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Packing densest

We present here some of the highlights of Kitaigorodskii s considerations [88], First, the problem of dense packing is examined for the plane groups of symmetry. The distinction between dense-packed, densest-packed, and maximum density was introduced for the plane layer of molecules. The plane was called dense-packed when coordination of six was achieved for the molecules. The term densest-packed meant six-coordination with any orientation of the molecules with respect to the unit cell axes. The term maximum density was used for the packing if six-coordination was possible at any orientation of the molecules with respect to the unit cell axes while the molecules retained their symmetry. [Pg.466]

We present here some of the highlights of Kitaigorodskii s considerations [9-22]. First, the problem of dense packing is examined for the plane groups of symmetry. The distinction between dense-packed, densest packed, and maximum density was introduced for the plane layer of molecules. The plane was... [Pg.430]

Figure Bl.21.1 shows a number of other clean umeconstnicted low-Miller-index surfaces. Most surfaces studied in surface science have low Miller indices, like (111), (110) and (100). These planes correspond to relatively close-packed surfaces that are atomically rather smooth. With fee materials, the (111) surface is the densest and smoothest, followed by the (100) surface the (110) surface is somewhat more open , in the sense that an additional atom with the same or smaller diameter can bond directly to an atom in the second substrate layer. For the hexagonal close-packed (licp) materials, the (0001) surface is very similar to the fee (111) surface the difference only occurs deeper into the surface, namely in the fashion of stacking of the hexagonal close-packed monolayers onto each other (ABABAB.. . versus ABCABC.. ., in the convenient layerstacking notation). The hep (1010) surface resembles the fee (110) surface to some extent, in that it also... Figure Bl.21.1 shows a number of other clean umeconstnicted low-Miller-index surfaces. Most surfaces studied in surface science have low Miller indices, like (111), (110) and (100). These planes correspond to relatively close-packed surfaces that are atomically rather smooth. With fee materials, the (111) surface is the densest and smoothest, followed by the (100) surface the (110) surface is somewhat more open , in the sense that an additional atom with the same or smaller diameter can bond directly to an atom in the second substrate layer. For the hexagonal close-packed (licp) materials, the (0001) surface is very similar to the fee (111) surface the difference only occurs deeper into the surface, namely in the fashion of stacking of the hexagonal close-packed monolayers onto each other (ABABAB.. . versus ABCABC.. ., in the convenient layerstacking notation). The hep (1010) surface resembles the fee (110) surface to some extent, in that it also...
A technologically important effect of the lanthanide contraction is the high density of the Period 6 elements (Fig. 16.5). The atomic radii of these elements are comparable to those of the Period 5 elements, but their atomic masses are about twice as large so more mass is packed into the same volume. A block of iridium, for example, contains about as many atoms as a block of rhodium of the same volume. However, each iridium atom is nearly twice as heavy as a rhodium atom, and so the density of the sample is nearly twice as great. In fact, iridium is one of the two densest elements its neighbor osmium is the other. Another effect of the contraction is the low reactivity—the nobility —of gold and platinum. Because their valence electrons are relatively close to the nucleus, they are tightly bound and not readily available for chemical reactions. [Pg.778]

Figure 9.32 The densest ordered packings of monospheres hep (a) and fee (b) octahedral (c) and tetrahedral (d) PBU/C closest packing ((a) or (b)), prismoidal PBU/C for packing with /7p=4.0 (e). Figure 9.32 The densest ordered packings of monospheres hep (a) and fee (b) octahedral (c) and tetrahedral (d) PBU/C closest packing ((a) or (b)), prismoidal PBU/C for packing with /7p=4.0 (e).
Figure 9.33 The variants of neighbor layers alternation in the densest regular packings location of spheres in the plane of the figure corresponds to layer arrangement A, next layers may be located to arrangements B or C. Figure 9.33 The variants of neighbor layers alternation in the densest regular packings location of spheres in the plane of the figure corresponds to layer arrangement A, next layers may be located to arrangements B or C.
Figure 9.35 A scheme of the densest packing of particles of a complicated form. Figure 9.35 A scheme of the densest packing of particles of a complicated form.
Emphasis to a similar approach has been given by Zvyagin (1993). He pointed out that many crystal structures can be represented as a composite of certain standard construction modules and various combinations, distributions and arrangements of these. The simplest example of a modular structure is the densest packing... [Pg.169]

Notice that the 111 planes are the close-packed layers of the structure and so have the densest packing of atoms, as we would expect. [Pg.446]

Close packing, which is described in more detail in Section 11.2.1.2, gives not only the densest packing of spheres but also represents the arrangement of lowest energy when an array of like charges is confined to a fixed volume. This rule not only applies separately to the cations and the anions in ceramics, it also applies to the arrangement of the atoms in a metal. One consequence is that the same cation lattices are found in both metals and in ceramic materials (O Keeffe and Hyde 1985). [Pg.136]

In view of this discussion, why compare the experimentally determined value of cesium adsorbed per square centimeter at the optimum emission with the number of available sites per square centimeter on the 110 plane rather than on any other plane There are two reasons (7) the 110 plane is the densest packed plane and is more likely to form on a tungsten surface than any other plane and 2) Martin (5) has shown that in the case of cesium on tungsten near the optimum activity, the 110 plane contributes more current than any other plane. Hence in the experiments described above, fc.pt is observed when the 110 plane reaches its optimum. The fact that the electron emission changes its trend abruptly when all the available sites on the 110 plane are filled fits in with the concept of a monolayer. [Pg.144]

Therefore, in this example, the number of particles was reduced to a reasonable value and, in the first instance, instead of the random packing shown in the previous section, a regular arrangement consisting of spherical particles was assumed. Similar to the arrangement of atoms in ideal crystals, two densest particle beds were chosen. For the body-centered cubic (bcc) arrangement of catalyst particles, the void fraction is equal to 32%, for the face-centered cubic (fee) arrangement, it is 26%. [Pg.11]

Each of these quantities divided by will then give the proportion by weight of each component for densest packing. After the proportions by weight have been determined, the proportions by volume may then... [Pg.138]

However, the planetary model which is also a densest packing model probably symbolizes Kepler s best attempt at attaining a unified... [Pg.80]

The symmetry of the crystal structure is a direct consequence of dense packing. The densest packing is when each building element makes the maximum number of contacts in the structure. First, the packing of equal spheres in atomic and ionic systems will be discussed. Then molecular packing will be considered. Only characteristic features and examples will be dealt with here, following Kitaigorodskii [38]. ... [Pg.441]

The question of densest packing of spheres has been an intriguing problem in mathematics for centuries it has been labeled one of the oldest math problems in the world [45],... [Pg.446]


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