The properties of gases and liquids
The properties of gases and liquids
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DOI:
10.1021/ed036p154.4
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发表时间:
1959-03
影响因子:
3
通讯作者:
K. Kobe
中科院分区:
文献类型:
--
作者:
K. Kobe
This book is meant to be a textbook for graduate students or advanced undergraduate students in chemistry (it is not a treatise for experts). For this purpose, the reviewer feels that it is not only an excellent work but is, indeed, the best available at the present time. For ex-ample, Lewis andRandall is out of date; MacDougall is out of print; Klotz is a little too classical and overemphasizes nu-merical work somewhat; and Guggenheim is too advanced for most beginners (though it would he the book of choice for a class consisting of potential theoretical chem-ists). Wall presents a nice balance be-tween theoretical and applied thermody-namics, and at the right level for the average chemistry graduate student. The problems are especially refreshing—departing in many cases from the usual exer-cises in numerical manipulation. An elementary presentation of statis-. tical mechanics is interspersed with the thermodynamics. This is becoming more popular, at least in books. The reviewer prefers in lectures, at least, to treat thermodynamics and statistical mechanics as separate courses, though an indispensable part of the thermodynamics course would be a molecular interpretation, in words, of as much thermodynamic data and as many equations as possible. Fortunately, the statistical mechanics in Wall’s book can be omitted at the instructor’s option. The reviewer finds one very annoying feature: following Lewis and Randall, Wall sees fit to use the partial molal Gibbs free energy symbol (Ft) instead of the chemical potential symbol (ah). This is unfortunate for two reasons:(a) the chemical potential plays a very special and important role (along with pressure and temperature) in determining phase and chemical equilibria and so deserves a special symbol; and (6) the chemical po-tential is relatedmathematically (as a differential coefficient) not only to F, but also to A, E, and H. Wall’s choice in this matter is especially surprising in a book which includes some statistical mechanics, since statistical mechanicians almost always use Hi-