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Synthetic diamond crystals

In this paper, we report the results of our investigations into the changes of chemical and energy properties of diamond grain surfaces with changes in physico-chemical and capillary properties of diamond crystallization media. We have carried out a set of special studies to establish main regularities of the correlations between properties of the crystallization media and adsorption-structural properties of synthetic diamond crystals. [Pg.504]

I. Sunagawa, Morphology of natural and synthetic diamond crystals, in Material Science of the Earth s Interior, I. Sunagawa (Ed.), Tokyo Terra Scientific Publishing Co, 1984, pp. 303-330. [Pg.568]

Figure 12.6. Typical high-pressure synthetic diamond crystals.. (Photograph courtesy of GE Superabrasives, Worthington, OH.)... Figure 12.6. Typical high-pressure synthetic diamond crystals.. (Photograph courtesy of GE Superabrasives, Worthington, OH.)...
Other Industrial Applications. High pressures are used industrially for many other specialized appHcations. Apart from mechanical uses in which hydrauhc pressure is used to supply power or to generate Hquid jets for mining minerals or cutting metal sheets and fabrics, most of these other operations are batch processes. Eor example, metallurgical appHcations include isostatic compaction, hot isostatic compaction (HIP), and the hydrostatic extmsion of metals. Other appHcations such as the hydrothermal synthesis of quartz (see Silica, synthetic quartz crystals), or the synthesis of industrial diamonds involve changing the phase of a substance under pressure. In the case of the synthesis of diamonds, conditions of 6 GPa (870,000 psi) and 1500°C are used (see Carbon, diamond, synthetic). [Pg.76]

Figure 4-150 shows the major components and design of the PDC bit. The polycrystalline diamond compacts, shown in Figure 4-151. The polycrystalline diamond compacts (of which General Electric s) consist of a thin layer of synthetic diamonds on a tungsten carbide disk. These compacts are produced as an integral blank by a high-pressure, high-temperature process. The diamond layer consists of many tiny crystals grown together at random orientations for maximum strength and wear resistance. Figure 4-150 shows the major components and design of the PDC bit. The polycrystalline diamond compacts, shown in Figure 4-151. The polycrystalline diamond compacts (of which General Electric s) consist of a thin layer of synthetic diamonds on a tungsten carbide disk. These compacts are produced as an integral blank by a high-pressure, high-temperature process. The diamond layer consists of many tiny crystals grown together at random orientations for maximum strength and wear resistance.
A single crystal synthetic diamond electrode was used, values of ko range between 4-10 ... [Pg.376]

Synthetic camphor, 24 540 Synthetic compounds, as plant growth regulators, 13 39-56 Synthetic crude oil, 13 640 Synthetic cyclic molecules, 24 35 Synthetic diamond, 3 530-543 catalyzed synthesis, 3 531-535 crystal growth, 3 535 crystal morphology, 3 534-535 crystal structure, 3 537-538 direct graphite-to-diamond process, 3 535-538... [Pg.916]

Diamonds are another allotrope whose crystal structure is similar to graphite. Natural diamonds were formed under higher pressure and extreme temperatures. Synthetic diamonds have been artificially produced since 1955. [Pg.191]

The adamantane structure is unique as it combines three annullated cyclohexane subunits in a nearly spherical overall shape and, as such, it can be regarded as a section of the diamond crystal lattice578. Due to this property, adamantane and other diamondoid molecules are popular as model compounds for synthetic and spectroscopic purposes579 780. [Pg.360]

Figure 2.1. Various forms exhibited by crystals, (a) Polyhedral crystals (b) hopper crystal (c) dendritic crystal (snow crystal, photographed by the late T. Kobayashi) (d) step pattern observed on a hematite crystal (0001) face (e) internal texture of a single crystal (diamond-cut stone, X-ray topograph taken by T.Yasuda) (f) synthetic single crystal boule. Si grown by the Czochralski method (g) synthetic corundum grown by the Verneuil method. Figure 2.1. Various forms exhibited by crystals, (a) Polyhedral crystals (b) hopper crystal (c) dendritic crystal (snow crystal, photographed by the late T. Kobayashi) (d) step pattern observed on a hematite crystal (0001) face (e) internal texture of a single crystal (diamond-cut stone, X-ray topograph taken by T.Yasuda) (f) synthetic single crystal boule. Si grown by the Czochralski method (g) synthetic corundum grown by the Verneuil method.
In the case of synthetic diamond, grown under high-temperature, high-pressure conditions from a high-temperature solution with metal or alloy as the solvent, diamond crystals exhibit a cubo-octahedral Tracht bounded by 100 and... [Pg.183]

The cubic form resembles diamond in its crystal structure and is almost as hard. The theoretical density is 3.48 g/mL. It is colodess and a good electrical insulator when pure traces of impurities add color and make it semiconducting, eg, a few ppm of Be make it blue and />-type whereas small amounts of S, Si, or CN favor yellow, -type crystals. It is possible to makep—n junctions by growing -type material on j -type seed crystals (12). If this is done carefully in an alkaline-earth nitride bath using a temperature difference technique, as with large diamond crystals (see Diamond, SYNTHETIC), the resulting diodes are several mm in size and emit blue light when forward-biased (13,14). [Pg.220]

As early as the 1850s, scientists tried to convert graphite into diamonds. It wasn t until 1954 that researchers produced the first synthetic diamonds by compressing carbon under extremely high pressure and heat. Scientists converted graphite powder into tiny diamond crystals using pressure of more than 68,000 atm, and a temperature of about 1,700°C for about 16 hours. [Pg.56]

Figure 23. Comparison of ESR signals from a single crystal of synthetic diamond in the TEioi cavity and in the loop-gap resonator. Spectra were obtained at room temperature with 2G field modulation. Spectrometer gains are indicated. A, Absorption signal, 1 mW, 9.3 GHz, 1 second time constant. B, Absorption signal, 2 pW, 8.8 GHz, 0.25 second time constant. C, Dispersion signal, other conditions same as in B. D, Dispersion signal, 1 mW, 8.8 GHz, 0.25 second time constant. From [53], with permission. Figure 23. Comparison of ESR signals from a single crystal of synthetic diamond in the TEioi cavity and in the loop-gap resonator. Spectra were obtained at room temperature with 2G field modulation. Spectrometer gains are indicated. A, Absorption signal, 1 mW, 9.3 GHz, 1 second time constant. B, Absorption signal, 2 pW, 8.8 GHz, 0.25 second time constant. C, Dispersion signal, other conditions same as in B. D, Dispersion signal, 1 mW, 8.8 GHz, 0.25 second time constant. From [53], with permission.
The cubic structure is the dominant crystal structure in both natural and synthetic diamond since the staggered conformation is more stable than the eclipsed due to the slightly lower energy (0.1-0.2 eV per carbon atom). Diamond polytypes and carbyne phases form only during the homogeneous nucleation and growth of diamond powder,... [Pg.10]


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See also in sourсe #XX -- [ Pg.293 ]




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