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Basal plane graphite

Fig. 2.1. The molecular orientations in the commensurate V3 V3 N2 monolayer on the graphite basal plane. Fig. 2.1. The molecular orientations in the commensurate V3 V3 N2 monolayer on the graphite basal plane.
The 3.48 A band has an intermediate value between the corresponding to the graphite basal plane -3.34 A- and the turbostratic carbonaceous structures, that according with Foley et al. [5] is 3.82 A. The 2.07 A band corresponds to the 2.03 A calculated by Foley for the inplane carbon-carbon bond, indicating then that the carbonaceous structure of both materials would be associated with an expanded graphitic structure, but in the case of SC-155 the carbonaceous structure is accompanied by an amorphous silica structure. [Pg.703]

Fig. I. Mechanisms suggested tor Iransfurmuiniii of u graphite basal plane sheet of alums into carbyne chains... Fig. I. Mechanisms suggested tor Iransfurmuiniii of u graphite basal plane sheet of alums into carbyne chains...
Elastic neutron diffraction was first performed (analyzer in Fig. 1 set to zero energy transfer) to establish the structure of the monolayer at low temperature. Three Bragg reflections were observed which could be indexed by a triangular lattice having a nearest-neighbor distance about 10% smaller than required for a 3 X /3 R30° commensurate structure (every third carbon hexagon in the graphite basal plane occupied). [Pg.251]

Figure 2. Inelastic neutron spectra from 36Ar monolayers adsorbed on Graf oil at 5 K (9). Curves plotted immediately below data are computed spectra for two different particle-orientation distribution functions (a) in-plane configuration with momentum transfer Q parallel to the preferred orientation of the graphite basal planes (b) out-of-plane configuration with Q perpendicular to the preferred basal planes. Curves at the bottom represent the calculated contribution to the observed spectra caused by in-plane scattering from misoriented crystallites. Figure 2. Inelastic neutron spectra from 36Ar monolayers adsorbed on Graf oil at 5 K (9). Curves plotted immediately below data are computed spectra for two different particle-orientation distribution functions (a) in-plane configuration with momentum transfer Q parallel to the preferred orientation of the graphite basal planes (b) out-of-plane configuration with Q perpendicular to the preferred basal planes. Curves at the bottom represent the calculated contribution to the observed spectra caused by in-plane scattering from misoriented crystallites.
Fig. 7. Cyclic voltammograms of background current for (a) and (b) polycrystalline diamond, (c) platinum, and (d) highly oriented pyrolytic graphite (basal plane) in 0.5 M H2SO4 (a) high-quality film (b) low-quality film [38], Reproduced by permission of The Electrochemical Society, Inc. Fig. 7. Cyclic voltammograms of background current for (a) and (b) polycrystalline diamond, (c) platinum, and (d) highly oriented pyrolytic graphite (basal plane) in 0.5 M H2SO4 (a) high-quality film (b) low-quality film [38], Reproduced by permission of The Electrochemical Society, Inc.

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See also in sourсe #XX -- [ Pg.408 ]

See also in sourсe #XX -- [ Pg.408 ]

See also in sourсe #XX -- [ Pg.408 ]

See also in sourсe #XX -- [ Pg.81 , Pg.180 , Pg.514 ]




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Atomic Hydrogen Adsorption on the Basal Plane of Graphite

Basal plane graphite electrode

Basal plane of the carbon/graphite

Basal plane of the carbon/graphite particles

Basal plane pyrolytic graphite

Basal plane pyrolytic graphite electrode

Basal planes

Basal planes of graphite

Electrode surfaces basal plane graphite

Graphitic planes

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