Page 60 - Modern Spatiotemporal Geostatistics
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Spatiotemporal  Geometry                    41

            The  generalization  of  the  Gaussian  coordinate  system  to  higher  dimen-
        sional  spaces  requires  the  use of  the  concept  (proposed  by  Riemann)  of  a
        manifold,  which  is a natural  extension  of  Euclidean space  (Riemann originally
        introduced  the  concept  of  a continuous  manifold  as a continuum  of  elements,
        such that a single  element  is defined by n  continuous  variable magnitudes; this
        definition  includes  the  analytical  conception  of  space  in  which  each  point  is
        defined  by n  coordinates).  In simple terms,  an n-dimensional  manifold  is a set
        of  points  such  that  each  point  can  serve  as the  origin  of  a  local  coordinate
        system  (also called a coordinate  patch)  that covers only  a portion  of the  space
        and  offers an internal  visualization of the  surface. A  set of  coordinate  patches
        that  covers the  whole  space  of  interest  is  called  an  atlas.  Since  it  requires
        two  Gaussian  coordinates  to  locate  a  point  on  an  ordinary  surface,  the sur-
        face  is called  a  two-dimensional  manifold.  If  Cartesian coordinates  are used,
        a  relation  among  three  of  them  is  needed to  describe such  a  manifold.  Rie-
        mann  extended  Gauss'  intrinsic  geometry of two-dimensional  surfaces  (n  =  2)
        to n-dimensional  manifolds  with n >  2, leading to the Riemannian  coordinate
        system,  as follows.

        DEFINITION    2.4:  The   Riemannian  coordinate  system  in  an  n-
        dimensional  manifold  consists  of  a  network  of  Uj-curves  (i  =  l,...,n)
        so that a  one-to-one  correspondence  is established  between  each  point
                                         (
        P  of the  manifold and the n-tuples HI, .. .,u n).
            The  Riemannian coordinates consistently  assign  to  each  point  on  a man-
        ifold  a  unique  n-tuple;  i.e., they  individuate,  but  neither  relate  nor measure.
        If  explicit  relations or  measures  are required  by the  physical situation  of  con-
        cern,  extra  constructions  are introduced,  like  the  metrical  structure  of  a small
        n-dimensional  region  around each  point  (see the  following  section).  In phys-
        ical  applications,  one  may  choose  to  change or  transform  the  parametric  net
        MI, ...,«„ to  suit  some specified objective.  Then,  one may have to  work with
        restricted  regions  (or  patches) of a manifold to  meet  the  requirements for  such
        a transformation  of  parameters.  In a Riemannian system, the jobs  of Cartesian
        lines are divided  between the coordinate  patches fixing positions  and the curves
        connecting  points on a manifold.  A  rigorous  mathematical  presentation  of  the
        Riemannian theory  of  space, which  is utilized  in  differential  geometry,  may be
        found  in  Chavel  (1995).
            Other  useful  non-Euclidean  coordinate  systems  include the  so-called geo-
        desies  coordinate  system.  According  to  this  system,  a  point  P  on a surface
        is  defined  by choosing  an  origin  O  and  then  measuring the  angle  <j)p  and  the
        distance  \OP\ to  point P  by means of the corresponding geodesic (Fig. 2.10).
        Depending  on  the  shape of  the  surface,  some  constraints  may apply.  In  the
        case  of  the  Earth,  e.g.,  a  maximum  limit  should  be set  for  the  distance such
        that  \OP\ < c/2, where c is the  circumference of the  Earth  (considered  as a
        sphere).  In addition,  the  Glebsch coordinates,  the  Boozer-Grad  coordinates,
        the  Hamada  coordinates,  and the  toroidal  coordinates  (e.g.,  D'haeseleer  et
         al,  1991) are systems of coordinates with certain  particular  physical  properties
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