# Surface Renewal Analysis for Energy Flux Exchanges in an Ecosystem: 1: Calculating Ramp Characteristics using R.

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**Summary**: The application of Surface Renewal (SR) analysis as an alternative to energy and gaseous flux measurements using eddy covariance has gained prominence as a less costly and reliable method. The R code provided in this post is the first of two posts. In this first post R programming language is applied to calculate ramp characteristics; namely: ramp amplitude (A) and ramp duration (τ). A sample dataset is provided to demonstrate the functionality of the code.

**INTRODUCTION**The surface energy balance equation explains the net solar radiation from the sun to and from the earth’s surface and is comprised of three important elements namely: latent heat (LE), sensible heat (H) and ground heat flux (G). LE is the latent heat flux that results from both evapotranspiration from the soil and vegetation. Sensible heat warms the layer above the surface while ground flux is associated with heat stored in the soil or pedozone. The sum of these 3 components totals the radiative flux which is a combination of both longwave and shortwave radiation energy. Quantification of these components within a watershed or field, assists scientific understanding of plant development, precipitation and water demands by competing users. There are several micrometeorological methods available to measure these components both directly and indirectly. The eddy covariance (EC) method utilizes an omnidirectional 3D sonic anemometer as well as either an open or closed-path infrared H

_{2}O gas analyzing system to measure LE. Solar radiation can be measured using radiometers. Soil heat plates placed at various depths, measure ground heat flux (G) while sensible heat is measured indirectly as the remainder after subtracting G and H from net solar radiation. The EC methodology is rather expensive and has several limitations which are discussed by several micrometeorologists (e.g. Castellvi et al., (2006); Castellvi et al, (2009a, 2009b); and Suvočarev et al., 2014)). The surface renewal method (SR) however provides an efficient and cheap option for estimating H, LE energy and methane (CH

_{4}) and carbon dioxide (CO

_{2}) gas exchange fluxes to and from varied ecosystems such as uniform pine forest (Katul et al., 1996); grapevine canopies (Spano et al., 2000); rice fields (Castellvi et al., 2006); and rangelands (Castellvi et al., 2008). The method is both cheaper and simple to implement on medium spatial scales such as livestock paddocks and feedlots. SR method does not require instrument levelling and has no limitations in orientation (Suvočarev et al., 2014)). Additionally, the SR method has demonstrated better energy balance closure (Castellvi, et al., 2008). To estimate H flux, measurements are taken at one height together with horizontal wind speeds and temperature. To estimate LE fluxes, measurements may be taken at one height together with horizontal wind speeds and moisture concentrations. The Surface Renewal (SR) process is derived from understandings of gaseous flux exchanges to or from an air parcel traveling at a known or specified height over a canopy. In the SR process an air parcel moves into the lower reaches of the canopy and remains for a duration τ (tau); before another parcel replaces it ejecting it upwards. Paw et al, (1995) created a diagram of this process and likened it to a ramp-like event.

The ramp is characterized by both an amplitude (A) and period (τ – Greek letter :tau). The purpose of this R code is to calculate these two characteristics for measuring both gaseous and energy flux exchanges occurring during the SR process. These values are then applied in estimating H, LE, CO

_{2}and CH

_{4}.

**Ramp Characteristics**

**Amplitude**Van Atta (1977) and Antonia and Van Atta (1978) (both cited in Synder et al., 2007) pioneered the surface renewal method. The researchers studied structure functions, ramp patterns and turbulence and their relationships. They utilized the structure function approach to estimate both amplitude and duration from moments recorded in the field (Equation 1). (Equation 1)

Where h(V

_{i }-V

_{i-j}) is the difference between two sequential high-frequency measurements (time lag interval,

*j*) of water vapor density or air temperature. M represents the total number of data points in the 0.5 hour time period.

*i*represents the summation index while

*n*is the structure function order. The R code builds of these procedures and calculates the 2

^{nd}, 3

^{rd}and 5

^{th}moments of a structure function following Van Atta (1977). Applying the three moments to calculate p and q; as: (Equation 2)

And; (Equation 3)

A cubic equation encompassing ramp amplitude is provided as: (Equation 4)

Equating y to 0 and solving for the real roots of the equation yields the ramp amplitude.

Ramp duration

Ramp duration

The “inverse ramp frequency” also known as the mean ramp event, τ , is calculated as: (Equation 5)

*j*represents the instance when the ratio between the third moment and observation time (seconds) is a maximum.

**The sample dataset (test.csv) utilized in this package consists of water vapor measurements (gm-3) recorded over 30 minutes (half an hour) at 20 Hz per second. Therefore a total of 36000 measurements are provided. The sample dataset can be downloaded here.**

Demonstration

Demonstration

R code

R code

The code provided below converts the H

_{2}O concentrations from g per m

^{3}to mmol per m

^{3}. Thereafter, 2nd, 3rd and 5th moments are calculated for each 1/20th of a second. These values are then applied to calculating two values;

*p*and

*q*.

*A*(amplitude) is derived by solving for the true roots of a cubic polynomial equation. The R code generates a numeric vector that consists of three values: 1)

*r*value – this is the time (seconds) when the ratio between the third moment and observation time (seconds) is a maximum. 2)

*τ*(Greek letter – tau) is the total ramp duration 3)

*A*is the amplitude of the ramp that models the SR process. In order for the package to function, two supporting packages are necessary. These are the

**NISTunits**and

**polynom**packages.

ipak <- function(pkg){ new.pkg <- pkg[!(pkg %in% installed.packages()[, “Package”])] if (length(new.pkg)) install.packages(new.pkg, dependencies = TRUE) sapply(pkg, require, character.only = TRUE) } ### usage of packages packages <- c(“NISTunits”,“polynom”,“bigmemory”) ipak(packages) ## Loading required package: NISTunits ## Loading required package: polynom ## Loading required package: bigmemory ## Loading required package: bigmemory.sri ## NISTunits polynom bigmemory ## TRUE TRUE TRUE require(NISTunits) ### cube root function Math.cbrt <- function(x) { sign(x) * abs(x)^(1/3) } #### #### set the directory and read file. In my case my dataset is stored in #### D:SurfaceRENEWAL folder setwd(“D:/SurfaceRENEWAL/”) df<-read.csv(“test.csv”, header=TRUE) ## creating empty data frame ### based on the value of hertz. In this case it is 20 Hz per second.. hertz<-20 dat <- data.frame(col1=numeric(hertz), col2=numeric(hertz), col3=numeric(hertz),stringsAsFactors = FALSE) ####convert to mmol m-3 df$H2O<-1000*df$H2O/18.01528 ### Creating and Initializing the table with three columns dat <- data.frame(col1=numeric(hertz), col2=numeric(hertz), col3=numeric(hertz),stringsAsFactors = FALSE) dat ## col1 col2 col3 ## 1 0 0 0 ## 2 0 0 0 ## 3 0 0 0 ## 4 0 0 0 ## 5 0 0 0 ## 6 0 0 0 ## 7 0 0 0 ## 8 0 0 0 ## 9 0 0 0 ## 10 0 0 0 ## 11 0 0 0 ## 12 0 0 0 ## 13 0 0 0 ## 14 0 0 0 ## 15 0 0 0 ## 16 0 0 0 ## 17 0 0 0 ## 18 0 0 0 ## 19 0 0 0 ## 20 0 0 0 for (p in 1:hertz) { #### initializing cumulative totals tempTot2<-0 tempTot3<-0 tempTot5<-0 #### the first column is the frequency #### the second column is the duration (in seconds) dat$col1[p]<-p dat$col2[p]<-p/hertz #### initializing temporary variables for calculating #### 2nd, 3rd and 5th moments tem2<-0 tem3<-0 tem5<-0 for (i in (p+1):nrow(df)) { tem2<-(df$H2O[i]-df$H2O[i-p])^2 tempTot2<-tem2+tempTot2 tem3<-(df$H2O[i]-df$H2O[i-p])^3 tempTot3<-tem3+tempTot3 tem5<-(df$H2O[i]-df$H2O[i-p])^5 tempTot5<-tem5+tempTot5 } dat$col3[p]<-(tempTot2/(nrow(df)-dat$col1[p])) dat$col4[p]<-(tempTot3/(nrow(df)-dat$col1[p])) dat$col5[p]<-(tempTot5/(nrow(df)-dat$col1[p])) } dat$moment2<-abs(dat$col3) dat$moment3<-abs(dat$col4) dat$moment5<-abs(dat$col5) #### Solution following Synder et al.(2007) #### values for p and q dat$p<-10*dat$col3 – (dat$col5/dat$col4) dat$q <- 10*dat$col4 #### solutions to the cubic equation after Synder et al., (2007) dat$D<-(((dat$q)^2)/4)+(((dat$p)^3)/27) for (i in 1:hertz) { if (dat$D[i]>0) { one1<-(dat$D[i])^0.5 one2

**Acknowledgements**

The author would like to acknowledge Andy Suyker for providing the test dataset. The authors also acknowledges the contributions of Kosana Suvočarev and Tala Awada.

**Castellvi, F., Martinez-Cob, A., & Perez-Coveta, O. (2006). Estimating sensible and latent heat fluxes over rice using surface renewal.**

References

References

*Agricultural and forest meteorology*,

*139*(1), 164-169. Castellvi, F., & Snyder, R. L. (2009). Combining the dissipation method and surface renewal analysis to estimate scalar fluxes from the time traces over rangeland grass near Ione (California).

*Hydrological processes*,

*23*(6), 842-857.

Castellví, F., & Snyder, R. L. (2009). On the performance of surface renewal analysis to estimate sensible heat flux over two growing rice fields under the influence of regional advection.

*Journal of hydrology*,

*375*(3), 546-553.

Castellvi, F., Snyder, R. L., & Baldocchi, D. D. (2008). Surface energy-balance closure over rangeland grass using the eddy covariance method and surface renewal analysis. A

*gricultural and forest meteorology*,

*148*(6), 1147-1160.

Katul, G., Hsieh, C. I., Oren, R., Ellsworth, D., & Phillips, N. (1996). Latent and sensible heat flux predictions from a uniform pine forest using surface renewal and flux variance methods.

*Boundary-Layer Meteorology*,

*80*(3), 249-282.

Mengistu, M. G., & Savage, M. J. (2010). Surface renewal method for estimating sensible heat flux.

*Water SA*,

*36*(1), 9-18.

Paw U, K. T., Snyder, R. L., Spano, D., & Su, H. B. (2005). Surface renewal estimates of scalar exchange.

*Agronomy*, 47, 455.

Snyder, R. L., Spano D., Duce K.T., Paw U, Anderson F. E. and Falk M. (2007). Surface Renewal Manual.

*University of California, Davis, California*.

Spano, D., Snyder, R. L., & Duce, P. (2000). Estimating sensible and latent heat flux densities from grapevine canopies using surface renewal.

*Agricultural and Forest Meteorology*,

*104*(3), 171-183.

Suvočarev, K., Shapland, T. M., Snyder, R. L., & Martínez-Cob, A. (2014). Surface renewal performance to independently estimate sensible and latent heat fluxes in heterogeneous crop surfaces.

*Journal of hydrology*,

*509*, 83-93.

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