Tps | R Documentation |
Fits a thin plate spline surface to irregularly spaced data. The smoothing parameter is chosen as a default by generalized cross-validation. The assumed model is additive Y = f(X) +e where f(X) is a d dimensional surface.
Tps(x, Y, m = NULL, p = NULL, scale.type = "range", lon.lat = FALSE,
miles = TRUE, method = "GCV", GCV = TRUE, ...)
fastTps(x, Y, m = NULL, p = NULL, aRange, lon.lat = FALSE,
find.trA = FALSE, REML = FALSE,theta=NULL, ...)
x |
Matrix of independent variables. Each row is a location or a set of independent covariates. |
Y |
Vector of dependent variables. |
m |
A polynomial function of degree (m-1) will be included in the model as the drift (or spatial trend) component. Default is the value such that 2m-d is greater than zero where d is the dimension of x. |
p |
Polynomial power for Wendland radial basis functions. Default is 2m-d where d is the dimension of x. |
scale.type |
The independent variables and knots are scaled to the specified scale.type. By default the scale type is "range", whereby the locations are transformed to the interval (0,1) by forming (x-min(x))/range(x) for each x. Scale type of "user" allows specification of an x.center and x.scale by the user. The default for "user" is mean 0 and standard deviation 1. Scale type of "unscaled" does not scale the data. |
aRange |
The tapering range that is passed to the Wendland compactly supported covariance. The covariance (i.e. the radial basis function) is zero beyond range aRange. The larger aRange the closer this model will approximate the standard thin plate spline. |
lon.lat |
If TRUE locations are interpreted as lognitude and
latitude and great circle distance is used to find distances among
locations. The aRange scale parameter for |
method |
Determines what "smoothing" parameter should be used. The default is to estimate standard GCV Other choices are: GCV.model, GCV.one, RMSE, pure error and REML. The differences are explained in the Krig help file. |
GCV |
If TRUE the decompositions are done to efficiently evaluate the estimate, GCV function and likelihood at multiple values of lambda. |
miles |
If TRUE great circle distances are in miles if FALSE distances are in kilometers |
find.trA |
If TRUE will estimate the effective degrees of freedom
using a simple Monte Carlo method (random trace). This will add to the
computational burden by approximately |
REML |
If TRUE find the MLE for lambda using restricted maximum likelihood instead of the full version. |
theta |
Same as aRange. |
... |
For For Arguments for Tps:
|
Overview
This is the classic nonparametric curve/surface estimate pioneered in statistics by Grace Wahba. The computational algorithm is based around a QR decomposition followed by an eigen decomposition on a reduced matrix derived from the spline radial basis functions. This insures a stable computation – basically bombproof – but is not the fastest. See the function mKrig and examples for fitting a thin plate spline using spatialProcess that uses a different linear algebra approach. This is implemented in the "fast" version albeit approximate version to exploit sparse matrices.
This function also works for just a single dimension and reproduces the well known cubic smoothing spline for m ==2
Finally we note that a thin plate spline is a limiting case of a Gaussian process estimate as the range parameter in the Matern family increases to infinity.
(Kriging).
A "fast" version of this function uses a compactly supported Wendland covariance and sparse linear algebra for handling larger datta sets. Although a good approximation to Tps for sufficiently large aRange its actual form is very different from the textbook thin-plate definition. The user will see that fastTps
is largely a wrapper for a call to spatialProcess
with the Wendland covariance function.
Background on the thin plate spline function, Tps A thin plate spline is the result of minimizing the residual sum of squares subject to a constraint that the function have a certain level of smoothness (or roughness penalty). Roughness is quantified by the integral of squared m-th order derivatives. For one dimension and m=2 the roughness penalty is the integrated square of the second derivative of the function. For two dimensions the roughness penalty is the integral of
(Dxx(f))**22 + 2(Dxy(f))**2 + (Dyy(f))**22
(where Duv denotes the second partial derivative with respect to u and v.) Besides controlling the order of the derivatives, the value of m also determines the base polynomial that is fit to the data. The degree of this polynomial is (m-1).
The smoothing parameter controls the amount that the data is smoothed. In the usual form this is denoted by lambda, the Lagrange multiplier of the minimization problem. Although this is an awkward scale, lambda = 0 corresponds to no smoothness constraints and the data is interpolated. lambda=infinity corresponds to just fitting the polynomial base model by ordinary least squares.
This estimator is implemented by passing the right generalized covariance function based on radial basis functions to the more general function Krig. One advantage of this implementation is that once a Tps/Krig object is created the estimator can be found rapidly for other data and smoothing parameters provided the locations remain unchanged. This makes simulation within R efficient (see example below). Tps does not currently support the knots argument where one can use a reduced set of basis functions. This is mainly to simplify the code and a good alternative using knots would be to use a valid covariance from the Matern family and a large range parameter.
Using a great circle distance function
The option to use great circle distance
to define the radial basis functions (lon.lat=TRUE
) is very useful
for small geographic domains where the spherical geometry is well approximated by a plane. However, for large domains the spherical distortion be large enough that the radial basis functions no longer define a positive definite system and Tps will report a numerical error. An alternative is to switch to a three
dimensional thin plate spline with the locations being the direction cosines. This will
give approximate great circle distances for locations that are close and also the numerical methods will always have a positive definite matrices. There are other radial basis functions that are specific to a spherical geometry but these are not implemented in fields.
Here is an example using this idea for RMprecip
and also some
examples of building grids and evaluating the Tps results on them:
# a useful function: dircos<- function(x1){ coslat1 <- cos((x1[, 2] * pi)/180) sinlat1 <- sin((x1[, 2] * pi)/180) coslon1 <- cos((x1[, 1] * pi)/180) sinlon1 <- sin((x1[, 1] * pi)/180) cbind(coslon1*coslat1, sinlon1*coslat1, sinlat1)} # fit in 3-d to direction cosines out<- Tps(dircos(RMprecip$x),RMprecip$y) xg<-make.surface.grid(fields.x.to.grid(RMprecip$x)) fhat<- predict( out, dircos(xg)) # coerce to image format from prediction vector and grid points. out.p<- as.surface( xg, fhat) surface( out.p) # compare to the automatic out0<- Tps(RMprecip$x,RMprecip$y, lon.lat=TRUE) surface(out0)
The function fastTps
is really a convenient wrapper function that
calls spatialProcess
with a suitable Wendland covariance
function. This means one can use all the additional functions for
prediction and simulation built for the spatialProcess
and
mKrig
objects. Some care needs to exercised in specifying
the support aRange
– a Goldilocks problem – where aRange
is large enough so that every location has a reasonable number
(say 10 or more ) of neighboring locations that have non-zero
covariances but also the number of neighbors is not so large that
the sparsity of the covariance matrix is compromised.
To figure out the neighborhood pattern are the spatial locations one can use the function nearest.dist
, sparse matrix format, and table
function.
set.seed(222) s<- cbind( runif(1e4),runif(1e4)) look<- nearest.dist(s,s, delta = .03) look<- spam2spind(look) stats( table( look$ind[,1]))
Here one has asummary of the number of nearest neighbors within a distance of .03 for these (randomly generated) locations. I see a minimum of 7 for at least one location so aRange should be larger than .03. Trial and error with different deltas can lead to a better choice.
Note that unlike Tps the locations are not
scaled to unit range and this can cause havoc in smoothing problems with
variables in very different units.
So rescaling the locations x<- scale(x)
is a good idea for putting the variables on a common scale
for smoothing. A conservative rule of thumb is to make aRange
large enough so that about 50 nearest neighbors are within this distance
for every observation location.
This function does have the potential to approximate estimates of Tps
for very large spatial data sets. See wendland.cov
and help on
the SPAM package, and the friendly spind format for more background.
Also, the function predictSurface.fastTps
has been made more
efficient for the
case of k=2 and m=2 – a common choice for parameters.
A list of class Krig. This includes the fitted values, the predicted surface evaluated at the observation locations, and the residuals. The results of the grid search minimizing the generalized cross validation function are returned in gcv.grid. Note that the GCV/REML optimization is done even if lambda or df is given. Please see the documentation on Krig for details of the returned arguments.
See "Nonparametric Regression and Generalized Linear Models"
by Green and Silverman. See "Additive Models" by Hastie and Tibshirani.
See Wahba, Grace. "Spline models for observational data." Society for industrial and applied mathematics, 1990.
Krig
,
mKrig
,
spatialProcess
,
Tps.cov
sim.spatialProcess
,
summary.Krig
,
predict.Krig
,
predictSE.Krig
,
predictSurface
,
predictSurface.fastTps
,
plot.Krig
,
surface.Krig
,
sreg
#2-d example
data(ozone2)
x<- ozone2$lon.lat
y<- ozone2$y[16,]
fit<- Tps(x,y) # fits a surface to ozone measurements.
set.panel(2,2)
plot(fit) # four diagnostic plots of fit and residuals.
set.panel()
# summary of fit and estiamtes of lambda the smoothing parameter
summary(fit)
surface( fit) # Quick image/contour plot of GCV surface.
# NOTE: the predict function is quite flexible:
look<- predict( fit, lambda=2.0)
# evaluates the estimate at lambda =2.0 _not_ the GCV estimate
# it does so very efficiently from the Krig fit object.
look<- predict( fit, df=7.5)
# evaluates the estimate at the lambda values such that
# the effective degrees of freedom is 7.5
# compare this to fitting a thin plate spline with
# lambda chosen so that there are 7.5 effective
# degrees of freedom in estimate
# Note that the GCV function is still computed and minimized
# but the lambda values used correpsonds to 7.5 df.
fit1<- Tps(x, y,df=7.5)
set.panel(2,2)
plot(fit1) # four diagnostic plots of fit and residuals.
# GCV function (lower left) has vertical line at 7.5 df.
set.panel()
# The basic matrix decompositions are the same for
# both fit and fit1 objects.
# predict( fit1) is the same as predict( fit, df=7.5)
# predict( fit1, lambda= fit$lambda) is the same as predict(fit)
# predict onto a grid that matches the ranges of the data.
out.p<-predictSurface( fit)
imagePlot( out.p)
# the surface function (e.g. surface( fit)) essentially combines
# the two steps above
# predict at different effective
# number of parameters
out.p<-predictSurface( fit, df=10)
## Not run:
# predicting on a grid along with a covariate
data( COmonthlyMet)
# predicting average daily minimum temps for spring in Colorado
# NOTE to create an 4km elevation grid:
# data(PRISMelevation); CO.elev1 <- crop.image(PRISMelevation, CO.loc )
# then use same grid for the predictions: CO.Grid1<- CO.elev1[c("x","y")]
obj<- Tps( CO.loc, CO.tmin.MAM.climate, Z= CO.elev)
out.p<-predictSurface( obj,
CO.Grid, ZGrid= CO.elevGrid)
imagePlot( out.p)
US(add=TRUE, col="grey")
contour( CO.elevGrid, add=TRUE, levels=c(2000), col="black")
## End(Not run)
## Not run:
#A 1-d example with confidence intervals
out<-Tps( rat.diet$t, rat.diet$trt) # lambda found by GCV
out
plot( out$x, out$y)
xgrid<- seq( min( out$x), max( out$x),,100)
fhat<- predict( out,xgrid)
lines( xgrid, fhat,)
SE<- predictSE( out, xgrid)
lines( xgrid,fhat + 1.96* SE, col="red", lty=2)
lines(xgrid, fhat - 1.96*SE, col="red", lty=2)
#
# compare to the ( much faster) B spline algorithm
# sreg(rat.diet$t, rat.diet$trt)
# Here is a 1-d example with 95 percent CIs where sreg would not
# work:
# sreg would give the right estimate here but not the right CI's
x<- seq( 0,1,,8)
y<- sin(3*x)
out<-Tps( x, y) # lambda found by GCV
plot( out$x, out$y)
xgrid<- seq( min( out$x), max( out$x),,100)
fhat<- predict( out,xgrid)
lines( xgrid, fhat, lwd=2)
SE<- predictSE( out, xgrid)
lines( xgrid,fhat + 1.96* SE, col="red", lty=2)
lines(xgrid, fhat - 1.96*SE, col="red", lty=2)
## End(Not run)
# More involved example adding a covariate to the fixed part of model
## Not run:
set.panel( 1,3)
# without elevation covariate
out0<-Tps( RMprecip$x,RMprecip$y)
surface( out0)
US( add=TRUE, col="grey")
# with elevation covariate
out<- Tps( RMprecip$x,RMprecip$y, Z=RMprecip$elev)
# NOTE: out$d[4] is the estimated elevation coefficient
# it is easy to get the smooth surface separate from the elevation.
out.p<-predictSurface( out, drop.Z=TRUE)
surface( out.p)
US( add=TRUE, col="grey")
# and if the estimate is of high resolution and you get by with
# a simple discretizing -- does not work in this case!
quilt.plot( out$x, out$fitted.values)
#
# the exact way to do this is evaluate the estimate
# on a grid where you also have elevations
# An elevation DEM from the PRISM climate data product (4km resolution)
data(RMelevation)
grid.list<- list( x=RMelevation$x, y= RMelevation$y)
fit.full<- predictSurface( out, grid.list, ZGrid= RMelevation)
# this is the linear fixed part of the second spatial model:
# lon,lat and elevation
fit.fixed<- predictSurface( out, grid.list, just.fixed=TRUE,
ZGrid= RMelevation)
# This is the smooth part but also with the linear lon lat terms.
fit.smooth<-predictSurface( out, grid.list, drop.Z=TRUE)
#
set.panel( 3,1)
fit0<- predictSurface( out0, grid.list)
image.plot( fit0)
title(" first spatial model (w/o elevation)")
image.plot( fit.fixed)
title(" fixed part of second model (lon,lat,elev linear model)")
US( add=TRUE)
image.plot( fit.full)
title("full prediction second model")
set.panel()
## End(Not run)
###
### fast Tps
# m=2 p= 2m-d= 2
#
# Note: aRange = 3 degrees is a very generous taper range.
# Use some trial aRange value with rdist.nearest to determine a
# a useful taper. Some empirical studies suggest that in the
# interpolation case in 2 d the taper should be large enough to
# about 20 non zero nearest neighbors for every location.
out2<- fastTps( RMprecip$x,RMprecip$y,m=2, aRange=3.0,
profileLambda=FALSE)
# note that fastTps produces a object of classes spatialProcess and mKrig
# so one can use all the
# the overloaded functions that are defined for these classes.
# predict, predictSE, plot, sim.spatialProcess
# summary of what happened note estimate of effective degrees of
# freedom
# profiling on lambda has been turned off to make this run quickly
# but it is suggested that one examines the the profile likelihood over lambda
print( out2)
## Not run:
set.panel( 1,2)
surface( out2)
#
# now use great circle distance for this smooth
# Here "aRange" for the taper support is the great circle distance in degrees latitude.
# Typically for data analysis it more convenient to think in degrees. A degree of
# latitude is about 68 miles (111 km).
#
fastTps( RMprecip$x,RMprecip$y,m=2, lon.lat=TRUE, aRange= 210 ) -> out3
print( out3) # note the effective degrees of freedom is different.
surface(out3)
set.panel()
## End(Not run)
## Not run:
#
# simulation reusing Tps/Krig object
#
fit<- Tps( rat.diet$t, rat.diet$trt)
true<- fit$fitted.values
N<- length( fit$y)
temp<- matrix( NA, ncol=50, nrow=N)
tau<- fit$tauHat.GCV
for ( k in 1:50){
ysim<- true + tau* rnorm(N)
temp[,k]<- predict(fit, y= ysim)
}
matplot( fit$x, temp, type="l")
## End(Not run)
#
#4-d example
fit<- Tps(BD[,1:4],BD$lnya,scale.type="range")
# plots fitted surface and contours
# default is to hold 3rd and 4th fixed at median values
surface(fit)
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