Introduction
This project aims to predict a team score, by evaluating data
collected for a specific Women’s National Basketball Association team,
in the 2024 season. By using linear regression, I developed a model for
the Chicago Sky, with the purpose of predicting a score based upon
median values for the variables selected in the model.
Data Summary with
Tables
Below are two tables displaying data for each team in the league
(Table 1) and the Chicago Sky (Table 2).
Table 1 presents the mean scores (yellow columns) and standard
deviations (blue columns) for each team in the league narrowed to the
following variables: team score, field goal percentage, total rebounds,
three point field goal percentage, and steals.
Table 2 presents data specific to the Chicago Sky, using the same
variables as in Table 1 but separated by whether the Chicago Sky
experienced a loss or win. It should be noted that there were only 40
observations due to the Chicago Sky not qualifying for the playoffs;
their regular season recorded 13 wins and 27 losses in 2024.
#table for entire league; column colors using Chicago Sky hex color codes
means_sd_score%>%
kbl(digits=2,caption="TABLE 1 - 2024 WNBA Team Stats")%>%
kable_classic(full_width=F,html_font = "Cambria")%>%
column_spec(2,background="#ffcd00")%>%
column_spec(3,background="#418fde")%>%
column_spec(4,background="#ffcd00")%>%
column_spec(5,background="#418fde")%>%
column_spec(6,background="#ffcd00")%>%
column_spec(7,background="#418fde")%>%
column_spec(8,background="#ffcd00")%>%
column_spec(9,background="#418fde")%>%
column_spec(10,background="#ffcd00")%>%
column_spec(11,background="#418fde")
TABLE 1 - 2024 WNBA Team Stats
|
team_name
|
mean_score
|
sd_score
|
mean_field
|
sd_field
|
mean_total
|
sd_total
|
mean_three
|
sd_three
|
mean_steals
|
sd_steals
|
|
Aces
|
85.52
|
9.56
|
45.27
|
5.82
|
33.78
|
5.88
|
35.27
|
7.08
|
6.80
|
2.67
|
|
Dream
|
76.93
|
10.59
|
41.28
|
6.78
|
35.95
|
4.41
|
30.83
|
9.32
|
7.14
|
2.82
|
|
Fever
|
84.50
|
10.17
|
45.56
|
5.38
|
35.10
|
5.49
|
35.00
|
8.99
|
5.88
|
2.29
|
|
Liberty
|
84.98
|
9.92
|
44.53
|
5.61
|
36.90
|
5.77
|
35.38
|
10.06
|
7.75
|
2.19
|
|
Lynx
|
82.36
|
11.39
|
45.21
|
6.34
|
33.15
|
5.06
|
37.80
|
9.43
|
8.36
|
3.17
|
|
Mercury
|
81.93
|
12.60
|
44.28
|
7.34
|
32.26
|
5.39
|
32.97
|
10.34
|
6.55
|
2.12
|
|
Mystics
|
79.30
|
8.69
|
43.36
|
4.82
|
31.85
|
4.66
|
36.64
|
8.69
|
7.28
|
2.24
|
|
Sky
|
77.40
|
9.62
|
42.44
|
5.22
|
36.60
|
5.57
|
31.74
|
11.62
|
7.00
|
3.30
|
|
Sparks
|
78.40
|
10.57
|
42.63
|
6.15
|
32.67
|
5.52
|
32.09
|
11.00
|
7.30
|
2.78
|
|
Storm
|
82.67
|
9.65
|
43.43
|
5.39
|
34.67
|
6.02
|
28.35
|
9.03
|
9.24
|
3.27
|
|
Sun
|
80.36
|
9.89
|
44.30
|
5.28
|
33.43
|
4.62
|
32.84
|
11.67
|
7.89
|
3.29
|
|
Wings
|
84.20
|
11.47
|
44.47
|
5.24
|
34.75
|
4.65
|
32.06
|
11.75
|
7.12
|
2.95
|
#table for my team based on win/loss
my_team_win%>%
kbl(digits=2,caption="TABLE 2 - 2024 Chicago Sky Team Stats by Win/Loss")%>%
kable_classic(full_width=F,html_font = "Cambria")%>%
row_spec(1,background="#418fde")%>%
row_spec(2,background="#ffcd00")
TABLE 2 - 2024 Chicago Sky Team Stats by Win/Loss
|
Result
|
mean_score
|
sd_score
|
mean_field
|
sd_field
|
mean_total
|
sd_total
|
mean_three
|
sd_three
|
mean_steals
|
sd_steals
|
|
Loss
|
73.04
|
8.16
|
40.66
|
4.81
|
35.85
|
6.38
|
31.47
|
12.13
|
6.30
|
2.87
|
|
Win
|
86.46
|
4.99
|
46.15
|
4.05
|
38.15
|
2.97
|
32.28
|
10.94
|
8.46
|
3.76
|
#turn off full-width by putting full_width=F in parentheses after kable_styling(); can change style by looking online for different fonts and designs; digits=2 rounds to 2 decimals
df_hist= data%>%
filter(team_name=="Sky") %>%
mutate(Result=case_when(team_winner==T~"Win",team_winner==F~"Loss"))
Graphs
Histogram and
Boxplot
The histogram below demonstrates the team score in a game versus the
number of games obtaining that score, split by Loss or Win. Both
histograms demonstrate a normal distribution.
The boxplot below demonstrates loss/win versus game points scored.
The boxplots demonstrate overlap in score ranges and have normal
distributions, with the boxes approximately centered in their respective
distributions.
#histogram code using team_score as x-axis and number of games with that score on y-axis,
#separated by win/loss (yellow/blue)
p=df_hist%>%
ggplot(aes(x=team_score,fill=Result))+
geom_histogram(color="#e9ecef",alpha=0.6,position='identity')+
scale_fill_manual(values=c("#418fde", "#ffcd00"))+
labs(title="2024 Chicago Sky - Team Score vs Number of Games",x="Team Score",
y = "Number of Games")
#boxplot of result vs game score separated by win/loss
p

boxplot(team_score ~ Result, data = df_hist,
col = c("#418fde","#ffcd00"),
main="Points Scored by Game Result",
xlab="Result", ylab="Points")

#just typing p will "call" object p, which is the graph and graph will appear below if you run p as an individual line
Models
First-Order
Model
A first-order model was constructed using the previously selected
variables (team score, field goal percentage, total rebounds, three
point field goal percentage, and steals). No multicollinearity was noted
(no r>|0.8|), and all variance inflation factors (VIF) were less than
2. As a result, no individual variables were removed from the
first-order model. The adjusted R-squared was 66.8% with F(4,35)=20.61,
p<.001.
Interaction
Model
A second, interaction model was built adding the following variables
to the first-order model: (field goal percentage * total rebounds),
(field goal percentage * three point field goal percentage), (field goal
percentage * steals), (total rebounds * three point field goal pct),
(total rebounds * steals), and (three point field goal percentage *
steals). No interaction term was found to be significant at the 15%
significance level. The adjusted R-squared for the interaction model was
63.2% with F(10,29)=7.70, p<.001.
Model Utility
Conclusion
Given no significant interaction terms, the first-order model was
retained for further analysis and prediction.
My final model is team_score=-10.3752861 + 1.3421353 * field_goal_pct
+ 0.5554673 * total_rebounds + 0.1597494 * three_point_field_goal_pct +
0.7731366* steals.
This model significantly predicts team score, F(4,35) = 20.6121077,
p<0.001, adjusted R-squared=0.6679394. See the table below for
further analysis.
|
|
|
|
Dependent variable:
|
|
|
|
|
|
team_score
|
|
|
|
field_goal_pct
|
1.342***
|
|
|
(0.188)
|
|
|
|
|
total_rebounds
|
0.555***
|
|
|
(0.166)
|
|
|
|
|
three_point_field_goal_pct
|
0.160*
|
|
|
(0.087)
|
|
|
|
|
steals
|
0.773***
|
|
|
(0.279)
|
|
|
|
|
Constant
|
-10.375
|
|
|
(10.685)
|
|
|
|
|
|
|
Observations
|
40
|
|
R2
|
0.702
|
|
Adjusted R2
|
0.668
|
|
Residual Std. Error
|
5.545 (df = 35)
|
|
F Statistic
|
20.612*** (df = 4; 35)
|
|
|
|
Note:
|
p<0.1; p<0.05;
p<0.01
|
Residual Analysis
Residual analysis was performed on the first-order model including a
fitted values plot, a residual histogram, Studentized Residual, a graph
of leverage, and a Cook’s D plot. The fitted values plot demonstrated
constant variance, and the residual histogram demonstrated a normal
distribution of the residuals. No outliers were noted in the Studentized
Residual (threshold=|3|). With a leverage threshold of 0.25, four games
were noted to have high leverage: September 19, 2024 versus the
Connecticut Sun (Observation 1); August 25, 2024 versus the Las Vegas
Aces (Observation 12); August 18, 2024 versus the Phoenix Mercury
(Observation 14); May 25,2024 versus the Connecticut Sun (Observation
37). Two games had Cook’s D values greater than the threshold of 0.1:
July 13, 2024 versus the New York Liberty (Observation 18) and June 4,
2024 versus the New York Liberty (Observation 33).
#residual analysis on model_1 as no interaction terms were significant
#includes versus fit, histogram, studentized residual, leverage (with threshold of 3), and Cook's D
ols_plot_resid_fit(model_1)

ols_plot_resid_hist(model_1)

ols_plot_resid_stud(model_1)

ols_plot_resid_lev(model_1, threshold = 3)

ols_plot_cooksd_chart(model_1)

Prediction
I built this model to predict my team’s points for a game in which
they achieved the median value for each variable. The predicted team
score is 78.5533285, with a 95% confidence interval of (76.7433284,
80.3633285).
---
title: "Assignment #6"
author: "Ry Bloomdahl"
date: "`r Sys.Date()`"
output:
  html_document: 
    toc: yes
    toc_depth: 4
    toc_float: yes
    number_sections: yes
    toc_collapsed: yes
    code_folding: hide
    code_download: yes
    smooth_scroll: yes
    theme: lumen
  pdf_document: 
    toc: yes
    toc_depth: 4
    fig_caption: yes
    number_sections: yes
    fig_width: 3
    fig_height: 3
  word_document: 
    toc: yes
    toc_depth: 4
    fig_caption: yes
    keep_md: yes
editor_options: 
  chunk_output_type: inline
---

```{css, echo = FALSE}
#TOC::before {
  content: "Table of Contents";
  font-weight: bold;
  font-size: 1.2em;
  display: block;
  color: navy;
  margin-bottom: 10px;
}


div#TOC li {     /* table of content  */
    list-style:upper-roman;
    background-image:none;
    background-repeat:none;
    background-position:0;
}

h1.title {    /* level 1 header of title  */
  font-size: 22px;
  font-weight: bold;
  color: DarkRed;
  text-align: center;
  font-family: "Gill Sans", sans-serif;
}

h4.author { /* Header 4 - and the author and data headers use this too  */
  font-size: 15px;
  font-weight: bold;
  font-family: system-ui;
  color: navy;
  text-align: center;
}

h4.date { /* Header 4 - and the author and data headers use this too  */
  font-size: 18px;
  font-weight: bold;
  font-family: "Gill Sans", sans-serif;
  color: DarkBlue;
  text-align: center;
}

h1 { /* Header 1 - and the author and data headers use this too  */
    font-size: 20px;
    font-weight: bold;
    font-family: "Times New Roman", Times, serif;
    color: darkred;
    text-align: left;
}

h2 { /* Header 2 - and the author and data headers use this too  */
    font-size: 18px;
    font-weight: bold;
    font-family: "Times New Roman", Times, serif;
    color: navy;
    text-align: left;
}

h3 { /* Header 3 - and the author and data headers use this too  */
    font-size: 16px;
    font-weight: bold;
    font-family: "Times New Roman", Times, serif;
    color: navy;
    text-align: left;
}

h4 { /* Header 4 - and the author and data headers use this too  */
    font-size: 14px;
  font-weight: bold;
    font-family: "Times New Roman", Times, serif;
    color: darkred;
    text-align: left;
}

/* Add dots after numbered headers */
.header-section-number::after {
  content: ".";

body { background-color:white; }

.highlightme { background-color:yellow; }

p { background-color:white; }

}
```

```{r setup, include=F}
setwd("~/STA 319")

data=read.csv("WNBA_2025_box-scores.csv", header=T)

library(ggplot2)
library(dplyr)
library(car)
library(olsrr)
#kableExtra is package for nice Markdown tables
library(kableExtra)

```

```{r wrangling, include=F}


summary(data)

#all wnba teams included, remove scores from all-star game
data= data %>%
  filter(team_name!="Team WNBA" & team_name!="Team USA")

#group data by team, find mean/std of all variables (part b and c)
means_sd_score = data %>%
  group_by(team_name) %>%
  summarize(mean_score=mean(team_score), sd_score=sd(team_score),
            mean_field=mean(field_goal_pct), sd_field=sd(field_goal_pct),
            mean_total=mean(total_rebounds), sd_total=sd(total_rebounds),
            mean_three=mean(three_point_field_goal_pct), sd_three=sd(three_point_field_goal_pct),
            mean_steals=mean(steals), sd_steals=sd(steals))

#part d
#select only variables we need and filter on my team
my_team = data %>%
  select(team_score, field_goal_pct, total_rebounds, 
         three_point_field_goal_pct, steals, team_name, team_winner) %>%
  filter(team_name=="Sky")%>%
  mutate(Result=case_when(team_winner==T~"Win",team_winner==F~"Loss"))

#groups cases by win v loss
#summarize all variables with mean and std for my team
my_team_win = my_team %>%
  group_by(Result) %>%
  summarize(mean_score=mean(team_score), sd_score=sd(team_score),
            mean_field=mean(field_goal_pct), sd_field=sd(field_goal_pct),
            mean_total=mean(total_rebounds), sd_total=sd(total_rebounds),
            mean_three=mean(three_point_field_goal_pct), sd_three=sd(three_point_field_goal_pct),
            mean_steals=mean(steals), sd_steals=sd(steals))

```

# Introduction
This project aims to predict a team score, by evaluating data collected for a specific Women's National Basketball Association team, in the 2024 season.  By using linear regression, I developed a model for the Chicago Sky, with the purpose of predicting a score based upon median values for the variables selected in the model.

## Data Summary with Tables

Below are two tables displaying data for each team in the league (Table 1) and the Chicago Sky (Table 2).  

Table 1 presents the mean scores (yellow columns) and standard deviations (blue columns) for each team in the league narrowed to the following variables: team score, field goal percentage, total rebounds, three point field goal percentage, and steals. 

Table 2 presents data specific to the Chicago Sky, using the same variables as in Table 1 but separated by whether the Chicago Sky experienced a loss or win.  It should be noted that there were only 40 observations due to the Chicago Sky not qualifying for the playoffs; their regular season recorded 13 wins and 27 losses in 2024.

```{r tables, include=T, fig.width=6, fig.height=7}
#table for entire league; column colors using Chicago Sky hex color codes
means_sd_score%>%
  kbl(digits=2,caption="TABLE 1 - 2024 WNBA Team Stats")%>%
  kable_classic(full_width=F,html_font = "Cambria")%>%
  column_spec(2,background="#ffcd00")%>%
  column_spec(3,background="#418fde")%>%
  column_spec(4,background="#ffcd00")%>%
  column_spec(5,background="#418fde")%>%
  column_spec(6,background="#ffcd00")%>%
  column_spec(7,background="#418fde")%>%
  column_spec(8,background="#ffcd00")%>%
  column_spec(9,background="#418fde")%>%
  column_spec(10,background="#ffcd00")%>%
  column_spec(11,background="#418fde")

#table for my team based on win/loss
my_team_win%>%
  kbl(digits=2,caption="TABLE 2 - 2024 Chicago Sky Team Stats by Win/Loss")%>%
  kable_classic(full_width=F,html_font = "Cambria")%>%
  row_spec(1,background="#418fde")%>%
  row_spec(2,background="#ffcd00")
#turn off full-width by putting full_width=F in parentheses after kable_styling(); can change style by looking online for different fonts and designs; digits=2 rounds to 2 decimals
df_hist= data%>%
  filter(team_name=="Sky") %>%
  mutate(Result=case_when(team_winner==T~"Win",team_winner==F~"Loss"))
```

# Graphs

## Histogram and Boxplot
The histogram below demonstrates the team score in a game versus the number of games obtaining that score, split by Loss or Win.  Both histograms demonstrate a normal distribution.  

The boxplot below demonstrates loss/win versus game points scored.  The boxplots demonstrate overlap in score ranges and have normal distributions, with the boxes approximately centered in their respective distributions.


```{r graphs, include=T, message=F, fig.width=6,fig.height=7}
#histogram code using team_score as x-axis and number of games with that score on y-axis, 
#separated by win/loss (yellow/blue)
p=df_hist%>%
  ggplot(aes(x=team_score,fill=Result))+
    geom_histogram(color="#e9ecef",alpha=0.6,position='identity')+
    scale_fill_manual(values=c("#418fde", "#ffcd00"))+
    labs(title="2024 Chicago Sky - Team Score vs Number of Games",x="Team Score", 
         y = "Number of Games")

#boxplot of result vs game score separated by win/loss     
p
boxplot(team_score ~ Result, data = df_hist,
        col = c("#418fde","#ffcd00"),
        main="Points Scored by Game Result",
        xlab="Result", ylab="Points")
#just typing p will "call" object p, which is the graph and graph will appear below if you run p as an individual line
```
# Models

## First-Order Model
A first-order model was constructed using the previously selected variables (team score, field goal percentage, total rebounds, three point field goal percentage, and steals).  No multicollinearity was noted (no r>|0.8|), and all variance inflation factors (VIF) were less than 2. As a result, no individual variables were removed from the first-order model. The adjusted R-squared was 66.8% with F(4,35)=20.61, p<.001.

## Interaction Model
A second, interaction model was built adding the following variables to the first-order model: (field goal percentage * total rebounds), (field goal percentage * three point field goal percentage), (field goal percentage * steals), (total rebounds * three point field goal pct), (total rebounds * steals), and (three point field goal percentage * steals).  No interaction term was found to be significant at the 15% significance level. The adjusted R-squared for the interaction model was 63.2% with F(10,29)=7.70, p<.001.

## Model Utility Conclusion
Given no significant interaction terms, the first-order model was retained for further analysis and prediction.

```{r first order model, results='asis',echo=F, include=F}
#first-order model for my team
model_1=lm(team_score~field_goal_pct+total_rebounds+three_point_field_goal_pct+steals,data=my_team)
model_1sum=summary(model_1)

#selecting specific variables to run correlation analysis on
cor_data=my_team %>%
  select(team_score,field_goal_pct,total_rebounds,three_point_field_goal_pct,steals)

#correlation code
cor(cor_data)

#variance inflation factor code run on model_1
vif(model_1)
#summary stats on model_1
summary(model_1)

#no highly correlated pairs noted, VIFs all<2

```

```{r interaction model, include=F}
#model_2 includes model_1 with 6 interaction factors
model_2=lm(team_score~field_goal_pct+total_rebounds+three_point_field_goal_pct+steals
           +field_goal_pct*total_rebounds+field_goal_pct*three_point_field_goal_pct+field_goal_pct*steals+total_rebounds*three_point_field_goal_pct+total_rebounds*steals+three_point_field_goal_pct*steals,data=my_team)

#summary stats for model_2
summary(model_2)

#no significant interactions to significance level of 15% noted so model_1 remains more appropriate
```

My final model is team_score=`r model_1$coefficient[1]` + `r model_1$coefficient[2]` * field_goal_pct + `r model_1$coefficient[3]` * total_rebounds + `r model_1$coefficient[4]` * three_point_field_goal_pct + `r model_1$coefficient[5]`* steals.

This model significantly predicts team score, F(`r model_1sum$fstatistic[2]`,`r model_1sum$fstatistic[3]`) = `r model_1sum$fstatistic[1]`, p<0.001, adjusted R-squared=`r model_1sum$adj.r.squared`.  See the table below for further analysis.
```{r,include=T, echo=F, results='asis', message=F}
library(stargazer)
stargazer(model_1,type="html")
```

# Residual Analysis

Residual analysis was performed on the first-order model including a fitted values plot, a residual histogram, Studentized Residual, a graph of leverage, and a Cook's D plot. The fitted values plot demonstrated constant variance, and the residual histogram demonstrated a normal distribution of the residuals. No outliers were noted in the Studentized Residual (threshold=|3|). With a leverage threshold of 0.25, four games were noted to have high leverage: September 19, 2024 versus the Connecticut Sun (Observation 1); August 25, 2024 versus the Las Vegas Aces (Observation 12); August 18, 2024 versus the Phoenix Mercury (Observation 14); May 25,2024 versus the Connecticut Sun (Observation 37). Two games had Cook's D values greater than the threshold of 0.1: July 13, 2024 versus the New York Liberty (Observation 18) and June 4, 2024 versus the New York Liberty (Observation 33).
```{r residuals, include=T,fig.width=6,fig.height=7}
#residual analysis on model_1 as no interaction terms were significant
#includes versus fit, histogram, studentized residual, leverage (with threshold of 3), and Cook's D
ols_plot_resid_fit(model_1)
ols_plot_resid_hist(model_1)
ols_plot_resid_stud(model_1)
ols_plot_resid_lev(model_1, threshold = 3)
ols_plot_cooksd_chart(model_1)
```

# Prediction
```{r prediction, include=F}
summary(cor_data)
#newdata frame for median of variables in model_1
newdata=data.frame(field_goal_pct=42.95,total_rebounds=37.00,three_point_field_goal_pct=33.30,steals=7)
#prediction for score based on median values of variables in model_1
prediction=predict(model_1,newdata,interval="confidence",level=.95)

#model_1 predicts score of 80 with a 95% CI[77,80]
```
I built this model to predict my team's points for a game in which they achieved the median value for each variable. The predicted team score is `r prediction[1]`, with a 95% confidence interval of (`r prediction[2]`, `r prediction[3]`). 


