Construct · 1 fields · 3 citations
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Gilbert N. Lewis introduced fugacity in his 1901 paper The law of physico-chemical change, offering it as a measure of a substance's escaping tendency, the effective pressure a real gas would appear to exert if it behaved ideally. Fugacity, from the Latin for fleeing, is an effective partial pressure that takes the place of the true pressure in thermodynamic equations so that a real gas obeys the same simple relations an ideal gas does, correcting for the molecular attractions and finite molecular volume that make the actual pressure an imperfect guide to how readily a substance will leave a phase. Lewis and Randall's 1923 textbook Thermodynamics and the Free Energy of Chemical Substances established fugacity, alongside the related quantity activity, as a standard tool of physical chemistry, and the ratio of fugacity to pressure, called the fugacity coefficient, records how far a gas departs from ideal behaviour and equals one for an ideal gas. Because it carries the units of pressure yet already folds in a substance's tendency to escape or expand from a phase, fugacity lets chemists compute chemical equilibrium and phase behaviour for real gases, liquids, and mixtures using expressions written for the ideal case.[1][2][3]
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