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Diamond, structure and properties

Chapter 1 contains a review of carbon materials, and emphasizes the stmeture and chemical bonding in the various forms of carbon, including the foui" allotropes diamond, graphite, carbynes, and the fullerenes. In addition, amorphous carbon and diamond fihns, carbon nanoparticles, and engineered carbons are discussed. The most recently discovered allotrope of carbon, i.e., the fullerenes, along with carbon nanotubes, are more fully discussed in Chapter 2, where their structure-property relations are reviewed in the context of advanced technologies for carbon based materials. The synthesis, structure, and properties of the fullerenes and... [Pg.555]

C14-0135. S ° of graphite is 3 times larger than S ° of diamond. Explain why this is so. (You may need to review the structures and properties of graphite and diamond in Section 11-.) Buckminsterfullerene is a solid that consists of individual molecules with formula Cgo. Is the molar entropy of buckminsterfullerene larger or smaller than that of graphite How about the entropy per gram Explain. [Pg.1044]

Since the main parameter influencing diamond-like carbon film structure is the energy of bombarding ions, it is expected that the same happens with a-C H films. In fact, it was found that in RFPECVD deposition of a-C H films, the variation of substrate self-bias results in strong changes of film growth, composition, structure, and properties. [Pg.225]

Silicon dioxide (silica, Si02) has a similar 3D structure and properties. The hardness of diamond enables it to be used as the leading edge on cutting tools. [Pg.122]

D13 Diamond, S., in Hydraulic Cement Pastes Their Structure and Properties. [Pg.417]

Wang and Ho have performed extensive TBMD simulations to study the structure and properties of amorphous carbon (a-C) over a wide range of densities [60-63], The simulations showed that a-C samples produced under different densities (i.e., under different compressive stresses) have very different structures. The general trend is that the sp bonding concentration increases when the a-C sample is generated under higher densities. Near the graphitic density (2.27 g/cm ), a-C is dominated by threefold atoms. Diamond-like yp -dominated a-C structures can be... [Pg.674]

The formation of nanoporous molecular networks can be illustrated by an example in which tetrahedral tetracations are Unked by coulombic forces to linear dianions. This may lead to a diamond-like network not unlike the aforementioned 1,3,5,7-tetracarboxyadamantane structure. It is our goal here to describe the directing influence of electrostatic templates on anionic networks in crystalline materials, with a focus primarily on the structural aspects of these materials. Complete detailed descriptions of their synthesis, structure and properties are available elsewhere [24-28]. [Pg.112]

Kollman (1944-2001), later famous for studies of proteins, calculated the structure and properties of polymeric water. They relied on claims that the experimentalists were working with a pure substance. Allen and Kollman were limited to computations of only moderate sophistication. Their study, published in 1970, predicted a structure similar to graphite (regular "ice" is similar to diamond). Their calculated energies for polywater and liquid water were quite similar. This begged a question that many chemists had raised earlier If "anomalous water" or polywater forms so readily (and is comparable in energy to liquid water), why had it not been seen before and, for that matter. [Pg.287]

Diamond, S. In Hydraulic Cement Pastes their structure and properties. University of Sheffield, April 1976, p. 2, Cement and Concrete Ass. Wexham Springs (1976)... [Pg.200]

Semiconductors can be divided into two classes, elemental semiconductors, which contain only one type of atom, and compound semiconductors, which contain two or more elements. The elemental semiconductors all come from group 4A. As we move down the periodic table, bond distances increase, which decreases orbital overlap. This decrease in overlap reduces the energy difference between the top of the valence band and the bottom of the conduction band. As a result, the band gap decreases on going from diamond (5.5 eV, an insulator) to silicon (1.11 eV) to germanium (0.67 eV) to gray tin (0.08 eV). In the heaviest group 4A element, lead, the band gap collapses altogether. As a result, lead has the structure and properties of a metal. [Pg.504]

After 1988, when the first syntheses of the detonation diamond were reported in the USA and the USSR [253, 254], the structure and properties of this material... [Pg.439]

Baranauskas V, Bin Li B, Peterlevitz AC, Tosin MC, Durrant SF (1999) Structure and properties of diamond films deposited on porous silicon. Thin Solid Films 355-356 233-238... [Pg.137]

Copper, zinc, and gallium are metals, with properties compatible with these values of the valence. Germanium under ordinary pressure is a metalloid, with the diamond structure and valence 4. At high pressure it is converted into another form, with greatly increased electric conductivity and density corresponding to the white tin structure and valence 2.56. [Pg.571]

Recent investigations have revealed the existence of a series of diamond polytypes such as the 6-H hexagonal diamond. The structure and properties of these polytypes are reviewed in Ch. 11Also under investigation is a hypothetical phase of carbon based on a three-dimensional network but with sp bonds. This phase could be harder than diamond, at least in theory.1 A carbon phase diagram incorporating these new polytypes has yet to be devised. [Pg.41]


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See also in sourсe #XX -- [ Pg.663 ]




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