Get source dataset from EcoSIS
dat_raw <- spectratrait::get_ecosis_data(ecosis_id = ecosis_id)
[1] "**** Downloading Ecosis data ****"
Downloading data...
Rows: 6312 Columns: 2162── Column specification ───────────────────────────────────────────────────────────────────────────────────────────────────────────────────────────────
Delimiter: ","
chr (10): Affiliation, Common Name, Domain, Functional_type, Latin Genus, Latin Species, PI, Project, Sample_ID, USDA Symbol
dbl (2152): LMA, 350, 351, 352, 353, 354, 355, 356, 357, 358, 359, 360, 361, 362, 363, 364, 365, 366, 367, 368, 369, 370, 371, 372, 373, 374, 375, ...
ℹ Use `spec()` to retrieve the full column specification for this data.
ℹ Specify the column types or set `show_col_types = FALSE` to quiet this message.Download complete!
head(dat_raw)
names(dat_raw)[1:40]
[1] "Affiliation" "Common Name" "Domain" "Functional_type" "LMA" "Latin Genus" "Latin Species" "PI"
[9] "Project" "Sample_ID" "USDA Symbol" "350" "351" "352" "353" "354"
[17] "355" "356" "357" "358" "359" "360" "361" "362"
[25] "363" "364" "365" "366" "367" "368" "369" "370"
[33] "371" "372" "373" "374" "375" "376" "377" "378"
Prepare new data for estimation
Start.wave <- 500
End.wave <- 2400
wv <- seq(Start.wave,End.wave,1)
Spectra <- as.matrix(dat_raw[,names(dat_raw) %in% wv])
colnames(Spectra) <- c(paste0("Wave_",wv))
head(Spectra)[1:6,1:10]
Wave_500 Wave_501 Wave_502 Wave_503 Wave_504 Wave_505 Wave_506 Wave_507 Wave_508 Wave_509
[1,] 0.044226 0.044605 0.044927 0.045473 0.046241 0.046878 0.047826 0.049090 0.050268 0.051525
[2,] 0.046855 0.047601 0.047944 0.048478 0.049381 0.050235 0.051161 0.052191 0.053322 0.054357
[3,] 0.043758 0.044171 0.044869 0.045465 0.045984 0.046933 0.047993 0.049090 0.050168 0.051441
[4,] 0.041154 0.041603 0.042088 0.042408 0.042639 0.043260 0.044140 0.045058 0.045700 0.046476
[5,] 0.037296 0.037944 0.038209 0.038677 0.039388 0.039948 0.040630 0.041501 0.042613 0.043731
[6,] 0.043878 0.044257 0.044723 0.045295 0.045949 0.046575 0.047378 0.048357 0.049392 0.050387
sample_info <- dat_raw[,names(dat_raw) %notin% seq(350,2500,1)]
head(sample_info)
sample_info2 <- sample_info %>%
select(Domain,Functional_type,Sample_ID,USDA_Species_Code=`USDA Symbol`,LMA_gDW_m2=LMA)
head(sample_info2)
plsr_data <- data.frame(sample_info2,Spectra)
rm(sample_info,sample_info2,Spectra)
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[complete.cases(plsr_data[,names(plsr_data) %in%
c(inVar,paste0("Wave_",wv))]),]
Prepare PLSR model
print("**** Applying PLSR model to estimate LMA from spectral observations ****")
[1] "**** Applying PLSR model to estimate LMA from spectral observations ****"
# setup model
dims <- dim(LeafLMA.plsr.coeffs)
LeafLMA.plsr.intercept <- LeafLMA.plsr.coeffs[1,]
LeafLMA.plsr.coeffs <- data.frame(LeafLMA.plsr.coeffs[2:dims[1],])
names(LeafLMA.plsr.coeffs) <- c("wavelength","coefs")
LeafLMA.plsr.coeffs.vec <- as.vector(LeafLMA.plsr.coeffs[,2])
sub_spec <- droplevels(plsr_data[,which(names(plsr_data) %in%
paste0("Wave_",seq(Start.wave,End.wave,1)))])
Apply PLSR model
plsr_pred <- as.matrix(sub_spec) %*% LeafLMA.plsr.coeffs.vec + LeafLMA.plsr.intercept[,2]
leafLMA <- plsr_pred[,1]^2 # convert to standard LMA units from sqrt(LMA)
names(leafLMA) <- "PLSR_LMA_gDW_m2"
# organize output
LeafLMA.PLSR.dataset <- data.frame(plsr_data[,which(names(plsr_data) %notin%
paste0("Wave_",seq(Start.wave,End.wave,1)))],
PLSR_LMA_gDW_m2=leafLMA, PLSR_Residuals=leafLMA-plsr_data[,inVar])
head(LeafLMA.PLSR.dataset)
Generate PLSR uncertainty estimates
print("**** Generate PLSR uncertainty estimates ****")
[1] "**** Generate PLSR uncertainty estimates ****"
jk_coef <- data.frame(LeafLMA.plsr.jk.coeffs[,3:dim(LeafLMA.plsr.jk.coeffs)[2]])
jk_coef <- t(jk_coef)
head(jk_coef)[,1:6]
[,1] [,2] [,3] [,4] [,5] [,6]
Wave_500 1.0005875 0.9952840 0.5652908 0.9793160 1.1052207 0.9370473
Wave_501 0.9584235 0.9631434 0.5230544 0.9330803 1.0477469 0.9042780
Wave_502 0.8960202 0.9065954 0.4597413 0.8710298 0.9658130 0.8628370
Wave_503 0.8722135 0.8936197 0.4420696 0.8456098 0.9272967 0.8513741
Wave_504 0.8452831 0.8644923 0.4159567 0.8110004 0.8903192 0.8320347
Wave_505 0.8240743 0.8378399 0.3902871 0.7829891 0.8570048 0.8150339
jk_int <- t(LeafLMA.plsr.jk.coeffs[,2])
head(jk_int)[,1:6]
[1] 7.787098 7.959443 8.015161 8.018586 7.658080 7.998432
jk_pred <- as.matrix(sub_spec) %*% jk_coef + matrix(rep(jk_int, length(plsr_data[,inVar])),
byrow=TRUE, ncol=length(jk_int))
jk_pred <- jk_pred^2
head(jk_pred)[,1:6]
[,1] [,2] [,3] [,4] [,5] [,6]
1 94.28721 96.77712 96.44452 95.11992 96.72830 95.33877
2 90.36051 90.57120 90.77562 89.77821 90.24826 89.61806
3 75.71088 77.91861 76.42730 76.11473 77.67179 76.68756
4 61.37001 61.30963 60.56606 60.72330 61.63712 60.69649
5 99.24456 101.75948 101.22916 99.96305 101.70397 100.16758
6 97.40414 97.65463 97.52687 97.00817 97.33677 96.08535
dim(jk_pred)
[1] 6312 1000
interval <- c(0.025,0.975)
Interval_Conf <- apply(X = jk_pred, MARGIN = 1, FUN = quantile,
probs=c(interval[1], interval[2]))
sd_mean <- apply(X = jk_pred, MARGIN = 1, FUN =sd)
sd_res <- sd(LeafLMA.PLSR.dataset$PLSR_Residuals)
sd_tot <- sqrt(sd_mean^2+sd_res^2)
LeafLMA.PLSR.dataset$LCI <- Interval_Conf[1,]
LeafLMA.PLSR.dataset$UCI <- Interval_Conf[2,]
LeafLMA.PLSR.dataset$LPI <- LeafLMA.PLSR.dataset$PLSR_LMA_gDW_m2-1.96*sd_tot
LeafLMA.PLSR.dataset$UPI <- LeafLMA.PLSR.dataset$PLSR_LMA_gDW_m2+1.96*sd_tot
head(LeafLMA.PLSR.dataset)
Generate PLSR estimated LMA observed vs predicted plot
rmsep_percrmsep <- spectratrait::percent_rmse(plsr_dataset = LeafLMA.PLSR.dataset,
inVar = inVar,
residuals = LeafLMA.PLSR.dataset$PLSR_Residuals,
range="full")
RMSEP <- rmsep_percrmsep$rmse
perc_RMSEP <- rmsep_percrmsep$perc_rmse
r2 <- round(summary(lm(LeafLMA.PLSR.dataset$PLSR_LMA_gDW_m2~
LeafLMA.PLSR.dataset[,inVar]))$adj.r.squared,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(LeafLMA.PLSR.dataset$LPI), max(LeafLMA.PLSR.dataset$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(LeafLMA.PLSR.dataset$PLSR_LMA_gDW_m2,LeafLMA.PLSR.dataset[,inVar],
li=LeafLMA.PLSR.dataset$LPI, ui=LeafLMA.PLSR.dataset$UPI, gap=0.009,sfrac=0.000,
lwd=1.6, xlim=c(rng_vals[1], rng_vals[2]), ylim=c(rng_vals[1], rng_vals[2]),
err="x", pch=21, col="black", pt.bg=scales::alpha("grey70",0.7), scol="grey80",
cex=2, xlab=paste0("Predicted ", paste(inVar), " (units)"),
ylab=paste0("Observed ", paste(inVar), " (units)"),
cex.axis=1.5,cex.lab=1.8)
abline(0,1,lty=2,lw=2)
plotrix::plotCI(LeafLMA.PLSR.dataset$PLSR_LMA_gDW_m2,LeafLMA.PLSR.dataset[,inVar],
li=LeafLMA.PLSR.dataset$LCI, ui=LeafLMA.PLSR.dataset$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

print(paste("Output directory: ", outdir))
[1] "Output directory: /var/folders/xp/h3k9vf3n2jx181ts786_yjrn9c2gjq/T//RtmpvH9zex"
# Observed versus predicted
write.csv(LeafLMA.PLSR.dataset,file=file.path(outdir,
paste0(inVar,'_PLSR_Estimates.csv')),
row.names=FALSE)
---
title: An example showing how to apply an existing PLSR model to new data. In this case applying the LMA model from Serbin et al., (2019; DOI - 10.1111/nph.16123) to a dataset collected at CONUS NEON field sites 
author: "Shawn P. Serbin, Julien Lamour, & Jeremiah Anderson"
date: "`r Sys.Date()`"
output:
  html_notebook: default
---

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

### Getting Started
### Load libraries
```{r, eval=TRUE, echo=TRUE}
list.of.packages <- c("pls","dplyr","reshape2","here","plotrix","ggplot2","gridExtra",
                      "spectratrait")
invisible(lapply(list.of.packages, library, character.only = TRUE))
```

### Setup other functions and options
```{r, echo=TRUE}
### Setup options

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

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

# What is the target variable?
inVar <- "LMA_gDW_m2"

# What is the source dataset from EcoSIS?
ecosis_id <- "5617da17-c925-49fb-b395-45a51291bd2d"

# 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
getwd()  # check wd
```

### Grab PLSR Coefficients from GitHub
```{r, echo=TRUE}
git_repo <- "https://raw.githubusercontent.com/serbinsh/SSerbin_etal_2019_NewPhytologist/master/"
print("**** Downloading PLSR coefficients ****")
githubURL <- paste0(git_repo,"SSerbin_multibiome_lma_plsr_model/sqrt_LMA_gDW_m2_PLSR_Coefficients_10comp.csv")
LeafLMA.plsr.coeffs <- spectratrait::source_GitHubData(githubURL)
rm(githubURL)
githubURL <- paste0(git_repo,"SSerbin_multibiome_lma_plsr_model/sqrt_LMA_gDW_m2_Jackkife_PLSR_Coefficients.csv")
LeafLMA.plsr.jk.coeffs <- spectratrait::source_GitHubData(githubURL)
rm(githubURL)
```

### Get source dataset from EcoSIS
```{r, echo=TRUE}
dat_raw <- spectratrait::get_ecosis_data(ecosis_id = ecosis_id)
head(dat_raw)
names(dat_raw)[1:40]
```

### Prepare new data for estimation
```{r, echo=TRUE}
Start.wave <- 500
End.wave <- 2400
wv <- seq(Start.wave,End.wave,1)
Spectra <- as.matrix(dat_raw[,names(dat_raw) %in% wv])
colnames(Spectra) <- c(paste0("Wave_",wv))
head(Spectra)[1:6,1:10]
sample_info <- dat_raw[,names(dat_raw) %notin% seq(350,2500,1)]
head(sample_info)

sample_info2 <- sample_info %>%
  select(Domain,Functional_type,Sample_ID,USDA_Species_Code=`USDA Symbol`,LMA_gDW_m2=LMA)
head(sample_info2)

plsr_data <- data.frame(sample_info2,Spectra)
rm(sample_info,sample_info2,Spectra)
```

#### Example data cleaning. 
```{r, echo=TRUE}
#### 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[complete.cases(plsr_data[,names(plsr_data) %in% 
                                                  c(inVar,paste0("Wave_",wv))]),]
```

#### Prepare PLSR model
```{r, echo=TRUE}
print("**** Applying PLSR model to estimate LMA from spectral observations ****")
# setup model
dims <- dim(LeafLMA.plsr.coeffs)
LeafLMA.plsr.intercept <- LeafLMA.plsr.coeffs[1,]
LeafLMA.plsr.coeffs <- data.frame(LeafLMA.plsr.coeffs[2:dims[1],])
names(LeafLMA.plsr.coeffs) <- c("wavelength","coefs")
LeafLMA.plsr.coeffs.vec <- as.vector(LeafLMA.plsr.coeffs[,2])
sub_spec <- droplevels(plsr_data[,which(names(plsr_data) %in% 
                                                   paste0("Wave_",seq(Start.wave,End.wave,1)))])
```

#### Apply PLSR model
```{r, echo=TRUE}
plsr_pred <- as.matrix(sub_spec) %*% LeafLMA.plsr.coeffs.vec + LeafLMA.plsr.intercept[,2]
leafLMA <- plsr_pred[,1]^2  # convert to standard LMA units from sqrt(LMA)
names(leafLMA) <- "PLSR_LMA_gDW_m2"

# organize output
LeafLMA.PLSR.dataset <- data.frame(plsr_data[,which(names(plsr_data) %notin% 
                                                      paste0("Wave_",seq(Start.wave,End.wave,1)))],
                                   PLSR_LMA_gDW_m2=leafLMA, PLSR_Residuals=leafLMA-plsr_data[,inVar])
head(LeafLMA.PLSR.dataset)
```

#### Generate PLSR uncertainty estimates
```{r, echo=TRUE}
print("**** Generate PLSR uncertainty estimates ****")
jk_coef <- data.frame(LeafLMA.plsr.jk.coeffs[,3:dim(LeafLMA.plsr.jk.coeffs)[2]])
jk_coef <- t(jk_coef)
head(jk_coef)[,1:6]
jk_int <- t(LeafLMA.plsr.jk.coeffs[,2])
head(jk_int)[,1:6]

jk_pred <- as.matrix(sub_spec) %*% jk_coef + matrix(rep(jk_int, length(plsr_data[,inVar])), 
                                                    byrow=TRUE, ncol=length(jk_int))
jk_pred <- jk_pred^2
head(jk_pred)[,1:6]
dim(jk_pred)
interval <- c(0.025,0.975)
Interval_Conf <- apply(X = jk_pred, MARGIN = 1, FUN = quantile, 
                       probs=c(interval[1], interval[2]))
sd_mean <- apply(X = jk_pred, MARGIN = 1, FUN =sd)
sd_res <- sd(LeafLMA.PLSR.dataset$PLSR_Residuals)
sd_tot <- sqrt(sd_mean^2+sd_res^2)
LeafLMA.PLSR.dataset$LCI <- Interval_Conf[1,]
LeafLMA.PLSR.dataset$UCI <- Interval_Conf[2,]
LeafLMA.PLSR.dataset$LPI <- LeafLMA.PLSR.dataset$PLSR_LMA_gDW_m2-1.96*sd_tot
LeafLMA.PLSR.dataset$UPI <- LeafLMA.PLSR.dataset$PLSR_LMA_gDW_m2+1.96*sd_tot
head(LeafLMA.PLSR.dataset)
```

#### Generate PLSR estimated LMA observed vs predicted plot
```{r, fig.height = 7, fig.width = 8, echo=TRUE}
rmsep_percrmsep <- spectratrait::percent_rmse(plsr_dataset = LeafLMA.PLSR.dataset, 
                                              inVar = inVar, 
                                              residuals = LeafLMA.PLSR.dataset$PLSR_Residuals, 
                                              range="full")
RMSEP <- rmsep_percrmsep$rmse
perc_RMSEP <- rmsep_percrmsep$perc_rmse
r2 <- round(summary(lm(LeafLMA.PLSR.dataset$PLSR_LMA_gDW_m2~
                         LeafLMA.PLSR.dataset[,inVar]))$adj.r.squared,2)
expr <- vector("expression", 3)
expr[[1]] <- bquote(R^2==.(r2))
expr[[2]] <- bquote(RMSEP==.(round(RMSEP,2)))
expr[[3]] <- bquote("%RMSEP"==.(round(perc_RMSEP,2)))
rng_vals <- c(min(LeafLMA.PLSR.dataset$LPI), max(LeafLMA.PLSR.dataset$UPI))
par(mfrow=c(1,1), mar=c(4.2,5.3,1,0.4), oma=c(0, 0.1, 0, 0.2))
plotrix::plotCI(LeafLMA.PLSR.dataset$PLSR_LMA_gDW_m2,LeafLMA.PLSR.dataset[,inVar], 
                li=LeafLMA.PLSR.dataset$LPI, ui=LeafLMA.PLSR.dataset$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(LeafLMA.PLSR.dataset$PLSR_LMA_gDW_m2,LeafLMA.PLSR.dataset[,inVar], 
                li=LeafLMA.PLSR.dataset$LCI, ui=LeafLMA.PLSR.dataset$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();
```
```{r, echo=TRUE}
print(paste("Output directory: ", outdir))

# Observed versus predicted
write.csv(LeafLMA.PLSR.dataset,file=file.path(outdir,
                                         paste0(inVar,'_PLSR_Estimates.csv')),
          row.names=FALSE)
```

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