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Solid thick-film

Figure 5-21. N(ls) core level spectra of the iiniim model compound PC20X adsorbed on ITO. The upper curve corresponds to a thick film, the central curve to an intermediate thick film, and the lower curve to an ultra thin Him, essentially a mono-layer in thickness. The bold solid lines are the filled curves and the thin solid and dolled lines are the Gaussian peak components lor physisorbed and chemisorbed PC20X, respectively. Figure 5-21. N(ls) core level spectra of the iiniim model compound PC20X adsorbed on ITO. The upper curve corresponds to a thick film, the central curve to an intermediate thick film, and the lower curve to an ultra thin Him, essentially a mono-layer in thickness. The bold solid lines are the filled curves and the thin solid and dolled lines are the Gaussian peak components lor physisorbed and chemisorbed PC20X, respectively.
The relationship of isoviscosity calculated by Eq (5) and a distance apart from the solid surface is shown in Fig. 7. For different kinds of solid materials with different surface energy, the isoviscosity becomes very large as the film thickness becomes thinner. It increases about several to more than ten times that of bulk fluid when it is close to the solid surface. In the thick film region, the isoviscosity remains a constant, which is approximately equal to the dynamic viscosity of bulk liquid. Therefore, the isoviscosity of lubricant smoothly... [Pg.40]

Theoretically, the diffusion coefficient can be described as a function of the disjoining pressure 77, the effective viscosity of lubricant, 77, and the friction between lubricant and solid surfaces. In relatively thick films, an expression derived from hydrodynamics applies to the diffusion coefficients. [Pg.229]

S. Harbeck, A. Szatvanyi, N. Barsan, U. Weimar, and V. Hoffmann. DRIFT studies of thick film un-doped and Pd-doped Sn02 sensors temperature changes effect and CO detection mechanism in the presence of water vapour . Thin Solid Films 436 (2003), 76-83. [Pg.117]

Fig. 8-41. Electron transfer reaction of hydrated redox particles in equilibrium on a metal electrode covered with a thick film (F, solid curve) and with a thin film (F, dashed curve) >cs = electron transfer current via the conduction band >scl = tunneling electron current through a depletion layer in the conduction band >vb = hole transfer current via the valence band. Fig. 8-41. Electron transfer reaction of hydrated redox particles in equilibrium on a metal electrode covered with a thick film (F, solid curve) and with a thin film (F, dashed curve) >cs = electron transfer current via the conduction band >scl = tunneling electron current through a depletion layer in the conduction band >vb = hole transfer current via the valence band.
Figure 20 Comparisons of BSD yields produced by impact of 0- to 40-eV electrons on 6-ML-thick films of the DNA backbone sugarlike analogs tetrahydrofuran (I), 3-hydroxytetrahydrofuran (II), and a-tetrahydrofuryl alcohol (III). The smooth solid lines serve as guides to the eye. (From Ref. 272.)... Figure 20 Comparisons of BSD yields produced by impact of 0- to 40-eV electrons on 6-ML-thick films of the DNA backbone sugarlike analogs tetrahydrofuran (I), 3-hydroxytetrahydrofuran (II), and a-tetrahydrofuryl alcohol (III). The smooth solid lines serve as guides to the eye. (From Ref. 272.)...
Monomolecularly thick films are spontaneously formed upon the immersion of a solid substrate (most commonly gold) into a surfactant solution (most commonly thiols). [Pg.206]

Reactive Pendant Groups on Styrene Backbones. The photolysis of p-acetoxystyrene (III) in acetonitrile solution gives results which are similar to those obtained in a comparable study in the solid-state using 1 /tm thick films in both cases the expected rearrangement is taking place as shown on Scheme 7. [Pg.273]

Figure 4. UV-absorption spectra of Varcum resin (solid line), o-chloro-m-cresol-formaldehyde Novolak resin (long dotted line), and m-cresol-benzaldehyde Novolak resin (short dotted line) 0.32- thick films were... Figure 4. UV-absorption spectra of Varcum resin (solid line), o-chloro-m-cresol-formaldehyde Novolak resin (long dotted line), and m-cresol-benzaldehyde Novolak resin (short dotted line) 0.32- thick films were...
Fig. 15. Temperature dependence of the resistivity for a 200-nm thick film of Gai- Mn As with x = 0.053 in the high-temperature paramagnetic region. Solid squares and open circles show experimental data and the fitting using eq. (2), respectively (Omiya et al. 2000). Fig. 15. Temperature dependence of the resistivity for a 200-nm thick film of Gai- Mn As with x = 0.053 in the high-temperature paramagnetic region. Solid squares and open circles show experimental data and the fitting using eq. (2), respectively (Omiya et al. 2000).
Fig. 18. Temperature dependence of the Hall coefficient h and resistivity p of a 1.3-ftm thick film of In, Mn As with x = 0.013. Rh can be modeled over a wide range of temperatures as Rq + cpx/Po, which is shown by the solid line assuming c = 5.6. The susceptibility x (depicted by the dashed line) is calculated assuming the Curie-Weiss law with x = 0.013, Mn spin S = 5/2, and the Curie-Weiss temperature 6 = 3.8 K... Fig. 18. Temperature dependence of the Hall coefficient h and resistivity p of a 1.3-ftm thick film of In, Mn As with x = 0.013. Rh can be modeled over a wide range of temperatures as Rq + cpx/Po, which is shown by the solid line assuming c = 5.6. The susceptibility x (depicted by the dashed line) is calculated assuming the Curie-Weiss law with x = 0.013, Mn spin S = 5/2, and the Curie-Weiss temperature 6 = 3.8 K...

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