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HYDC02  12/5/05  5:38 PM  Page 47






                                                                                 Physical hydrogeology  47
















































                   Fig. 2.19 Types of springs. After Ford and
                   Williams (1989).

                   abstraction decreased, but with no apparent effect on  supported by an upward effective stress, σ , on the
                                                                                                 e
                   groundwater levels in the recharge zone), such that  aquifer material and the water pressure contained in
                   the water-bearing formation was demonstrating elas-  the pore space, P , such that:
                                                                            w
                   tic behaviour in releasing water from storage. Later,
                   in deriving the general partial differential equation  σ = σ + P               eq. 2.25
                                                                T   e   w
                   describing transient groundwater flow, Jacob (1940)
                   formally described the elastic behaviour of porous  If the porewater pressure is decreased by groundwa-
                   rocks. There are two mechanisms that explain how  ter pumping or by natural groundwater outflow, the
                   water is produced by confined aquifers: the porosity  stress on the aquifer material will increase causing it
                   of the aquifer is reduced by compaction and ground-  to undergo compression.
                   water is released; and the water itself expands since  Compressibility is a material property that
                   water is slightly compressible.             describes the change in volume (strain) induced in a
                     As shown in Fig. 2.23, the total downward stress,  material under an applied stress and is the inverse of
                   σ , applied at the top of a confined aquifer is   the modulus of elasticity (equal to a change in stress
                    T
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