By Edward O. Wilson
ISBN-10: 0375414568
ISBN-13: 9780375414565
"One of the world’s most crucial scientists, Edward O. Wilson can be an abundantly gifted author who has two times received the Pulitzer Prize. during this, his such a lot own and well timed e-book thus far, he assesses the precarious kingdom of the environment, studying the mass extinctions taking place in our time and the common treasures we're approximately to lose perpetually. but, instead of eschewing doomsday prophesies, he spells out a selected plan to avoid wasting our international whereas there's nonetheless time. His imaginative and prescient is a hopeful one, as economically sound because it is environmentally precious. Eloquent, functional and clever, this booklet might be learn and studied by means of a person serious about the destiny of the ordinary world.
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Additional resources for The Future of Life
Sample text
In layered thin-film structures, phases such as solid solutions and compounds are frequently accessed horizontally across the phase diagram during an isothermal anneal. This should be contrasted with bulk materials where equilibrium phase changes commonly proceed vertically downward from elevated temperatures. 1 KINETICS MACROSCOPIC TRANSPORT Whenever a material system is not in thermodynamic equilibrium, driving forces arise naturally to push it toward equilibrium. Such a situation can occur, for example, when the free energy of a microscopic system varies from point to point because of compositional inhomogeneities.
The resultant phases that form as a function of initial reactant proportions and temperature are depicted on binary equilibrium phase diagrams. Collections of these have been published for metal, semiconductor, and ceramic systems and are among the most frequently consulted references in the field of materials. Unless noted otherwise, these diagrams hold at atmospheric pressure, in which case the variance is reduced by one. The Gibbs phase rules now states F = n + 1 or F = 3 - ~ . Thus, three phases at most can coexist in equilibrium.
To understand its use suppose it is desired to deposit 27 Thermodynamics of Materials - 50 O 1 o o Z- O lo0 nO LI. I11 -150 X O tl. O tr w z w w w _ 20c f tl. , 1 400 1 -800 1 1200 1 1600 2600 TEMPERATURE ~ Figure 1-11 Standard free energy of oxide formation vs temperature: O, melting point of metal; E], boiling point of metal (1 atm). Reprinted with permission from A. G. Guy, Introduction to Materials Science, McGraw-Hill, New York, 1972. thin-film metal interconnections on a SiO 2 substrate for microelectronic purposes.
The Future of Life by Edward O. Wilson
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