Experimental Data and Eos Modeling for the Density of Natural Gas and Oil Constituents at Pressures to 40000 Psia and Temperatures to 500 °F

Monday, November 8, 2010: 8:50 AM
Canyon A (Hilton)
Hseen Baled1, Robert M. Enick1, Mark . A McHugh2, Kun Liu2, Yue Wu2, B. D. Morreale3, Michael V. Ciocco4 and Deepak Tapriyal4, (1)Chemical and Petroleum Engineering, University of Pittsburgh, Pittsburgh, PA, (2)Department of Chemical and Life Science Engineering, Virginia Commonwealth University, Richmond, VA, (3)Office of Research and Development, U.S. Department of Energy, National Energy Technology Laboratory, Pittsburgh, PA, (4)NETL, South Park, PA

The production of petroleum fluids from very deep reservoirs requires accurate modeling of the fluid density and viscosity at pressures and temperatures (P-T) as high as 40000 psia and 500°F, respectively. Although correlations for the density of the components of natural gas and petroleum fluids are available in the literature, many of these equation-of-state correlations are based on a limited range of experimental data obtained at modest P-T conditions. We have initiated an experimental program to obtain density data that covers the entire P-T range of interest for deep reservoirs for model compounds including methane, propane, n-pentane, n-octane, iso-octane, cyclooctane, n-decane, n-hexadecane, and toluene. These density data, along with available literature data, are used to assess the performance of the SAFT, the perturbed chain SAFT (PC-SAFT), Peng-Robinson (PR), Soave-Redlich-Kwong (SRK), SRK with temperature-dependent volume translation, and the SRK with temperature- and density-dependent volume translation. The preliminary modeling results show that the PC-SAFT equation of state yields very low values of the percent average absolute deviation (AADP) of the density for each model component. For example, AADP values for the density of n-pentane, toluene, and n-decane are 0.82%, 0.59%, and 0.88%, respectively. The AADP obtained with the cubic equations of state are significantly larger; for n-pentane the AADP is 4.38% and 6.62% for the PR and the SRK, respectively. In contrast, the SRK with temperature-dependent volume translation predicted n-pentane density isotherms that cross one another at high pressures; hence, this model was not investigated further. More details will be presented for the experimental and modeling studies described here.

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See more of this Session: Thermodynamic and Transport Properties Under Pressure
See more of this Group/Topical: Engineering Sciences and Fundamentals