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            If  we  now pass an electrical current between the two faces, the resistance of
            the block is Rwl,/A, or, substituting eq. 6.4, Rwli/fAl. The resistivity of the
            block is therefore:




            Substituting this result into the definition of F  (eq. 6.3), we obtain:




              The  Formation  Resistivity  Factor  is  a  dimensionless  material  constant
           that is proportional to the square of the tortuosity and inversely proportional
           to the  porosity  of  the  material. It  is  independent of  the resistivity, and  so
           also  of the salinity of the pore fluid.  Not all rocks  with, say, 20% porosity
           will have the same formation factor because their  tortuosities will normally
           differ. Note that the tortuosity  of  a rock, which is also important for fluid
            now, can be  obtained from      (but see Winsauer et a)., 1952: they  mea-
            sured the tortuosity  by an independent electrical method and concluded that
            Ff =
              Archie (1942) also inferred from experimental data that:

            F  = af-“                                                          (6.6)
            where the factor a is close to unity, and the exponent rn varies between 1.4
            for unconsolidated sands and about 2.3 for indurated sandstones (it is unity
            for  straight  pores).  This empirical result  seems to bear little relationship to
            eq.  6.5,  but  it  is  intuitively  reasonable  to  suppose  that  tortuosity  is  an
            inverse function of  porosity  - the greater the porosity, the smaller the tor-
            tuosity. Winsauer et al.’s tabulation  (1952, p.  266, table 11) may be used to
            obtain an empirical relationship between porosity and tortuosity.  If  we take
            their  measured  tortuosity,  it is  closely  approximated  by  f-2’3:  if  we  take
            mas the measure of tortuosity, it is closely approximated by 0.9 f-”  . Sub-
            stituting these results into eq. 6.5, the first suggests that F  = f-2.3,  while the
            second suggests F  =  0.8 f-’. If  the aberrant (third) data point is omitted, the
            second suggests F  = 0.6 f-’.’. These data are plotted on Fig. 6-2.
               In  addition to Archie’s formula, as eq. 6.6 is called, the following are also
            in  common  use,  and  there  is  no  significant  practical  difference  between
            them :
            F  = 0.81 f-2                for sand

            F= f-2                       for hard sandstone
            F  = 0.62 f-’.”              “Humble Formula”

             These results,  amply justified  by  decades of use, suggest that JFf is a better
             measure of  tortuosity than the direct measurement used by Winsauer and his
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