Beattie-Bridgeman equation of state: Difference between revisions

Latest revision as of 18:24, 6 February 2008

The Beattie-Bridgeman equation of state is given by (Ref. 1 Eq. 1)

p = \frac{R T (1 - ϵ)}{v^{2}} (v + B) - \frac{A}{v^{2}}

where

A = A_{0} (1 - \frac{a}{v})

B = B_{0} (1 - \frac{b}{v})

and

ϵ = \frac{c}{v T^{3}}

where $p$ is the pressure, $T$ is the temperature and $R$ is the molar gas constant.

@@ Line 12: / Line 12: @@
 :<math>\epsilon = \frac{c}{vT^3}</math>
+where <math>p</math> is the [[pressure]], <math>T</math> is the [[temperature]] and <math>R</math> is the [[molar gas constant]].
 ==References==
 #[http://dx.doi.org/10.1021/ja01406a005 James A. Beattie and Oscar C. Bridgeman "A NEW EQUATION OF STATE FOR FLUIDS. I. APPLICATION TO GASEOUS ETHYL ETHER AND CARBON DIOXIDE", Journal of the American Chemical Society '''49''' pp.  1665 - 1667 (1927)]
+#[http://dx.doi.org/10.1021/ja01399a001 James A. Beattie and Oscar C. Bridgeman "A NEW EQUATION OF STATE FOR FLUIDS. II. APPLICATION TO HELIUM, NEON, ARGON, HYDROGEN, NITROGEN, OXYGEN, AIR AND METHANE", Journal of the American Chemical Society '''50''' pp. 3133 - 3138 (1928)]
 [[category: equations of state]]