Critical points: Difference between revisions
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<math>C_V(T) \rightarrow \infty ~{\rm as} ~ T \rightarrow T_c \pm</math>. Such a result is again inconsistent with classical theory." | <math>C_V(T) \rightarrow \infty ~{\rm as} ~ T \rightarrow T_c \pm</math>. Such a result is again inconsistent with classical theory." | ||
Thus in the vicinity of the liquid-vapour critical point, both the [[Compressibility | isothermal compressibility]] | |||
and the [[heat capacity]] at constant pressure diverge to infinity. | |||
===Gamma divergence=== | |||
When approaching the critical point along the critical isochore the divergence is of the form | |||
:<math>\left. \right. C_p \sim \kappa_T \sim (T-T_c)^{-\gamma} \sim (p-p_c)^{-\gamma}</math> | |||
where <math>\gamma</math> is 1.0 for the [[Van der Waals equation of state]], and is usually 1.2 to 1.3. | |||
===Epsilon divergence=== | |||
When approaching the critical point along the critical isotherm the divergence is of the form | |||
:<math>\left. \right. \kappa_T \sim (p-p_c)^{-\epsilon}</math> | |||
where <math>\gamma</math> is 2/3 for the [[Van der Waals equation of state]], and is usually 0.75 to 0.8. | |||
==References== | ==References== | ||
#[http://dx.doi.org/10.1080/00268978300102111 G. A. Martynov; G. N. Sarkisov "Exact equations and the theory of liquids. V", Molecular Physics '''49''' pp. 1495-1504 (1983)] | #[http://dx.doi.org/10.1080/00268978300102111 G. A. Martynov; G. N. Sarkisov "Exact equations and the theory of liquids. V", Molecular Physics '''49''' pp. 1495-1504 (1983)] |
Revision as of 16:16, 3 July 2007
Critical points are singularities in the partition function. In the critical point vicinity (Ref. 1 Eq. 17a)
and
For a review of the critical region see the work of Michael E. Fisher (Ref. 2).
... Turning now to the question of specific heats, it has long been known
that real gases exhibit a large ``anomalous" specific-heat maximum
above which lies near the critical isochore and which is not expected on classical theory..." (Ref. 3)
also
... measurements (Ref 4) of for argon along the critical isochore suggest strongly that . Such a result is again inconsistent with classical theory."
Thus in the vicinity of the liquid-vapour critical point, both the isothermal compressibility and the heat capacity at constant pressure diverge to infinity.
Gamma divergence
When approaching the critical point along the critical isochore the divergence is of the form
where is 1.0 for the Van der Waals equation of state, and is usually 1.2 to 1.3.
Epsilon divergence
When approaching the critical point along the critical isotherm the divergence is of the form
where is 2/3 for the Van der Waals equation of state, and is usually 0.75 to 0.8.
References
- G. A. Martynov; G. N. Sarkisov "Exact equations and the theory of liquids. V", Molecular Physics 49 pp. 1495-1504 (1983)
- Michael E. Fisher "Correlation Functions and the Critical Region of Simple Fluids", Journal of Mathematical Physics 5 pp. 944-962 (1964)
- A. Michels, J.M. Levelt and G.J. Wolkers "Thermodynamic properties of argon at temperatures between 0°C and −140°C and at densities up to 640 amagat (pressures up to 1050 atm.)", Physica 24 pp. 769-794 (1958)
- M. I. Bagatskii and A. V. Voronel and B. G. Gusak "", Journal of Experimental and Theoretical Physics 16 pp. 517- (1963)
- Robert B. Griffiths and John C. Wheeler "Critical Points in Multicomponent Systems", Physical Review A 2 1047 - 1064 (1970)