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CHAPTER 2

                           GAS TRANSPORT MECHANISMS





                           STEPHEN W. WEBB
                           Sandia National Laboratories, P. O. Box 5800, Albuquerque, NM 87185, USA


                           Gas-phase momentum transport in porous media consists of advective and diffu-
                           sive components. In this chapter, the individual advective and diffusive components
                           will be presented separately first, followed by a discussion of the combined mecha-
                           nisms. Gas-only situations will be discussed for all the mechanisms. Two-phase, or
                           unsaturated, flow effects are included in Chapter 5.
                             The conservation equations presented below are given in a simplified form. For
                           a complete derivation of the various conservation equations, including underlying
                           assumptions, see Whitaker (Chapter 6 of this book).
                             Energy transport is not discussed in this chapter. Gas-phase energy transport in
                           porous media is treated by Plumb (Chapter 27 of this book). Energy transport is also
                           discussed in Nield and Bejan (1999) and Kaviany (1995).


                           2.1  GAS-PHASE ADVECTION
                           2.1.1  Darcy’s Law

                           Gas-phase advection in porous media is generally analyzed using Darcy’s law (Darcy,
                           1856), which simply states that the gas Darcy velocity, u g , is directly proportional
                           to the gas-phase pressure gradient, ∇P g , and the gas-phase permeability, k g . Darcy’s
                           law can be written as

                                                         k g
                                                  u g =−    ∇P g − ρ g g
                                                        µ g
                           where µ g is the gas-phase viscosity and g is the gravitational constant. In terms of
                           mass flux, the equation is

                                                            k g
                                              F g = ρ g u g =−  ρ g (∇P g − ρ g g)
                                                            µ g
                                                            5
                           C. Ho and S. Webb (eds.), Gas Transport in Porous Media, 5–26.
                           © 2006 Springer.
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