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Orientation silicon carbide

The fuel for the Peach Bottom reactor consisted of a uranium-thorium dicarbide kernel, overcoated with pyrolytic carbon and silicon carbide which were dispersed in carbon compacts (see Section 5), and encased in graphite sleeves [37]. There were 804 fuel elements oriented vertically in the reactor core. Helium coolant flowed upward through the tricusp-shaped coolant channels between the fuel elements. A small helium purge stream was diverted through the top of each element and flowed downward through the element to purge any fission products leaking from the fuel compacts to the helium purification system. The Peach... [Pg.448]

FIGURE 5.6 This is a fractured sample of a ceramic composite (alumina with 30 volume-percent silicon carbide whiskers). The lighter regions of circular or cylindrical shape are randomly oriented whiskers protruding from the fractured surface. The rod-like depressions in the surface mark places where whiskers nearly parallel with the fracture were pulled out. Courtesy, Roy W. Rice, W. R. Grace and Company. [Pg.82]

The average cross section of identical, but randomly oriented ellipsoids will, in general, exhibit three peaks in the frequency range between co, and o)t. An example of this is given in Fig. 12.7, where Cabs for a silicon carbide ellipsoid is shown as a function of frequency. [Pg.348]

What advantages do ceramics such as Silicon Carbide (eChapter 21.7) have relative to metals What are the disadvantages of ceramics Rotate the 3D model, and see if you can find a special orientation where planes of atoms are separated by largely empty space, devoid of bonds. What does the result of this investigation say about the physical properties of ceramics ... [Pg.947]

HRTEM observations of three differently misoriented interphase boundaries between hexagonal boron nitride (h-BN) and 3C silicon carbide (3C SiC) grains showing an orientation dependence on equilibrium film thickness. In (a) and (b) the (0001) of the highly anisotropic b-BN are parallel to the interface, whereas in (c) they make an angle of 68° with the interphase boundary (reprinted from Ultramicroscopy, Knowles KM and Turan S, The dependence of equilibrium film thickness on grain orientation at interphase boundaries in ceramic-ceramic composites, 83(3/4) 245-259 (2000) with kind permission of Elsevier Science). [Pg.472]

Heteroepitaxy of diamond on c-BN has been successful (e.g., 105,106) due to the identical crystal stractures with a close lattice match (only 1.3% mismatch) between the two and the high surface energy ( 4.8 J/m ) of the c-BN (111) plane. The heteroepitaxy of diamond on silicon could be the key to electronic device apphcations of diamond. However, diamond has a large lattice mismatch with silicon (52%) and a much higher surface energy than silicon (6 J/m for diamond, 1.5 J/m for silicon), hi spite of this, there are several reports of oriented diamond film deposition on substrates like silicon, silicon carbide, etc., by various techniques (e.g., 108-112). [Pg.344]

Tomizawa et al. [217] performed pin-on-disk experiments on friction of SSiC against itself in water at room temperature. The authors found a friction coeflBcient of 0.26 and noted that wear of sintered silicon carbide occurs by a combination of tribochemical dissolution and the formation of pits by fracture of SiC grains. The amount of material removal varied from one SiC grain to the other, due to a strong dependence of tribochemical wear on crystallographic orientation of SiC grains. [Pg.725]

That silicon carbide and silica indeed have structures of this kind has been shown by X-ray crystallography. (Both compounds are pol5miorphic, but in each case, the different forms have the same arrangement of nearest neighbours, and differ only in the relative orientation of more distant neighbours.)... [Pg.36]

The covalent bond has localized electrons, and has little or no net charge transfer from one atom to the other. Silicon and diamond are prototypes of solids having covalent bonds, and the bonds in hydrogen and nitrogen molecules are also purely covalent. These bonds are oriented in space with respect to each other. Four-coordination (four nearest-neighbor atoms) often indicates covalency. Examples of covalent bonds in binary compounds are found in the solid silicon carbide (SiC) and nitrogen chloride molecules (NCI3). [Pg.10]

Structures have been produced that utilize all of the above materials and even some other binders. Found in this group of materials are carbon fibers infiltrated and held together with pyrolytic carbon, silicon carbide, glassy carbon, FIFE, methyl methacrylate, epoxies, and petroleum pitches as well as combinations thereof. The structures may contain randomly oriented chopped fibers or long filaments oriented in random, 2, 3 and n dimensions. [Pg.465]

Carbon-carbon composites can be produced with a multitude of structures. The simplest have two-dimensional order and consist of stacked plies of carbon fabric held together by a carbon matrix. The fabric fibers may be any of those described previously, prepared from the pyrolysis of polyacrylonitrile and the like. The matrix could be derived from petroleum pitch or be infiltrated pyrolytic carbon or even silicon carbide. The latter are generally referred to as SiC/C composites. From two-dimensional, the next progression in structure is three-dimensional on to n-dimensional. This terminology refers to fiber orientation within the matrix. [Pg.471]

Figure 84. Pressureless-sintered silicon carbide doped with boron carbide. Electrolytically etched, BF. Grain face etching. Color etching reveals different grain orientations. Figure 84. Pressureless-sintered silicon carbide doped with boron carbide. Electrolytically etched, BF. Grain face etching. Color etching reveals different grain orientations.
Table 2 shows the dielectric properties of a range of ceramic materials under various conditions and near the two frequencies for which Industrial equipment can be readily purchased. It is evident that the effective losses of various ceramics depend upon the material density and the temperature, frequency and field orientation, giving a range of effective loss factors from above 70 for silicon carbide to 3 x 10 for boron nitride. This latter cereimic can be considered as transparent to microwave energy and may be used as an insulating material in microwave Industrial equipment or as a microwave window in waveguides. In fact, any material with an effective loss factor... [Pg.298]


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