Clausius equation of state: Difference between revisions
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Carl McBride (talk | contribs) m (Added comment on derivation of a, b, and c) |
Carl McBride (talk | contribs) m (Rewording + internal link) |
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:<math>\left[ p + \frac{a}{T(v+c)^2}\right] (v-b) =RT.</math> | :<math>\left[ p + \frac{a}{T(v+c)^2}\right] (v-b) =RT.</math> | ||
At the [[critical points | critical point]] one has <math>\left.\frac{\partial p}{\partial v}\right|_{T=T_c}=0 </math>, and <math>\left.\frac{\partial^2 p}{\partial v^2}\right|_{T=T_c}=0 </math>, which leads to | |||
:<math>a = v_c - \frac{RT_c}{4P_c}</math> | :<math>a = v_c - \frac{RT_c}{4P_c}</math> |
Revision as of 13:23, 20 October 2009
The Clausius equation of state, proposed in 1880 by Rudolf Julius Emanuel Clausius [1] is given by (Equations 3 and 4 in [2])
At the critical point one has , and , which leads to
and
where is the pressure, is the temperature, is the volume per mol, and is the molar gas constant. is the critical temperature and is the pressure at the critical point, and is the critical volume per mol.