Beattie-Bridgeman equation of state: Difference between revisions

Revision as of 18:35, 7 June 2007

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

p={\frac {RT(1-\epsilon )}{v^{2}}}(v+B)-{\frac {A}{v^{2}}}

where

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

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

and

\epsilon ={\frac {c}{vT^{3}}}

@@ Line 1: / Line 1: @@
+The '''Beattie-Bridgeman equation of state''' is given by (Ref. 1 Eq. 1)
+:<math>p= \frac{RT (1- \epsilon)}{v^2}(v+B) - \frac{A}{v^2}</math>
+where
+:<math>A = A_0 \left(1 - \frac{a}{v} \right)</math>
+:<math>B = B_0 \left(1 - \frac{b}{v} \right)</math>
+and
+:<math>\epsilon = \frac{c}{vT^3}</math>
 ==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)]
 [[category: equations of state]]