Page 163 - Fundamentals of Reservoir Engineering
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DARCY'S LAW AND APPLICATIONS                               102



                                                                                    ∆h

                                                               water
                                                               manometers






                                  q cc / sec
                                                                                             h
                                                         l





                                                             z
                             + z





                                                     datum plane; z = 0, p = 1 atm.

                     Fig. 4.2   Orientation of Darcy's apparatus with respect to the Earth's gravitational field


                     It is worthwhile considering the significance of the ∆h term appearing in Darcy's law.
                     The pressure at any point in the flow path, fig. 4.2, which has an elevation z, relative to
                     the datum plane, can be expressed in absolute units as

                           p = ρg(h-z)


                     with respect to the prevailing atmospheric pressure. In this equation h is the liquid
                     elevation of the upper manometer, again, with respect to z = 0 and ρ is the liquid
                     (water) density. The equation can be alternatively expressed as

                                  p
                           hg =  (  +  gz)                                                           (4.2)
                                  ρ

                     If equ. (4.1) is written in differential form as

                                  dh
                           u =  K                                                                    (4.3)
                                  dl

                     then differentiating equ. (4.2) and substituting in equ. (4.3) gives

                                Kd p              K d(hg)

                           u =          +  gz    =                                                   (4.4)
                                gdl ρ             g    dl

                                p
                     The term (    + gz), in this latter equation, has the same units as hg which are:
                                ρ
                     distance × force per unit mass, that is, potential energy per unit mass. This fluid
                     potential is usually given the symbol Φ and defined as the work required, by a
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