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Unit cell edge lengths

The unit-cell edge length of lithium fluoride is 401.8 pm. What is the smallest angle at which the x-ray beam generated from a molybdenum source (X = 71.07 pm) must strike the planes making up the faces of the unit cell for the beam to be diffracted from those planes Refer to Major Technique 3 on x-ray diffraction, which follows this set of exercises. [Pg.333]

An imaginary metal crystallizes in a cubic lattice. The unit cell edge length is 100. picometers (1 picometer = 1 x 10 12 meter). The density of this metal is 200. g/cm3. The atomic mass of the metal is 60.2 g/mol. How many of these metal atoms are there within a unit cell ... [Pg.129]

Several phases are known to have this structure a short selection is presented in the following list with indicative values of the lattice parameter (unit cell edge length) ... [Pg.145]

As stated in Problem 3.1, copper crystallizes into a face-centered cubic lattice with a unit cell edge length a = 3.62 A. Calculate the number of Cu atoms per cm exposed on each surface of the (100), (110), and (111) planes. [Pg.39]

Oxidation of FeCl2 solutions at pH 7-8 in the presence of soluble Al led to Al substituted lepidocrocite with an Al/(Fe-i-Al) of up to 0.14 the a, h and c unit cell edge lengths fell linearly as the Al content increased (Schwertmann Wolska, 1990). The Bhf at 4.2K also decreased linearly over the same range of Al substitution, i. e. [Pg.46]

Fig. 3.6 Relationship between the unit cell edge length b of synthetic goethites and the level of structurally incorporated Al ", Mn ", Cr ", Co " and V " (data from Schulze Schwertmann, 1984 Stiers Schwertmann, 1985 Schwertmann et al., 1989 Gerth, 1990 and Schwertmann Pfab, 1994, respectively). Fig. 3.6 Relationship between the unit cell edge length b of synthetic goethites and the level of structurally incorporated Al ", Mn ", Cr ", Co " and V " (data from Schulze Schwertmann, 1984 Stiers Schwertmann, 1985 Schwertmann et al., 1989 Gerth, 1990 and Schwertmann Pfab, 1994, respectively).
Fig. 3.7 Top Relationship between the unit cell edge length a of synthetic goethites and various structurally incorporated metals. Bottom Rate of change of a per mol of substituted metal (= slope of the upper curves) vs. ionic radius of the respective metal cations (Gerth, 1990, with permission). Fig. 3.7 Top Relationship between the unit cell edge length a of synthetic goethites and various structurally incorporated metals. Bottom Rate of change of a per mol of substituted metal (= slope of the upper curves) vs. ionic radius of the respective metal cations (Gerth, 1990, with permission).
Fig. 3.9 Effect of Al-substitution in synthetic hematites on (Left) the unit cell edge length a of hematites synthesized at various temperatures (Stanjek Schwertmann, 1992, with permission), and (Right) the magnetic hyperfine field Bhf of hematites formed at 70 °C and 1000°C dotted lines indicate 95% confidence limits (Murad Schwertmann 1986 with permission). Fig. 3.9 Effect of Al-substitution in synthetic hematites on (Left) the unit cell edge length a of hematites synthesized at various temperatures (Stanjek Schwertmann, 1992, with permission), and (Right) the magnetic hyperfine field Bhf of hematites formed at 70 °C and 1000°C dotted lines indicate 95% confidence limits (Murad Schwertmann 1986 with permission).
The thermal transformation of feroxyhyte (5 -FeOOH) was studied by Carlson and Schwertmann (1980). Synthetic feroxyhyte transformed to hematite with non-uni-formly broadened XRD lines at 240 °C (DTA). As the temperature increased further, an exothermic peak appeared and the crystallinity of the hematite improved. In an atmosphere of N2 the transformation of natural feroxyhyte was impeded. As the temperature rose, the crystallinity of this feroxyhyte improved and at 460 °C, the a unit cell edge length dropped from 0.5062 to 0.5027 nm. As this sample contained organic impurities, the final transformation product in this case, even at 800 °C, was maghemite (see p. 368). [Pg.378]

Thallium(I) bromide crystallizes in the CsCl lattice. Its density is 7557 kg/m3 and its unit cell edge-length, a, is 397 pm. From these data, estimate Avogadro s number. [Pg.179]

Figure 12 Changes in the unit-cell edge lengths (A) of sodiiun aluminosilicate natrolite as a function of pressure. Polyhedral representations of natrolite at (a) 0.40 GPa and (b) 1.51 GPa viewed along [001], the chain/channel axis. Each representation is repeated on the right without the framework component to emphasize the channel contents. Note the formation of the hydrogen-bonded water nanotubes at 1.51 GPa. Red circles represent the oxygen of the water molecules yellow ones sodium cations. Blue (azure) tetrahedra dlustrate an ordered distribution of Si (Al) atoms in the framework... Figure 12 Changes in the unit-cell edge lengths (A) of sodiiun aluminosilicate natrolite as a function of pressure. Polyhedral representations of natrolite at (a) 0.40 GPa and (b) 1.51 GPa viewed along [001], the chain/channel axis. Each representation is repeated on the right without the framework component to emphasize the channel contents. Note the formation of the hydrogen-bonded water nanotubes at 1.51 GPa. Red circles represent the oxygen of the water molecules yellow ones sodium cations. Blue (azure) tetrahedra dlustrate an ordered distribution of Si (Al) atoms in the framework...
If the peak positions are used to determine the unit cell edge lengths, a further correction of the peak position (so far not incorporated in available Rietveld models) is needed for very small crystals the broad peaks of which may show an (apparent) shift A°20 due to inconstancy of the Lorenz-polarization and structure factor over the angular range of the peak. [Pg.44]

The composition of the resulting magnetite is close to stoichiometric as indicated by chemical analysis (Fe2,o8Feo.9204), Mossbauer spectroscopy (Fe2,o3Feo.9704), and unit cell edge length (0.83997(3) nm). The crystals form cubes, bounded by 111 faces and vary in size between 0.05-0.2 p.m (Fig. 11-2) the surface area is 4 m /g. The XRD lines are sharp... [Pg.136]

One metal atom sphere) at each corner point in a unit cell One metal atom sphere) at the center of the unit cell Total atoms in unit cell = 8(l/8)+l(l) = 2 [ two atoms (radius r) per unit cell (edge length a)]... [Pg.54]

J3a. The unit cell edge length will, therefore, be given by... [Pg.398]

The unit cell for a cubic close-packed lattice is the fee unit cell. For this cell, the relation between the radius of the atom r and the unit cell edge length a is... [Pg.406]


See other pages where Unit cell edge lengths is mentioned: [Pg.9]    [Pg.16]    [Pg.18]    [Pg.32]    [Pg.32]    [Pg.44]    [Pg.47]    [Pg.48]    [Pg.56]    [Pg.329]    [Pg.378]    [Pg.404]    [Pg.450]    [Pg.452]    [Pg.947]    [Pg.615]    [Pg.283]    [Pg.43]    [Pg.47]    [Pg.84]    [Pg.90]    [Pg.142]    [Pg.7]    [Pg.55]    [Pg.55]    [Pg.398]    [Pg.401]    [Pg.408]    [Pg.408]    [Pg.413]   
See also in sourсe #XX -- [ Pg.12 , Pg.45 , Pg.84 ]




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Cell length

Edge length

Unit cell length

Units length

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