Abstract
Ceramics show the widest range of electrical properties of any class of material. At one extreme we have high-temperature superconductors, which have no resistance to an electrical current. At the other extreme we have electrical insulators. Ceramic superconductors have not yet ful-filled many of the expectations and predications for useful applications, whereas insulating ceramics are used for a number of critical applications such as packages for integrated circuits. Without the use of insulating ceramics the development of powerful personal computers would not have been so rapid. Between the two extremes are ceramics that behave very much like metals, and there are the semiconductors, which are all ceramics. Ceramics with metal-like conductivity are used as electrodes and in thick-film resistors. Semiconductors such as SiC are important for high-temperature electronics. In this chapter we will explain why ceramics show such a diverse range of electrical properties. The important concepts are related to our earlier discussion of bonding and energy bands.
In some ceramics the only species that can move in an applied electric field are the ions in the structure. Generally, the movement of ions is slow, but in a class of ceramics called fast ion conductors, they can move very rapidly. In cubic zirconia the diffusion of oxygen ions at high temperature is particularly fast, and this ceramic is used as the electrolyte in solid oxide fuel cells. Fuel cells are becoming a key part of a diverse energy plan for the twenty-first century.
We will begin by describing the conduction mechanisms in ceramics and looking at some specific applications. We will finish by describing one of the most fascinating developments in ceramics—high-temperature superconductors.
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General References
Cox, P.A. (1987) The Electronic Structure and Chemistry of Solids, Oxford University Press, Oxford. A very good description of electronic properties.
Cyrot, M. and Pavuna, D. (1992) Introduction to Superconductivity and High-Tc Materials, World Scientific, Singapore. A clear introduction to the field. Treats the theoretical models at a level above that used here but within the range of most upper division MSE undergraduates and graduate students.
Duffy, J.A. (1990) Bonding, Energy Levels and Bands in Inorganic Solids, Longman Scientific and Technical, Harlow, Essex, UK. Straightforward description of energy bands in solids.
Hench, L.L. and West, J.K. (1990) Principles of Electronic Ceramics, Wiley, New York. Comprehensive background to electronic ceramics.
Moulson, A.J. and Herbert, J.M. (1992) Electroceramics, Chapman & Hall, London. An excellent account of the properties and applications of electroceramics.
Owens, F.J. and Poole, C.P. Jr. (1996) The New Superconductors, Plenum Press, New York.
Specific References
Bardeen, J., Cooper, L.N., and Schrieffer, J.R. (1957) “Theory of superconductivity,” Phys. Rev. 108, 1175. The BCS theory in all its technical detail.
Josephson, B.D. (1962) “Possible new effects in superconductive tunneling,” Phys. Lett. 1, 251. The eponymous junction.
Nye, J.F. (1985) Physical Properties of Crystals, Clarendon Press, Oxford. This is the standard reference for tensor representation. Chapter XI covers transport properties including electrical conductivity. The representation of σ by tensors is not necessary to understand the electrical behavior of materials. Its significance becomes clear when we want to specify certain properties of anisotropic single crystals.
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(2007). Conducting Charge or Not. In: Ceramic Materials. Springer, New York, NY. https://doi.org/10.1007/978-0-387-46271-4_30
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DOI: https://doi.org/10.1007/978-0-387-46271-4_30
Publisher Name: Springer, New York, NY
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