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Types of Space

BeryUium is used in sateUite stmctures in the form of both sheet and extmded tubing and is a very important material for aU types of space optics. BeryUium oxide ceramic apphcations take advantage of high room temperature thermal conductivity, very low electrical conductivity, and high transparency to microwaves in microelectronic substrate apphcations. [Pg.69]

Table 6.17 shows recommended operative temperatures and maximum mean air velocities for different types of spaces. The table is based on ISO EN 7730 and CR 1 7.52. [Pg.395]

A realistic model of a solution requires at least several hundred solvent molecules. To prevent the outer solvent molecules from boiling off into space, and minimizing surface effects, periodic boundary conditions are normally employed. The solvent molecules are placed in a suitable box, often (but not necessarily) having a cubic geometry (it has been shown that simulation results using any of the five types of space filling polyhedra are equivalent ). This box is then duplicated in all directions, i.e. the central box is suiTounded by 26 identical cubes, which again is surrounded by 98 boxes etc. If a... [Pg.386]

Fig ures 5-43 and 5—44 illustrate the band bending and the concentration profile of charge carriers in these four types of space charge layers. [Pg.174]

Another important feature of close-packed structures is the shape and number of the small amounts of space trapped in between the spheres. Two different types of space are contained within a close-packed structure the first we will consider is called an octahedral hole. Figure 1.5(a) shows two close-packed layers again but now with the octahedral holes shaded. Six spheres surround each of these holes three in layer A and three in layer B. The centres of these spheres lay at the corners... [Pg.2]

Similarly, Figure 1.6(a) shows two close-packed layers, now with the second type of space, tetrahedral holes, shaded. Four spheres surround each of these holes with centres at the corners of a tetrahedron (Figure 1.6(b)). If n spheres are in the array, then there are 2n tetrahedral holes. [Pg.5]

Previously (Section 9.3), we have alluded briefly to various distinguishable types of mathematical spaces with differing degrees of algebraic and geometrical structure. We now wish to clarify these distinctions more carefully, in order to introduce a new type of space that differs profoundly from more familiar Euclidean-like varieties. [Pg.424]

Periodic repclitions of a space lattice cell in three dimensions from the original cell vvill completely partition space without overlapping or omissions. El is possible to develop a limited number of such three-dimensional patterns. Bravais. in 1848. demonsirated geometrically that there were but fourteen types of space lattice cells possible, and that these fourteen types could be subdivided into six groups called systems. Each system may be distinguished hy symmetry features, which can be related lo four symmetry elements ... [Pg.1006]

A relatively recent type of space-time symmetry has been introduced to explain the results of certain high-cncrgy scattering experiments. This is scale symmetry and it pertains to the rescaling or dilation of the space-time coordinates of a system without changing the physics of the system. Other symmetries, such as chirality, are more of an abstract nature, but aid the theorist in an effort to bring order into the vast array of possible elementary particle reactions. [Pg.1211]

Fig. 3.18 Types of space-charge region in an n-type semiconductor, dependent on the potential applied relative to the flat band potential, Un,. U represents potential (V) and Ec sur the electronic energy corresponding to Ec close to the surface, (a) c,sur = E no space-charge region (b) c,sur> E (U < U ) formation of an accumulation layer (c) c,sur formation of a depletion layer (d) c,sur efb (U U ) formation of an inversion layer. Fig. 3.18 Types of space-charge region in an n-type semiconductor, dependent on the potential applied relative to the flat band potential, Un,. U represents potential (V) and Ec sur the electronic energy corresponding to Ec close to the surface, (a) c,sur = E no space-charge region (b) c,sur> E (U < U ) formation of an accumulation layer (c) c,sur<Ffb (U > formation of a depletion layer (d) c,sur efb (U U ) formation of an inversion layer.
Unit cells are further subclassified as simple cubic/ face-centered cubic, body-centered cubic, base-centered rhombic, etc. but in order to avoid duplication in classification (Exercise 3), certain of the possibilities are left out (for example, face-centered tetragonal, side-centered rhombic), Actually 14 distinct types of space lattice are recognized. A number of cubic unit ceils and one body-centered tetragonal cell... [Pg.310]

A fifth type of space charge layer, the deep depletion layer, may be formed under non-equilibrium conditions at the semiconductor surface when a high voltage is applied such that an inversion layer should form, but either (a) minority carriers are not available to accumulate at the surface in the time allotted or (b) the minority carriers are consumed in an electrochemical reaction as soon as they reach the surface. Such a space charge layer is unlikely to form within semiconductor electrodes at open circuit and is included here solely for completeness. [Pg.300]

Three additional concepts may be introduced by means of Fig. 2A. First, all measurements of the diffracted beams are made relative to the incident x-ray beam so that the diffracted beam leaves the crystal at an angle 20, as illustrated. Thus, while the diffraction condition is determined by the angle between the incident and diffracted beams relative to a lattice plane, the measured position of the diffracted beam is determined relative to the incident beam. Second, there is a reciprocal relation between the spacing between lattice planes and the positions of the diffraction spots small lattice spacings give diffraction spots with large values of 20. This leads to two types of space. The crystal coordinate system is in real space, whereas the diffrac-... [Pg.47]

If the contents of a unit cell have symmetry, containing a number of units of pattern (atoms, molecules), the number of distinct types of space lattice becomes fourteen (Fig. 82) (Bravais, 1818). And when other symmetry operations are recognised (e.g. rotation of the lattice) there are found to be 230 distinct varieties of crystal symmetr ... [Pg.140]

Three types of space charge layers, namely, depletion layer, accumulation layer, and inversion layer, may occur in a semiconductor depending on the bias and equilibrium conditions as shown in Fig. 1.7. [Pg.10]

FIGURE 1,7. Types of space charge layers on an n-type semiconductor surface, (a) Depletion layer (b) accumulation layer (c) inversion layer. After Morrison. ... [Pg.10]

When the concentration of the sodium hydroxide in which the cellulose is immersed reaches 13 per cent, a new type of space lattice begins to make its appearance which increases in predominance until the change is complete at a concentration of 19 per cent. This phenomenon is accompanied by the formation of alkali cellulose , CjHioOj.NaOH. When the alkali is removed by immersion in acid the spatial arrangement of the glucose molecules does not return to the original state but remains within unit cells in which the dimensions a and b are 8T and 91 A (0-81 and 0-91nm) instead of 8-2 A and 7-8 A (0-82 and 0-78nm) for native cellulose as shown... [Pg.59]

The main types of equipment considered here are the hydraulic sprayers, such as compression (Figure 5.1) and lever-operated knapsack sprayers (Figures 5.2, 5.3) normally used for residual applications to surfaces. Hydraulic sprays may also be applied with motorised pumps on knapsack sprayers, or larger units are carried on a trolley (Figure 5.4) or small vehicle. Pesticides formulated for dilution in water are frequently applied at volumes of around 100-500 litres per hectare. Other types of space treatments and more specialised equipment are considered later. [Pg.75]

This implies a somewhat modified type of space quantisation, since by (19) ... [Pg.240]

The relationship of this type of space charge to that arising in the purely electronic boundary-layer theory of chemisorption is discussed elsewhere (8). [Pg.450]

Bravais proved that if the contents of a unit cell have symmetry, the number of distinct types of space lattices becomes fourteen. These are the only lattices that can fill all space and are commonly termed the 14 Bravais lattices. Since there are seven crystal systems, it might be thought that by combining the seven crystal systems with the idea of a primitive lattice a total of seven distinct Bravais lattices would be obtained. However, it turns out that the trigonal and hexagonal lattices so constructed are equivalent, and therefore only six lattices can be formed in this way. These lattices, which are given the label P, define the primitive unit cells (or P-cells) in each case. [Pg.78]

The holding plate 70, as best shown in Fig. 15, is provided with two types of spaced perforations 72 and 73, the former constituting circular boles and the latter being in the form of spaced, substantially semi-circular openings separated by an intermediate bridging member 74 integral with the plate 70. [Pg.712]

In this work, we conduct a Monte-Carlo simulation on the Markov chains representing the two types of space system architectures considered (Monolith and Space-Based Network). These Markov chains are discussed in section 3.1. The probabilistic nature of... [Pg.660]

In addition to the depletion layer, other types of space charges can also form in a semiconductor. These are illustrated in Fig. 2.14. If the number of adsorbed negative (positive) surface charges increases beyond a certain number for an n-type (p-type) semiconductor, the Fermi level crosses the middle of the bandgap and the surface region becomes p-type (n-type). This is called an inversion layer. Formation of an inversion layer is not always possible if the dominant charge carriers in the inversion layer are annihilated faster than they are (thermally)... [Pg.34]

Fig. 2.14 Different types of space charges in n- and p-type semiconductors. A normal depletion layer contains only ionized donors or acceptors. An inversion layer is formed when the Fermi level crosses the midgap energy, and the minority carriers outnumber the majority carriers in a thin layer at the surface. When these minority carriers are consumed faster than they are generated, a deep depletion layer forms under these conditions the surface is not in thermal equilibrium and the Fermi level is not well defined in this region. In an accumulation layer, the adsorbed surface charges are compensated by majority charge carriers that accumulate at the surface... Fig. 2.14 Different types of space charges in n- and p-type semiconductors. A normal depletion layer contains only ionized donors or acceptors. An inversion layer is formed when the Fermi level crosses the midgap energy, and the minority carriers outnumber the majority carriers in a thin layer at the surface. When these minority carriers are consumed faster than they are generated, a deep depletion layer forms under these conditions the surface is not in thermal equilibrium and the Fermi level is not well defined in this region. In an accumulation layer, the adsorbed surface charges are compensated by majority charge carriers that accumulate at the surface...

See other pages where Types of Space is mentioned: [Pg.55]    [Pg.149]    [Pg.253]    [Pg.125]    [Pg.110]    [Pg.3]    [Pg.55]    [Pg.39]    [Pg.329]    [Pg.345]    [Pg.48]    [Pg.167]    [Pg.272]    [Pg.465]    [Pg.815]    [Pg.3091]    [Pg.285]    [Pg.285]    [Pg.227]    [Pg.619]    [Pg.37]   


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