NAME

     angsyn - uses least squares to  predict  amplitudes  of  CDP
     data from a reflectivity equation.


SYNOPSIS

     angsyn [ -Nntap ] [ -Ootap ] [ -vRMS Velocity File ] [ -rs ]
     [ -re ] [ -as ] [ -ae ] [ -md ] [ -xt ] [ -? ] [ -h ]


DESCRIPTION

     angsyn predicts the amplitudes of seismic  data  through  an
     unconstrained  least  squares  fit  of  the  input data to a
     reflectivity equation.  Input may be either  angle-dependent
     gathers  (angle-T  domain) created by program ANGST or stan-
     dard (X-T domain) CDPs.  The  amplitudes  are  predicted  by
     fitting  the  input amplitudes, sample by sample, in an iso-
     time sense, to a  linearized  form  of  the  Knott-Zoeppritz
     equation.  The output contains only the predicted amplitudes
     in a data set the same size as the input.

     It is important to note that the output  data  is  primarily
     valuable  for  QC  only.  A stack of the output data will be
     same as a stack of the input data, since both the prediction
     and stacking procedure "assume" that the noise on the CDP is
     uncorrelated and averages to zero.  If, however,  the  input
     data is angle gathers, the incremental stacks of the gathers
     to produce angle-limited stacks WILL be somewhat  different.
     Attributes  created from the output data will be the same as
     those computed from the input as long as the reqression used
     to   compute   the   attributes   is   based   on  the  same
     equation(given below).  Note: when running inside XIKP the 0
     connector  is for the input data, the 1 connector is for the
     output data, and the 3 connector is for the RMS P-velocity.

     The basis equation for the least squares regression is given
     by

     R(t) = A + D*tan^2(theta) + E*tan^2(theta)*sin^2(theta), where

     theta  is  the  incident  angle  at  time t and "^2" denotes
     squaring.  The coefficients A, D,  and  E  are  computed  by
     minimizing  the  difference  between  the observed amplitude
     values and the values predicted by R(t).  Once  the  coeffi-
     cients  are  computed, the R(t) may then be computed for the
     given angle field.

     Program angsyn gets its data  and  parameters  from  command
     line  arguments.  These arguments specify the input data and
     velocity files, the output data set, and  other  computation
     limitations.

  Command line arguments
     -N ntap
          Enter the input data set name immediately after  typing
          -N.   This  input file should include the complete path
          name if the file  resides  in  a  different  directory.
          Example  -n/b/tsp/dummy  tells  the program to look for
          file 'dummy' in directory '/b/tsp'.  (Default = stdin).
          Note:  when  running inside XIKP the 0 connector is for
          the input data, the 1 connector is for the output data,
          and the 3 connector is for the RMS P-velocity.

     -O otap
          Enter the output data set name immediately after typing
          -O.   Specify  the  full  path  to  write the file to a
          directory other than  the  current  working  directory.
          (Default = stdout ). Note: when running inside XIKP the
          0 connector is for the input data, the 1  connector  is
          for the output data, and the 3 connector is for the RMS
          P-velocity.

     -v RMS velocity file
          Enter the name of the file containing the  RMS  veloci-
          ties  corresponding to the input data set, one velocity
          record for each CDP.  This is typically the output from
          program  VELIN or program VOMIT.  (Default = NONE. This
          parameter is REQUIRED when the input is X-T domain.  It
          will  otherwise  be ignored). Note: when running inside
          XIKP the 0 connector is for the input data, the 1  con-
          nector  is  for the output data, and the 3 connector is
          for the RMS P-velocity.

     -rs start record
          Enter the sequential number of the record on  which  to
          begin  processing.   All data prior to this record will
          be skipped and not output.  (Default = first)

     -re end record
          Enter the sequential number of the record on  which  to
          end processing.  All data following this record will be
          skipped and not output.  (Default = last)

     -as mininum angle
          Enter the minimum incident angle, in degrees, to  limit
          the  data  values  used  in  the weighted stacks.  Data
          corresponding to incident angles less than  this  value
          are ignored.  (Default = 0 degrees)

     -ae maximum angle
          Enter the maximum incident angle, in degrees, to  limit
          the  data  values  used  in  the weighted stacks.  Data
          corresponding to  incident  angles  greater  than  this
          value are ignored. (Default = 45 degrees)


     -md ray tracing mode for X-T input
          Enter the flag to  indicate  the  type  of  ray-tracing
          solution  desired.   A  value of 0 gives a straight ray
          solution.   A value of 1 gives a curved  ray  solution.
          A  value  of 2 give a perturbed curved ray solution ein
          the smooth curved ray solution is "perturbed" in accor-
          dance  with the true input velocity function.  (Default
          = 1).

     -xt X-T Domain flag
          If this flag is present, the input data are assumed  to
          be  in  the  X-T domain and ray tracing will be used to
          define the incident angle field for the regression pro-
          cedure. (Default = no, the input data are assumed to be
          in angle-T domain.)

     -?  Enter the command line argument '-?' to get online help.
     The program terminates after the help screen is printed.

     -h Same as -?, except a list of the output  traces  is  also
     printed.   The  program  terminates after the help screen is
     printed.


SEE ALSO

        angst(1)
        square(1)
        attin(1)
        sscale
        sscaleu


REFERENCES

     Aki, K. and Richards, P.G.,  1980,   Quantitave  Seismology:
     Theory and Methods, Freeman, San Francisco.

     Castagna, J.P., Batzle,  M.L.,  and  Eastwood,  R.L.,  1985,
     Relationships   Between  Compressional-Wave  and  Shear-Wave
     Velocities In Clastic Silicate Rocks, Geophysics,  Vol.  50,
     pp 571-581.

     Castagna, J.P., Batzle, M.L., and Kan, T.K., 1992, Rock Phy-
     sics  - The Link Between Rock Properties and AVO Response in
     Offset-Dependent Reflectivity - Theory and Practice  of  AVO
     Analysis,  J.P.  Castagna  and M.M. Backus (eds), Society of
     Exploration Geophysics.

     Castagna, J.P., and Smith,, S.W., 1994,  Comparison  of  AVO
     Indicators:  A  Modeling  Study,   Geophysics,  Vol. 59,  pp
     1849-1855.

     Smith, G.C. and Gidlow, P.M., 1987,  Weighted  Stacking  for
     Rock  Property  Estimation and Detection of Gas, Geophysical
     Prospecting, Vol. 35, pp 993-1014.
     Thomsen, L.P., 1982, Amplitude Vs. Range Attributes: Interim
     Report,  Amoco Production Company Research Department Report
     T82-E-10.

     Thomsen, L.A. and Hanson, K.E., 1985, Linear RDA: S  and  P,
     Amoco  Production  Company Research Department Report T86-E-
     44.


AUTHOR

        Richard Crider STAT  Houston


COPYRIGHT

     copyright 2001, Amoco Production Company
               All Rights Reserved
          an affiliate of BP America Inc.






































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