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sandstone at normal hydrostatic pressures acts as a drain to the water expelled
            by  compaction of  the adjacent mudstones (Fig. 3-16). In general, therefore,
            the  pore  water  moves vertically across the bedding of  the mudstones, then
            laterally within the sandstone*.
              The geological context of abnormally pressured mudstones is dominantly re-
            gressive sequences in which the sandstones tend to thicken towards the land
            of the time, and wedge out in the seaward direction (Fig. 3-17). The geometry
            of  the drains therefore  imposes a landward direction of  migration within the
            sandstones. The top of  abnormal pressures tends, as Dickinson (1951,1953)
            found for the Louisiana Gulf  Coast, to become younger  in the direction of
            the regression. We  shall examine these features in more detail in Chapter 14.




















            Fig.  3-17. Regional pore-water migration in sandstones of  regressive sequences tends to be
            towards the land from which the regression came.


            * It  is sometimes argued  that mudstone pore water migrates laterally “because that is the
            direction  of  greatest permeability”.  We have seen that permeability is but one of the com-
            ponents of  fluid flow, and flow direction is determined by the direction of the fluid poten-
            tial gradient.  ‘fhe quantity  of  water flowing across a  surface  in unit time is proportional
            to the  area  normal  to flow  and  to the potential or hydraulic gradient  (the loss of total
            head  divided  by the length of  the porous material in the direction of  flow; Ahll). To get a
            feel for the quantities and  directions of  compaction flow, consider a rectangular mass of
            mudstone, 10 x  10 x  0.5  km, entirely surrounded  by permeable sands at normal hydro-
            static pressures.  During compaction, the hydraulic gradient  from a point in the centre of
            the mudstone is x/0.25  vertically  and x/5 horizontally  - a factor of  20 in favour of  ver-
            tical  flow. The two horizontal surface areas total 200 km2 ; the four vertical surfaces total
            20 km2 - a factor of  10 in favour of vertical flow. So horizontal permeability would have
            to  be of  the order of  200 times the vertical  permeability  for equal  quantities to be lost
            from  the sides as from  the top and bottom. In reality, mudstones tend to have lenticular
            interfaces with sandstones (except at faults), and the ratio of thickness to lateral extent is
            commonly  much  greater than that  used  in  this simple model. There is no evidence that
            anisotropy  in  mudstone  permeability  is  anywhere  near  sufficient  to lead  to significant
            quantities of  lateral flow in mudstones.
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