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Spatiotemporal  Geometry                    67

        POSTULATE    2.11:  The geometry assumed in a physical application can
        have  significant  effects  on the  spatiotemporal  map  produced.
        The term  "map"  in this  case  may include  both spatiotemporal  estimation  and
        simulation  of  natural variables (e.g.,  kriging estimation  and turning bands sim-
        ulation).  Some practical  demonstrations  of  Postulate  2.11  follow.
        EXAMPLE   2.31:  In  Christakos  et  al.  (2000a),  a two-dimensional  field  with a
        constant  mean and an exponential  covariance c x(h)  =  exp(—1.5  \h\)  h =
        (hi,  h%)  was  considered.  A  metric  should  in  principle  be  derived  based  on
        a  physical  model  of  the  field.  For  the  sake  of  illustration,  assume  that  the
        physically  appropriate  metric  for this field  had the non-Euclidean form  |/ii|  +
         |/i2  .  Under these conditions,  spatial  estimates were generated on the  basis  of
        a  hard data  set Xhard  using a geostatistical  kriging technique,  thus  leading  to
        the  map in  Figure  2.16a.
        Practitioners  of  geostatistics  often  favor  a theory-free  approach that focuses
        solely  on  the  data  set  available  and  ignores  physical  models.  By  ignoring,
         e.g., the  underlying  physics and using commercial geostatistics  software (which
        allows  only  for  the  Euclidean  metric  \//if  +  h%  in  covariance  modeling  and
        kriging), the  same data  set Xhard  as  above results in the  map of  Figure  2.16b.
        As  was  expected,  the  two  maps  display  considerable differences.  The  map
        generated  by  the  standard  means  (Fig.  2.16b)  is  based  on  a  convenient  but
        inadequate  choice  of  metric,  whereas  the  correct  one  (Fig.  2.16a)  properly
        accounts for the physical geometry.
             Most  mapping  techniques  of  classical  geostatistics  have  been  developed
        assuming Cartesian coordinate systems (e.g.,  Deutch and Journel, 1992).  How-
        ever,  as is demonstrated  in  Example  2.32,  this  system  of  coordinates  may  be
        inadequate for  many  physical situations  and can  lead to  inaccurate maps.
        EXAMPLE   2.32:  Figure  2.17  presents variograms and  maps  of  paleo-sea  sur-
        face conditions  from  a study  by Schafer-Neth and Stattegger  (1998).  The vari-
        ogram and map obtained  using Cartesian coordinates are considerably different
        than  those  produced  using  spherical coordinates.  While  analysis  in  terms  of
        spherical  coordinates  provided  an  adequate representation  of  spatial  variabil-
        ity,  the  Cartesian coordinates  were  shown  to  be  inappropriate  because  they
        caused  a distortion  of  spatial  dependencies in  the  case of  large scales  and  led
        to  inaccurate  predictions.  Estimation  in  terms  of  spherical  coordinates  pro-
        duced  maps that  were in  better  agreement with  the  data  and  offered  a  more
        realistic  description  of  physical  reality  than  maps  produced  using  Cartesian
        coordinates.
            The  implications  of  producing  an inaccurate map—as a  result  of  making
        the  incorrect  metric  assumption—may  be  even  more  serious  at  subsequent
        stages of  BME  analysis.  For example, a map of  porous geometry  that  is based
        on  a  physically  inappropriate  metrical  structure  and  that  serves  as input  to
        the  subsurface laws could  lead to  erroneous predictions  of  subsurface flow  and
        contaminant  transport  processes.
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