Overview

This is an R Markdown Notebook to illustrate how to develop pixel-scale spectra-trait PLSR models. This example uses image data from NEON AOP and associated field measurements of leaf nitrogen content collected across a range of CONUS NEON sites. For more information refer to the dataset EcoSIS page: https://ecosis.org/package/canopy-spectra-to-map-foliar-functional-traits-over-neon-domains-in-eastern-united-states

Getting Started

Load libraries

list.of.packages <- c("pls","dplyr","here","plotrix","ggplot2","gridExtra","spectratrait")
invisible(lapply(list.of.packages, library, character.only = TRUE))

Setup other functions and options

### Setup other functions and options
# not in
`%notin%` <- Negate(`%in%`)

# Script options
pls::pls.options(plsralg = "oscorespls")
pls::pls.options("plsralg")
$plsralg
[1] "oscorespls"
# Default par options
opar <- par(no.readonly = T)

# What is the target variable? What is the variable name in the input dataset?
inVar <- "Nitrogen"

# What is the source dataset from EcoSIS?
ecosis_id <- "b9dbf3db-5b9c-4ab2-88c2-26c8b39d0903"

# Specify output directory, output_dir 
# Options: 
# tempdir - use a OS-specified temporary directory 
# user defined PATH - e.g. "~/scratch/PLSR"
output_dir <- "tempdir"

Set working directory (scratch space)

The working directory was changed to /private/var/folders/xp/h3k9vf3n2jx181ts786_yjrn9c2gjq/T/RtmpCUhr0h inside a notebook chunk. The working directory will be reset when the chunk is finished running. Use the knitr root.dir option in the setup chunk to change the working directory for notebook chunks.
[1] "/private/var/folders/xp/h3k9vf3n2jx181ts786_yjrn9c2gjq/T/RtmpCUhr0h"

Grab data from EcoSIS

print(paste0("Output directory: ",getwd()))  # check wd
[1] "Output directory: /Users/sserbin/Data/GitHub/spectratrait/vignettes"
dat_raw <- spectratrait::get_ecosis_data(ecosis_id = ecosis_id)
[1] "**** Downloading Ecosis data ****"
Downloading data...

── Column specification ────────────────────────────────────────────────────────────────────────────────────────────────────────
cols(
  .default = col_double(),
  Affiliation = col_character(),
  PI = col_character(),
  Plot_ID = col_character(),
  Project = col_character()
)
ℹ Use `spec()` for the full column specifications.

Download complete!
head(dat_raw)
names(dat_raw)[1:40]
 [1] "Affiliation"       "Boron"             "Calcium"           "Carbon"            "Carotenoids_area"  "Carotenoids_mass" 
 [7] "Cellulose"         "Chlorophylls_area" "Chlorophylls_mass" "Copper"            "EWT"               "Fiber"            
[13] "Flavonoids"        "LMA"               "Lignin"            "Magnesium"         "Manganese"         "NSC"              
[19] "Nitrogen"          "PI"                "Phenolics"         "Phosphorus"        "Plot_ID"           "Potassium"        
[25] "Project"           "SLA"               "Sample_Year"       "Starch"            "Sugar"             "Sulfur"           
[31] "Water"             "d13C"              "d15N"              "384"               "389"               "394"              
[37] "399"               "404"               "409"               "414"              

Create full plsr dataset

# identify the trait data and other metadata
sample_info <- dat_raw[,names(dat_raw) %notin% seq(300,2600,1)]
head(sample_info)

# spectra matrix
Spectra <- as.matrix(dat_raw[,names(dat_raw) %notin% names(sample_info)])

# set the desired spectra wavelength range to include
Start.wave <- 500
End.wave <- 2400
wv <- seq(Start.wave,End.wave,1)
final_spec <- Spectra[,round(as.numeric(colnames(Spectra))) %in% wv]
colnames(final_spec) <- c(paste0("Wave_",colnames(final_spec)))

## Drop bad spectra data - for canopy-scale reflectance, often the "water band" wavelengths
## are too noisy to use for trait estimation.  Its possible to remove these wavelengths
## prior to model fitting. Its best to first identify which wavelengths to drop
## before attempting PLSR, as these ranges may need to be considered on a case-by-case 
## basis or generalized for multiple datasets
dropwaves <- c(1350:1440, 1826:1946)
final_spec <- final_spec[,colnames(final_spec) %notin% paste0("Wave_",dropwaves)]
wv <- as.numeric(gsub(pattern = "Wave_",replacement = "", x = colnames(final_spec)))

## Drop bad spectra data - for canopy-scale reflectance, often the "water band" wavelengths
## are too noisy to use for trait estimation.  Its possible to remove these wavelengths
## prior to model fitting. Its best to first identify which wavelengths to drop
## before attempting PLSR, as these ranges may need to be considered on a case-by-case 
## basis or generalized for multiple datasets
dropwaves <- c(1350:1440, 1826:1946)
final_spec <- final_spec[,colnames(final_spec) %notin% paste0("Wave_",dropwaves)]
wv <- as.numeric(gsub(pattern = "Wave_",replacement = "", x = colnames(final_spec)))

# assemble example dataset
sample_info2 <- sample_info %>%
  select(Plot_ID,Sample_Year,SLA,Nitrogen)
site_plot <- data.frame(matrix(unlist(strsplit(sample_info2$Plot_ID, "_")), 
                               ncol=2, byrow=TRUE))
colnames(site_plot) <- c("Plot_Num","SampleID")
sample_info3 <- data.frame(site_plot,sample_info2)

plsr_data <- data.frame(sample_info3,final_spec*0.01)
rm(sample_info,sample_info2,sample_info3,Spectra, site_plot)

Example data cleaning.

# Example data cleaning.  End user needs to do what's appropriate for their 
# data. This may be an iterative process.
# Keep only complete rows of inVar and spec data before fitting
#
plsr_data <- plsr_data %>%  # remove erroneously high values, or "bad spectra"
  filter(Nitrogen<50) %>%
  filter(Wave_859<80) %>%
  filter(Wave_859>15)
plsr_data <- plsr_data[complete.cases(plsr_data[,names(plsr_data) %in% 
                                                  c(inVar,paste0("Wave_",wv))]),]

Create cal/val datasets

## Make a stratified random sampling in the strata USDA_Species_Code and Domain

method <- "base" #base/dplyr
# base R - a bit slow
# dplyr - much faster
split_data <- spectratrait::create_data_split(dataset=plsr_data, approach=method, split_seed=2356326,
                                              prop=0.8, group_variables="Plot_Num")
D02   Cal: 80.46%
D03   Cal: 80.328%
D05   Cal: 80%
D06   Cal: 79.73%
D07   Cal: 79.245%
D08   Cal: 79.817%
D09   Cal: 79.63%
names(split_data)
[1] "cal_data" "val_data"
cal.plsr.data <- split_data$cal_data
head(cal.plsr.data)[1:8]
val.plsr.data <- split_data$val_data
head(val.plsr.data)[1:8]
rm(split_data)

# Datasets:
print(paste("Cal observations: ",dim(cal.plsr.data)[1],sep=""))
[1] "Cal observations: 517"
print(paste("Val observations: ",dim(val.plsr.data)[1],sep=""))
[1] "Val observations: 130"
cal_hist_plot <- qplot(cal.plsr.data[,paste0(inVar)],geom="histogram",
                       main = paste0("Cal. Histogram for ",inVar),
                       xlab = paste0(inVar),ylab = "Count",fill=I("grey50"),col=I("black"),
                       alpha=I(.7))
val_hist_plot <- qplot(val.plsr.data[,paste0(inVar)],geom="histogram",
                       main = paste0("Val. Histogram for ",inVar),
                       xlab = paste0(inVar),ylab = "Count",fill=I("grey50"),col=I("black"),
                       alpha=I(.7))
histograms <- grid.arrange(cal_hist_plot, val_hist_plot, ncol=2)

ggsave(filename = file.path(outdir,paste0(inVar,"_Cal_Val_Histograms.png")), plot = histograms, 
       device="png", width = 30, 
       height = 12, units = "cm",
       dpi = 300)
# output cal/val data
write.csv(cal.plsr.data,file=file.path(outdir,paste0(inVar,'_Cal_PLSR_Dataset.csv')),
          row.names=FALSE)
write.csv(val.plsr.data,file=file.path(outdir,paste0(inVar,'_Val_PLSR_Dataset.csv')),
          row.names=FALSE)

Create calibration and validation PLSR datasets

cal_spec <- as.matrix(cal.plsr.data[, which(names(cal.plsr.data) %in% paste0("Wave_",wv))])
cal.plsr.data <- data.frame(cal.plsr.data[, which(names(cal.plsr.data) %notin% paste0("Wave_",wv))],
                            Spectra=I(cal_spec))
head(cal.plsr.data)[1:5]

val_spec <- as.matrix(val.plsr.data[, which(names(val.plsr.data) %in% paste0("Wave_",wv))])
val.plsr.data <- data.frame(val.plsr.data[, which(names(val.plsr.data) %notin% paste0("Wave_",wv))],
                            Spectra=I(val_spec))
head(val.plsr.data)[1:5]

plot cal and val spectra

par(mfrow=c(1,2)) # B, L, T, R
spectratrait::f.plot.spec(Z=cal.plsr.data$Spectra,wv=wv,plot_label="Calibration")
spectratrait::f.plot.spec(Z=val.plsr.data$Spectra,wv=wv,plot_label="Validation")

dev.copy(png,file.path(outdir,paste0(inVar,'_Cal_Val_Spectra.png')), 
         height=2500,width=4900, res=340)
quartz_off_screen 
                3 
dev.off();
quartz_off_screen 
                2 
par(mfrow=c(1,1))

Use permutation to determine optimal number of components

if(grepl("Windows", sessionInfo()$running)){
  pls.options(parallel = NULL)
} else {
  pls.options(parallel = parallel::detectCores()-1)
}

method <- "pls" #pls, firstPlateau, firstMin
random_seed <- 1245565
seg <- 50
maxComps <- 16
iterations <- 80
prop <- 0.70
if (method=="pls") {
  # pls package approach - faster but estimates more components....
  nComps <- spectratrait::find_optimal_components(dataset=cal.plsr.data, targetVariable=inVar,
                                                  method=method, 
                                                  maxComps=maxComps, seg=seg, 
                                                  random_seed=random_seed)
  print(paste0("*** Optimal number of components: ", nComps))
} else {
  nComps <- spectratrait::find_optimal_components(dataset=cal.plsr.data, targetVariable=inVar,
                                                  method=method, 
                                                  maxComps=maxComps, iterations=iterations, 
                                                  seg=seg, prop=prop, 
                                                  random_seed=random_seed)
}
[1] "*** Identifying optimal number of PLSR components ***"
[1] "*** Running PLS permutation test ***"
[1] "*** Optimal number of components: 12"
dev.copy(png,file.path(outdir,paste0(paste0(inVar,"_PLSR_Component_Selection.png"))), 
         height=2800, width=3400,  res=340)
quartz_off_screen 
                3 
dev.off();
quartz_off_screen 
                2 

Fit final model

plsr.out <- plsr(as.formula(paste(inVar,"~","Spectra")),scale=FALSE,ncomp=nComps,validation="LOO",
                 trace=FALSE,data=cal.plsr.data)
fit <- plsr.out$fitted.values[,1,nComps]
pls.options(parallel = NULL)

# External validation fit stats
par(mfrow=c(1,2)) # B, L, T, R
pls::RMSEP(plsr.out, newdata = val.plsr.data)
(Intercept)      1 comps      2 comps      3 comps      4 comps      5 comps      6 comps      7 comps      8 comps  
      6.538        5.984        5.792        5.662        5.284        5.235        5.149        5.252        5.121  
    9 comps     10 comps     11 comps     12 comps  
      4.896        4.855        4.755        4.646  
plot(pls::RMSEP(plsr.out,estimate=c("test"),newdata = val.plsr.data), main="MODEL RMSEP",
     xlab="Number of Components",ylab="Model Validation RMSEP",lty=1,col="black",cex=1.5,lwd=2)
box(lwd=2.2)

R2(plsr.out, newdata = val.plsr.data)
(Intercept)      1 comps      2 comps      3 comps      4 comps      5 comps      6 comps      7 comps      8 comps  
 -0.0001616    0.1621284    0.2150431    0.2498762    0.3467097    0.3586424    0.3796062    0.3544358    0.3863604  
    9 comps     10 comps     11 comps     12 comps  
  0.4391471    0.4484252    0.4708911    0.4948347  
plot(pls::R2(plsr.out,estimate=c("test"),newdata = val.plsr.data), main="MODEL R2",
     xlab="Number of Components",ylab="Model Validation R2",lty=1,col="black",cex=1.5,lwd=2)
box(lwd=2.2)
dev.copy(png,file.path(outdir,paste0(paste0(inVar,"_Validation_RMSEP_R2_by_Component.png"))), 
         height=2800, width=4800,  res=340)
quartz_off_screen 
                3 
dev.off();
quartz_off_screen 
                2 
par(opar)

PLSR fit observed vs. predicted plot data

#calibration
cal.plsr.output <- data.frame(cal.plsr.data[, which(names(cal.plsr.data) %notin% "Spectra")], 
                              PLSR_Predicted=fit,
                              PLSR_CV_Predicted=as.vector(plsr.out$validation$pred[,,nComps]))
cal.plsr.output <- cal.plsr.output %>%
  mutate(PLSR_CV_Residuals = PLSR_CV_Predicted-get(inVar))
head(cal.plsr.output)
cal.R2 <- round(pls::R2(plsr.out,intercept=F)[[1]][nComps],2)
cal.RMSEP <- round(sqrt(mean(cal.plsr.output$PLSR_CV_Residuals^2)),2)

val.plsr.output <- data.frame(val.plsr.data[, which(names(val.plsr.data) %notin% "Spectra")],
                              PLSR_Predicted=as.vector(predict(plsr.out, 
                                                               newdata = val.plsr.data, 
                                                               ncomp=nComps, type="response")[,,1]))
val.plsr.output <- val.plsr.output %>%
  mutate(PLSR_Residuals = PLSR_Predicted-get(inVar))
head(val.plsr.output)
val.R2 <- round(pls::R2(plsr.out,newdata=val.plsr.data,intercept=F)[[1]][nComps],2)
val.RMSEP <- round(sqrt(mean(val.plsr.output$PLSR_Residuals^2)),2)

rng_quant <- quantile(cal.plsr.output[,inVar], probs = c(0.001, 0.999))
cal_scatter_plot <- ggplot(cal.plsr.output, aes(x=PLSR_CV_Predicted, y=get(inVar))) + 
  theme_bw() + geom_point() + geom_abline(intercept = 0, slope = 1, color="dark grey", 
                                          linetype="dashed", size=1.5) + xlim(rng_quant[1], 
                                                                              rng_quant[2]) + 
  ylim(rng_quant[1], rng_quant[2]) +
  labs(x=paste0("Predicted ", paste(inVar), " (units)"),
       y=paste0("Observed ", paste(inVar), " (units)"),
       title=paste0("Calibration: ", paste0("Rsq = ", cal.R2), "; ", paste0("RMSEP = ", 
                                                                            cal.RMSEP))) +
  theme(axis.text=element_text(size=18), legend.position="none",
        axis.title=element_text(size=20, face="bold"), 
        axis.text.x = element_text(angle = 0,vjust = 0.5),
        panel.border = element_rect(linetype = "solid", fill = NA, size=1.5))

cal_resid_histogram <- ggplot(cal.plsr.output, aes(x=PLSR_CV_Residuals)) +
  geom_histogram(alpha=.5, position="identity") + 
  geom_vline(xintercept = 0, color="black", 
             linetype="dashed", size=1) + theme_bw() + 
  theme(axis.text=element_text(size=18), legend.position="none",
        axis.title=element_text(size=20, face="bold"), 
        axis.text.x = element_text(angle = 0,vjust = 0.5),
        panel.border = element_rect(linetype = "solid", fill = NA, size=1.5))

rng_quant <- quantile(val.plsr.output[,inVar], probs = c(0.001, 0.999))
val_scatter_plot <- ggplot(val.plsr.output, aes(x=PLSR_Predicted, y=get(inVar))) + 
  theme_bw() + geom_point() + geom_abline(intercept = 0, slope = 1, color="dark grey", 
                                          linetype="dashed", size=1.5) + xlim(rng_quant[1], 
                                                                              rng_quant[2]) + 
  ylim(rng_quant[1], rng_quant[2]) +
  labs(x=paste0("Predicted ", paste(inVar), " (units)"),
       y=paste0("Observed ", paste(inVar), " (units)"),
       title=paste0("Validation: ", paste0("Rsq = ", val.R2), "; ", paste0("RMSEP = ", 
                                                                           val.RMSEP))) +
  theme(axis.text=element_text(size=18), legend.position="none",
        axis.title=element_text(size=20, face="bold"), 
        axis.text.x = element_text(angle = 0,vjust = 0.5),
        panel.border = element_rect(linetype = "solid", fill = NA, size=1.5))

val_resid_histogram <- ggplot(val.plsr.output, aes(x=PLSR_Residuals)) +
  geom_histogram(alpha=.5, position="identity") + 
  geom_vline(xintercept = 0, color="black", 
             linetype="dashed", size=1) + theme_bw() + 
  theme(axis.text=element_text(size=18), legend.position="none",
        axis.title=element_text(size=20, face="bold"), 
        axis.text.x = element_text(angle = 0,vjust = 0.5),
        panel.border = element_rect(linetype = "solid", fill = NA, size=1.5))

# plot cal/val side-by-side
scatterplots <- grid.arrange(cal_scatter_plot, val_scatter_plot, cal_resid_histogram, 
                             val_resid_histogram, nrow=2,ncol=2)

ggsave(filename = file.path(outdir,paste0(inVar,"_Cal_Val_Scatterplots.png")), 
       plot = scatterplots, device="png", width = 32, height = 30, units = "cm",
       dpi = 300)

Generate Coefficient and VIP plots

vips <- spectratrait::VIP(plsr.out)[nComps,]

par(mfrow=c(2,1))
plot(plsr.out$coefficients[,,nComps], x=wv,xlab="Wavelength (nm)",
     ylab="Regression coefficients",lwd=2,type='l')
box(lwd=2.2)
plot(wv, vips, xlab="Wavelength (nm)",ylab="VIP",cex=0.01)
lines(wv, vips, lwd=3)
abline(h=0.8, lty=2, col="dark grey")
box(lwd=2.2)
dev.copy(png, file.path(outdir, paste0(inVar,'_Coefficient_VIP_plot.png')), 
         height=3100, width=4100, res=340)
quartz_off_screen 
                3 
dev.off();
quartz_off_screen 
                2 
par(opar)

Bootstrap validation

[1] "*** Running permutation test.  Please hang tight, this can take awhile ***"
[1] "Options:"
[1] "Max Components: 12 Iterations: 500 Data Proportion (percent): 70"
[1] "*** Providing PRESS and coefficient array output ***"

Jackknife coefficient plot

spectratrait::f.plot.coef(Z = t(bootstrap_coef), wv = wv, 
                          plot_label="Bootstrap regression coefficients", 
                          position = 'bottomleft')
abline(h=0,lty=2,col="grey50")
box(lwd=2.2)
dev.copy(png,file.path(outdir,paste0(inVar,'_Bootstrap_Regression_Coefficients.png')), 
         height=2100, width=3800, res=340)
quartz_off_screen 
                3 
dev.off();
quartz_off_screen 
                2 

Bootstrap validation plot

rmsep_percrmsep <- spectratrait::percent_rmse(plsr_dataset = val.plsr.output, 
                                              inVar = inVar, 
                                              residuals = val.plsr.output$PLSR_Residuals, 
                                              range="full")
RMSEP <- rmsep_percrmsep$rmse
perc_RMSEP <- rmsep_percrmsep$perc_rmse
r2 <- round(pls::R2(plsr.out, newdata = val.plsr.data, intercept=F)$val[nComps],2)
expr <- vector("expression", 3)
expr[[1]] <- bquote(R^2==.(r2))
expr[[2]] <- bquote(RMSEP==.(round(RMSEP,2)))
expr[[3]] <- bquote("%RMSEP"==.(round(perc_RMSEP,2)))
rng_vals <- c(min(val.plsr.output$LPI), max(val.plsr.output$UPI))
par(mfrow=c(1,1), mar=c(4.2,5.3,1,0.4), oma=c(0, 0.1, 0, 0.2))
plotrix::plotCI(val.plsr.output$PLSR_Predicted,val.plsr.output[,inVar], 
                li=val.plsr.output$LPI, ui=val.plsr.output$UPI, gap=0.009,sfrac=0.000, 
                lwd=1.6, xlim=c(rng_vals[1], rng_vals[2]), ylim=c(rng_vals[1], rng_vals[2]), 
                err="x", pch=21, col="black", pt.bg=scales::alpha("grey70",0.7), scol="grey80",
                cex=2, xlab=paste0("Predicted ", paste(inVar), " (units)"),
                ylab=paste0("Observed ", paste(inVar), " (units)"),
                cex.axis=1.5,cex.lab=1.8)
abline(0,1,lty=2,lw=2)
plotrix::plotCI(val.plsr.output$PLSR_Predicted,val.plsr.output[,inVar], 
                li=val.plsr.output$LCI, ui=val.plsr.output$UCI, gap=0.009,sfrac=0.004, 
                lwd=1.6, xlim=c(rng_vals[1], rng_vals[2]), ylim=c(rng_vals[1], rng_vals[2]), 
                err="x", pch=21, col="black", pt.bg=scales::alpha("grey70",0.7), scol="black",
                cex=2, xlab=paste0("Predicted ", paste(inVar), " (units)"),
                ylab=paste0("Observed ", paste(inVar), " (units)"),
                cex.axis=1.5,cex.lab=1.8, add=T)
legend("topleft", legend=expr, bty="n", cex=1.5)
legend("bottomright", legend=c("Prediction Interval","Confidence Interval"), 
       lty=c(1,1), col = c("grey80","black"), lwd=3, bty="n", cex=1.5)
box(lwd=2.2)
dev.copy(png,file.path(outdir,paste0(inVar,"_PLSR_Validation_Scatterplot.png")), 
         height=2800, width=3200,  res=340)
quartz_off_screen 
                3 
dev.off();
quartz_off_screen 
                2 

Output bootstrap results

out.jk.coefs <- data.frame(Iteration=seq(1,length(bootstrap_intercept),1),
                           Intercept=bootstrap_intercept,t(bootstrap_coef))
names(out.jk.coefs) <- c("Iteration","Intercept",paste0("Wave_",wv))
head(out.jk.coefs)[1:6]
write.csv(out.jk.coefs,file=file.path(outdir,paste0(inVar,'_Bootstrap_PLSR_Coefficients.csv')),
          row.names=FALSE)

Create core PLSR outputs

print(paste("Output directory: ", getwd()))
[1] "Output directory:  /Users/sserbin/Data/GitHub/spectratrait/vignettes"
# Observed versus predicted
write.csv(cal.plsr.output,file=file.path(outdir,
                                         paste0(inVar,'_Observed_PLSR_CV_Pred_',nComps,
                                                'comp.csv')),row.names=FALSE)

# Validation data
write.csv(val.plsr.output,file=file.path(outdir,
                                         paste0(inVar,'_Validation_PLSR_Pred_',nComps,
                                                'comp.csv')),row.names=FALSE)

# Model coefficients
coefs <- coef(plsr.out,ncomp=nComps,intercept=TRUE)
write.csv(coefs,file=file.path(outdir,paste0(inVar,'_PLSR_Coefficients_',
                                             nComps,'comp.csv')),
          row.names=TRUE)

# PLSR VIP
write.csv(vips,file=file.path(outdir,paste0(inVar,
                                            '_PLSR_VIPs_',nComps,
                                            'comp.csv')))

Confirm files were written to temp space

print("**** PLSR output files: ")
[1] "**** PLSR output files: "
print(list.files(outdir)[grep(pattern = inVar, 
                               list.files(outdir))])
 [1] "Nitrogen_Bootstrap_PLSR_Coefficients.csv"       "Nitrogen_Bootstrap_Regression_Coefficients.png"
 [3] "Nitrogen_Cal_PLSR_Dataset.csv"                  "Nitrogen_Cal_Val_Histograms.png"               
 [5] "Nitrogen_Cal_Val_Scatterplots.png"              "Nitrogen_Cal_Val_Spectra.png"                  
 [7] "Nitrogen_Coefficient_VIP_plot.png"              "Nitrogen_Observed_PLSR_CV_Pred_12comp.csv"     
 [9] "Nitrogen_PLSR_Coefficients_12comp.csv"          "Nitrogen_PLSR_Component_Selection.png"         
[11] "Nitrogen_PLSR_Validation_Scatterplot.png"       "Nitrogen_PLSR_VIPs_12comp.csv"                 
[13] "Nitrogen_Val_PLSR_Dataset.csv"                  "Nitrogen_Validation_PLSR_Pred_12comp.csv"      
[15] "Nitrogen_Validation_RMSEP_R2_by_Component.png" 
---
title: Spectra-trait PLSR example using NEON AOP pixel spectra and field-sampled leaf nitrogen content from CONUS NEON sites
author: "Shawn P. Serbin, Julien Lamour, & Jeremiah Anderson"
output:
  html_notebook: default
  pdf_document: default
  html_document:
    df_print: paged
  github_document: default
params:
  date: !r Sys.Date()
---

```{r setup, include=FALSE}
knitr::opts_chunk$set(echo = TRUE)
```

### Overview
This is an [R Markdown](http://rmarkdown.rstudio.com) Notebook to illustrate how to develop
pixel-scale spectra-trait PLSR models. This example uses image data from NEON AOP and associated field measurements of leaf nitrogen content collected across a range of CONUS NEON sites.  For more information refer to the dataset EcoSIS page:
https://ecosis.org/package/canopy-spectra-to-map-foliar-functional-traits-over-neon-domains-in-eastern-united-states

### Getting Started
### Load libraries
```{r, eval=TRUE, echo=TRUE}
list.of.packages <- c("pls","dplyr","here","plotrix","ggplot2","gridExtra","spectratrait")
invisible(lapply(list.of.packages, library, character.only = TRUE))
```

### Setup other functions and options
```{r, echo=TRUE}
### Setup other functions and options
# not in
`%notin%` <- Negate(`%in%`)

# Script options
pls::pls.options(plsralg = "oscorespls")
pls::pls.options("plsralg")

# Default par options
opar <- par(no.readonly = T)

# What is the target variable? What is the variable name in the input dataset?
inVar <- "Nitrogen"

# What is the source dataset from EcoSIS?
ecosis_id <- "b9dbf3db-5b9c-4ab2-88c2-26c8b39d0903"

# Specify output directory, output_dir 
# Options: 
# tempdir - use a OS-specified temporary directory 
# user defined PATH - e.g. "~/scratch/PLSR"
output_dir <- "tempdir"
```

### Set working directory (scratch space)
```{r, echo=FALSE}
if (output_dir=="tempdir") {
  outdir <- tempdir()
} else {
  if (! file.exists(output_dir)) dir.create(output_dir,recursive=TRUE)
  outdir <- file.path(path.expand(output_dir))
}
setwd(outdir) # set working directory
print(getwd())  # check wd
```

### Grab data from EcoSIS
```{r, echo=TRUE}
print(paste0("Output directory: ",getwd()))  # check wd
dat_raw <- spectratrait::get_ecosis_data(ecosis_id = ecosis_id)
head(dat_raw)
names(dat_raw)[1:40]
```

### Create full plsr dataset
```{r, echo=TRUE}
# identify the trait data and other metadata
sample_info <- dat_raw[,names(dat_raw) %notin% seq(300,2600,1)]
head(sample_info)

# spectra matrix
Spectra <- as.matrix(dat_raw[,names(dat_raw) %notin% names(sample_info)])

# set the desired spectra wavelength range to include
Start.wave <- 500
End.wave <- 2400
wv <- seq(Start.wave,End.wave,1)
final_spec <- Spectra[,round(as.numeric(colnames(Spectra))) %in% wv]
colnames(final_spec) <- c(paste0("Wave_",colnames(final_spec)))

## Drop bad spectra data - for canopy-scale reflectance, often the "water band" wavelengths
## are too noisy to use for trait estimation.  Its possible to remove these wavelengths
## prior to model fitting. Its best to first identify which wavelengths to drop
## before attempting PLSR, as these ranges may need to be considered on a case-by-case 
## basis or generalized for multiple datasets
dropwaves <- c(1350:1440, 1826:1946)
final_spec <- final_spec[,colnames(final_spec) %notin% paste0("Wave_",dropwaves)]
wv <- as.numeric(gsub(pattern = "Wave_",replacement = "", x = colnames(final_spec)))

## Drop bad spectra data - for canopy-scale reflectance, often the "water band" wavelengths
## are too noisy to use for trait estimation.  Its possible to remove these wavelengths
## prior to model fitting. Its best to first identify which wavelengths to drop
## before attempting PLSR, as these ranges may need to be considered on a case-by-case 
## basis or generalized for multiple datasets
dropwaves <- c(1350:1440, 1826:1946)
final_spec <- final_spec[,colnames(final_spec) %notin% paste0("Wave_",dropwaves)]
wv <- as.numeric(gsub(pattern = "Wave_",replacement = "", x = colnames(final_spec)))

# assemble example dataset
sample_info2 <- sample_info %>%
  select(Plot_ID,Sample_Year,SLA,Nitrogen)
site_plot <- data.frame(matrix(unlist(strsplit(sample_info2$Plot_ID, "_")), 
                               ncol=2, byrow=TRUE))
colnames(site_plot) <- c("Plot_Num","SampleID")
sample_info3 <- data.frame(site_plot,sample_info2)

plsr_data <- data.frame(sample_info3,final_spec*0.01)
rm(sample_info,sample_info2,sample_info3,Spectra, site_plot)
```

#### Example data cleaning.
```{r, echo=TRUE}
# Example data cleaning.  End user needs to do what's appropriate for their 
# data. This may be an iterative process.
# Keep only complete rows of inVar and spec data before fitting
#
plsr_data <- plsr_data %>%  # remove erroneously high values, or "bad spectra"
  filter(Nitrogen<50) %>%
  filter(Wave_859<80) %>%
  filter(Wave_859>15)
plsr_data <- plsr_data[complete.cases(plsr_data[,names(plsr_data) %in% 
                                                  c(inVar,paste0("Wave_",wv))]),]
```

### Create cal/val datasets
```{r, fig.height = 5, fig.width = 12, echo=TRUE}
## Make a stratified random sampling in the strata USDA_Species_Code and Domain

method <- "base" #base/dplyr
# base R - a bit slow
# dplyr - much faster
split_data <- spectratrait::create_data_split(dataset=plsr_data, approach=method, split_seed=2356326,
                                              prop=0.8, group_variables="Plot_Num")
names(split_data)
cal.plsr.data <- split_data$cal_data
head(cal.plsr.data)[1:8]
val.plsr.data <- split_data$val_data
head(val.plsr.data)[1:8]
rm(split_data)

# Datasets:
print(paste("Cal observations: ",dim(cal.plsr.data)[1],sep=""))
print(paste("Val observations: ",dim(val.plsr.data)[1],sep=""))

cal_hist_plot <- qplot(cal.plsr.data[,paste0(inVar)],geom="histogram",
                       main = paste0("Cal. Histogram for ",inVar),
                       xlab = paste0(inVar),ylab = "Count",fill=I("grey50"),col=I("black"),
                       alpha=I(.7))
val_hist_plot <- qplot(val.plsr.data[,paste0(inVar)],geom="histogram",
                       main = paste0("Val. Histogram for ",inVar),
                       xlab = paste0(inVar),ylab = "Count",fill=I("grey50"),col=I("black"),
                       alpha=I(.7))
histograms <- grid.arrange(cal_hist_plot, val_hist_plot, ncol=2)
ggsave(filename = file.path(outdir,paste0(inVar,"_Cal_Val_Histograms.png")), plot = histograms, 
       device="png", width = 30, 
       height = 12, units = "cm",
       dpi = 300)
# output cal/val data
write.csv(cal.plsr.data,file=file.path(outdir,paste0(inVar,'_Cal_PLSR_Dataset.csv')),
          row.names=FALSE)
write.csv(val.plsr.data,file=file.path(outdir,paste0(inVar,'_Val_PLSR_Dataset.csv')),
          row.names=FALSE)
```

### Create calibration and validation PLSR datasets
```{r, echo=TRUE}
cal_spec <- as.matrix(cal.plsr.data[, which(names(cal.plsr.data) %in% paste0("Wave_",wv))])
cal.plsr.data <- data.frame(cal.plsr.data[, which(names(cal.plsr.data) %notin% paste0("Wave_",wv))],
                            Spectra=I(cal_spec))
head(cal.plsr.data)[1:5]

val_spec <- as.matrix(val.plsr.data[, which(names(val.plsr.data) %in% paste0("Wave_",wv))])
val.plsr.data <- data.frame(val.plsr.data[, which(names(val.plsr.data) %notin% paste0("Wave_",wv))],
                            Spectra=I(val_spec))
head(val.plsr.data)[1:5]
```

### plot cal and val spectra
```{r, fig.height = 5, fig.width = 12, echo=TRUE}
par(mfrow=c(1,2)) # B, L, T, R
spectratrait::f.plot.spec(Z=cal.plsr.data$Spectra,wv=wv,plot_label="Calibration")
spectratrait::f.plot.spec(Z=val.plsr.data$Spectra,wv=wv,plot_label="Validation")

dev.copy(png,file.path(outdir,paste0(inVar,'_Cal_Val_Spectra.png')), 
         height=2500,width=4900, res=340)
dev.off();
par(mfrow=c(1,1))
```

### Use permutation to determine optimal number of components
```{r, fig.height = 6, fig.width = 10, echo=TRUE}
if(grepl("Windows", sessionInfo()$running)){
  pls.options(parallel = NULL)
} else {
  pls.options(parallel = parallel::detectCores()-1)
}

method <- "pls" #pls, firstPlateau, firstMin
random_seed <- 1245565
seg <- 50
maxComps <- 16
iterations <- 80
prop <- 0.70
if (method=="pls") {
  # pls package approach - faster but estimates more components....
  nComps <- spectratrait::find_optimal_components(dataset=cal.plsr.data, targetVariable=inVar,
                                                  method=method, 
                                                  maxComps=maxComps, seg=seg, 
                                                  random_seed=random_seed)
  print(paste0("*** Optimal number of components: ", nComps))
} else {
  nComps <- spectratrait::find_optimal_components(dataset=cal.plsr.data, targetVariable=inVar,
                                                  method=method, 
                                                  maxComps=maxComps, iterations=iterations, 
                                                  seg=seg, prop=prop, 
                                                  random_seed=random_seed)
}
dev.copy(png,file.path(outdir,paste0(paste0(inVar,"_PLSR_Component_Selection.png"))), 
         height=2800, width=3400,  res=340)
dev.off();
```

### Fit final model
```{r, fig.height = 5, fig.width = 12, echo=TRUE}
plsr.out <- plsr(as.formula(paste(inVar,"~","Spectra")),scale=FALSE,ncomp=nComps,validation="LOO",
                 trace=FALSE,data=cal.plsr.data)
fit <- plsr.out$fitted.values[,1,nComps]
pls.options(parallel = NULL)

# External validation fit stats
par(mfrow=c(1,2)) # B, L, T, R
pls::RMSEP(plsr.out, newdata = val.plsr.data)
plot(pls::RMSEP(plsr.out,estimate=c("test"),newdata = val.plsr.data), main="MODEL RMSEP",
     xlab="Number of Components",ylab="Model Validation RMSEP",lty=1,col="black",cex=1.5,lwd=2)
box(lwd=2.2)

R2(plsr.out, newdata = val.plsr.data)
plot(pls::R2(plsr.out,estimate=c("test"),newdata = val.plsr.data), main="MODEL R2",
     xlab="Number of Components",ylab="Model Validation R2",lty=1,col="black",cex=1.5,lwd=2)
box(lwd=2.2)
dev.copy(png,file.path(outdir,paste0(paste0(inVar,"_Validation_RMSEP_R2_by_Component.png"))), 
         height=2800, width=4800,  res=340)
dev.off();
par(opar)
```

### PLSR fit observed vs. predicted plot data
```{r, fig.height = 15, fig.width = 15, echo=TRUE} 
#calibration
cal.plsr.output <- data.frame(cal.plsr.data[, which(names(cal.plsr.data) %notin% "Spectra")], 
                              PLSR_Predicted=fit,
                              PLSR_CV_Predicted=as.vector(plsr.out$validation$pred[,,nComps]))
cal.plsr.output <- cal.plsr.output %>%
  mutate(PLSR_CV_Residuals = PLSR_CV_Predicted-get(inVar))
head(cal.plsr.output)
cal.R2 <- round(pls::R2(plsr.out,intercept=F)[[1]][nComps],2)
cal.RMSEP <- round(sqrt(mean(cal.plsr.output$PLSR_CV_Residuals^2)),2)

val.plsr.output <- data.frame(val.plsr.data[, which(names(val.plsr.data) %notin% "Spectra")],
                              PLSR_Predicted=as.vector(predict(plsr.out, 
                                                               newdata = val.plsr.data, 
                                                               ncomp=nComps, type="response")[,,1]))
val.plsr.output <- val.plsr.output %>%
  mutate(PLSR_Residuals = PLSR_Predicted-get(inVar))
head(val.plsr.output)
val.R2 <- round(pls::R2(plsr.out,newdata=val.plsr.data,intercept=F)[[1]][nComps],2)
val.RMSEP <- round(sqrt(mean(val.plsr.output$PLSR_Residuals^2)),2)

rng_quant <- quantile(cal.plsr.output[,inVar], probs = c(0.001, 0.999))
cal_scatter_plot <- ggplot(cal.plsr.output, aes(x=PLSR_CV_Predicted, y=get(inVar))) + 
  theme_bw() + geom_point() + geom_abline(intercept = 0, slope = 1, color="dark grey", 
                                          linetype="dashed", size=1.5) + xlim(rng_quant[1], 
                                                                              rng_quant[2]) + 
  ylim(rng_quant[1], rng_quant[2]) +
  labs(x=paste0("Predicted ", paste(inVar), " (units)"),
       y=paste0("Observed ", paste(inVar), " (units)"),
       title=paste0("Calibration: ", paste0("Rsq = ", cal.R2), "; ", paste0("RMSEP = ", 
                                                                            cal.RMSEP))) +
  theme(axis.text=element_text(size=18), legend.position="none",
        axis.title=element_text(size=20, face="bold"), 
        axis.text.x = element_text(angle = 0,vjust = 0.5),
        panel.border = element_rect(linetype = "solid", fill = NA, size=1.5))

cal_resid_histogram <- ggplot(cal.plsr.output, aes(x=PLSR_CV_Residuals)) +
  geom_histogram(alpha=.5, position="identity") + 
  geom_vline(xintercept = 0, color="black", 
             linetype="dashed", size=1) + theme_bw() + 
  theme(axis.text=element_text(size=18), legend.position="none",
        axis.title=element_text(size=20, face="bold"), 
        axis.text.x = element_text(angle = 0,vjust = 0.5),
        panel.border = element_rect(linetype = "solid", fill = NA, size=1.5))

rng_quant <- quantile(val.plsr.output[,inVar], probs = c(0.001, 0.999))
val_scatter_plot <- ggplot(val.plsr.output, aes(x=PLSR_Predicted, y=get(inVar))) + 
  theme_bw() + geom_point() + geom_abline(intercept = 0, slope = 1, color="dark grey", 
                                          linetype="dashed", size=1.5) + xlim(rng_quant[1], 
                                                                              rng_quant[2]) + 
  ylim(rng_quant[1], rng_quant[2]) +
  labs(x=paste0("Predicted ", paste(inVar), " (units)"),
       y=paste0("Observed ", paste(inVar), " (units)"),
       title=paste0("Validation: ", paste0("Rsq = ", val.R2), "; ", paste0("RMSEP = ", 
                                                                           val.RMSEP))) +
  theme(axis.text=element_text(size=18), legend.position="none",
        axis.title=element_text(size=20, face="bold"), 
        axis.text.x = element_text(angle = 0,vjust = 0.5),
        panel.border = element_rect(linetype = "solid", fill = NA, size=1.5))

val_resid_histogram <- ggplot(val.plsr.output, aes(x=PLSR_Residuals)) +
  geom_histogram(alpha=.5, position="identity") + 
  geom_vline(xintercept = 0, color="black", 
             linetype="dashed", size=1) + theme_bw() + 
  theme(axis.text=element_text(size=18), legend.position="none",
        axis.title=element_text(size=20, face="bold"), 
        axis.text.x = element_text(angle = 0,vjust = 0.5),
        panel.border = element_rect(linetype = "solid", fill = NA, size=1.5))

# plot cal/val side-by-side
scatterplots <- grid.arrange(cal_scatter_plot, val_scatter_plot, cal_resid_histogram, 
                             val_resid_histogram, nrow=2,ncol=2)
ggsave(filename = file.path(outdir,paste0(inVar,"_Cal_Val_Scatterplots.png")), 
       plot = scatterplots, device="png", width = 32, height = 30, units = "cm",
       dpi = 300)
```

### Generate Coefficient and VIP plots
```{r, fig.height = 9, fig.width = 10, echo=TRUE}
vips <- spectratrait::VIP(plsr.out)[nComps,]

par(mfrow=c(2,1))
plot(plsr.out$coefficients[,,nComps], x=wv,xlab="Wavelength (nm)",
     ylab="Regression coefficients",lwd=2,type='l')
box(lwd=2.2)
plot(wv, vips, xlab="Wavelength (nm)",ylab="VIP",cex=0.01)
lines(wv, vips, lwd=3)
abline(h=0.8, lty=2, col="dark grey")
box(lwd=2.2)
dev.copy(png, file.path(outdir, paste0(inVar,'_Coefficient_VIP_plot.png')), 
         height=3100, width=4100, res=340)
dev.off();
par(opar)
```

### Bootstrap validation
```{r, echo=FALSE}
if(grepl("Windows", sessionInfo()$running)){
  pls.options(parallel =NULL)
} else {
  pls.options(parallel = parallel::detectCores()-1)
}

### PLSR bootstrap permutation uncertainty analysis
iterations <- 500    # how many permutation iterations to run
prop <- 0.70          # fraction of training data to keep for each iteration
plsr_permutation <- spectratrait::pls_permutation(dataset=cal.plsr.data, targetVariable=inVar,
                                                  maxComps=nComps, 
                                                  iterations=iterations, prop=prop,
                                                  verbose = FALSE)
bootstrap_intercept <- plsr_permutation$coef_array[1,,nComps]
bootstrap_coef <- plsr_permutation$coef_array[2:length(plsr_permutation$coef_array[,1,nComps]),
                                              ,nComps]
rm(plsr_permutation)

# apply coefficients to left-out validation data
interval <- c(0.025,0.975)
Bootstrap_Pred <- val.plsr.data$Spectra %*% bootstrap_coef + 
  matrix(rep(bootstrap_intercept, length(val.plsr.data[,inVar])), byrow=TRUE, 
         ncol=length(bootstrap_intercept))
Interval_Conf <- apply(X = Bootstrap_Pred, MARGIN = 1, FUN = quantile, 
                       probs=c(interval[1], interval[2]))
sd_mean <- apply(X = Bootstrap_Pred, MARGIN = 1, FUN = sd)
sd_res <- sd(val.plsr.output$PLSR_Residuals)
sd_tot <- sqrt(sd_mean^2+sd_res^2)
val.plsr.output$LCI <- Interval_Conf[1,]
val.plsr.output$UCI <- Interval_Conf[2,]
val.plsr.output$LPI <- val.plsr.output$PLSR_Predicted-1.96*sd_tot
val.plsr.output$UPI <- val.plsr.output$PLSR_Predicted+1.96*sd_tot
head(val.plsr.output)
```

### Jackknife coefficient plot
```{r, fig.height = 6, fig.width = 10, echo=TRUE}
spectratrait::f.plot.coef(Z = t(bootstrap_coef), wv = wv, 
                          plot_label="Bootstrap regression coefficients", 
                          position = 'bottomleft')
abline(h=0,lty=2,col="grey50")
box(lwd=2.2)
dev.copy(png,file.path(outdir,paste0(inVar,'_Bootstrap_Regression_Coefficients.png')), 
         height=2100, width=3800, res=340)
dev.off();
```


### Bootstrap validation plot
```{r, fig.height = 7, fig.width = 8, echo=TRUE}
rmsep_percrmsep <- spectratrait::percent_rmse(plsr_dataset = val.plsr.output, 
                                              inVar = inVar, 
                                              residuals = val.plsr.output$PLSR_Residuals, 
                                              range="full")
RMSEP <- rmsep_percrmsep$rmse
perc_RMSEP <- rmsep_percrmsep$perc_rmse
r2 <- round(pls::R2(plsr.out, newdata = val.plsr.data, intercept=F)$val[nComps],2)
expr <- vector("expression", 3)
expr[[1]] <- bquote(R^2==.(r2))
expr[[2]] <- bquote(RMSEP==.(round(RMSEP,2)))
expr[[3]] <- bquote("%RMSEP"==.(round(perc_RMSEP,2)))
rng_vals <- c(min(val.plsr.output$LPI), max(val.plsr.output$UPI))
par(mfrow=c(1,1), mar=c(4.2,5.3,1,0.4), oma=c(0, 0.1, 0, 0.2))
plotrix::plotCI(val.plsr.output$PLSR_Predicted,val.plsr.output[,inVar], 
                li=val.plsr.output$LPI, ui=val.plsr.output$UPI, gap=0.009,sfrac=0.000, 
                lwd=1.6, xlim=c(rng_vals[1], rng_vals[2]), ylim=c(rng_vals[1], rng_vals[2]), 
                err="x", pch=21, col="black", pt.bg=scales::alpha("grey70",0.7), scol="grey80",
                cex=2, xlab=paste0("Predicted ", paste(inVar), " (units)"),
                ylab=paste0("Observed ", paste(inVar), " (units)"),
                cex.axis=1.5,cex.lab=1.8)
abline(0,1,lty=2,lw=2)
plotrix::plotCI(val.plsr.output$PLSR_Predicted,val.plsr.output[,inVar], 
                li=val.plsr.output$LCI, ui=val.plsr.output$UCI, gap=0.009,sfrac=0.004, 
                lwd=1.6, xlim=c(rng_vals[1], rng_vals[2]), ylim=c(rng_vals[1], rng_vals[2]), 
                err="x", pch=21, col="black", pt.bg=scales::alpha("grey70",0.7), scol="black",
                cex=2, xlab=paste0("Predicted ", paste(inVar), " (units)"),
                ylab=paste0("Observed ", paste(inVar), " (units)"),
                cex.axis=1.5,cex.lab=1.8, add=T)
legend("topleft", legend=expr, bty="n", cex=1.5)
legend("bottomright", legend=c("Prediction Interval","Confidence Interval"), 
       lty=c(1,1), col = c("grey80","black"), lwd=3, bty="n", cex=1.5)
box(lwd=2.2)
dev.copy(png,file.path(outdir,paste0(inVar,"_PLSR_Validation_Scatterplot.png")), 
         height=2800, width=3200,  res=340)
dev.off();
```

### Output bootstrap results
```{r, echo=TRUE}
out.jk.coefs <- data.frame(Iteration=seq(1,length(bootstrap_intercept),1),
                           Intercept=bootstrap_intercept,t(bootstrap_coef))
names(out.jk.coefs) <- c("Iteration","Intercept",paste0("Wave_",wv))
head(out.jk.coefs)[1:6]
write.csv(out.jk.coefs,file=file.path(outdir,paste0(inVar,'_Bootstrap_PLSR_Coefficients.csv')),
          row.names=FALSE)
```

### Create core PLSR outputs
```{r, echo=TRUE}
print(paste("Output directory: ", getwd()))

# Observed versus predicted
write.csv(cal.plsr.output,file=file.path(outdir,
                                         paste0(inVar,'_Observed_PLSR_CV_Pred_',nComps,
                                                'comp.csv')),row.names=FALSE)

# Validation data
write.csv(val.plsr.output,file=file.path(outdir,
                                         paste0(inVar,'_Validation_PLSR_Pred_',nComps,
                                                'comp.csv')),row.names=FALSE)

# Model coefficients
coefs <- coef(plsr.out,ncomp=nComps,intercept=TRUE)
write.csv(coefs,file=file.path(outdir,paste0(inVar,'_PLSR_Coefficients_',
                                             nComps,'comp.csv')),
          row.names=TRUE)

# PLSR VIP
write.csv(vips,file=file.path(outdir,paste0(inVar,
                                            '_PLSR_VIPs_',nComps,
                                            'comp.csv')))
```

### Confirm files were written to temp space
```{r, echo=TRUE}
print("**** PLSR output files: ")
print(list.files(outdir)[grep(pattern = inVar, 
                               list.files(outdir))])

```