Critical points: Difference between revisions

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[[Image:press_temp.png|thumb|right]]
==Introduction==
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>
For an interesting discourse on the "discovery" of the gas-liquid critical point, the  Bakerian Lecture of [[Thomas Andrews]]
and the [[pressure]] is known as the ''critical pressure'' <math>(P_c)</math>.
makes interesting reading (Ref. 1).
For an interesting discourse on the "discovery" of the liquid-vapour critical point, the  Bakerian Lecture of [[Thomas Andrews]]
Critical points are singularities in the [[partition function]].
makes good reading <ref>[http://links.jstor.org/sici?sici=0261-0523%281869%29159%3C575%3ATBLOTC%3E2.0.CO%3B2-0 Thomas Andrews "The Bakerian Lecture: On the Continuity of the Gaseous and Liquid States of Matter", Philosophical Transactions of the Royal Society of London '''159''' pp. 575-590 (1869)]</ref>. Critical points are singularities in the [[partition function]].
In the critical point vicinity  (Ref. 2 Eq. 17a)
In the critical point vicinity  (Ref. <ref>[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)]</ref> Eq. 17a)


:<math> \left.\frac{\partial P}{\partial n}\right\vert_{T}  \simeq 0</math>  
:<math> \left.\frac{\partial P}{\partial n}\right\vert_{T}  \simeq 0</math>  
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:<math>n \int_0^{\infty} c(r) ~4 \pi r^2 ~{\rm d}r \simeq  1</math>
:<math>n \int_0^{\infty} c(r) ~4 \pi r^2 ~{\rm d}r \simeq  1</math>


For a review of the critical region see the work of Michael E. Fisher (Ref. 3).
For a review of the critical region see the work of Michael E. Fisher <ref>[http://dx.doi.org/10.1063/1.1704197  Michael E. Fisher "Correlation Functions and the Critical Region of Simple Fluids", Journal of Mathematical Physics '''5''' pp. 944-962 (1964)]</ref>
 
<blockquote>
"... Turning now to the question of specific heats, it has long been known
"... Turning now to the question of specific heats, it has long been known
that real gases exhibit a large ``anomalous" specific-heat maximum
that real gases exhibit a large ``anomalous" specific-heat maximum
above <math>T_c</math> which lies near the critical isochore and which is not expected on classical theory..." (Ref. 3)
above <math>T_c</math> which lies near the critical isochore and which is not expected on classical theory..."
 
</blockquote>
also
also
 
<blockquote>
"... measurements (Ref 4) of <math>C_V(T)</math> for argon along the critical isochore suggest strongly that
"... measurements (Ref. <ref>[http://dx.doi.org/10.1016/S0031-8914(58)80093-2  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)]</ref> ) of <math>C_V(T)</math> for argon along the critical isochore suggest strongly that
<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."
 
</blockquote>
Thus in the vicinity of the liquid-vapour critical point, both the [[Compressibility | isothermal compressibility]]  
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.
and the [[heat capacity]] at constant pressure diverge to infinity.
==Critical exponents==
==Liquid-liquid critical point==
:''Main article: [[Critical exponents]]''
==Solid-liquid critical point==
==Solid-liquid critical point==
*[http://dx.doi.org/10.1063/1.3213616 Måns Elenius and Mikhail Dzugutov "Evidence for a liquid-solid critical point in a simple monatomic system", Journal of Chemical Physics 131, 104502 (2009)]
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
<ref>L. D. Landau and E. M. Lifshitz, "Statistical Physics" (Course of Theoretical Physics, Volume 5) 3rd Edition Part 1, Chapter XIV, Pergamon Press (1980) &sect; 83 p. 258</ref>. However, recent work using the [[Z2 potential]] suggests that this may not be the last word on the subject.
<ref>[http://dx.doi.org/10.1063/1.3213616 Måns Elenius and Mikhail Dzugutov "Evidence for a liquid-solid critical point in a simple monatomic system", Journal of Chemical Physics 131, 104502 (2009)]</ref>.
==Tricritical points==
==Tricritical points==
*[http://dx.doi.org/10.1103/PhysRevLett.24.715  Robert B. Griffiths "Thermodynamics Near the Two-Fluid Critical Mixing Point in He<sup>3</sup> - He<sup>4</sup>", Physical Review Letters '''24'''  715-717 (1970)]
*[http://dx.doi.org/10.1103/PhysRevLett.24.715  Robert B. Griffiths "Thermodynamics Near the Two-Fluid Critical Mixing Point in He<sup>3</sup> - He<sup>4</sup>", Physical Review Letters '''24'''  715-717 (1970)]
*[http://dx.doi.org/10.1063/1.451007 Lech Longa "On the tricritical point of the nematic–smectic A phase transition in liquid crystals", Journal of Chemical Physics '''85''' pp. 2974-2985 (1986)]
*[http://dx.doi.org/10.1063/1.451007 Lech Longa "On the tricritical point of the nematic–smectic A phase transition in liquid crystals", Journal of Chemical Physics '''85''' pp. 2974-2985 (1986)]
==Critical exponents==
:''Main article: [[Critical exponents]]''
==See also==
==See also==
*[[Binder cumulant]]
*[[Binder cumulant]]
==Recomended reading==
*[[Law of corresponding states]]
==References==
<references/>
'''Related reading'''
* M. I. Bagatskii and A. V. Voronel and B. G. Gusak "", Journal of Experimental and Theoretical Physics '''16''' pp. 517- (1963)
* [http://dx.doi.org/10.1103/PhysRevA.2.1047 Robert B. Griffiths and John C. Wheeler "Critical Points in Multicomponent Systems", Physical Review A '''2''' 1047 - 1064 (1970)]
* [http://dx.doi.org/10.1103/RevModPhys.46.597 Michael E. Fisher "The renormalization group in the theory of critical behavior", Reviews of Modern Physics '''46''' pp. 597 - 616 (1974)]
* [http://dx.doi.org/10.1146/annurev.pc.37.100186.001201  J. V. Sengers and  J. M. H. Levelt Sengers "Thermodynamic Behavior of Fluids Near the Critical Point", Annual Review of Physical Chemistry '''37''' pp. 189-222 (1986)]
* [http://dx.doi.org/10.1103/PhysRevLett.93.015701  Kamakshi Jagannathan and Arun Yethiraj "Molecular Dynamics Simulations of a Fluid near Its Critical Point", Physical Review Letters '''93''' 015701 (2004)]
* Cyril Domb "The Critical Point: A Historical Introduction To The Modern Theory Of Critical Phenomena", Taylor and Francis (1996) ISBN 9780748404353
* Cyril Domb "The Critical Point: A Historical Introduction To The Modern Theory Of Critical Phenomena", Taylor and Francis (1996) ISBN 9780748404353
==References==
#[http://links.jstor.org/sici?sici=0261-0523%281869%29159%3C575%3ATBLOTC%3E2.0.CO%3B2-0 Thomas Andrews "The Bakerian Lecture: On the Continuity of the Gaseous and Liquid States of Matter", Philosophical Transactions of the Royal Society of London '''159''' pp. 575-590 (1869)]
#[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/10.1063/1.1704197  Michael E. Fisher "Correlation Functions and the Critical Region of Simple Fluids", Journal of Mathematical Physics '''5''' pp. 944-962 (1964)]
#[http://dx.doi.org/10.1016/S0031-8914(58)80093-2  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)
#[http://dx.doi.org/10.1103/PhysRevA.2.1047 Robert B. Griffiths and John C. Wheeler "Critical Points in Multicomponent Systems", Physical Review A '''2''' 1047 - 1064 (1970)]
#[http://dx.doi.org/10.1103/RevModPhys.46.597 Michael E. Fisher "The renormalization group in the theory of critical behavior", Reviews of Modern Physics '''46''' pp. 597 - 616 (1974)]
#[http://dx.doi.org/10.1146/annurev.pc.37.100186.001201  J. V. Sengers and  J. M. H. Levelt Sengers "Thermodynamic Behavior of Fluids Near the Critical Point", Annual Review of Physical Chemistry '''37''' pp. 189-222 (1986)]
#[http://dx.doi.org/10.1103/PhysRevLett.93.015701  Kamakshi Jagannathan and Arun Yethiraj "Molecular Dynamics Simulations of a Fluid near Its Critical Point", Physical Review Letters '''93''' 015701 (2004)]
[[category: statistical mechanics]]
[[category: statistical mechanics]]
[[category:classical thermodynamics]]
[[category:classical thermodynamics]]

Revision as of 14:53, 9 September 2009

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 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 [1]. Critical points are singularities in the partition function. In the critical point vicinity (Ref. [2] Eq. 17a)

and

For a review of the critical region see the work of Michael E. Fisher [3]

"... 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. [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.

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 [5]. However, recent work using the Z2 potential suggests that this may not be the last word on the subject. [6].

Tricritical points

Critical exponents

Main article: Critical exponents

See also

References

Related reading