Critical points: Difference between revisions

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[[Image:press_temp.png|thumb|right]]
[[Image:press_temp.png|thumb|right]]
The '''critical point''' is a point found at the end of the liquid-vapour coexistence curve (the red point shown on the [[pressure-temperature]] plot on the right). At this point the [[temperature]] is known as the ''critical temperature'' <math>(T_c)</math>
The '''critical point''', discovered in 1822 by Charles Cagniard de la Tour <ref>Charles Cagniard de la Tour "", Annales de chimie et de physique '''21''' pp. 127- (1822)</ref>, is a point found at the end of the liquid-vapour coexistence curve (the red point shown on the [[pressure-temperature]] plot on the right). At this point the [[temperature]] is known as the ''critical temperature'' <math>(T_c)</math>
and the [[pressure]] is known as the ''critical pressure'' <math>(P_c)</math>.
and the [[pressure]] is known as the ''critical pressure'' <math>(P_c)</math>.
For an interesting discourse on the "discovery" of the liquid-vapour critical point, the  Bakerian Lecture of [[Thomas Andrews]]
For an interesting discourse on the "discovery" of the liquid-vapour critical point, the  Bakerian Lecture of [[Thomas Andrews]]

Revision as of 17:01, 20 November 2009

The critical point, discovered in 1822 by Charles Cagniard de la Tour [1], is a point found at the end of the liquid-vapour coexistence curve (the red point shown on the pressure-temperature plot on the right). At this point the temperature is known as the critical temperature and the pressure is known as the critical pressure . For an interesting discourse on the "discovery" of the liquid-vapour critical point, the Bakerian Lecture of Thomas Andrews makes good reading [2]. Critical points are singularities in the partition function. In the critical point vicinity (Ref. [3] Eq. 17a)

and

For a review of the critical region see the work of Michael E. Fisher [4]

"... 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..."

also

"... measurements (Ref. [5] ) 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.

Liquid-liquid critical point

Solid-liquid critical point

It is widely held that there is no solid-liquid critical point. The reasoning behind this was given on the grounds of symmetry by Landau and Lifshitz [6]. However, recent work using the Z2 potential suggests that this may not be the last word on the subject. [7].

Tricritical points

Critical exponents

Main article: Critical exponents

See also

References

Related reading