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Babatunde A. Bamgbade a,b, Yue Wu a,b, Mark A. McHugh a,b, Hseen O. Baled a,c,
Robert M. Enick a,c, Ward Burgess a, Deepak Tapriyal a,d,, Bryan D. Morreale a
• a National Energy Technology Laboratory RUA, Pittsburgh PA
• b Virginia Commonwealth University, Richmond VA
• c University of Pittsburgh, Pittsburgh PA •
• d URS, Pittsburgh, PA 15236, USA
Website: www.netl.doe.gov
Customer Service: 1-800-553-7681
Chemical and Life Science Engineering Department
Website: http://www.chemical.egr.vcu.edu/
The petrochemical industries need predictive
thermodynamic models that are accurate at high-
temperature, high-pressure (HTHP) conditions at
temperatures to 533 K and pressures to 276
MPa, particularly with respect to density
prediction. Traditional cubic equations fail to
provide reliable predictions at HTHP conditions.
Incorporation of a HTHP volume correction term
improves the performance of the cubic equations.
Also, the performance of PC-SAFT with
parameters obtained from fitting HTHP
experimental data are reported.
Introduction
Soave-Redlich-Kwong Volume translated (VT)
(SRK-EoS) SRK-EoS
Volume translation, c, is correlated to reduced
temperature
A and B are correlated to molecular weight and acentric
factor
 
caRT
P
v b v v b

 
    
caRT
P
v c b v c v c b

 
    
expEoS rc v v v A B T      
  0 1 3 5
2 4 6
1 1 1
, , exp exp expA B f M k k k k
k M k M k M

  
      
         
     
Volume Translated Cubic EoS
Experimental Technique
Experimental Pentane PVT
data
Experimental Pentane PVT
data
40 mol% n-C6H14 + 60 mol% n-C16H34
Volume Translated Cubic EoS
Pentane
Pentane
HTHP Volume translated parameters have been
obtained for aromatics, normal and cyclic
hydrocarbons, from 7- 276 MPa and up to 533 K
a
hc
= ma
hs
- (m -1)ln(ghs
)
a
hs
=
4h - 3h2
(1- h)2
ghs
=
2 -h
2(1-h)3
PC-SAFT
a
res
= a
hc
+ a
disp
2
2 3 3 3
1 22 ( , ) ( , )
disp
B B
a m I m Cm I m
k T k T
 
     
   
     
   
C = 1+ m
8h - 2h2
(1-h)4
+ (1- m)
20h - 27h2
+12h3
- 2h4
[(1-h)(2 -h)]2
æ
èç
ö
ø÷
-1
Adjust reduced density, η, until Pcalc =
Pexperimental
Pentane
Dotted lines: NIST smoothed data
Lines: HTHP PC-SAFT
Dashed lines: GS PC-SAFT
Decane
Dotted lines: NIST smoothed data
Lines: HTHP PC-SAFT
Dashed lines: GS PC-SAFT
HTHP PC-SAFT parameters give superior performance
at pressure from 7- 276 MPa but do not perform as well
as the GS PC-SAFT parameters at pressures below 7 MPa
Conclusions
The performance of the cubic and PC-SAFT EoS are
improved at HTHP conditions that are important in
ultra deep well production of oils, condensates, and
natural gas. Parameters for the newly improved
equations are obtained from HTHP experimental
density data, up to 533K and 276 MPa.
Further work is in progress to increase the HTHP
experimental database to obtain even more robust
parameters for these equations of state. A group
contribution approach is being investigated to predict
PC-SAFT parameters at these HTHP conditions.
Acknowledgment
This technical effort was performed in support of the
National Energy Technology Laboratory's Office of Research
and Development support of the Strategic Center for Natural
Gas and Oil under RES contract DE-FE0004000
Hydrocarbon Mixtures: Phase behavior, density, and modeling
with PC-SAFT and a volume-translated, cubic EoS
W. Burgess, D. Tapriyal, H. Baled, R.M. Enick, Y. Wu, M.A. McHugh, B.D. Morreale, Fluid Phase Equilibria, 319, 55 (2012).
J.H. Dymond, K.J. Young, J.D. Isdale, J. Chem. Thermodyn., 11, 887 (1979).
E.U. Franck, S. Kerschbaum, G. Wiegand, Ber. Gesellschaft Phys. Chem. 102, 1794 (1998).
K. Liu, Y. Wu, M.A. McHugh, H. Baled, R.M. Enick, B.D. Morreale, J. SCF, 55, 701 (2010).
40 mol% n-C6H14 + 60 mol% n-C16H34

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AICHE2012--BB 14Oct2012

  • 1. Babatunde A. Bamgbade a,b, Yue Wu a,b, Mark A. McHugh a,b, Hseen O. Baled a,c, Robert M. Enick a,c, Ward Burgess a, Deepak Tapriyal a,d,, Bryan D. Morreale a • a National Energy Technology Laboratory RUA, Pittsburgh PA • b Virginia Commonwealth University, Richmond VA • c University of Pittsburgh, Pittsburgh PA • • d URS, Pittsburgh, PA 15236, USA Website: www.netl.doe.gov Customer Service: 1-800-553-7681 Chemical and Life Science Engineering Department Website: http://www.chemical.egr.vcu.edu/ The petrochemical industries need predictive thermodynamic models that are accurate at high- temperature, high-pressure (HTHP) conditions at temperatures to 533 K and pressures to 276 MPa, particularly with respect to density prediction. Traditional cubic equations fail to provide reliable predictions at HTHP conditions. Incorporation of a HTHP volume correction term improves the performance of the cubic equations. Also, the performance of PC-SAFT with parameters obtained from fitting HTHP experimental data are reported. Introduction Soave-Redlich-Kwong Volume translated (VT) (SRK-EoS) SRK-EoS Volume translation, c, is correlated to reduced temperature A and B are correlated to molecular weight and acentric factor   caRT P v b v v b         caRT P v c b v c v c b         expEoS rc v v v A B T         0 1 3 5 2 4 6 1 1 1 , , exp exp expA B f M k k k k k M k M k M                            Volume Translated Cubic EoS Experimental Technique Experimental Pentane PVT data Experimental Pentane PVT data 40 mol% n-C6H14 + 60 mol% n-C16H34 Volume Translated Cubic EoS Pentane Pentane HTHP Volume translated parameters have been obtained for aromatics, normal and cyclic hydrocarbons, from 7- 276 MPa and up to 533 K a hc = ma hs - (m -1)ln(ghs ) a hs = 4h - 3h2 (1- h)2 ghs = 2 -h 2(1-h)3 PC-SAFT a res = a hc + a disp 2 2 3 3 3 1 22 ( , ) ( , ) disp B B a m I m Cm I m k T k T                       C = 1+ m 8h - 2h2 (1-h)4 + (1- m) 20h - 27h2 +12h3 - 2h4 [(1-h)(2 -h)]2 æ èç ö ø÷ -1 Adjust reduced density, η, until Pcalc = Pexperimental Pentane Dotted lines: NIST smoothed data Lines: HTHP PC-SAFT Dashed lines: GS PC-SAFT Decane Dotted lines: NIST smoothed data Lines: HTHP PC-SAFT Dashed lines: GS PC-SAFT HTHP PC-SAFT parameters give superior performance at pressure from 7- 276 MPa but do not perform as well as the GS PC-SAFT parameters at pressures below 7 MPa Conclusions The performance of the cubic and PC-SAFT EoS are improved at HTHP conditions that are important in ultra deep well production of oils, condensates, and natural gas. Parameters for the newly improved equations are obtained from HTHP experimental density data, up to 533K and 276 MPa. Further work is in progress to increase the HTHP experimental database to obtain even more robust parameters for these equations of state. A group contribution approach is being investigated to predict PC-SAFT parameters at these HTHP conditions. Acknowledgment This technical effort was performed in support of the National Energy Technology Laboratory's Office of Research and Development support of the Strategic Center for Natural Gas and Oil under RES contract DE-FE0004000 Hydrocarbon Mixtures: Phase behavior, density, and modeling with PC-SAFT and a volume-translated, cubic EoS W. Burgess, D. Tapriyal, H. Baled, R.M. Enick, Y. Wu, M.A. McHugh, B.D. Morreale, Fluid Phase Equilibria, 319, 55 (2012). J.H. Dymond, K.J. Young, J.D. Isdale, J. Chem. Thermodyn., 11, 887 (1979). E.U. Franck, S. Kerschbaum, G. Wiegand, Ber. Gesellschaft Phys. Chem. 102, 1794 (1998). K. Liu, Y. Wu, M.A. McHugh, H. Baled, R.M. Enick, B.D. Morreale, J. SCF, 55, 701 (2010). 40 mol% n-C6H14 + 60 mol% n-C16H34