Yang-Yang anomaly: Difference between revisions

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(New page: The '''Yang-Yang anomaly''' <ref>[http://dx.doi.org/10.1103/PhysRevLett.13.303 C. N. Yang and C. P. Yang "Critical Point in Liquid-Gas Transitions", Physical Review Letters '''13''' pp. ...)
 
m (Corrected typo.)
 
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Given that experimentally it is found that  <math>C_V</math> diverges at the  [[Critical points | critical temperature]] this implies that
Given that experimentally it is found that  <math>C_V</math> diverges at the  [[Critical points | critical temperature]] this implies that
either <math>\partial^2 p/\partial T^2</math> or <math>\partial^2 \mu/\partial T^2</math>, or both, diverge as <math>T \rightarrow T_c^-</math>.
either <math>\partial^2 p/\partial T^2</math> or <math>\partial^2 \mu/\partial T^2</math>, or both, diverge as <math>T \rightarrow T_c^-</math>.
Fisher and Orkoulas <ref>[http://dx.doi.org/10.1103/PhysRevLett.85.696 Michael E. Fisher and G. Orkoulas "The Yang-Yang Anomaly in Fluid Criticality: Experiment and Scaling Theory", Physical Review Letters '''85''' pp. 696-699 (2000)]</ref> showed the ''both'' diverge.
Fisher and Orkoulas <ref>[http://dx.doi.org/10.1103/PhysRevLett.85.696 Michael E. Fisher and G. Orkoulas "The Yang-Yang Anomaly in Fluid Criticality: Experiment and Scaling Theory", Physical Review Letters '''85''' pp. 696-699 (2000)]</ref> showed that ''both'' terms diverge.
==References==
==References==
<references/>
<references/>
[[category: statistical mechanics]]
[[category: statistical mechanics]]

Latest revision as of 14:50, 19 April 2010

The Yang-Yang anomaly [1] provides (Eq. 3):


CV=VT∂2p∂T2|V−NT∂2μ∂T2|V


where CV is the heat capacity at constant volume and μ is the chemical potential. Given that experimentally it is found that CV diverges at the critical temperature this implies that either ∂2p/∂T2 or ∂2μ/∂T2, or both, diverge as T→Tc−. Fisher and Orkoulas [2] showed that both terms diverge.

References[edit]