Further Readings and Figure References

(1988) Carbon Fibers and Filaments, Springer Series in Materials Science, vol. 5, Springer, Berlin. 

Greenwood, N.N. and Earnshaw, A. (2005) Chemistry of the Elements, 2nd edn, Elsevier Butterworth Heinemann, Amsterdam. 

(1999) The Diamond Makers, Cambridge University Press, Cambridge. 

Huheey, J., Keiter, E., and Keiter, R. (1995) Anorganische Chemie, 2nd edn, W. de Gruyter, Berlin, 

Gmelin Handbook of Inorganic and Organo-metallic Chemistry, 8th edn, (1967-1978) Springer Verlag, Heidelberg. 

---

Those patents are also listed in the references at the end of this book. Innogy selected the positive and negative electrolytes of sodium bromide ( anolyte ) and sodium polysulphide ( catholyte ). Sodium polysulphide is shown in Figure 2.2, as a Lewis structure, as in the textbook of chemistry (Mortimer, 1975). Further reading on polysulphides is available in Porterfield (1993), Lessner (1986 1988) and Murray (1983). 

Wine phenols are commonly referred to as polyphenols , due as may be seen in Figure 2, to the presence of multiple phenolic groups in their structures, which confer on these compounds various properties linked to health benefits, specifically the antioxidant properties attributed to the consumption of moderate amounts of red wine. Much has been published on this subject and the area and references to reviews may be found in Further reading section. 

The outcome of the fact that the WLF equation exhibits universal constants is that the fractional free volume at the glass transition temperature and the thermal expansion coefficient of the free volume also have universal values. Figure 5.19 shows schematically the temperature dependence of the free volume. Other approaches which can be categorized as free volume theories have been proposed. We refer to the further reading listed at the end of this chapter for more detailed information. 

The wave functions from surface states decay exponentially into vacuum and into the solid. They could not be described as Bloch states i (r + z) = fr(r)e with real wave vectors k. In contrast, they possess real energies but complex wave vectors k = ir/a + iq, resulting in the exponential decay f(z) = (0)e e of the oscillatory part of the wave function into the bulk as sketched in Figure 9.30. Complex wave vectors are forbidden in the bulk because the wave function would grow to infinity and therefore can not be normalized. At a surface, however, the exponential increase is terminated and the wave function decays exponentially into the vacuum. Such a wave function could be normahzed and represents electrons localized at the surface. For further reading we refer to Ref [66] and Chapter 5. 

Besides providing a single-source reference, this book also provides information for specific applications. This means that someone practicing in a particular area can immediately go to their application, without necessarily having to read through other chapters. They can determine for themselves what is useful for them. The reader can save time and more quickly use the information provided by experts in each area. Nearly 1300 references and over 800 figures, and 140 fables are provided for fhose that need further information on a particular topic. 

Here, we briefly overview the basic definitions and relations used to describe curvilinear coordinate systems in Euclidean space. These definitions are used to derive the governing equations in Section 5.4. The kinematics of the membrane is also expressed in differential geometry. For further discussion on the topic refer to Carmo [17] and Kreyszig [18]. A two-dimensional surface 5 is characterized by a general set of coordinates as shown in Figure 5.1. The point ( k in the parameter domain V and its mapping x on the surface 5 are defined by the vector x = Jt( k % )-The associated tangent vectors read... 

---