Yang-Yang anomaly

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


\[C_V = VT \left. \frac{\partial^2 p}{\partial T^2} \right\vert_V -NT \left. \frac{\partial^2 \mu}{\partial T^2} \right\vert_V \]


where \(C_V\) is the heat capacity at constant volume and \(\mu\) is the chemical potential. Given that experimentally it is found that \(C_V\) diverges at the critical temperature this implies that either \(\partial^2 p/\partial T^2\) or \(\partial^2 \mu/\partial T^2\), or both, diverge as \(T \rightarrow T_c^-\). Fisher and Orkoulas [2] showed that both terms diverge.

[edit] References

  1. C. N. Yang and C. P. Yang "Critical Point in Liquid-Gas Transitions", Physical Review Letters 13 pp. 303-305 (1964)
  2. 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)
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