surface



       surface  - adjustable tension continuous curvature surface
       gridding algorithm


SYNOPSIS

       surface      [      xyzfile       ]       -Goutputfile.grd
       -Ix_inc[m|c][/y_inc[m|c]]   -Rwest/east/south/north[r]   [
       -Aaspect_ratio ] [ -Cconvergence_limit ] [  -H[nrec]  ]  [
       -Lllower  ]  [  -Luupper  ]  [ -Nmax_iterations ] [ -Q ] [
       -Ssearch_radius[m] ] [ -Ttension_factor[ib] ] [ -V[l] ]  [
       -Zover-relaxation_factor ] [ -: ] [ -bi[s][n] ]


DESCRIPTION

       surface  reads  randomly-spaced (x,y,z) triples from stan­
       dard input [or xyzfile] and produces a binary  grdfile  of
       gridded values z(x,y) by solving:

               (1 - T) * L (L (z)) + T * L (z) = 0

       where  T  is a tension factor between 0 and 1, and L indi­
       cates the Laplacian operator.  T = 0  gives  the  "minimum
       curvature"  solution  which is equivalent to SuperMISP and
       the ISM packages. Minimum curvature  can  cause  undesired
       oscillations  and  false local maxima or minima (See Smith
       and Wessel, 1990), and you may wish to use T > 0  to  sup­
       press these effects.  Experience suggests T ~ 0.25 usually
       looks good for potential field data and T should be larger
       (T  ~  0.35) for steep topography data. T = 1 gives a har­
       monic surface (no maxima or minima are possible except  at
       control data points). It is recommended that the user pre-
       process the data with blockmean, blockmedian, or blockmode
       to  avoid  spatial  aliasing and eliminate redundant data.
       You may impose lower and/or upper bounds on the  solution.
       These  may be entered in the form of a fixed value, a grd­
       file with values, or simply be the  minimum/maximum  input
       data values.

       xyzfile
              3  column  ASCII  file  [or binary, see -b] holding
              (x,y,z) data values. If no file is specified,  sur­
              face will read from standard input.

       -G     Output file name. Output is a binary 2-D .grd file.

       -I     x_inc [and optionally y_inc] is the  grid  spacing.
              Append  m to indicate minutes or c to indicate sec­
              onds.

       -R     west, east, south, and north specify the Region  of
              interest. To specify boundaries in degrees and min­
              utes [and  seconds],  use  the  dd:mm[:ss]  format.
              Append  r if lower left and upper right map coordi­
              nates are given instead of wesn.

       -A     Aspect ratio. If desired, grid  anisotropy  can  be
              added  to  the equations. Enter aspect_ratio, where
              dy = dx / aspect_ratio relates the grid dimensions.
              [Default = 1 assumes isotropic grid.]

       -C     Convergence  limit.  Iteration  is  assumed to have
              converged when the maximum absolute change  in  any
              grid  value  is less than convergence_limit. (Units
              same as data z units). [Default is  scaled  to  0.1
              percent of typical gradient in input data.]

       -H     Input  file(s)  has  Header  record(s).  Number  of
              header records can be changed by editing your .gmt­
              defaults  file.  If  used,  GMT default is 1 header
              record.  Not used with binary data.

       -L     Without any modifier, this option indicates that  x
              is  longitude  and  may be periodic in 360 degrees.
              With optional arguments it will instead impose lim­
              its  on  the output solution. llower sets the lower
              bound. lower can be the  name  of  a  grdfile  with
              lower bound values, a fixed value, d to set to min­
              imum input value, or u for unconstrained [Default].
              uupper  sets the upper bound and can be the name of
              a grdfile with upper bound values, a fixed value, d
              to  set  to  maximum  input  value, or u for uncon­
              strained [Default].

       -N     Number of iterations.  Iteration  will  cease  when
              convergence_limit  is  reached  or  when  number of
              iterations  reaches  max_iterations.  [Default   is
              250.]

       -Q     Suggest grid dimensions which have a highly compos­
              ite greatest common factor. This allows surface  to
              use  several  intermediate  steps  in the solution,
              yielding faster run times and better  results.  The
              sizes  suggested  by -Q can be achieved by altering
              -R and/or -I. You can recover the  -R  and  -I  you
              want later by using grdsample or grdcut on the out­
              put of surface.

       -S     Search radius. Enter search_radius in same units as
              x,y  data;  append  m to indicate minutes.  This is
              used to initialize the grid before the first itera­
              tion; it is not worth the time unless the grid lat­
              tice is prime  and  cannot  have  regional  stages.
              [Default = 0.0 and no search is made.]

       -T     Tension  factor[s].  These must be between 0 and 1.
              Tension may be used in the interior solution (above
              equation,  where  it  suppresses  spurious oscilla­
              edges). Using zero for both  values  results  in  a
              minimum  curvature  surface with free edges, i.e. a
              natural bicubic spline.  Use  -Ttension_factori  to
              set  interior tension, and -Ttension_factorb to set
              boundary tension. If you do not append i or b, both
              will  be  set  to the same value.  [Default = 0 for
              both gives minimum curvature solution.]

       -V     Selects verbose  mode,  which  will  send  progress
              reports  to  stderr [Default runs "silently"].  -Vl
              will report the convergence after  each  iteration;
              -V  will  report  only  after each regional grid is
              converged.

       -Z     Over-relaxation factor. This parameter is  used  to
              accelerate  the convergence; it is a number between
              1 and 2.  A  value  of  1  iterates  the  equations
              exactly, and will always assure stable convergence.
              Larger values overestimate the incremental  changes
              during  convergence, and will reach a solution more
              rapidly but may become unstable. If you use a large
              value for this factor, it is a good idea to monitor
              each iteration with the -Vl option. [Default =  1.4
              converges quickly and is almost always stable.]

       -:     Toggles  between  (longitude,latitude)  and  (lati­
              tude,longitude) input/output. [Default  is  (longi­
              tude,latitude)].  Applies to geographic coordinates
              only.

       -bi    Selects binary input. Append s for single precision
              [Default  is  double].   Append n for the number of
              columns in the binary file(s).  [Default is 3 input
              columns].


EXAMPLES

       To  grid  5 by 5 minute gravity block means from the ASCII
       data in hawaii_5x5.xyg, using a tension_factor =  0.25,  a
       convergence_limit  = 0.1 milligal, writing the result to a
       file called hawaii_grd.grd, and monitoring each iteration,
       try:

       surface      hawaii_5x5.xyg      -R198/208/18/25      -I5m
       -Ghawaii_grd.grd -T0.25 -C0.1 -VL


BUGS

       surface will complain when more than  one  data  point  is
       found  for  any  node  and suggest that you run blockmean,
       blockmedian, or blockmode first. If you  did  run  blockm*
       and still get this message it usually means that your grid
       spacing is so small that you need  more  decimals  in  the
       output  format used by blockm*. You may specify more deci­
       binary input and/or output using single or  double  preci­
       sion storage.


SEE ALSO

       blockmean(l),    blockmedian(l),   blockmode(l),   gmt(l),
       nearneighbor(l), triangulate(l)


REFERENCES

       Smith, W. H. F, and P. Wessel, 1990, Gridding with contin­
       uous   curvature   splines  in  tension,  Geophysics,  55,
       293-305.










































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