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Silicon temperature effects

In all silicate minerals formed under crustal conditions silicon is coordinated to four oxygen atoms. In high-pressure transformations, silicon commonly increases its coordination number. The longer- the Si—O distances in tetrahedral silicates the higher the pressure transformations to phases with octahedral silicon. The average Si—O bond distance for the pressure transformation is 159 pm. This distance is achieved at room temperature at pressures in all measured silicates and may be a minimum for tetrahedryl Si—O bonds 300 kbar is an upper pressure limit for the silicon tetrahedron and SOkbar is a lower pressure limit for octahedral silicon. Temperature has little effect on Si—O bond distances in either tetrahedra or octahedra... [Pg.110]

The silicon /3-effect has been exploited to convert aziridines to 2-imidazolines and oxazolidines <2005JA16366>. This reaction presumably goes through siliranium ion 344, which can then react with an electrophile to form 345 or 346. It has also been shown that zinc dihalides are effective in catalyzing the formation of 345, but require elevated temperatures (Scheme 89) <2005TL4103>. [Pg.37]

The solubility parameter model has difficulty with temperature effects and also fails to predict solubilities in several instances, such as with silicones. However it is a good starting point for estimating the solubility characteristics of a SCF as a function of temperature and pressure. The most likely temperatures and pressures under which a material is soluble in a supercritical fluid are where the solubility parameters are within a value of unity of each other. See Fig. 1, taken from Fig. 2 of Ref 5 by Allada, for a graph of 6 versus T and P for CO2. This effect allows one to selectively remove a particular component from a material by tuning the 5 of the SCF using T and P. [Pg.270]

SOI and strained silicon transistors are comparable to or smaller than the phonon s mean free path (which, for silicon, has been estimated as 300 nm at 300K) [53], In this limit, the film surfaces alter the phonon dispersion relations [76], and the phonon-surface scattering may become the predominant scattering mechanism [3, 53], Since phonons are the main carriers of thermal energy in silicon, these effects alter the thermal conductivity, which differs from that of bulk silicon [10, 36, 77], Measurements of the thermal conductivities of silicon films of thicknesses down to 74 nm found a reduction of 50% with respect to the bulk value at 300K [53], This reduction depends on the temperature and the thickness of the film [3, 53],... [Pg.390]

For coverages beyond 15 monolayers, there is still no pure Au present, but only a Au film containing dissolved Si between two regions of silicide. There is, additionally, a surface enrichment of silicon. The effect of heating is to diffuse more Au further into the Si substrate, leaving a surface more silicon-rich. Figure 33 is a schematic representation of the composition of a room temperature deposit. [Pg.257]

Rixecker G, Wiedmann I, Rosinus A, et al. High-temperature effects in the fracture mechanical behaviour of silicon carbide liquid-phase sintered with AIN-Y2O3 additives. J.Euro. Ceram Soc., 2001,21 1 013-1 019. [Pg.343]

An interesting example of surface tension flow induced by temperature effects alone has been noted in thin films of silicone liquids on horizontal glass or metal plates heated to 400°C. Because of the great difference between the temperature of the plate and the air above it, there is a sharp vertical temperature gradient in the liquid film. The surface of any thin spot in the film will be hotter and have a lower surface tension than thicker portions near it. Consequently the film is unstable and the liquid draws up into small droplets, distributed over a much thinner film against which they nevertheless show zero contact angles. The droplets spread as soon as the temperature is lowered. [Pg.378]

Usable in Hot Climates. Most organic sealants perform satisfactorily when temperatures are warm. But silicones remain effective in such hot locations as the sandwich panel of a solar collector or around heat ducts or hot pipes. However, the designer must choose the right silicone, since some perform up to 150 C, some to 200 C and 250 C. These temperatures can be contrasted to the 70 C to 120 C operating maximum of nonsilicones. [Pg.126]

Rixecker, I. Wiedmann, A. Rosinus, and F. Aldinger, High-Temperature Effects in the Fracture Mechanical Behaviour of Silicon Carbide Liquid-Phase Sintered with AIN-YrOj Addittives, JEur.Ceram.Soc., 21,1013-19(2001). [Pg.63]

Stebbins JF, McMillan P (1993) Compositional and temperature effects on five-coordinated silicon in ambient pressure sihcate glasses. J Non Cryst Sol 160 116-125 Stebbins JF, Xu Z (1997) NMR evidence for excess non-bridging oxygen in an aluminosilicate glass. Nature 390 60-62... [Pg.167]

Setzu S, Lerondel G, Romestain R (1998) Temperature effect on the roughness of the formation interface of P-type porous silicon. J Appl Phys 84(6) 3129-3133... [Pg.570]

Zangooie S, Jansson R, Arwin H (1999) Ellipsometric characterization of anisotropic porous silicon Fabry-Perot filters and investigation of temperature effects on capillary condensation efficiency. J Appl Phys 86(2) 850-858... [Pg.657]

As epoxy and silicone rubber are completely immiscible, the addition of a compatibilizer is necessary to obtain a satisfactory dispersion of the rubber in the resin. The main objective of Kasemura and coworkers [216] was to find an appropriate surface-active agent to reduce the interfacial tension between the resin and the rubber, in order to compatibilize the two components. These authors achieved adequate compatibility in the epoxy resin with the use of a polyester-modified silicone oil to disperse an RTV (room temperature vulcanizing) silicone rubber or silicone diamine. The results showed that the impact fracture energy of the resin was increased by the addition of the RTV silicone rubber, up to two times that of the unmodified resin, whereas the addition of silicone diamine had almost no effect, possibly because the molecular weight was too low. Moreover, T-peel strengths of aluminum plates bonded by epoxy resin filled with RTV silicone rubber and with silicone diamine effectively increased with the silicone content, showing a maximum at 10-20 pph. By scanning electron microscopy, many particles of silicone rubber, 1-20 xm, were observed across the whole of the fracture surface. [Pg.440]

Illustration 3.9 Diffusion of a Dopant into a Silicon Chip Temperature Effect on Transport Rates... [Pg.136]


See other pages where Silicon temperature effects is mentioned: [Pg.177]    [Pg.682]    [Pg.208]    [Pg.66]    [Pg.1334]    [Pg.1517]    [Pg.61]    [Pg.376]    [Pg.392]    [Pg.122]    [Pg.533]    [Pg.275]    [Pg.442]    [Pg.173]    [Pg.3173]    [Pg.380]    [Pg.3]    [Pg.214]    [Pg.29]    [Pg.183]    [Pg.6335]    [Pg.6349]    [Pg.213]    [Pg.202]    [Pg.184]    [Pg.265]   
See also in sourсe #XX -- [ Pg.198 ]




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