Page 70 - gas transport in porous media
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Chapter 5: Two-Phase Gas Transport
                                                                                            63
                             While the van Genuchten and Brooks and Corey two-phase characteristic curves
                           maylooksimilar, thereareimportantdifferenceswhentheyareusedinflowsituations.
                           McWhorter and Sunada (1990) and Webb (1992) evaluated the differences between
                           the two sets of characteristic curves for analytical two-phase flow situations. The
                           differencesinthesaturationprofilesaresignificant, probablyduetothedifferentshape
                           of the gas-phase relative permeability expressions. In general, the van Genuchten (and
                           Parker) set of curves lead to a much sharper interface, while the Brooks and Corey
                           predictions are much more blunt.


                           5.1.3  Brinkman Extension
                           The Brinkman extension for two-phase (unsaturated) flow has been analyzed by
                           Whitaker (1994). The Brinkman correction terms are negligible for practical two-
                           phase flow problems in porous media and are generally ignored.


                           5.1.4  Forchheimer Extension

                           The Forchheimer correction would be important for two-phase flow when the
                           Reynolds number is sufficiently large compared to one. However, a formal anal-
                           ysis of the Forchheimer extension for two-phase (unsaturated) flow has not been
                           performed.


                           5.1.5  Low Permeability Effects
                           Section 2.1.5 presented the low permeability effects for all-gas conditions. For unsat-
                           urated flow in porous media, Reinecke and Sleep (2002) investigated the variation
                           of the Klinkenberg coefficient for air, b air , including summarizing previous investi-
                           gations. They developed a correlation for the Knudsen diffusion coefficient and the
                           Klinkenberg parameter for unsaturated flow conditions as a function of effective gas
                           permeability, which is simply the gas-saturated permeability times the gas relative
                           permeability. Their Klinkenberg parameter correlation for air is
                                                      b air = 5.57 k −24
                                                                g,e
                                                      2
                           where b air is in Pa and k g,e is in m . Note that the units for the above equation for k g,e
                                            2
                           were specified as cm in the original reference (equation 30). The correct units for
                                   2
                           k g,e are m (Sleep, personal communication, 2005) as given above.
                                                                     2
                             At an effective gas permeability of about 10 −11  m , the above correlation is about
                           the same as Heid et al. (1950). As the effective permeability decreases, the above
                           correlation gives a smaller value of the Klinkenberg factor, or a smaller effect on the
                           permeability, than either the Heid et al. (1950) or Jones and Owens (1980) correla-
                           tions presented in Chapter 2. This difference may be due to the fact that liquid will
                           preferentially block smaller pores, which have the most influence on gas slippage.
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