Note: A new GRASS GIS stable version has been released: GRASS GIS 7. Go directly to the new manual page here
User can define a raster map named maskmap, which will be used as a mask. The approximation is skipped for cells which have zero or NULL value in mask. NULL values will be assigned to these cells in all output raster maps. Data points are checked for identical points and points that are closer to each other than the given dmin are removed. If sparsely digitized contours or isolines are used as input, additional points are computed between each 2 points on a line if the distance between them is greater than specified dmax. Parameter zmult allows user to rescale the values used for approximation (useful e.g. for transformation of elevations given in feet to meters, so that the proper values of slopes and curvatures can be computed).
Regularized spline with tension is used for the approximation. The tension parameter tunes the character of the resulting surface from thin plate to membrane. Smoothing parameter smooth controls the deviation between the given points and the resulting surface and it can be very effective in smoothing noisy data while preserving the geometrical properties of the surface. With the smoothing parameter set to zero (smooth=0) the resulting surface passes exactly through the data points (spatial interpolation is performed). When smoothing parameter is used, it is also possible to output a vector point file devi containing deviations of the resulting surface from the given data.
If the number of given points is greater than segmax, segmented processing is used . The region is split into quadtree-based rectangular segments, each having less than segmax points and approximation is performed on each segment of the region. To ensure smooth connection of segments the approximation function for each segment is computed using the points in the given segment and the points in its neighborhood which are in the rectangular window surrounding the given segment. The number of points taken for approximation is controlled by npmin, the value of which must be larger than segmax. User can choose to output vector maps treefile and overfile which represent the quad tree used for segmentation and overlapping neighborhoods from which additional points for approximation on each segment were taken.
Predictive error of surface approximation for given parameters can be computed using the -c flag. A crossvalidation procedure is then performed using the data given in the vector map input and the estimated predictive errors are stored in the vector point file cvdev. When using this flag, no raster output files are computed. Anisotropic surfaces can be interpolated by setting anisotropy angle theta and scaling factor scalex. The program writes values of selected input and internally computed parameters to the history file of raster map elev.
Topographic parameters are computed directly from the approximation function so that the important relationships between these parameters are preserved. The equations for computation of these parameters and their interpretation is described in Mitasova and Hofierka, 1993 or Neteler and Mitasova, 2004). Slopes and aspect are computed in degrees (0-90 and 1-360 respectively). The aspect raster map has value 0 assigned to flat areas (with slope less than 0.1%) and to singular points with undefined aspect. Aspect points downslope and is 90 to the North, 180 to the West, 270 to the South and 360 to the East, the values increase counterclockwise. Curvatures are positive for convex and negative for concave areas. Singular points with undefined curvatures have assigned zero values.
Tension and smoothing allow user to tune the surface character.
For most landscape scale applications the default values should provide adequate results.
The program gives warning when significant overshoots appear in the resulting
surface and higher tension or smoothing should be used.
To select parameters that will produce a surface with desired properties,
it is useful to know that the method is scale dependent and the tension
works as a rescaling parameter (high tension "increases the distances
between the points" and reduces the range of impact of each point, low
tension "decreases the distance" and the points influence each other
over longer range). Surface with tension set too high behaves
like a membrane (rubber sheet stretched over the data points) with peak
or pit ("crater") in each given point and everywhere else the surface goes
rapidly to trend. If digitized contours are used as input data, high tension
can cause artificial waves along contours. Lower tension and higher smoothing
is suggested for such a case.
Surface with tension set too low behaves like a stiff steel
plate and overshoots can appear in areas with rapid change of gradient
and segmentation can be visible. Increase in tension should solve the problems.
There are two options how tension can be applied in relation
to dnorm (dnorm rescales the coordinates depending on the average
data density so that the size of segments with segmax=40 points
is around 1 - this ensures the numerical stability of the computation):
1. Default: the given tension
is applied to normalized data (x/dnorm..), that means that
the distances are multiplied (rescaled) by tension/dnorm. If density
of points is changed, e.g., by using higher dmin, the dnorm
changes and tension needs to be changed too to get the same result.
Because the tension is applied to normalized data its suitable value
is usually within the 10-100 range and does not depend on the actual scale
(distances) of the original data (which can be km for regional applications
or cm for field experiments).
2. Flag -t : The given tension
is applied to un-normalized data (rescaled tension = tension*dnorm/1000
is applied to normalized data (x/dnorm) and therefore dnorm
cancels out) so here tension truly works as a rescaling parameter.
For regional applications with distances between points in km. the suitable
tension can be 500 or higher, for detailed field scale analysis it can
be 0.1. To help select how much the data need to be rescaled the program
writes
dnorm and rescaled tension fi=tension*dnorm/1000 at the
beginning of the program run. This rescaled tension should be around
20-30. If it is lower or higher, the given tension parameter
should be changed accordingly.
The default is a recommended choice, however for the applications where the user needs to change density of data and preserve the approximation character the -t flag can be helpful.
Anisotropic data (e.g. geologic phenomena) can be interpolated using theta
and scalex defining orientation
and ratio of the perpendicular axes put on the longest/shortest side of the feature, respectively.
Theta is measured in degrees from East, counterclockwise. Scalex is a ratio of axes sizes.
Setting scalex in the range 0-1, results in a pattern prolonged in the
direction defined by theta. Scalex value 0.5 means that modeled feature is approximately
2 times longer in the direction of theta than in the perpendicular direction.
Scalex value 2 means that axes ratio is reverse resulting in a pattern
perpendicular to the previous example. Please note that anisotropy
option has not been extensively tested and may include bugs (for example , topographic
parameters may not be computed correctly) - if there are
problems, please report to GRASS bugtracker
(accessible from http://grass.osgeo.org/).
For data with values changing over several magnitudes (sometimes the concentration or density data) it is suggested to interpolate the log of the values rather than the original ones.
The program checks the numerical stability of the algorithm by computing the values in given points, and prints the root mean square deviation (rms) found into the history file of raster map elev. For computation with smoothing set to 0. rms should be 0. Significant increase in tension is suggested if the rms is unexpectedly high for this case. With smoothing parameter greater than zero the surface will not pass exactly through the data points and the higher the parameter the closer the surface will be to the trend. The rms then represents a measure of smoothing effect on data. More detailed analysis of smoothing effects can be performed using the output deviations option.
Spearfish example (we simulate randomly distributed elevation measures):
g.region rast=elevation.10m -p # random elevation extraction r.random elevation.10m vector_output=elevrand n=200 v.info -c elevrand v.db.select elevrand # interpolation based on all points v.surf.rst elevrand zcol=value elev=elev_full r.colors elev_full rast=elevation.10m d.rast elev_full d.vect elevrand # interpolation based on subset of points (only those over 1300m/asl) v.surf.rst elevrand zcol=value elev=elev_partial where="value > 1300" r.colors elev_partial rast=elevation.10m d.rast elev_partial d.vect elevrand where="value > 1300"
The program writes the values of parameters used in computation into the comment part of history file elev as well as the following values which help to evaluate the results and choose the suitable parameters: minimum and maximum z values in the data file (zmin_data, zmax_data) and in the interpolated raster map (zmin_int, zmax_int), rescaling parameter used for normalization (dnorm), which influences the tension.
If visible connection of segments appears, the program should be rerun with higher npmin to get more points from the neighborhood of given segment and/or with higher tension.
When the number of points in a vector map is not too large (less than 800), the user can skip segmentation by setting segmax to the number of data points or segmax=700.
The program gives warning when user wants to interpolate outside the rectangle given by minimum and maximum coordinates in the vector map, zoom into the area where the given data are is suggested in this case.
When a mask is used, the program takes all points in the given region for approximation, including those in the area which is masked out, to ensure proper approximation along the border of the mask. It therefore does not mask out the data points, if this is desirable, it must be done outside v.surf.rst.
For examples of applications see GRASS4 implementation and GRASS5 and GRASS6 implementation.
The user must run g.region before the program to set the region and resolution for approximation.
Original version of program (in FORTRAN) and GRASS enhancements:
Lubos Mitas, NCSA, University of Illinois at Urbana Champaign, Illinois,
USA (1990-2000); Department of Physics, North Carolina State University, Raleigh
Helena Mitasova, USA CERL, Department of Geography, University of Illinois at
Urbana-Champaign, USA (1990-2001); MEAS, North Carolina State University, Raleigh
Modified program (translated to C, adapted for GRASS, new segmentation
procedure):
Irina Kosinovsky, US Army CERL, Dave Gerdes, US Army CERL
Modifications for new sites format and timestamping:
Darrel McCauley, Purdue University, Bill Brown, US Army CERL
Update for GRASS5.7, GRASS6 and addition of crossvalidation: Jaroslav Hofierka, University of Presov; Radim Blazek, ITC-irst
Mitasova, H., Mitas, L. and Harmon, R.S., 2005, Simultaneous spline approximation and topographic analysis for lidar elevation data in open source GIS, IEEE GRSL 2 (4), 375- 379.
Hofierka, J., 2005, Interpolation of Radioactivity Data Using Regularized Spline with Tension. Applied GIS, Vol. 1, No. 2, pp. 16-01 to 16-13. DOI: 10.2104/ag050016
Hofierka J., Parajka J., Mitasova H., Mitas L., 2002, Multivariate Interpolation of Precipitation Using Regularized Spline with Tension. Transactions in GIS 6(2), pp. 135-150.
H. Mitasova, L. Mitas, B.M. Brown, D.P. Gerdes, I. Kosinovsky, 1995, Modeling spatially and temporally distributed phenomena: New methods and tools for GRASS GIS. International Journal of GIS, 9 (4), special issue on Integrating GIS and Environmental modeling, 433-446.
Mitasova, H. and Mitas, L., 1993: Interpolation by Regularized Spline with Tension: I. Theory and Implementation, Mathematical Geology ,25, 641-655.
Mitasova, H. and Hofierka, J., 1993: Interpolation by Regularized Spline with Tension: II. Application to Terrain Modeling and Surface Geometry Analysis, Mathematical Geology 25, 657-667.
Mitas, L., and Mitasova H., 1988, General variational approach to the approximation problem, Computers and Mathematics with Applications, v.16, p. 983-992.
Neteler, M. and Mitasova, H., 2008, Open Source GIS: A GRASS GIS Approach, 3rd Edition, Springer, New York, 406 pages.
Talmi, A. and Gilat, G., 1977 : Method for Smooth Approximation of Data, Journal of Computational Physics, 23, p.93-123.
Wahba, G., 1990, : Spline Models for Observational Data, CNMS-NSF Regional Conference series in applied mathematics, 59, SIAM, Philadelphia, Pennsylvania.
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