Assignment Objectives

  • Enhance understanding the procedure of Bootstrap hypothesis testing.

  • Implement the procedures for detecting overfitting/underfitting issues in practical applications using bootstrap likelihood ratio test.

Policies of Using AI Tools

Policy on AI Tool Use: Please adhere to the AI tool policy specified in the course syllabus. The direct copying of AI-generated content is strictly prohibited. All submitted work must reflect your own understanding; where external tools are consulted, content must be thoroughly rephrased and synthesized in your own words.

Code Inclusion Requirement: Any code included in your essay must be properly commented to explain the purpose and/or expected output of key code lines. Submitting AI-generated code without meaningful, student-added comments will not be accepted.

Testing Overfitting/Underfitting

In Machine Learning and Statistics, overfitting occurs when a model is too complex and learns noise, leading to poor performance on new data, while underfitting happens when a model is too simple to capture important patterns, resulting in high errors overall; both issues are explained by the Bias–Variance Tradeoff and can cause unreliable predictions in real-world applications.

The probability density function (PDF) of the Weibull distribution is:

\[ f(t; \lambda, \beta) = \frac{\beta}{\lambda} \left( \frac{t}{\lambda} \right)^{\beta-1} \exp\left[ -\left( \frac{t}{\lambda} \right)^\beta \right], \quad t \ge 0 \] where \(\lambda > 0\) is the scale parameter (characteristic life) and \(\beta > 0\) is the shape parameter.

When \(\beta = 1\), the Weibull PDF simplifies to the exponential PDF:

\[ f(t; \lambda) = \frac{1}{\lambda} \exp\left( -\frac{t}{\lambda} \right) \] with constant hazard rate \(h(t) = 1/\lambda\).

This assignment focuses on performing a hypothesis test for the shape parameter (\(\beta\)) of the Weibull distribution within a reliability mode

\[\begin{align} H_0&: \beta = 1 \quad \text{(Exponential model, simpler)} \\ H_1&: \beta \neq 1 \quad \text{(Weibull model, more complex)} \end{align}\]

Steps of the BLRT

  • Fit models under \(H_0\) and \(H_1\)} to the original data, compute \(\Lambda_{\text{obs}}\).

  • Generate bootstrap samples under \(H_0\)}:

    • Estimate parameters under \(H_0\) from the original data.
    • Generate \(B\) datasets by sampling from the model under \(H_0\) (parametric bootstrap) or by resampling residuals/cases (nonparametric bootstrap; parametric is common for BLRT).
  • For each bootstrap sample \(b = 1,\dots,B\):

    • Fit \(H_0\) and \(H_1\) models.
    • Compute \(\Lambda_b = -2[\ell_{0,b} - \ell_{1,b}]\).
  • Approximate p-value:

\[ p = \frac{1}{B} \sum_{b=1}^B I(\Lambda_b \ge \Lambda_{\text{obs}}) \] (Often a small adjustment is made for stability: \((1 + \#\{\Lambda_b \ge \Lambda_{\text{obs}}\})/(B+1)\)).


Question: Reliability Application

A wind energy company monitors the reliability of gearboxes in 75 identical wind turbines located in a coastal wind farm. The gearbox is a critical component; its failure often leads to costly downtime and repairs. Previous studies suggest that the hazard rate (failure risk) may increase over time due to mechanical wear (fatigue, pitting, bearing degradation). Engineers want to test whether the failure time distribution follows an exponential model (constant hazard, random failures) or a Weibull model with shape parameter \(k>1\) (increasing hazard, indicative of aging/degradation). The failure times (in months) are:

   5.2,  7.8,  9.1, 11.3, 12.5, 13.0, 14.2, 15.1, 15.9, 16.7, 17.2, 17.8, 18.4, 18.9, 
  19.3, 19.7, 20.2, 20.6, 21.0, 21.5, 21.9, 22.3, 22.7, 23.1, 23.5, 23.9, 24.3, 24.7, 
  25.1, 25.5, 25.9, 26.3, 26.7, 27.1, 27.5, 27.9, 28.3, 28.7, 29.1, 29.5, 29.9, 30.3, 
  30.7, 31.1, 31.5, 31.9, 32.3, 32.7, 33.1, 33.5, 33.9, 34.3, 34.7, 35.1, 35.5, 35.9, 
  36.3, 36.7, 37.1, 37.5, 37.9, 38.3, 38.7, 39.1, 39.5, 39.9, 40.3, 40.7, 41.1, 41.5,
  41.9, 42.3, 42.7, 43.1, 43.5

This assignment focuses on hypothesis \(H_0: \beta = 1\) (exponential) against \(H_1: \beta \neq 1\) (Weibull). This framework detects overfitting (fitting a Weibull when exponential is true) and underfitting (fitting exponential when Weibull with \(\beta \neq 1\) is true).

a). Find the MLE of the Weibull parameters \(\lambda\) (scale) and \(\beta\) (shape), denoted by \(\hat{\lambda}\) and \(\hat{\beta}\), respectively, using the optim() procedure. [Hint: You should provide explicit expressions for the log-likelihood and gradient functions of the Weibull distribution parameters.]

############################################################
# (a) Weibull MLE
############################################################

t <- c(
  12.4, 18.7, 25.3, 30.1, 33.5, 35.2, 38.9, 40.3, 42.7, 45.1,
  47.6, 49.8, 52.4, 55.0, 57.3, 60.2, 62.8, 65.1, 67.9, 70.5,
  72.3, 75.6, 78.2, 80.9, 83.4, 85.7, 88.1, 90.6, 93.2, 95.8,
  98.4, 101.0, 104.5, 107.3, 110.6, 113.2, 116.8, 120.1, 123.7, 127.4,
  130.9, 134.5, 138.2, 142.0, 146.3, 150.7, 155.2, 160.8, 168.4, 175.9
)

weibull_nll <- function(par, t) {
  lambda <- par[1]
  beta   <- par[2]
  
  if (lambda <= 0 || beta <= 0) return(Inf)
  
  ll <- sum(log(beta/lambda) +
            (beta - 1)*log(t/lambda) -
            (t/lambda)^beta)
  
  return(-ll)
}

fit <- optim(c(mean(t), 1), weibull_nll, t = t, hessian = TRUE)

lambda_hat <- fit$par[1]
beta_hat   <- fit$par[2]

lambda_hat
[1] 99.02759
beta_hat 
[1] 2.205876

b). Find the MLE of the exponential parameter \(\lambda\) (scale), denoted by \(\hat{\lambda}\), using any procedure. [Hint: You should provide explicit expressions for the log-likelihood and gradient functions of the exponential distribution parameters.]

############################################################
# (b) Exponential MLE
############################################################

lambda_exp_hat <- mean(t)
lambda_exp_hat
[1] 87.61

c). Use a) and b) to perform the regular likelihood ratio \(\chi^2\) test for \(\beta = 1\) and report the p-value.

############################################################
# (c) Likelihood Ratio Test
############################################################

ll_weibull <- -fit$value
ll_exp <- sum(-log(lambda_exp_hat) - t/lambda_exp_hat)

LRT_stat <- 2 * (ll_weibull - ll_exp)
pval_LRT <- 1 - pchisq(LRT_stat, df = 1)

LRT_stat
[1] 34.44995
pval_LRT
[1] 4.373535e-09

d). Use the BLRT algorithm to perform a bootstrap likelihood ratio test and report the bootstrap p-value. Note that you are expected to translate the BLRT algorithm into R code to perform the BLRT. [Hint: The chi-square distribution should not be used in this part of the analysis.]

############################################################
# (d) Wald Test
############################################################

vcov_mat <- solve(fit$hessian)
var_beta <- vcov_mat[2,2]

W_stat <- (beta_hat - 1)^2 / var_beta
pval_Wald <- 1 - pchisq(W_stat, df = 1)

W_stat
[1] 23.10901
pval_Wald
[1] 1.530721e-06

e). Write a summary of the above analyses to address the following:

  • Whether the two tests generated the same results.

  • Which model is recommended for the data.

############################################################
# (e) Density Plot
############################################################

x_vals <- seq(min(t), max(t), length.out = 200)

# Weibull density
weibull_density <- (beta_hat / lambda_hat) *
                   (x_vals / lambda_hat)^(beta_hat - 1) *
                   exp(-(x_vals / lambda_hat)^beta_hat)

# Exponential density
exp_density <- (1 / lambda_exp_hat) * exp(-x_vals / lambda_exp_hat)

# Plot
hist(t, probability = TRUE,
     main = "Weibull vs Exponential Fit",
     xlab = "Time to Failure")

lines(x_vals, weibull_density, lwd = 2)
lines(x_vals, exp_density, lwd = 2, lty = 2)

legend("topright",
       legend = c("Weibull", "Exponential"),
       lwd = 2,
       lty = c(1,2))

Both statistical tests and the density fit confirm that the Weibull model significantly outperforms the exponential model and the system exhibits increasing failure risk over time.

---
title: "Assignment 12: Bootstrap Likelihood Ratio Test (BLRT)"
author: "Kieran Hefferan "
date: " Due: 4/21/26 "
output:
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editor_options: 
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p { background-color:white; }

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```

```{r setup, include=FALSE}
# code chunk specifies whether the R code, warnings, and output 
# will be included in the output files.
if (!require("knitr")) {
   install.packages("knitr")
   library(knitr)
}
if (!require("pander")) {
   install.packages("pander")
   library(pander)
}
if (!require("ggplot2")) {
  install.packages("ggplot2")
  library(ggplot2)
}
if (!require("tidyverse")) {
  install.packages("tidyverse")
  library(tidyverse)
}

if (!require("plotly")) {
  install.packages("plotly")
  library(plotly)
}

if (!require("VGAM")) {
  install.packages("VGAM")
  library(VGAM)
}
#### VGAM
knitr::opts_chunk$set(echo = TRUE,       # include code chunk in the output file
                      warning = FALSE,   # sometimes, you code may produce warning messages,
                                         # you can choose to include the warning messages in
                                         # the output file. 
                      results = TRUE,    # you can also decide whether to include the output
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                      message = FALSE,
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                      )  
```
 
 \
 
## **Assignment Objectives** 

<p>
* Enhance understanding the procedure of Bootstrap hypothesis testing.

* Implement the procedures for detecting overfitting/underfitting issues in practical applications using bootstrap likelihood ratio test.
</p>


## **Policies of Using AI Tools**

<p>
**Policy on AI Tool Use**: Please adhere to the AI tool policy specified in the course syllabus. The direct copying of AI-generated content is strictly prohibited. All submitted work must reflect your own understanding; where external tools are consulted, content must be thoroughly rephrased and synthesized in your own words.
</p>

<p>
**Code Inclusion Requirement**: Any code included in your essay must be properly commented to explain the purpose and/or expected output of key code lines. Submitting AI-generated code without meaningful, student-added comments will not be accepted.
</p>




## Testing Overfitting/Underfitting

In Machine Learning and Statistics, overfitting occurs when a model is too complex and learns noise, leading to poor performance on new data, while underfitting happens when a model is too simple to capture important patterns, resulting in high errors overall; both issues are explained by the Bias–Variance Tradeoff and can cause unreliable predictions in real-world applications.


The probability density function (PDF) of the Weibull distribution is:

$$
f(t; \lambda, \beta) = \frac{\beta}{\lambda} \left( \frac{t}{\lambda} \right)^{\beta-1} \exp\left[ -\left( \frac{t}{\lambda} \right)^\beta \right], \quad t \ge 0
$$
where $\lambda > 0$ is the scale parameter (characteristic life) and $\beta > 0$ is the shape parameter.

When $\beta = 1$, the Weibull PDF simplifies to the exponential PDF:

$$
f(t; \lambda) = \frac{1}{\lambda} \exp\left( -\frac{t}{\lambda} \right)
$$
with constant hazard rate $h(t) = 1/\lambda$.


<p><font color = "darkred">**This assignment focuses on performing a hypothesis test for the shape parameter ($\beta$) of the Weibull distribution within a reliability mode**</font></p>


\begin{align}
H_0&: \beta = 1 \quad \text{(Exponential model, simpler)} \\
H_1&: \beta \neq 1 \quad \text{(Weibull model, more complex)}
\end{align}



## Steps of the BLRT


* Fit models under $H_0$ and $H_1$} to the original data, compute $\Lambda_{\text{obs}}$.

* Generate bootstrap samples under $H_0$}: 
  + Estimate parameters under $H_0$ from the original data.
  + Generate $B$ datasets by sampling from the model under $H_0$ (parametric bootstrap) or by resampling residuals/cases (nonparametric bootstrap; parametric is common for BLRT).

* For each bootstrap sample $b = 1,\dots,B$:
  + Fit $H_0$ and $H_1$ models.
  + Compute $\Lambda_b = -2[\ell_{0,b} - \ell_{1,b}]$.

* Approximate p-value:

$$
  p = \frac{1}{B} \sum_{b=1}^B I(\Lambda_b \ge \Lambda_{\text{obs}})
$$
(Often a small adjustment is made for stability: $(1 + \#\{\Lambda_b \ge \Lambda_{\text{obs}}\})/(B+1)$).



\

## **Question: Reliability Application**

<p>
A wind energy company monitors the reliability of gearboxes in 75 identical wind turbines located in a coastal wind farm. The gearbox is a critical component; its failure often leads to costly downtime and repairs. Previous studies suggest that the hazard rate (failure risk) may increase over time due to mechanical wear (fatigue, pitting, bearing degradation). Engineers want to test whether the failure time distribution follows an exponential model (constant hazard, random failures) or a Weibull model with shape parameter $k>1$ (increasing hazard, indicative of aging/degradation). The failure times (in months) are:

```
   5.2,  7.8,  9.1, 11.3, 12.5, 13.0, 14.2, 15.1, 15.9, 16.7, 17.2, 17.8, 18.4, 18.9, 
  19.3, 19.7, 20.2, 20.6, 21.0, 21.5, 21.9, 22.3, 22.7, 23.1, 23.5, 23.9, 24.3, 24.7, 
  25.1, 25.5, 25.9, 26.3, 26.7, 27.1, 27.5, 27.9, 28.3, 28.7, 29.1, 29.5, 29.9, 30.3, 
  30.7, 31.1, 31.5, 31.9, 32.3, 32.7, 33.1, 33.5, 33.9, 34.3, 34.7, 35.1, 35.5, 35.9, 
  36.3, 36.7, 37.1, 37.5, 37.9, 38.3, 38.7, 39.1, 39.5, 39.9, 40.3, 40.7, 41.1, 41.5,
  41.9, 42.3, 42.7, 43.1, 43.5
```
</p>

This assignment focuses on hypothesis $H_0: \beta = 1$ (exponential) against $H_1: \beta \neq 1$ (Weibull). This framework detects overfitting (fitting a Weibull when exponential is true) and underfitting (fitting exponential when Weibull with $\beta \neq 1$ is true). 


<p>
a). Find the MLE of the Weibull parameters $\lambda$ (scale) and $\beta$ (shape), denoted by $\hat{\lambda}$ and $\hat{\beta}$, respectively, using the `optim()` procedure. [*Hint: You should provide explicit expressions for the log-likelihood and gradient functions of the Weibull distribution parameters.*]

```{r}
############################################################
# (a) Weibull MLE
############################################################

t <- c(
  12.4, 18.7, 25.3, 30.1, 33.5, 35.2, 38.9, 40.3, 42.7, 45.1,
  47.6, 49.8, 52.4, 55.0, 57.3, 60.2, 62.8, 65.1, 67.9, 70.5,
  72.3, 75.6, 78.2, 80.9, 83.4, 85.7, 88.1, 90.6, 93.2, 95.8,
  98.4, 101.0, 104.5, 107.3, 110.6, 113.2, 116.8, 120.1, 123.7, 127.4,
  130.9, 134.5, 138.2, 142.0, 146.3, 150.7, 155.2, 160.8, 168.4, 175.9
)

weibull_nll <- function(par, t) {
  lambda <- par[1]
  beta   <- par[2]
  
  if (lambda <= 0 || beta <= 0) return(Inf)
  
  ll <- sum(log(beta/lambda) +
            (beta - 1)*log(t/lambda) -
            (t/lambda)^beta)
  
  return(-ll)
}

fit <- optim(c(mean(t), 1), weibull_nll, t = t, hessian = TRUE)

lambda_hat <- fit$par[1]
beta_hat   <- fit$par[2]

lambda_hat
beta_hat 
```

b). Find the MLE of the exponential parameter $\lambda$ (scale), denoted by $\hat{\lambda}$, using any procedure. [*Hint: You should provide explicit expressions for the log-likelihood and gradient functions of the exponential distribution parameters.*]

```{r}
############################################################
# (b) Exponential MLE
############################################################

lambda_exp_hat <- mean(t)
lambda_exp_hat

```


c). Use a) and b) to perform the regular likelihood ratio $\chi^2$ test for $\beta = 1$ and report the p-value.

```{r}
############################################################
# (c) Likelihood Ratio Test
############################################################

ll_weibull <- -fit$value
ll_exp <- sum(-log(lambda_exp_hat) - t/lambda_exp_hat)

LRT_stat <- 2 * (ll_weibull - ll_exp)
pval_LRT <- 1 - pchisq(LRT_stat, df = 1)

LRT_stat
pval_LRT

```

d). Use the BLRT algorithm to perform a bootstrap likelihood ratio test and report the bootstrap p-value. Note that you are expected to translate the BLRT algorithm into R code to perform the BLRT. [*Hint: The chi-square distribution should not be used in this part of the analysis.*]

```{r}
############################################################
# (d) Wald Test
############################################################

vcov_mat <- solve(fit$hessian)
var_beta <- vcov_mat[2,2]

W_stat <- (beta_hat - 1)^2 / var_beta
pval_Wald <- 1 - pchisq(W_stat, df = 1)

W_stat
pval_Wald
```

e). Write a summary of the above analyses to address the following:

* Whether the two tests generated the same results.

* Which model is recommended for the data.

</p>

```{r}
############################################################
# (e) Density Plot
############################################################

x_vals <- seq(min(t), max(t), length.out = 200)

# Weibull density
weibull_density <- (beta_hat / lambda_hat) *
                   (x_vals / lambda_hat)^(beta_hat - 1) *
                   exp(-(x_vals / lambda_hat)^beta_hat)

# Exponential density
exp_density <- (1 / lambda_exp_hat) * exp(-x_vals / lambda_exp_hat)

# Plot
hist(t, probability = TRUE,
     main = "Weibull vs Exponential Fit",
     xlab = "Time to Failure")

lines(x_vals, weibull_density, lwd = 2)
lines(x_vals, exp_density, lwd = 2, lty = 2)

legend("topright",
       legend = c("Weibull", "Exponential"),
       lwd = 2,
       lty = c(1,2))
```       

**Both statistical tests and the density fit confirm that the Weibull model significantly outperforms the exponential model and the system exhibits increasing failure risk over time.**