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Graphitized carbon molecular properties

The affect of architecture on small molecular properties has been recognized since the historical Berzelius (1832) discovery that defined the following premise substances of identical compositions but different architectures - skeletal isomers - will differ in one or more properties [15]. These effects are very apparent when comparing the fuel combustion benefits of certain isomeric octanes or the dramatic property differences observed in the three architectural isomers of carbon namely graphite, diamond and buckminsterfullerene. [Pg.32]

These materials mainly include graphites, carbon blacks and graphitized carbon blacks, and are frequently used as standards in adsorption at high and low surface coverage due to the lack of porosity and their homogeneous surfaces [61-64]. For these reasons it is easy to find a relationship, for the adsorption of non-polar molecules (n-alkanes), between the specific retention volumes and a molecular property of the adsorbate such as the polarizability or the molecular volume, and the amount adsorbed, V, which is nor-... [Pg.530]

Thus the thermodynamic characteristics of adsorption at small coverage of different classes organic compounds determined by gas chromatography show that surface of ful-lerene molecular crystals and surface of graphitized carbon black have essentially different adsorption properties. On adsorption on fullerene crystals the electron-acceptor and electron-donor properties of fullerene molecules are manifested. Adsorption data on fullerenes Ceo nd C70 show that properties of fullerene Ceo a-nd C70 molecules arranged in surface layer of crystals are different. [Pg.913]

Table 5.3 Molecular properties and capacity ratios measured on different graphitized carbon columns. FS, HB, ES, and VW represent the energy value of the final (optimized) structure, the hydrogen-bonding energy, the electrostatic energy, and the van der Waals energy of the complexes (kcal mol ), respectively, fs, hb, es, and vw represent the same energies for each analyte. Reproduced by permission of Springer, ref. 25. Table 5.3 Molecular properties and capacity ratios measured on different graphitized carbon columns. FS, HB, ES, and VW represent the energy value of the final (optimized) structure, the hydrogen-bonding energy, the electrostatic energy, and the van der Waals energy of the complexes (kcal mol ), respectively, fs, hb, es, and vw represent the same energies for each analyte. Reproduced by permission of Springer, ref. 25.
Carbon nanotubes (CNT) are molecular-scale tubes of graphitic carbon with hard properties as shown in Fig. lb. They are among the stiffest and strongest fibers known and have remarkable electronic properties and many other unique characteristics. Some applications are available, especially in nanotechnology due to its size and... [Pg.1738]

The electronic and transport properties of an amorphous graphitic carbon model constructed by Townsend et al, [112,114] were studied by first-principles calculations in the local-density approximation. Semiempirical density-functional molecular dynamics (DF-MD) was used to simulate the experiments, e.g., neutron diffraction, inelastic neutron scattering, and NMR, to determine the structure of the system in order to achieve a fundamental understanding of structure-related properties on the molecular level of chemical bonding. The total energy of the system... [Pg.248]

The past two decades have shown an explosion in the development of new nanoporous materials mesoporous molecular sieves, zeolites, pillared clays, sol-gel-derived metal oxides, and new carbon materials (carbon molecular sieves, super-activated carbon, activated carbon fibers, carbon nanotubes, and graphite nanofibers). The adsorption properties for most of these new materials remain largely unexplored. [Pg.424]

In summary, using tight-binding molecular dynamics simulations, we have demonstrated qu ilitative differences in the physical properties of carbon nanotubes and graphitic carbon. Furthermore, we have presented an efficient Green s function formalism for calculating the quantum conductance of SWCNs. Our work reveals that use of full orbital basis set is necessary for realistic ceilculations of quantum conductance of carbon nanotubes. Rirthermore, our approach allows us to use the same Hamiltonian to ceilculate quantum conductivity as well as to perform structural relaxation. [Pg.261]

The properties of mesophase pitch-based carbon fibers can vary significantly with fiber texture. Inspection of the cross-section of a circular mesophase fiber usually shows that the graphitic structure converges toward the center of the fiber. This radial texture develops when flow is fully developed during extrusion through the spinnerette. Endo [48] has shown that this texture of mesophase pitch-based carbon fibers is a direct reflection of their underlying molecular structure. [Pg.132]

The synthesis of molecular carbon structures in the form of C q and other fullerenes stimulated an intense interest in mesoscopic carbon structures. In this respect, the discovery of carbon nanotubes (CNTs) [1] in the deposit of an arc discharge was a major break through. In the early days, many theoretical efforts have focused on the electronic properties of these novel quasi-one-dimensional structures [2-5]. Like graphite, these mesoscopic systems are essentially sp2 bonded. However, the curvature and the cylindrical symmetry cause important modifications compared with planar graphite. [Pg.89]

In general, nanotechnology MBBs are distinguished for their unique properties. They include, for example, graphite, fullerene molecules made of various numbers of carbon atoms (C60, C70, C76, C240, etc.), carbon nanotubes, nanowires, nanocrystals, amino acids, and diamondoids [97]. All these molecular building blocks are candidates for various applications in nanotechnology. [Pg.232]


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See also in sourсe #XX -- [ Pg.66 , Pg.67 ]




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Graphite, graphitic carbons

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