Anthony R. West - Solid State Chemistry and its Applications

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SOLID STATE CHEMISTRY AND ITS APPLICATIONS
A comprehensive treatment of solid state chemistry complete with supplementary material and full colour illustrations from a leading expert in the field. Solid State Chemistry and its Applications, Second Edition
Student Edition
Significant updates and new content in this second edition include:
A more extensive overview of important families of inorganic solids including spinels, perovskites, pyrochlores, garnets, Ruddlesden-Popper phases and many more New methods to synthesise inorganic solids, including sol-gel methods, combustion synthesis, atomic layer deposition, spray pyrolysis and microwave techniques Advances in electron microscopy, X-ray and electron spectroscopies New developments in electrical properties of materials, including high Tc superconductivity, lithium batteries, solid oxide fuel cells and smart windows Recent developments in optical properties, including fibre optics, solar cells and transparent conducting oxides Advances in magnetic properties including magnetoresistance and multiferroic materials Homogeneous and heterogeneous ceramics, characterization using impedance spectroscopy Thermoelectric materials, MXenes, low dimensional structures, memristors and many other functional materials Expanded coverage of glass, including metallic and fluoride glasses, cement and concrete, geopolymers, refractories and structural ceramics Overview of binary oxides of all the elements, their structures, properties and applications Featuring full color illustrations throughout, readers will also benefit from online supplementary materials including access to CrystalMaker® software and over 100 interactive crystal structure models.
Perfect for advanced students seeking a detailed treatment of solid state chemistry, this new edition of
will also earn a place as a desk reference in the libraries of experienced researchers in chemistry, crystallography, physics, and materials science.

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Solid State Chemistry and its Applications - изображение 162

i.e. with A in tetrahedral sites and B in octahedral sites. Examples of normal spinels are MgAl 2O 4and MgTi 2O 4. In inverse spinels, half of the B ions occupy tetrahedral sites, leaving the remaining B ions and all the A ions in octahedral sites, i.e.

Solid State Chemistry and its Applications - изображение 163

Table 1.22 Some compounds with the spinel structure

Compound Type a /Å Structure Compound Type a/ Structure
MgAl 2O 4 2, 3 8.0800 Normal Mgln 2O 4 2, 3 8.81 Inverse
CoAl 2O 4 2, 3 8.1068 Normal Mgln 2S 4 2, 3 10.708 Inverse
CuCr 2S 4 2, 3 9.629 Normal Mg 2TiO 4 2, 4 8.44 Inverse
CuCr 2Se 4 2, 3 10.357 Normal Zn 2SnO 4 2, 4 8.70 Inverse
CuCr 2Te 4 2, 3 11.051 Normal Zn 2TiO 4 2, 4 8.467 Inverse
MgTi 2O 4 2, 3 8.474 Normal LiAlTiO 4 1, 3, 4 8.34 Li in tet
Co 2GeO 4 2, 4 8.318 Normal LiMnTiO 4 1, 3, 4 8.30 Li in tet
Fe 2GeO 4 2, 4 8.411 Normal LiZnSbO 4 1, 2, 5 8.55 Li in tet
MgFe 2O 4 2, 3 8.389 Inverse LiCoSbO 4 1, 2, 5 8.56 Li in tet
NiFe 2O 4 2, 3 8.3532 Inverse

Usually the A and B cations in octahedral sites are disordered. Examples of inverse spinels are MgFe 2O 4and Mg 2TiO 4.

In addition to normal and inverse spinels, a complete range of intermediate cation distributions is possible and, in some cases, the distribution changes with temperature. The cation distribution may be quantified using a parameter, γ , which is the fraction of A ions on the octahedral sites:

normal: [A]tet[B2]octO4 γ = 0

inverse: [B]tet[A, B]octO4 γ = 1

random: [B0.67A0.33]tet[A0.67B1.33]octO4 γ = 0.67.

The cation distribution in spinels and the degree of inversion, γ , have been studied in considerable detail. Several factors influence γ , including the site preferences of ions in terms of size, covalent bonding effects and crystal field stabilisation energies (see Chapter 2). The γ value in any particular spinel is given by the net effect of these various parameters taken together. Some compounds with the spinel structure are given in Table 1.22.

1.17.10 Olivine

The olivine structure, typified by the minerals forsterite, Mg 2SiO 4, and triphylite, LiFePO 4, is the hcp analogue of the spinel structure. One‐eighth of the tetrahedral sites are occupied by Si or P and half of the octahedral sites by Mg or Li, Fe within an hcp oxide array. There are two crystallographically distinct octahedral sites in olivine, which are occupied in ordered fashion by Li and Fe in LiFePO 4. The crystal structure is shown in Fig. 1.45 and some olivines are listed in Table 1.23. Olivines occur mainly with oxides but also with sulphides, selenides and some fluorides. Various cation charge combinations occur, such that in oxides the three cations have a net charge 8+.

Olivines (mainly forsterite and fayalite) are believed to be the main mineralogical constituent of the Earth's upper mantle. At high pressures, many olivines transform to the spinel structure and spinels are probably the main constituent of the Earth's lower mantle. Volume changes associated with the olivine to spinel phase transformation may have had fundamental geological consequences during the evolution of the Earth, involving the formation of mountain ranges and under‐sea ridges. When spinel material from the lower mantle was pushed upwards to the Earth's surface, it transformed to olivine due to the reduction in pressure. The reverse transformation, olivine to spinel, with a volume contraction may be a contributing factor to earthquakes.

Figure 145 Olivine structure of LiFePO4 Modified from J J Biendicho and - фото 164

Figure 1.45 Olivine structure of LiFePO4.

Modified from J. J. Biendicho and A. R. West, Solid State Ionics203, 33 (2011).

Table 1.23 Some compounds with the olivine structure

General formula
Octahedral site Tetrahedral site hcp anion Examples
II 2 IV O 4 Mg 2SiO 4(forsterite) Fe 2SiO 4(fayalite) CaMgSiO 4(monticellite) γ ‐Ca 2SiO 4A 2GeO 4: A = Mg, Ca, Sr, Ba, Mn
III 2 II O 4 Al 2BeO 4(chrysoberyl) Cr 2BeO 4
II, III III′ O 4 MgAlBeO 4
I, II V O 4 LiFePO 4(triphylite) LiMnPO 4(lithiophylite)
I, III IV O 4 LiRESiO 4: RE = Ho, …, Lu NaREGeO 4: RE = Sm, …, Lu LiREGeO 4: RE = Dy, …, Lu
II 2 IV S 4 Mn 2SiS 4Mg 2SnS 4Ca 2GeS 4
I 2 II F 4 γ ‐Na 2BeF 4

Unit cell: orthorhombic; for LiFePO 4, a = 10.33, b = 6.01, c = 4.70 Å; Z = 4.

There is much current interest in LiFePO 4as the cathode material in rechargeable lithium batteries. On charging, Li deintercalates from the structure and a corresponding amount of Fe is oxidised from Fe 2+to Fe 3+, as follows:

Lithium ions occupy channels parallel to the y axis Fig 145 which allows - фото 165

Lithium ions occupy channels parallel to the y axis, Fig. 1.45, which allows them to leave and enter the structure readily during cell charge and discharge. This is an example of a solid state redox reaction with a cell potential of about 3.08 V. LiFePO 4, and associated LiMnPO 4, are of interest because the redox reaction and the process of lithium removal and insertion are reversible over many cycles, giving a high cell capacity, and the materials are cheap, non‐toxic and environmentally friendly.

1.17.11 Corundum, ilmenite and LiNbO 3

These three closely related structure types can be regarded, ideally, as hcp oxide ions with cations occupying two‐thirds of the octahedral sites. Conceptually, they are related to the NiAs structure in which all the octahedral sites are occupied, and to the CdI 2structure in which only half the octahedral sites are occupied, Table 1.4. The crystal structures are shown in Fig. 1.46 and some compounds adopting these structures are listed in Table 1.24. Corundum contains only one cation, Al 3+, whereas ilmenite contains two cations that are ordered over the octahedral sites that are occupied by Al in corundum. In LiNbO 3, the same octahedral sites are occupied but the cation ordering arrangement is different.

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