March 3 - 5,1999, Karlsruhe, Germany - FZK
March 3 - 5,1999, Karlsruhe, Germany - FZK
March 3 - 5,1999, Karlsruhe, Germany - FZK
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the real ones [24], but the more advanced mixing<br />
rules and the regression of their parameters also<br />
contribute greatly to this considerable accuracy.<br />
Figure 4.<br />
10<br />
0 -10-<br />
® -15-<br />
1 -20 H<br />
-25 -<br />
-30-<br />
-35<br />
spec. Volume at 250 bar<br />
*•• spec. Volume at 300 bar<br />
•*- Enthalpy at 250 bar<br />
*- Enthalpy at 300 bar<br />
Relative error when calculating properties<br />
of the mixture H 20-C0 2 with<br />
Xco2=0.05 by weighting the pure values<br />
compared to reference data<br />
i*0 530 580<br />
Temperature [°C]<br />
-•-VTBMSR<br />
-+-RKS<br />
Figure 5. Relative error on the enthalpy of the<br />
Ff 20-C0 2 system (x CO2=0.05), 300bar<br />
Conclusions<br />
It has been shown that the proposed EOS, involving<br />
a volume-translation, a sophisticated afunction<br />
with polar parameters and more complicated<br />
mixing rules, specifies reasonable accuracy for<br />
the modeling of the thermodynamic behavior of<br />
aqueous mixtures at elevated pressures and temperatures<br />
- even in the supercritical region. Around<br />
the critical points, their closeness to the real values<br />
drop but only for small regions.<br />
The structure of the EOS is relatively simple and<br />
the parameters c,- and p-, can be related to density and<br />
caloric properties, respectively, although there are<br />
some interactions. Therefore, only slight effort is<br />
required to predict the physical properties. This<br />
enables the EOS to be deployed usefully in process<br />
modeling and simulation.<br />
Acknowledgement<br />
The author would like to thank his former students<br />
Jens-Martin Doering and Martin Junginger for<br />
their major contribution to this work made by performing<br />
the regressions and computing the results.<br />
PR<br />
650<br />
630<br />
110<br />
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submitted in <strong>1999</strong>