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Simple cubic lattice unit cell

Calculate the number of spheres in these unit cells simple cubic, body-centered cubic, and face-centered cubic cells. Assume that the spheres are of equal size and that they are only at the lattice points. [Pg.420]

The summation is over the different types of ion in the unit cell. The summation ca written as an analytical expression, depending upon the lattice structure (the orij Mott-Littleton paper considered the alkali halides, which form simple cubic lattices) evaluated in a manner similar to the Ewald summation this typically involves a summc over the complete lattice from which the explicit sum for the inner region is subtractec... [Pg.641]

The easiest ciystal lattice to visualize is the simple cubic stracture. In a simple cubic crystal, layers of atoms stack one directly above another, so that all atoms lie along straight lines at right angles, as Figure 11-26 shows. Each atom in this structure touches six other atoms four within the same plane, one above the plane, and one below the plane. Within one layer of the crystal, any set of four atoms forms a square. Adding four atoms directly above or below the first four forms a cube, for which the lattice is named. The unit cell of the simple cubic lattice, shown in... [Pg.788]

Thus, the planes of the lattice are found to be important and can be defined by moving along one or more of the lattice directions of the unitcell to define them. Also important are the symmetry operations that can be performed within the unit-cell, as we have illustrated in the preceding diagram. These give rise to a total of 14 different lattices as we will show below. But first, let us confine our discussion to just the simple cubic lattice. [Pg.37]

Simple cubic lattice The eight corners of a cubic unit cell are occupied by one kind of atom,... [Pg.209]

Thus, the reciprocal lattice of a simple cubic lattice is also simple cubic. It is shown in Fig. 5.7 in the xy plane, where it is clear that the bisectors of the first nearest-neighbour (100) reciprocal lattice vectors from a closed volume about the origin which is not cut by the second or any further near-neighbour bisectors. Hence, the Brillouin zone is a cube of volume (2n/a)2 that from eqn (2.38) contains as many allowed points as there are primitive unit cells in the crystal. The second, third, and fourth zones can... [Pg.117]

Following the procedure we used for NaCl, the number of atoms, ions, or molecules per unit cell is 1 for the simple cubic lattice, 4 for the fee lattice, and 2 for the bcc lattice. [Pg.101]

For particular lattices with two molecules per unit cell, with simple structure and nearest-neighbor interactions (linear alternating chains, square 2D lattices, or simple cubic lattices of the NaCl type), the absorption occurs for two values of q q = 0 (the b component) and q = Q (the a component) see Section II.B.l.b. In these simple lattices the environment of the site is symmetric and the complete inversion in P, TP, (2.77) is not necessary, because, in the coupling of P, to P, only the completely symmetric state S> intervenes ... [Pg.58]

The chain width of a hydrocarbon molecule (4.6 A) is taken as the linear dimension of a lattice site. Consequently, in the simple cubic lattice, a cube with a side equal to 4.6 A represents the unit cell. Since the effective length per methylene group in an all-trans chain is 1.275 A, 3.6 methylene groups are located in a cube and will be considered to represent a segment. In the lattice, a site has four nearest neighbors in the same layer and one in each of the adjacent layers. In addition, only two relative orientations of two consecutive bonds can occur, namely the collinear and the bent one at 90°. The bending energies of the collinear and bent bond pairs are taken zero and e, respectively. [Pg.612]

Polonium is the only element known to crystallize in the simple cubic lattice, with its atoms at the intersections of three sets of equally spaced planes that meet at right angles. Each unit cell contains one Po atom, separated from each of its six nearest neighbors by 3.35 A. [Pg.871]

Most salts crystallize as ionic solids with ions occupying the unit cell. Sodium chloride (Figure 13-28) is an example. Many other salts crystallize in the sodium chloride (face-centered cubic) arrangement. Examples are the halides of Li+, K+, and Rb+, and M2+X2 oxides and sulfides such as MgO, CaO, CaS, and MnO. Two other common ionic structures are those of cesium chloride, CsCl (simple cubic lattice), and zincblende, ZnS (face-centered cubic lattice), shown in Figure 13-29. Salts that are isomorphous with the CsCl structure include CsBr, Csl, NH4CI, TlCl, TlBr, and TIL The sulfides of Be2+, Cd2+, and Hg2+, together with CuBr, Cul, Agl, and ZnO, are isomorphous with the zincblende structure (Figure 13-29c). [Pg.523]

In discussing infrared absorption spectra, we refer, first of all, to the papers by Dows and Schettino (54) and of Schettino and Salvi (55). Dows and Schettino (54) investigated the CO2 crystal spectrum in the frequency region corresponding to the combination tone of the intramolecular vibrations v and 1/3 u /y3 Ri 3720 cm-1). Schettino and Salvi (55) measured the infrared (IR) spectra of N2O and OCS crystals. The CO2 and N2O molecules are linear, have no permanent dipole moments, and form a simple cubic lattice upon crystallization. This lattice has four molecules per unit cell, which are oriented along the axes of a tetrahedron. The OCS molecule is also linear, but it forms a crystal of the trigonal system with one molecule per unit cell. [Pg.202]

Fig. 5.6 Unit cells of (a) a simple cubic lattice and (b) a body-centred cubic lattice. Fig. 5.6 Unit cells of (a) a simple cubic lattice and (b) a body-centred cubic lattice.
Figure 12.23 The crystal lattice and the unit cell. A, The lattice is an array of points that defines the positions of the particles in a crystal structure. It is shown here as points connected by lines. A unit cell (colored) is the simplest array of pointsthat, when repeated in all directions, produces the lattice. A simple cubic unit cell, one of 14 types in nature, is shown. B, A checkerboard is a two-dimensional analogy for a lattice. Figure 12.23 The crystal lattice and the unit cell. A, The lattice is an array of points that defines the positions of the particles in a crystal structure. It is shown here as points connected by lines. A unit cell (colored) is the simplest array of pointsthat, when repeated in all directions, produces the lattice. A simple cubic unit cell, one of 14 types in nature, is shown. B, A checkerboard is a two-dimensional analogy for a lattice.
Using your largest spheres, construct a single simple cubic lattice unit cell. Using dots to represent centers of atoms, draw a diagram to represent your model. [Pg.237]

Fig. 2 Future applications of DNA nanotechnology, (a) A guest in a simple cubic lattice. The DNA lattice is drawn as a portion of simple cubic lattice made from 6-arm junctions. The guests are represented by the kidney-bean-shaped features in every unit cell, (b) DNA as scaffolding. Two branched junctions are shown, and a molecular wire is attached to them. When the two junctions cohere with each other, so does the molecular wire, which forms a synapse. View this art in color at www. dekker.com.)... Fig. 2 Future applications of DNA nanotechnology, (a) A guest in a simple cubic lattice. The DNA lattice is drawn as a portion of simple cubic lattice made from 6-arm junctions. The guests are represented by the kidney-bean-shaped features in every unit cell, (b) DNA as scaffolding. Two branched junctions are shown, and a molecular wire is attached to them. When the two junctions cohere with each other, so does the molecular wire, which forms a synapse. View this art in color at www. dekker.com.)...
Show that in a simple cubic lattice, (a) there is one sphere per unit cell, and (b) approximately 52% of the volume of the unit cell is occupied. [Pg.151]

Section 11.7 In a crystalline soUd, particles are arranged in a regularly repeating pattern. An amorphous solid is one whose particles show no such order. The essential structural features of a crystalline solid can be represented by its unit cell, toe smallest part of toe crystal that can, by simple displacement, reproduce the three-dimensional structure. The three-dimensional structures of a crystal can also be represented by its crystal lattice. The points in a crystal lattice represent positions in toe structure where there are identical environments. The simplest unit cells are cubic. There are three kinds of cubic unit cells primitive cubic, body-centered cubic, and face-centered cubic. [Pg.441]

The structure is dehned by one simple cubic lattice parameter and for a=3.795 A hve atoms in the CaTiOs unit cell have the coordinates ... [Pg.33]

Fig. 3.1. Primitive unit cell and Brillouin zone for simple cubic lattice... Fig. 3.1. Primitive unit cell and Brillouin zone for simple cubic lattice...
The cubic crystal system has three possible cubic unit cells simple (or primitive) cubic, body-centered cubic, and face-centered cubic. These cells are illustrated in Figure 11.32. A simple cubic unit cell is a cubic unit cell in which lattice points are situated only at the corners. A body-centered cubic unit cell is a cubic unit cell in which there is a lattice point at the center of the cubic cell in addition to... [Pg.449]


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