Smoothing Methods
Several candidate smoothing methods will be tested to determine the
most accurate. Each method and some accuracy measures are displayed in
the table below. By RMSE and MAE metrics, Holt-Winters Multiplicative
Damped is the best candidate method.
fit1 = ses(train.air, h=12)
fit2 = holt(train.air, initial="optimal", h = 12)
fit3 = holt(train.air, damped = TRUE, h = 12)
fit4 = holt(train.air, exponential = TRUE, damped = TRUE, h = 12)
fit5 = hw(train.air, h = 12, seasonal = "additive")
fit6 = hw(train.air, h = 12, seasonal = "multiplicative")
fit7 = hw(train.air, h = 12, seasonal = "additive", damped = TRUE)
fit8 = hw(train.air, h = 12, seasonal = "multiplicative", damped = TRUE)
accuracy.table = round(rbind(accuracy(fit1), accuracy(fit2), accuracy(fit3), accuracy(fit4),
accuracy(fit5), accuracy(fit6), accuracy(fit7), accuracy(fit8)),4)
row.names(accuracy.table)=c("SES","Holt Linear","Holt Add. Damped", "Holt Exp. Damped",
"HW Add.","HW Exp.","HW Add. Damp", "HW Exp. Damp")
pander(accuracy.table, caption = "Accuracy Measures of Various Exponential Smoothing Models")
Accuracy Measures of Various Exponential Smoothing
Models
| SES |
2.22 |
31.21 |
23.9 |
0.4136 |
8.912 |
0.785 |
0.2863 |
| Holt Linear |
0.069 |
31.15 |
23.83 |
-0.5842 |
8.965 |
0.7826 |
0.2861 |
| Holt Add. Damped |
1.49 |
31.19 |
23.93 |
-0.0254 |
8.969 |
0.7859 |
0.286 |
| Holt Exp. Damped |
1.406 |
31.21 |
23.95 |
-0.0447 |
8.984 |
0.7867 |
0.2858 |
| HW Add. |
0.7468 |
15.41 |
11.57 |
0.259 |
5.002 |
0.38 |
0.1636 |
| HW Exp. |
1.369 |
9.95 |
7.533 |
0.2993 |
2.998 |
0.2474 |
0.3048 |
| HW Add. Damp |
1.638 |
15.51 |
11.67 |
0.6132 |
5.063 |
0.3833 |
0.1705 |
| HW Exp. Damp |
1.431 |
8.482 |
6.764 |
0.4725 |
2.857 |
0.2221 |
-0.0371 |
The different methods are graphed below, separated by linear and
seasonal methods. Unsurprisingly with such seasonal data, the seasonal
methods appear most appropriate.
par(mfrow=c(2,1), mar=c(3,4,3,1))
pred.id = 133:144
plot(1:132, train.air, lwd=2, type = "o", ylab = "Airline Passengers", xlab = "",
xlim = c(1,144), ylim = c(80,550), cex=0.3,
main = "Non-Seasonal Smoothing Methods")
lines(pred.id, fit1$mean, col="red")
lines(pred.id, fit2$mean, col="blue")
lines(pred.id, fit3$mean, col="green")
lines(pred.id, fit4$mean, col="violet")
points(pred.id, fit1$mean, pch=16, col="red", cex = 0.5)
points(pred.id, fit2$mean, pch=17, col="blue", cex = 0.5)
points(pred.id, fit3$mean, pch=19, col="green", cex = 0.5)
points(pred.id, fit4$mean, pch=21, col="violet", cex = 0.5)
legend("bottomright", lty=1, col=c("red","blue","green","violet"), pch=c(16,17,19,21),
c("SES","Holt Linear", "Holt Linear Damped", "Holt Multiplicitave Damped"),
cex = 0.7, bty = "n")
plot(1:132, train.air, lwd=2, type = "o", ylab = "Airline Passengers", xlab = "",
xlim = c(1,144), ylim = c(80,700), cex = 0.3,
main = "Holt-Winters Trend and Seasonal Smoothing Methods")
lines(pred.id, fit5$mean, col="red")
lines(pred.id, fit6$mean, col="blue")
lines(pred.id, fit7$mean, col="green")
lines(pred.id, fit8$mean, col="violet")
##
points(pred.id, fit5$mean, pch=16, col="red", cex = 0.5)
points(pred.id, fit6$mean, pch=17, col="blue", cex = 0.5)
points(pred.id, fit7$mean, pch=19, col="green", cex = 0.5)
points(pred.id, fit8$mean, pch=21, col="violet", cex = 0.5)
###
legend("bottomright", lty=1, col=c("red","blue","green", "violet"),pch=c(16,17,19,21),
c("HW Additive","HW Multiplicative","HW Additive Damped", "HW Multiplicative Damped"),
cex = 0.7, bty="n")

We select Holt-Winters Multiplicative with Damping based on RMES and
MAE. The smoothing parameters are given in the table below.
final.model = hw(air, h =12, seasonal = "multiplicative", damped = TRUE)
smoothing.parameter = final.model$model$par[1:3]
pander(smoothing.parameter, caption = "Est. Values of the smoothing parameters")
---
title: "Exponential Smoothing Methods"
author: "Noah Brechbill"
date: "`r Sys.Date()`"
output:
  html_document:
    toc: yes
    toc_float: yes
    toc_depth: 4
    fig_width: 6
    fig_height: 6
    fig_caption: yes
    number_sections: yes
    toc_collapsed: yes
    code_folding: hide
    code_download: yes
    smooth_scroll: yes
    theme: lumen
editor_options: 
  markdown: 
    wrap: 72
---

```{css, echo = FALSE}
/* Cascading Style Sheets (CSS) is a stylesheet language used to describe the presentation of a document written in HTML or XML. it is a simple mechanism for adding style (e.g., fonts, colors, spacing) to Web documents. */

h1.title {  /* Title - font specifications of the report title */
  font-size: 24px;
  color: DarkRed;
  text-align: center;
  font-weight: bold;
  font-family: "Gill Sans", sans-serif;
}
h4.author { /* Header 4 - font specifications for authors  */
  font-size: 20px;
  font-family: system-ui;
  font-weight: bold;
  color: DarkRed;
  text-align: center;
}
h4.date { /* Header 4 - font specifications for the date  */
  font-size: 18px;
  font-family: system-ui;
  font-weight: bold;
  color: DarkBlue;
  text-align: center;
}
h1 { /* Header 1 - font specifications for level 1 section title  */
    font-size: 22px;
    font-family: system-ui;
  font-weight: bold;
    color: navy;
    text-align: left;
}
h2 { /* Header 2 - font specifications for level 2 section title */
    font-size: 20px;
  font-weight: bold;
    font-family: "Times New Roman", Times, serif;
    color: navy;
    text-align: left;
}

h3 { /* Header 3 - font specifications of level 3 section title  */
    font-size: 18px;
  font-weight: bold;
    font-family: "Times New Roman", Times, serif;
    color: navy;
    text-align: left;
}

h4 { /* Header 4 - font specifications of level 4 section title  */
    font-size: 18px;
  font-weight: bold;
    font-family: "Times New Roman", Times, serif;
    color: darkred;
    text-align: left;
}

body { background-color:white; }

.highlightme { background-color:yellow; }

p { background-color:white; }
```

```{r setup, include=FALSE}
load_packages <- function(pkg_list) {
  for (pkg in pkg_list) {
    if (!require(pkg, character.only = TRUE)) {
      install.packages(pkg, dependencies = TRUE)
      library(pkg, character.only = TRUE)
    }
  }
}

packages <- c("tidyverse", "pander", "forecast")
load_packages(packages)

knitr::opts_chunk$set(echo = TRUE,      
                      warning = FALSE,   
                      message = FALSE,  
                      results = TRUE,
                      comment = NA,
                      fig.align = "center"
                      )   
air <- AirPassengers
```

## Data

The data set used in this analysis count the total passengers on an
airline from 1949 to 1960, counted monthly. This data set is built inn
to R and does not need to be downloaded.

## Training/Testing Split

The data is split into training and testing subsets. The last year (12
observations) is withheld and will be used to determine accuracy of the
smoothing methods.

```{r}
train.air <- ts(air[1:132], start = 1949, frequency = 12)
test.air <- ts(air[133:144], start = 1960, frequency = 12)

```

## Original Data

The recorded training data is displayed in the graph below. A annual
moving average is included to display the positive trend through the
seasonality.

```{r}
trend.air <- ma(train.air, order = 12, centre = TRUE)
par(mar=c(2,2,2,2))
plot(train.air, xlab="", ylab="Total Passengers", col="darkred", lwd =2)
title(main = "Airline Passengers Over Time with Moving Average")
lines(trend.air, lwd =2, col = "blue")
legend("topleft", c("Original Series", "12-Month Moving Average"), lwd=rep(2,2),
       col=c("darkred", "blue"), bty="n")

```

## Smoothing Methods

Several candidate smoothing methods will be tested to determine the most
accurate. Each method and some accuracy measures are displayed in the
table below. By RMSE and MAE metrics, Holt-Winters Multiplicative Damped
is the best candidate method.

```{r}
fit1 = ses(train.air, h=12)
fit2 = holt(train.air, initial="optimal", h = 12)
fit3 = holt(train.air, damped = TRUE, h = 12)
fit4 = holt(train.air, exponential = TRUE, damped = TRUE, h = 12)
fit5 = hw(train.air, h = 12, seasonal = "additive")
fit6 = hw(train.air, h = 12, seasonal = "multiplicative")
fit7 = hw(train.air, h = 12, seasonal = "additive", damped = TRUE)
fit8 = hw(train.air, h = 12, seasonal = "multiplicative", damped = TRUE)

accuracy.table = round(rbind(accuracy(fit1), accuracy(fit2), accuracy(fit3), accuracy(fit4),
                             accuracy(fit5), accuracy(fit6), accuracy(fit7), accuracy(fit8)),4)
row.names(accuracy.table)=c("SES","Holt Linear","Holt Add. Damped", "Holt Exp. Damped",
                            "HW Add.","HW Exp.","HW Add. Damp", "HW Exp. Damp")
pander(accuracy.table, caption = "Accuracy Measures of Various Exponential Smoothing Models")

```

The different methods are graphed below, separated by linear and
seasonal methods. Unsurprisingly with such seasonal data, the seasonal
methods appear most appropriate.

```{r}
par(mfrow=c(2,1), mar=c(3,4,3,1))
pred.id = 133:144
plot(1:132, train.air, lwd=2, type = "o", ylab = "Airline Passengers", xlab = "",
     xlim = c(1,144), ylim = c(80,550), cex=0.3,
     main = "Non-Seasonal Smoothing Methods")
lines(pred.id, fit1$mean, col="red")
lines(pred.id, fit2$mean, col="blue")
lines(pred.id, fit3$mean, col="green")
lines(pred.id, fit4$mean, col="violet")
points(pred.id, fit1$mean, pch=16, col="red", cex = 0.5)
points(pred.id, fit2$mean, pch=17, col="blue", cex = 0.5)
points(pred.id, fit3$mean, pch=19, col="green", cex = 0.5)
points(pred.id, fit4$mean, pch=21, col="violet", cex = 0.5)

legend("bottomright", lty=1, col=c("red","blue","green","violet"), pch=c(16,17,19,21),
       c("SES","Holt Linear", "Holt Linear Damped", "Holt Multiplicitave Damped"),
       cex = 0.7, bty = "n")


plot(1:132, train.air, lwd=2, type = "o", ylab = "Airline Passengers", xlab = "",
     xlim = c(1,144), ylim = c(80,700), cex = 0.3,
     main = "Holt-Winters Trend and Seasonal Smoothing Methods")
lines(pred.id, fit5$mean, col="red")
lines(pred.id, fit6$mean, col="blue")
lines(pred.id, fit7$mean, col="green")
lines(pred.id, fit8$mean, col="violet")
##
points(pred.id, fit5$mean, pch=16, col="red", cex = 0.5)
points(pred.id, fit6$mean, pch=17, col="blue", cex = 0.5)
points(pred.id, fit7$mean, pch=19, col="green", cex = 0.5)
points(pred.id, fit8$mean, pch=21, col="violet", cex = 0.5)
###
legend("bottomright", lty=1, col=c("red","blue","green", "violet"),pch=c(16,17,19,21),
       c("HW Additive","HW Multiplicative","HW Additive Damped", "HW Multiplicative Damped"), 
       cex = 0.7, bty="n")
```

We select Holt-Winters Multiplicative with Damping based on RMES and
MAE. The smoothing parameters are given in the table below.

```{r}
final.model = hw(air, h =12, seasonal = "multiplicative", damped = TRUE)
smoothing.parameter = final.model$model$par[1:3]
pander(smoothing.parameter, caption = "Est. Values of the smoothing parameters")
```
