Loading packages and
creating in the data set
We’ll start by loading the tidyverse:
Since the variance of the slope, \(b_1\), depends on \(S_{XX}\):
\[S_{XX} =
\sum_{i=1}^n(X_i-\bar{X})^2\]
We need to keep the \(X_i\) the same
throughout the simulation for each iteration. We’ll keep it simple and
let \(x_i = 2i\) with \(i = 1, ..., 10\)
X <- 2*(1:10)
X
## [1] 2 4 6 8 10 12 14 16 18 20
The \(S_{XX}\) is:
# S_XX = sum (X_i - X_bar)^2
S_XX <- sum((X - mean(X))^2)
S_XX
## [1] 330
When performing a simulation, we need to create a model to generate
our data. The population model for our simulation is:
\[Y_i = 20 + 40X_i + \varepsilon_i \\
\varepsilon_i \sim N(0, 660)\]
For each simulation we run, we’ll generate \(Y_i\) using the model above
Theoretical
distribution for \(b_1\)
According to the slides we saw in class, as long as
\[Y_i \sim N(\beta_0 + \beta_1 X_i,
\sigma^2)\]
are are independent, then the distribution of \(b_1\) is:
\[b_1 \sim N\left(\beta_1,
\frac{\sigma^2}{S_{XX}}\right)\]
Since we control the population, we know the distribution \(b_1\) for our example should follow:
\[b_1 \sim N\left(40,
\frac{660}{330}\right)\]
Simulating 10,000
samples of n = 10
We’ll generate 10,000 samples of 10 \(Y_i\) values each based on the model stated
above, which is theoretically akin to taking a random sample from a
population.
From each sample, we’ll save the following info:
- The sample
- \(b_0\)
- \(b_1\)
- \(SSE\)
# Simulation and sample sizes
m <- 1e5
sample_size <- 10
# Setting the parameters of the model
beta0 <- 20; beta1 <- 40; sigma2_e <- 660
# Data frame to save the result:
sim_df <-
data.frame(
sample = 1:m,
b0 = -100,
b1 = -100,
SSE = -1
)
Before we conduct the full simulation, let’s generate one sample and
calculate the stats needed as an example:
### Let's generate a random sample for sake of showing how:
set.seed(4210)
# The response from the model:
Y_loop <- beta0 + beta1 * X +
# Random error term
rnorm(sample_size, mean = 0, sd = sqrt(sigma2_e))
# Find b1:
b1_loop <-
# S_XY
sum((X - mean(X))*(Y_loop - mean(Y_loop))) / S_XX
# Finding b0:
b0_loop <- mean(Y_loop) - b1_loop * mean(X)
# Calculating y_hat
Y_hat_loop <- b0_loop + b1_loop * X
# Residuals:
res_loop <- Y_loop - Y_hat_loop
# SSE:
SSE_loop <- sum(res_loop^2)
# Now we'll save the results in the first row
sim_df[1, 2:ncol(sim_df)] <- c(b0_loop, b1_loop, SSE_loop)
tibble(sim_df)
## # A tibble: 100,000 × 4
## sample b0 b1 SSE
## <int> <dbl> <dbl> <dbl>
## 1 1 23.5 39.8 1657.
## 2 2 -100 -100 -1
## 3 3 -100 -100 -1
## 4 4 -100 -100 -1
## 5 5 -100 -100 -1
## 6 6 -100 -100 -1
## 7 7 -100 -100 -1
## 8 8 -100 -100 -1
## 9 9 -100 -100 -1
## 10 10 -100 -100 -1
## # ℹ 99,990 more rows
Now we’ll add the remaining sample stats to the data frame:
# Performing the simulation:
for (i in 2:m){
# The response from the model:
Y_loop <- beta0 + beta1 * X +
# Random error term
rnorm(sample_size, mean = 0, sd = sqrt(sigma2_e))
# Find b1:
b1_loop <- sum((X - mean(X))*(Y_loop - mean(Y_loop))) / S_XX
# Finding b0:
b0_loop <- mean(Y_loop) - b1_loop * mean(X)
# Calculating y_hat
Y_hat_loop <- b0_loop + b1_loop * X
# Residuals:
res_loop <- Y_loop - Y_hat_loop
# SSE:
SSE_loop <- sum(res_loop^2)
# Now we'll save the results in the first row
sim_df[i, 2:ncol(sim_df)] <- c(b0_loop, b1_loop, SSE_loop)
}
tibble(sim_df)
## # A tibble: 100,000 × 4
## sample b0 b1 SSE
## <int> <dbl> <dbl> <dbl>
## 1 1 23.5 39.8 1657.
## 2 2 16.1 41.0 3318.
## 3 3 28.9 38.7 5290.
## 4 4 57.0 37.9 2793.
## 5 5 24.6 40.2 2391.
## 6 6 19.8 39.6 4262.
## 7 7 13.7 40.4 2323.
## 8 8 40.0 38.4 3262.
## 9 9 10.3 40.1 3662.
## 10 10 -6.51 41.2 4166.
## # ℹ 99,990 more rows
Distribution of \(b_1\)
Let’s create a histogram of our simulated slopes and superimpose a
Normal curve on it.
Reminder: If the theory is correct, then:
\[b_1 \sim N\left(40,
\frac{660}{330}\right)\]
ggplot(
data = sim_df,
mapping = aes(
x = b1
)
) +
geom_histogram(
# Need to swap from count to density on the y-axis to place a normal curve
mapping = aes(y = after_stat(density)),
bins = 40,
fill = 'steelblue',
color = 'white'
) +
# Adding the Normal curve:
stat_function(
fun = dnorm,
args = list(mean = beta1, sd = sqrt(sigma2_e/S_XX)),
color = 'red',
linewidth = 1,
alpha = 0.5
) +
theme_bw() +
labs(
title = 'Histogram of simulated slopes'
) +
scale_y_continuous(
expand = c(0, 0, 0.05, 0)
)

Histogram looks pretty accurate!
What about the test statistics and p-values? Do they ‘line up’ with
what the theory says?
Result: If \(H_0\)
is true, then the p-value is a random variable that follows a uniform
distribution between 0 and 1:
\[\text{p-val} | H_0 \sim
\text{Uniform}(0, 1)\]
Type I error rate:
\(\sigma^2\) known
So if we calculate the test statistic and p-value for all of our
simulated samples, then 5% of our samples should give us a p-value below
0.05 (or whatever significance level you choose)
\[P(\text{p-val} < \alpha) =
\alpha\]
# Finding the p-values:
sim_df <-
sim_df |>
mutate(
# Test statistic
test_stat = (b1 - beta1) / sqrt(sigma2_e/S_XX),
# Now p-value for Beta1 =\= 40
p_val_sigma = 2*pnorm(abs(test_stat), lower.tail = F)
)
sim_df |>
dplyr::select(sample, b1, test_stat, p_val_sigma) |>
tibble()
## # A tibble: 100,000 × 4
## sample b1 test_stat p_val_sigma
## <int> <dbl> <dbl> <dbl>
## 1 1 39.8 -0.138 0.890
## 2 2 41.0 0.693 0.488
## 3 3 38.7 -0.937 0.349
## 4 4 37.9 -1.50 0.134
## 5 5 40.2 0.164 0.870
## 6 6 39.6 -0.259 0.795
## 7 7 40.4 0.255 0.799
## 8 8 38.4 -1.17 0.244
## 9 9 40.1 0.0506 0.960
## 10 10 41.2 0.849 0.396
## # ℹ 99,990 more rows
Let’s plot them and calculate the probability of rejecting a true
\(H_0\):
# Calculating the probability of a type 1 error
prob_type1_alpha_5 <- mean(sim_df$p_val_sigma < 0.05)
# How wide to make each bin
binwidth = 0.01
ggplot(
data = sim_df,
mapping = aes(
x = p_val_sigma,
fill = if_else(p_val_sigma < 0.05, 'tomato', 'steelblue')
)
) +
geom_histogram(
# Need to swap from count to density on the y-axis to place a normal curve
mapping = aes(y = after_stat(count) / (m * binwidth)),
breaks = seq(0, 1, binwidth),
#fill = 'steelblue',
color = 'white'
) +
# Adding the Uniform 'curve':
stat_function(
fun = dunif,
args = list(min = 0, max = 1),
color = 'red',
linewidth = 1,
alpha = 0.5
) +
# Adding the probability of Type 1
labs(
title = 'Distribution of p-values when Ho is true and sigma is known',
subtitle = paste('When alpha = 5% the chance of Type I error is',
scales::percent(prob_type1_alpha_5)),
caption = paste('Results from a simulation of', scales::comma(m),
'simulations each with a sample size of', sample_size),
x = 'P-value',
y = 'Density'
) +
theme_bw() +
scale_fill_identity() +
scale_y_continuous(
expand = c(0, 0, 0.05, 0)
)

The distribution above assumes we know what \(\sigma^2\) is, which we usually don’t. What
happens if we swap \(\sigma^2\) with
the MSE?
Type I error rate:
\(\sigma^2\)
unknown
Instead of using the standard deviation of \(b_1\), we’ll have to use the standard
error:
\[SE(b_1) =
\sqrt{\frac{MSE}{S_{XX}}}\]
We can calculate the \(MSE\) for
each sample by:
\[MSE = \frac{SSE}{n-2}\]
So let’s find the Standard error, test stat, and p-value using the
\(MSE\):
\[z = \frac{b_1 -
\beta_{1,0}}{\sqrt{\frac{MSE}{S_{XX}}}}\]
# Finding the p-values:
sim_df <-
sim_df |>
mutate(
MSE = SSE / (sample_size - 2),
# Test statistic using mse
test_stat_mse = (b1 - beta1) / sqrt(MSE/S_XX),
# Now p-value for Beta1 =\= 40
p_val_mse = 2*pnorm(abs(test_stat_mse), lower.tail = F)
)
sim_df |>
dplyr::select(sample, b1, MSE, test_stat_mse, p_val_mse) |>
tibble()
## # A tibble: 100,000 × 5
## sample b1 MSE test_stat_mse p_val_mse
## <int> <dbl> <dbl> <dbl> <dbl>
## 1 1 39.8 207. -0.246 0.806
## 2 2 41.0 415. 0.874 0.382
## 3 3 38.7 661. -0.936 0.349
## 4 4 37.9 349. -2.06 0.0396
## 5 5 40.2 299. 0.244 0.807
## 6 6 39.6 533. -0.289 0.773
## 7 7 40.4 290. 0.384 0.701
## 8 8 38.4 408. -1.48 0.138
## 9 9 40.1 458. 0.0607 0.952
## 10 10 41.2 521. 0.956 0.339
## # ℹ 99,990 more rows
Plot of the test
statistic using MSE instead of \(\sigma^2\)
The histogram of the test statistic is shown below. Does it look like
the Standard Normal distribution fit the histogram?
gg_test_stat_mse_hist <-
ggplot(
# There are a few extreme values, so we'll only look at -5 < z < 5
data = sim_df |>
filter(between(test_stat_mse, -5, 5)),
mapping = aes(
x = test_stat_mse
)
) +
geom_histogram(
# Need to swap from count to density on the y-axis to place a normal curve
mapping = aes(y = after_stat(density)),
bins = 40,
fill = 'steelblue',
color = 'white'
) +
theme_bw() +
labs(
title = paste('Histogram of', scales::comma(m), 'test statistics for the slope'),
subtitle = 'Calculated using the MSE',
x = 'Test statistics'
) +
scale_y_continuous(
expand = c(0, 0, 0.05, 0)
) +
scale_x_continuous(
breaks = -5:5
)
gg_test_stat_mse_hist +
# Adding the Normal curve:
stat_function(
fun = dnorm,
args = list(mean = 0, sd = 1),
color = 'red',
linewidth = 1,
alpha = 0.5
) +
labs(
caption = 'Standard Normal Distribution Overlayed on the Histogram'
)

The Normal curve looks close, but the middle bars are consistently
below the line while the tails are above the line. That typically
indicates that a wider distribution is needed instead of a Normal
distribution.
Let’s check the p-values as well!
Plot of the
p-values using MSE and Normal distribution
Again, plotting them and calculate the probability of rejecting a
true \(H_0\) assuming the test
statistic follows a Standard Normal:
# Calculating the probability of a type 1 error
prob_type1_alpha_5_mse <- mean(sim_df$p_val_mse < 0.05)
# Creating the graph
ggplot(
data = sim_df,
mapping = aes(
x = p_val_mse,
fill = if_else(p_val_mse < 0.05, 'tomato', 'steelblue'),
# group = 1
)
) +
geom_histogram(
# Need to swap from count to density on the y-axis to place a normal curve
mapping = aes(y = after_stat(count) / (m * binwidth)),
breaks = seq(0, 1, binwidth),
color = 'white'
) +
# Adding the Uniform 'curve':
stat_function(
fun = dunif,
args = list(min = 0, max = 1),
color = 'red',
linewidth = 1,
alpha = 0.5
) +
# Adding the probability of Type 1
labs(
title = 'Distribution of p-values when H0 is true, using a Normal with sigma unknown',
subtitle = paste('alpha = 5% and Type I probability is',
scales::percent(prob_type1_alpha_5_mse)),
caption = paste('Results from a simulation of', scales::comma(m),
'simulations each with a sample size of', sample_size),
x = 'P-value',
y = 'Density'
) +
theme_bw() +
scale_fill_identity() +
scale_y_continuous(
expand = c(0, 0, 0.05, 0)
)

Our chance of a Type I error is almost twice the significance level!
Why?
P-value using a
t-distribution
Like what you did waaaay back in your introductory stats class, when
you replace \(\sigma^2\) with its
sample statistic equivalent, the test statistic is no longer Normally
distributed.

Instead, the test stat will follow a **t-distribution* with degrees
of freedom equal to the denominator of the formula to calculate \(\hat{\sigma}^2\):
\[\hat{\sigma}^2 = \sqrt{\frac{SSE}{n -
2}}\]
So if we use \(MSE\) in place of
\(\sigma^2\), then the test statistic
will follow a t-distribution with \(n -
2\) degrees of freedom!
Histogram of the
test statistic with a t-distribution
gg_test_stat_mse_hist +
# Adding the Normal curve:
stat_function(
fun = dt,
args = list(df = sample_size - 2),
color = 'red',
linewidth = 1,
alpha = 0.5
) +
labs(
caption = paste('t-distribution with', sample_size - 2,
'df overlayed on the histogram')
)

The t-distribution fits great!
Histogram of
p-values using MSE and t-distribution
The code chunk below will calculate the p-value using the
t-distribution with df = 8:
# Finding the p-values:
sim_df <-
sim_df |>
mutate(
# Now p-value for Beta1 =\= 40 using a t-distribution
t_p_val = 2*pt(abs(test_stat_mse), df = sample_size - 2, lower.tail = F)
)
sim_df |>
dplyr::select(sample, b1, MSE, test_stat_mse, t_p_val) |>
tibble()
## # A tibble: 100,000 × 5
## sample b1 MSE test_stat_mse t_p_val
## <int> <dbl> <dbl> <dbl> <dbl>
## 1 1 39.8 207. -0.246 0.812
## 2 2 41.0 415. 0.874 0.407
## 3 3 38.7 661. -0.936 0.377
## 4 4 37.9 349. -2.06 0.0735
## 5 5 40.2 299. 0.244 0.813
## 6 6 39.6 533. -0.289 0.780
## 7 7 40.4 290. 0.384 0.711
## 8 8 38.4 408. -1.48 0.176
## 9 9 40.1 458. 0.0607 0.953
## 10 10 41.2 521. 0.956 0.367
## # ℹ 99,990 more rows
Again, plotting the p-values calculated above and calculate the
probability of rejecting a true \(H_0\)
assuming the test statistic follows a t-distribution:
# Calculating the probability of a type 1 error
prob_type1_alpha_5_t <- mean(sim_df$t_p_val < 0.05)
# Graph
ggplot(
data = sim_df,
mapping = aes(
x = t_p_val,
fill = if_else(t_p_val < 0.05, 'tomato', 'steelblue'),
# group = 1
)
) +
geom_histogram(
# Need to swap from count to density on the y-axis to place a normal curve
mapping = aes(y = after_stat(count) / (m * binwidth)),
breaks = seq(0, 1, binwidth),
color = 'white'
) +
# Adding the Uniform 'curve':
stat_function(
fun = dunif,
args = list(min = 0, max = 1),
color = 'red',
linewidth = 1,
alpha = 0.5
) +
# Adding the probability of Type 1
labs(
title = 'Distribution of p-values when Ho is true, using MSE, and t-distribution',
subtitle = paste('alpha = 5% and Type I probability is',
scales::percent(prob_type1_alpha_5_t)),
caption = paste('Results from a simulation of', scales::comma(m),
'simulations each with a sample size of', sample_size),
x = 'P-value',
y = 'Density'
) +
theme_bw() +
scale_fill_identity() +
scale_y_continuous(
expand = c(0, 0, 0.05, 0)
)

Now it matches!
---
title: "Distribution of the sample slope"
author: "Chapter 2"
date: "STA 4210"
output:
  html_document:
    fig_width: 8
    fig_height: 6
    fig_caption: yes
    number_sections: yes
    code_folding: hide
    code_download: yes
    smooth_scroll: yes
    theme: lumen
---

```{r setup, include=FALSE}
knitr::opts_chunk$set(echo = TRUE)
```

## Loading packages and creating in the data set

We'll start by loading the `tidyverse`:

```{r package, include=F, message=F, warning=F}
# Packages
library(tidyverse)
```

Since the variance of the slope, $b_1$, depends on $S_{XX}$:

$$S_{XX} = \sum_{i=1}^n(X_i-\bar{X})^2$$

We need to keep the $X_i$ the same throughout the simulation for each iteration. We'll keep it simple and let $x_i = 2i$ with $i = 1, ..., 10$

```{r pop_df}
X <- 2*(1:10)

X
```

The $S_{XX}$ is:

```{r S_XX}
# S_XX = sum (X_i - X_bar)^2
S_XX <- sum((X - mean(X))^2)
S_XX
```

When performing a simulation, we need to create a model to generate our data. The population model for our simulation is:

$$Y_i = 20 + 40X_i + \varepsilon_i \\ \varepsilon_i \sim N(0, 660)$$

For each simulation we run, we'll generate $Y_i$ using the model above

## Theoretical distribution for $b_1$

According to the slides we saw in class, as long as

$$Y_i \sim N(\beta_0 + \beta_1 X_i, \sigma^2)$$

are are independent, then the distribution of $b_1$ is:

$$b_1 \sim N\left(\beta_1, \frac{\sigma^2}{S_{XX}}\right)$$

Since we control the population, we know the distribution $b_1$ for our example should follow:

$$b_1 \sim N\left(40, \frac{660}{330}\right)$$

## Simulating 10,000 samples of n = 10

We'll generate 10,000 samples of 10 $Y_i$ values each based on the model stated above, which is theoretically akin to taking a random sample from a population.

From each sample, we'll save the following info:

1)  The sample
2)  $b_0$
3)  $b_1$
4)  $SSE$

```{r sim_df}
# Simulation and sample sizes
m <- 1e5
sample_size <- 10

# Setting the parameters of the model
beta0 <- 20; beta1 <- 40; sigma2_e <- 660

# Data frame to save the result:
sim_df <- 
  data.frame(
    sample = 1:m,
    b0 = -100,
    b1 = -100,
    SSE = -1
  )
```

Before we conduct the full simulation, let's generate one sample and calculate the stats needed as an example:

```{r sample_1}
### Let's generate a random sample for sake of showing how:
set.seed(4210)
# The response from the model:
Y_loop <- beta0 + beta1 * X + 
          # Random error term
          rnorm(sample_size, mean = 0, sd = sqrt(sigma2_e))

# Find b1:
b1_loop <- 
  # S_XY
  sum((X - mean(X))*(Y_loop - mean(Y_loop))) / S_XX

# Finding b0:
b0_loop <- mean(Y_loop) - b1_loop * mean(X)

# Calculating y_hat
Y_hat_loop <- b0_loop + b1_loop * X

# Residuals:
res_loop <- Y_loop - Y_hat_loop

# SSE:
SSE_loop <- sum(res_loop^2)

# Now we'll save the results in the first row
sim_df[1, 2:ncol(sim_df)] <- c(b0_loop, b1_loop, SSE_loop)


tibble(sim_df)
```

Now we'll add the remaining sample stats to the data frame:

```{r add_samples}
# Performing the simulation:
for (i in 2:m){
  # The response from the model:
  Y_loop <- beta0 + beta1 * X + 
            # Random error term
            rnorm(sample_size, mean = 0, sd = sqrt(sigma2_e))
  
  # Find b1:
  b1_loop <- sum((X - mean(X))*(Y_loop - mean(Y_loop))) / S_XX
  
  # Finding b0:
  b0_loop <- mean(Y_loop) - b1_loop * mean(X)
  
  # Calculating y_hat
  Y_hat_loop <- b0_loop + b1_loop * X
  
  # Residuals:
  res_loop <- Y_loop - Y_hat_loop
  
  # SSE:
  SSE_loop <- sum(res_loop^2)
  
  # Now we'll save the results in the first row
  sim_df[i, 2:ncol(sim_df)] <- c(b0_loop, b1_loop, SSE_loop)
}

tibble(sim_df)
```

## Distribution of $b_1$

Let's create a histogram of our simulated slopes and superimpose a Normal curve on it.

Reminder: If the theory is correct, then:

$$b_1 \sim N\left(40, \frac{660}{330}\right)$$

```{r}
ggplot(
  data = sim_df,
  mapping = aes(
    x = b1
  )
) + 
  geom_histogram(
    # Need to swap from count to density on the y-axis to place a normal curve
    mapping = aes(y = after_stat(density)),
    bins = 40,
    fill = 'steelblue',
    color = 'white'
  ) + 
  # Adding the Normal curve:
  stat_function(
    fun = dnorm,
    args = list(mean = beta1, sd = sqrt(sigma2_e/S_XX)),
    color = 'red',
    linewidth = 1,
    alpha = 0.5
  ) + 
  theme_bw()  +
  labs(
    title = 'Histogram of simulated slopes'
  ) + 
  scale_y_continuous(
    expand = c(0, 0, 0.05, 0)
  )
  
```

Histogram looks pretty accurate!

What about the test statistics and p-values? Do they 'line up' with what the theory says?

**Result**: If $H_0$ is true, then the p-value is a random variable that follows a uniform distribution between 0 and 1:

$$\text{p-val} | H_0 \sim \text{Uniform}(0, 1)$$

### Type I error rate: $\sigma^2$ known

So if we calculate the test statistic and p-value for all of our simulated samples, then 5% of our samples should give us a p-value below 0.05 (or whatever significance level you choose)

$$P(\text{p-val} < \alpha) = \alpha$$

```{r p_val_sim_sigma_known}
# Finding the p-values:
sim_df <- 
  sim_df |>
  mutate(
    # Test statistic
    test_stat = (b1 - beta1) / sqrt(sigma2_e/S_XX),
    # Now p-value for Beta1 =\= 40
    p_val_sigma = 2*pnorm(abs(test_stat), lower.tail = F)
  )

sim_df |>
  dplyr::select(sample, b1, test_stat, p_val_sigma) |>
  tibble()
```

Let's plot them and calculate the probability of rejecting a true $H_0$:

```{r p_val_plot, warning = F}
# Calculating the probability of a type 1 error
prob_type1_alpha_5 <- mean(sim_df$p_val_sigma < 0.05)

# How wide to make each bin
binwidth = 0.01

ggplot(
  data = sim_df,
  mapping = aes(
    x = p_val_sigma,
    fill = if_else(p_val_sigma < 0.05, 'tomato', 'steelblue')
  )
) + 
  geom_histogram(
    # Need to swap from count to density on the y-axis to place a normal curve
    mapping = aes(y = after_stat(count) / (m * binwidth)),
    breaks = seq(0, 1, binwidth),
    #fill = 'steelblue',
    color = 'white'
  ) + 
  # Adding the Uniform 'curve':
  stat_function(
    fun = dunif,
    args = list(min = 0, max = 1),
    color = 'red',
    linewidth = 1,
    alpha = 0.5
  ) + 
  # Adding the probability of Type 1
  labs(
    title = 'Distribution of p-values when Ho is true and sigma is known',
    subtitle = paste('When alpha = 5% the chance of Type I error is', 
                     scales::percent(prob_type1_alpha_5)),
    caption = paste('Results from a simulation of', scales::comma(m), 
                    'simulations each with a sample size of', sample_size),
    x = 'P-value',
    y = 'Density'
  ) +
  theme_bw()  +
  scale_fill_identity() + 
  scale_y_continuous(
    expand = c(0, 0, 0.05, 0)
  )
```

The distribution above assumes we know what $\sigma^2$ is, which we usually don't. What happens if we swap $\sigma^2$ with the MSE?




### Type I error rate: $\sigma^2$ **unknown**

Instead of using the standard deviation of $b_1$, we'll have to use the standard error:

$$SE(b_1) = \sqrt{\frac{MSE}{S_{XX}}}$$

We can calculate the $MSE$ for each sample by:

$$MSE = \frac{SSE}{n-2}$$

So let's find the Standard error, test stat, and p-value using the $MSE$:

$$z = \frac{b_1 - \beta_{1,0}}{\sqrt{\frac{MSE}{S_{XX}}}}$$

```{r p_val_sim_MSE}
# Finding the p-values:
sim_df <- 
  sim_df |>
  mutate(
    MSE = SSE / (sample_size - 2),
    # Test statistic using mse
    test_stat_mse = (b1 - beta1) / sqrt(MSE/S_XX),
    # Now p-value for Beta1 =\= 40
    p_val_mse = 2*pnorm(abs(test_stat_mse), lower.tail = F)
  )

sim_df |>
  dplyr::select(sample, b1, MSE, test_stat_mse, p_val_mse) |>
  tibble()
```

#### Plot of the test statistic using MSE instead of $\sigma^2$

The histogram of the test statistic is shown below. Does it look like the Standard Normal distribution fit the histogram?

```{r test_stat_hist_mse_normal}
gg_test_stat_mse_hist <- 
  ggplot(
    # There are a few extreme values, so we'll only look at -5 < z < 5
    data = sim_df |>
      filter(between(test_stat_mse, -5, 5)),
    mapping = aes(
      x = test_stat_mse
    )
  ) + 
  geom_histogram(
    # Need to swap from count to density on the y-axis to place a normal curve
    mapping = aes(y = after_stat(density)),
    bins = 40,
    fill = 'steelblue',
    color = 'white'
  ) + 
  theme_bw()  +
  labs(
    title = paste('Histogram of', scales::comma(m), 'test statistics for the slope'),
    subtitle = 'Calculated using the MSE',
    x = 'Test statistics'
  ) + 
  scale_y_continuous(
    expand = c(0, 0, 0.05, 0)
  ) + 
  scale_x_continuous(
    breaks = -5:5
  )


gg_test_stat_mse_hist + 
  # Adding the Normal curve:
  stat_function(
    fun = dnorm,
    args = list(mean = 0, sd = 1),
    color = 'red',
    linewidth = 1,
    alpha = 0.5
  ) + 
  labs(
    caption = 'Standard Normal Distribution Overlayed on the Histogram'
  )
```

The Normal curve looks close, but the middle bars are consistently below the line while the tails are above the line. That typically indicates that a wider distribution is needed instead of a Normal distribution.

Let's check the p-values as well!

#### Plot of the p-values using MSE and Normal distribution

Again, plotting them and calculate the probability of rejecting a true $H_0$ assuming the test statistic follows a Standard Normal:

```{r p_val_plot_mse, warning = F}
# Calculating the probability of a type 1 error
prob_type1_alpha_5_mse <- mean(sim_df$p_val_mse < 0.05)

# Creating the graph
ggplot(
  data = sim_df,
  mapping = aes(
    x = p_val_mse,
    fill = if_else(p_val_mse < 0.05, 'tomato', 'steelblue'),
   # group = 1
  )
) + 
  geom_histogram(
    # Need to swap from count to density on the y-axis to place a normal curve
    mapping = aes(y = after_stat(count) / (m * binwidth)),
    breaks = seq(0, 1, binwidth),
    color = 'white'
  ) + 
  # Adding the Uniform 'curve':
  stat_function(
    fun = dunif,
    args = list(min = 0, max = 1),
    color = 'red',
    linewidth = 1,
    alpha = 0.5
  ) + 
  # Adding the probability of Type 1
  labs(
    title = 'Distribution of p-values when H0 is true, using a Normal with sigma unknown',
    subtitle = paste('alpha = 5% and Type I probability is', 
                     scales::percent(prob_type1_alpha_5_mse)),
    caption = paste('Results from a simulation of', scales::comma(m), 
                    'simulations each with a sample size of', sample_size),
    x = 'P-value',
    y = 'Density'
  ) +
  theme_bw()  +
  scale_fill_identity() + 
  scale_y_continuous(
    expand = c(0, 0, 0.05, 0)
  )
```

Our chance of a Type I error is almost twice the significance level! Why?

### P-value using a t-distribution

Like what you did waaaay back in your introductory stats class, when you replace $\sigma^2$ with its sample statistic equivalent, the test statistic is no longer Normally distributed.

![](https://encrypted-tbn0.gstatic.com/images?q=tbn:ANd9GcQ3f9Ig7B5nddPtupa9CsXBn5kWwlX8xSiD2pOh4ML-FBiJLbKS8baMljo&s=10){width="50%" height="50%"}

Instead, the test stat will follow a \*\*t-distribution\* with degrees of freedom equal to the denominator of the formula to calculate $\hat{\sigma}^2$:

$$\hat{\sigma}^2 = \sqrt{\frac{SSE}{n - 2}}$$

So if we use $MSE$ in place of $\sigma^2$, then the test statistic will follow a t-distribution with $n - 2$ degrees of freedom!

#### Histogram of the test statistic with a t-distribution

```{r test_stat_t_dist}
gg_test_stat_mse_hist + 
  # Adding the Normal curve:
  stat_function(
    fun = dt,
    args = list(df = sample_size - 2),
    color = 'red',
    linewidth = 1,
    alpha = 0.5
  ) + 
  labs(
    caption = paste('t-distribution with', sample_size - 2, 
                    'df overlayed on the histogram')
  )
```

The t-distribution fits great!

#### Histogram of p-values using MSE and t-distribution

The code chunk below will calculate the p-value using the t-distribution with df = 8:

```{r p_val_sim_tdist}
# Finding the p-values:
sim_df <- 
  sim_df |>
  mutate(
    # Now p-value for Beta1 =\= 40 using a t-distribution
    t_p_val = 2*pt(abs(test_stat_mse), df = sample_size - 2, lower.tail = F)
  )

sim_df |>
  dplyr::select(sample, b1, MSE, test_stat_mse, t_p_val) |>
  tibble()
```

Again, plotting the p-values calculated above and calculate the probability of rejecting a true $H_0$ assuming the test statistic follows a t-distribution:

```{r p_val_plot_tdist, warning = F}
# Calculating the probability of a type 1 error
prob_type1_alpha_5_t <- mean(sim_df$t_p_val < 0.05)

# Graph
ggplot(
  data = sim_df,
  mapping = aes(
    x = t_p_val,
    fill = if_else(t_p_val < 0.05, 'tomato', 'steelblue'),
   # group = 1
  )
) + 
  geom_histogram(
    # Need to swap from count to density on the y-axis to place a normal curve
    mapping = aes(y = after_stat(count) / (m * binwidth)),
    breaks = seq(0, 1, binwidth),
    color = 'white'
  ) + 
  # Adding the Uniform 'curve':
  stat_function(
    fun = dunif,
    args = list(min = 0, max = 1),
    color = 'red',
    linewidth = 1,
    alpha = 0.5
  ) + 
  # Adding the probability of Type 1
  labs(
    title = 'Distribution of p-values when Ho is true, using MSE, and t-distribution',
    subtitle = paste('alpha = 5% and Type I probability is', 
                     scales::percent(prob_type1_alpha_5_t)),
    caption = paste('Results from a simulation of', scales::comma(m), 
                    'simulations each with a sample size of', sample_size),
    x = 'P-value',
    y = 'Density'
  ) +
  theme_bw()  +
  scale_fill_identity() + 
  scale_y_continuous(
    expand = c(0, 0, 0.05, 0)
  )
```

Now it matches!
