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                                                                                 Physical hydrogeology  59




                     Examples of analytical solutions to one-dimensional                       BO X
                     groundwater flow problems                                                  2.9


                     To illustrate the basic steps involved in the mathematical analysis of  h =−  Q  ⋅  0 +
                     groundwater flow problems, consider the one-dimensional flow  0  Kb  c
                     problem shown in Fig. 1 for a confined aquifer with thickness, b. The
                                                               ∴ c = h
                     total flow at any point in the horizontal (x) direction is given by the  0
                     equation of continuity of flow:
                                                               which gives the solution:
                     Q = q ⋅ b                            eq. 1
                                                                h =  h −  Q  x                       eq. 5
                     where q, the flow per unit width (specific discharge), is found from  0  Kb
                     Darcy’s law:
                                                               The specific solution given in equation 5 relates h to location, x, in
                                                                terms of two parameters, Q and Kb (transmissivity), and one bound-
                     q  =− K  h d                         eq. 2  ary value, h . The solution is the equation of a straight line and pre-
                           x d                                        0
                                                               dicts the position of the potentiometric surface as shown in Fig. 1.
                                                               Also note, by introducing a new pair of values of x where h is known,
                     where x increases in the direction of flow. Combining equations 1
                                                               for example x = D, h = h , we can use the following equation to
                     and 2 gives the general differential equation:            D
                                                               evaluate the parameter combination Q/Kb since:
                     Q  =− Kb  h d                        eq. 3  Q  h −  h
                                                                  =
                            x d                                       0  D                           eq. 6
                                                                Kb    D
                     By integrating equation 3, it is possible to express the groundwater
                                                               If we know Kb, we can find Q, or vice versa.
                     head, h, in terms of x and Q:
                                                                 As a further example, the following groundwater flow problem
                                                                provides an analytical solution to the situation of a confined aquifer
                       dh       Kb  dx                          receiving constant recharge, or leakage. A conceptualization of the
                            Q
                        =−
                                                                problem is shown in Fig. 2 and it should be noted that recharge, W,
                                                                at the upper boundary of the aquifer is assumed to be constant
                     ∴= −  Q  x  +   c                    eq. 4  everywhere.
                      h


                          Kb                                     Between x = 0 and x = L, continuity and flow equations can be
                                                                written as:
                     c is the constant of integration and can be determined by use of a
                     supplementary equation expressing a known combination of h and  Q = W(L − x)    eq. 7
                     x. For example, for the boundary condition x = 0, h = h and by
                                                        0
                     applying this condition to equation 4 gives:















                     Fig. 1 Definition sketch of steady flow through a uniform  Fig. 2 Definition sketch of steady flow through a uniform
                     thickness, homogeneous confined aquifer.   thickness, homogeneous confined aquifer with constant recharge.
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