THE VARIATION OF MOLAR ISOBARIC HEAT CAPACITY, MOLAR ENTROPY AND MOLAR ENTHALPY IN THE IDEAL GAS STATE AND OF THE ISOTHERMAL ENTHALPY-PRESSURE COEFFICIENT, SECOND VIRIAL COEFFICIENT AND SPEED OF SOUND AT THE ZERO-PRESSURE LIMIT

Chlorine ◽  
1985 ◽  
pp. 69-71
2007 ◽  
Vol 21 (06) ◽  
pp. 947-953 ◽  
Author(s):  
YAHUI ZHENG ◽  
JIULIN DU

By application of the nonextensive statistics to the ideal gas model, we establish a nonextensive gas model. If we regard the nonextensive gas as a real gas, we can use the nonextensive parameter q ∈ ℝ in Tsallis statistics to describe Joule coefficient, Joule–Thomson coefficient, second virial coefficient and etc. We also derive an expression, with a multiplier T1-q, of the heat capacity of the nonextensive gas. We can prove that in the quasi-equilibrium system there is 1 - q > 0, 2 so the heat capacity still vanishes if temperature tends to zero, just as that in Boltzmann-Gibbs statistics.


1995 ◽  
Vol 105 (2) ◽  
pp. 173-192 ◽  
Author(s):  
Günter Esper ◽  
Wolfgang Lemming ◽  
Wilhelm Beckermann ◽  
Friedrich Kohler

1992 ◽  
Vol 88 (3) ◽  
pp. 427-432 ◽  
Author(s):  
Mario Massucci ◽  
Antony P. du'Gay ◽  
Ana M. Diaz-Laviada ◽  
Christopher J. Wormald

1997 ◽  
Vol 137 (1-2) ◽  
pp. 121-131 ◽  
Author(s):  
Y.Y. Duan ◽  
L.Q. Sun ◽  
L. Shi ◽  
M.S. Zhu ◽  
L.Z. Han

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