are fits to the data with outliers (all points). Figure 8.5. Outliers in calibration (a) near the center of the data causing a shift in intercept and (b) at the extreme of the data (a point with high leverage), causing change in slope. The solid lines are fits to the data without outliers (solid points). The dashed lines are fits to the data with outliers (all points).
FiO. 18. Benzotropylia(l),polyacenes (2), cyclopolyenes (3) and polyenes (4). Thiophenes O, benzothiopyrylia a, A. Model A solid points, Model B outlined marks. For explanation see text. [Pg.56]

CP common pointed(solid pointed CSC Central Scientific Co, Chicago 13, 111... [Pg.735]

Fig. 5.11. Plateau modulus vs. concentration for polymethyl methacrylate 0 (142) and cis-polyisoprene (167). The solid points are undiluted samples... Fig. 5.11. Plateau modulus vs. concentration for polymethyl methacrylate 0 (142) and cis-polyisoprene (167). The solid points are undiluted samples...
In considering true transition points we have considered only one, the liquid/ solid point, to be of practical significance. The other two points considered to be of practical importance—namely, the attainment of 5% and 90% maximum tensile strength—we have called critical points as opposed to transition points. We have not been able, as yet, to find simple reliable tests to replace tensile measurements. [Pg.166]

The 3 Operation The easiest way to see how 3 is related to our previous notation is to examine Figure 11.16a and compare it to Figure 11.166. These diagrams show all the points generated by clockwise rotation from an initial point 1 lying somewhere on the upper half (solid points) of a sphere. The open points lie on the lower half of the sphere as viewed from above. The numbers 1 to 6 show the order in which the points are generated, which is different in the two cases. The set of points, however, is exactly the same and thus 3 is the crystallographer s equivalent for S6. [Pg.377]

Logarithmic plots of the Freundlich equation, Q = kpn, where Q is the amount of methane adsorbed at a pressure p, and k and n are constants, for methane adsorption at 0°, 30° and 50°C. in Figures 6 and 7 indicate that the equation is valid up to at least 1000 torr. Equilibrium sorption points obtained on different samples in a manostatic adsorption apparatus are shown as solid points in Figures 6 and 7. The exponent n varied from 0.72 at 0° to 0.87 at 50°C. for the Pocahontas coal and from 0.78 at 0° to 0.94 at 50°C. for Pittsburgh coal (Table III). [Pg.392]

Open and solid points denote adsorption and desorption, respectively. [Pg.352]

Figure 38. Comparison of synchrotron PES18 (open points) and (e,2e)171 (solid points) branching ratios for CO and N2. Figure 38. Comparison of synchrotron PES18 (open points) and (e,2e)171 (solid points) branching ratios for CO and N2.
Figure 9. Laboratory angular distributions for Ne and Ar + He. Solid points are experimental solid and dashed curves are calculated from potentials of Fig. 10. Figure 9. Laboratory angular distributions for Ne and Ar + He. Solid points are experimental solid and dashed curves are calculated from potentials of Fig. 10.
Figure 6. First-order rate constant for SiH4 decomposition as a function of pressure and temperature. The solid points represent rate measurements by Purnell and Walsh (218). 1 torr = 133.322 Pa. Figure 6. First-order rate constant for SiH4 decomposition as a function of pressure and temperature. The solid points represent rate measurements by Purnell and Walsh (218). 1 torr = 133.322 Pa.
Figure 4. Lippert plot for 10 /xM PRODAN in CF3H. The solid points are the experimental data. The dashed line represents the theoretical prediction for PRODAN. Figure 4. Lippert plot for 10 /xM PRODAN in CF3H. The solid points are the experimental data. The dashed line represents the theoretical prediction for PRODAN.
The redox potentials and the strain energies at the cobalt(III) and cobalt(II) oxidation states of die most stable conformers of a number of hexaaminecobalt(III/II) complexes are listed in Table 10.1. The strain energy difference between the two oxidation states was found to correlate with the experimentally determined reduction potential11331. Fig. 10.2 shows a plot of the redox potentials of the hexaaminecobalt(III/II) complexes from Table 10.1 as a function of die strain energy differences between the oxidized and reduced forms. The experimentally determined redox potentials are given as solid points while the line corresponds to the calculated potentials. Based on Eq. 10.1,... [Pg.110]

NbRh is monoclinic with nine molecules per unit cell, a = 2.806, b = 4.772, c = 20.250 A, and (3 = 90.53°. Close-packed layers are stacked along c. Figure 9.7 shows a projection of A, B, and C positions. The A layer is shown by solid points and solid lines, B positions are joined by dotted lines, and C positions are joined by dashed lines. Each close-packed layer has equal numbers of Nb and Rh atoms, with rows of Nb and Rh atoms giving rectangular patterns for Nb or Rh. This is the pattern for L1/2 shown in Figure 3.11a. The unusual close-packed sequence is ABA BCB CAC, giving nine repeating layers and the notation 9Pi/2i/2(m). Odd sequences such at this... [Pg.201]


See other pages where Solid point is mentioned: [Pg.1612]    [Pg.1275]    [Pg.29]    [Pg.285]    [Pg.393]    [Pg.200]    [Pg.81]    [Pg.57]    [Pg.750]    [Pg.59]    [Pg.69]    [Pg.465]    [Pg.246]    [Pg.610]   
See also in sourсe #XX -- [ Pg.92 , Pg.250 ]

See also in sourсe #XX -- [ Pg.26 , Pg.27 , Pg.30 , Pg.73 , Pg.74 , Pg.139 , Pg.140 , Pg.158 , Pg.159 , Pg.160 , Pg.161 , Pg.162 , Pg.163 , Pg.351 ]




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