Big Chemical Encyclopedia

Chemical substances, components, reactions, process design ...

Articles Figures Tables About

Hydrogen schematic model

Figure 12. Top Schematic model showing the mechanism of lithium storage in hydrogen containing carbons as proposed in Ref. [2471. Below Schematic charge/discharge curve of a hydrogen containing carbon. Figure 12. Top Schematic model showing the mechanism of lithium storage in hydrogen containing carbons as proposed in Ref. [2471. Below Schematic charge/discharge curve of a hydrogen containing carbon.
Figure 3.3 Schematic model of a hydrogen molecule with two positive nuclei (separated by distance, r) embedded in a uniform charge cloud with spherical radius, R. Figure 3.3 Schematic model of a hydrogen molecule with two positive nuclei (separated by distance, r) embedded in a uniform charge cloud with spherical radius, R.
Asymmetric diarylmethanes, hydrogenolytic behaviors, 29 229-270, 247-252 catalytic hydrogenolysis, 29 243-258 kinetics and scheme, 29 252-258 M0O3-AI2O3 catalyst, 29 259-269 relative reactivity, 29 255-257 schematic model, 29 254 Asymmetric hydrogenations, 42 490-491 Asymmetric synthesis, 25 82, 83 examples of, 25 82 Asymmetry factor, 42 123-124 Atom-by-species matrix, 32 302-303, 318-319 Atomic absorption, 27 317 Atomic catalytic activities of sites, 34 183 Atomic displacements, induced by adsorption, 21 212, 213 Atomic rate or reaction definition, 36 72-73 structure sensitivity and, 36 86-87 Atomic species, see also specific elements adsorbed... [Pg.51]

Fig. 14. Schematic model of adsorption of hydrogen on a stepped platinum surface [Pt(997) or Pt(S) — 9(111) X (111)]. Shading denotes various partial charge of hydrogen atoms ( S6). Fig. 14. Schematic model of adsorption of hydrogen on a stepped platinum surface [Pt(997) or Pt(S) — 9(111) X (111)]. Shading denotes various partial charge of hydrogen atoms ( S6).
Figure 18. Schematic model of the structure of Pt particles on an voltammogram in relation to the electrode potential. The hydrogen, double layer, and oxide regions are based on cyclic voltammetry. The lattice disorder decreases in the order D>A>C>B." (Reproduced with permission from ref 40. Copyright 1993 ElsevierSequoia S.A., Lausanne.)... Figure 18. Schematic model of the structure of Pt particles on an voltammogram in relation to the electrode potential. The hydrogen, double layer, and oxide regions are based on cyclic voltammetry. The lattice disorder decreases in the order D>A>C>B." (Reproduced with permission from ref 40. Copyright 1993 ElsevierSequoia S.A., Lausanne.)...
Fig. 2. Schematic model of silk fibroin (-) fibroin molecule (-) hydrogen bond. Fig. 2. Schematic model of silk fibroin (-) fibroin molecule (-) hydrogen bond.
Fig. 25. Schematized model of enanlio-differentiating hydrogenation on MRNi. Fig. 25. Schematized model of enanlio-differentiating hydrogenation on MRNi.
Fig. 27. Schematized model of activation of hydrogen on the metal catalyst. Fig. 27. Schematized model of activation of hydrogen on the metal catalyst.
Figure 19.2 Schematic model of the biomimetic material Ml for the sensing of long-chain carboxy-lates. Hydrophobic forces bind the tail to the wall, enabling hydrogen bonding interactions of the analyte s head group with the urea group of the phenoxazinone dye. The result is a color and fluorescence modulation. Lower left inactive nonhydrophobized material M2. Lower right inactive molecular probe PI. Figure 19.2 Schematic model of the biomimetic material Ml for the sensing of long-chain carboxy-lates. Hydrophobic forces bind the tail to the wall, enabling hydrogen bonding interactions of the analyte s head group with the urea group of the phenoxazinone dye. The result is a color and fluorescence modulation. Lower left inactive nonhydrophobized material M2. Lower right inactive molecular probe PI.
Figure 6.49 Schematic presentation of (a) the slip dissolution and (b) the hydrogen embrittlement models 02... Figure 6.49 Schematic presentation of (a) the slip dissolution and (b) the hydrogen embrittlement models 02...
Fig. 6.22. Schematic model showing the distribution of hydrogen binding energies. The more distorted Si—Si weak bonds trap hydrogen in deeper states. The dispersive hydrogen diffusion corresponds to the trapping and release from the weak bonds and Si—H bond sites (Street el at. 1988a). Fig. 6.22. Schematic model showing the distribution of hydrogen binding energies. The more distorted Si—Si weak bonds trap hydrogen in deeper states. The dispersive hydrogen diffusion corresponds to the trapping and release from the weak bonds and Si—H bond sites (Street el at. 1988a).
Palladium is one of the most frequently used metals in heterogeneous catalysis, used for hydrogenation as well as oxidation reactions. As discussed below, a variety of palladium model catalyst surfaces were used to characterize CO adsorption and the coadsorption and reaction of CO with hydrogen, both under UHV and at atmospheric pressure. Figure 14 shows schematic models of smooth and stepped... [Pg.162]

Fig. 28. Thermal desorption spectra of hydrogen acquired after exposure of Pd/Al203 and Pdf 1 1 1) to H2 Cooling in 2 X 10 mbar of H2 from 300 to 100 K (approximately 80 L upper traces) and cooling in 2 X 10 mbar of H2 from 300 to 150 K (approximately 150 L lower traces). Schematic models and STM images of the palladium model catalysts are shown on the right. For simplicity, the ball model shows a smaller particle but with the correct proportions adapted from (68) with permission from Elsevier. Fig. 28. Thermal desorption spectra of hydrogen acquired after exposure of Pd/Al203 and Pdf 1 1 1) to H2 Cooling in 2 X 10 mbar of H2 from 300 to 100 K (approximately 80 L upper traces) and cooling in 2 X 10 mbar of H2 from 300 to 150 K (approximately 150 L lower traces). Schematic models and STM images of the palladium model catalysts are shown on the right. For simplicity, the ball model shows a smaller particle but with the correct proportions adapted from (68) with permission from Elsevier.
In Section 2.3 we studied the tent map, a schematic model for ionization that was able to produce fractal structures as a result of ionization. An important question is therefore whether the results presented in Section 2.3 are only of academic interest, or whether fractal structures can appear as a result of ionization in physical systems. In order to answer this question we return to the microwave-driven one-dimensional hydrogen atom. As we know from the previous chapter, this model is ionizing and realistic enough to qualitatively reproduce measured ionization data. Therefore this model is expected to be a fair representative for a large class of chaotic ionization processes. [Pg.204]

Fig. 6.2. Schematic model of nearly sinusoidal two-well potential with asymmetry A for hydrogen in metals, showing ground and first excited eigenstates. Heavy tines for the states show where the particle is likely to be. Fig. 6.2. Schematic model of nearly sinusoidal two-well potential with asymmetry A for hydrogen in metals, showing ground and first excited eigenstates. Heavy tines for the states show where the particle is likely to be.
Fig. 38 Schematic model of hydrogen bonding between C=0 groups in PDLLA and the surface P-OH groups in HA nanoparticles. Reprinted with permission from [170], Copyright 2007, American Chemical Society... Fig. 38 Schematic model of hydrogen bonding between C=0 groups in PDLLA and the surface P-OH groups in HA nanoparticles. Reprinted with permission from [170], Copyright 2007, American Chemical Society...
FIgura 2 Schematic model of hydrogen bonding of CN groups (4). [Pg.327]

In view of this discussion, it is clear that even the detailed model of eqs (1.1)-(1,3) should not be taken as a faithful description of polyethylene (PE), but rather as a prototypical schematic model of linear polymers. In the context of simulations of lipid monolayers,it has been suggested that it is necessary to shift the center of gravity of the united atom off the position of the carbon atom at the chain backbone (anisotropic united atom model). Very recent work " (see also Chapter 8) suggests that it is more satisfactory to include the hydrogen atoms explicitly, if one wishes to describe PE properly. For the reasons quoted above, such work is restricted to relatively... [Pg.6]

Figure C3.2.18.(a) Model a-helix, (b) hydrogen bonding contacts in tire helix, and (c) schematic representation of tire effective Hamiltonian interactions between atoms in tire protein backbone. From [23]. Figure C3.2.18.(a) Model a-helix, (b) hydrogen bonding contacts in tire helix, and (c) schematic representation of tire effective Hamiltonian interactions between atoms in tire protein backbone. From [23].
Because XPS is a surface sensitive technique, it recognizes how well particles are dispersed over a support. Figure 4.9 schematically shows two catalysts with the same quantity of supported particles but with different dispersions. When the particles are small, almost all atoms are at the surface, and the support is largely covered. In this case, XPS measures a high intensity Ip from the particles, but a relatively low intensity Is for the support. Consequently, the ratio Ip/Is is high. For poorly dispersed particles, Ip/Is is low. Thus, the XPS intensity ratio Ip/Is reflects the dispersion of a catalyst on the support. Several models have been reported that derive particle dispersions from XPS intensity ratios, frequently with success. Hence, XPS offers an alternative determination of dispersion for catalysts that are not accessible to investigation by the usual techniques used for particle size determination, such as electron microscopy and hydrogen chemisorption. [Pg.138]

Figure 5.9 Schematic cyclic voltammogram showing the electro-oxidation of the electrode (dashed box). The curve was generated from measurements by Jerkiewicz et al. [2004] of Pt in 0.5 M H2SO4 with a reversible hydrogen reference electrode (RHE). For each separable potential range, an atomistic model of the electrode structure is shown above. Figure 5.9 Schematic cyclic voltammogram showing the electro-oxidation of the electrode (dashed box). The curve was generated from measurements by Jerkiewicz et al. [2004] of Pt in 0.5 M H2SO4 with a reversible hydrogen reference electrode (RHE). For each separable potential range, an atomistic model of the electrode structure is shown above.
Fig. 8. Schematic total energy level diagram of the D(H,0) donors in Ge based on the tunneling hydrogen model (Reprinted with permission from the American Physical Society, Jobs, B., Haller, E.E., and Falicov, L.M. (1980). Phys. Rev. B 22, 832.)... Fig. 8. Schematic total energy level diagram of the D(H,0) donors in Ge based on the tunneling hydrogen model (Reprinted with permission from the American Physical Society, Jobs, B., Haller, E.E., and Falicov, L.M. (1980). Phys. Rev. B 22, 832.)...

See other pages where Hydrogen schematic model is mentioned: [Pg.49]    [Pg.89]    [Pg.107]    [Pg.383]    [Pg.287]    [Pg.1310]    [Pg.488]    [Pg.182]    [Pg.216]    [Pg.481]    [Pg.335]    [Pg.46]    [Pg.279]    [Pg.536]    [Pg.192]    [Pg.83]    [Pg.6]    [Pg.356]    [Pg.15]    [Pg.27]    [Pg.59]    [Pg.98]    [Pg.211]    [Pg.381]    [Pg.450]    [Pg.512]    [Pg.513]   
See also in sourсe #XX -- [ Pg.326 ]




SEARCH



Hydrogen model

Hydrogenic model

Schematic models

© 2024 chempedia.info