The aatemp data come from the U.S. Historical Climatology Network. They are the annual mean temperatures (in degrees F) in Ann Arbor, Michigan going back about 150 years.

a. Is there a linear trend?

attach(aatemp)
The following objects are masked from aatemp (pos = 3):

    temp, year
lmod<-lm(temp~year)
summary(lmod)

Call:
lm(formula = temp ~ year)

Residuals:
    Min      1Q  Median      3Q     Max 
-3.9843 -0.9113 -0.0820  0.9946  3.5343 

Coefficients:
             Estimate Std. Error t value Pr(>|t|)   
(Intercept) 24.005510   7.310781   3.284  0.00136 **
year         0.012237   0.003768   3.247  0.00153 **
---
Signif. codes:  0 ‘***’ 0.001 ‘**’ 0.01 ‘*’ 0.05 ‘.’ 0.1 ‘ ’ 1

Residual standard error: 1.466 on 113 degrees of freedom
Multiple R-squared:  0.08536,   Adjusted R-squared:  0.07727 
F-statistic: 10.55 on 1 and 113 DF,  p-value: 0.001533
# par(mfrow=c(2,2))
plot(lmod)

abline(h=0)

From the first diagnostic graph (Residuals vs. fitted) above, I do see that the trend is linear, and it isn’t homoscedastic or is it non-linear.

In the Normal Q-Q plot, normal residuals should follow the line approximately. Here, the residuals look normal.

par(mfrow=c(1,1))
plot(temp~year)
abline(coefficients(lmod))

NA
NA

Ans: So the trend is a linear trend.

b. Observations in successive years may be correlated. Fit a model that estimates this correlation. Does this change your opinion about the trend?

n <- length(residuals(lmod))
plot(tail(residuals(lmod),n-1) ~ head(residuals(lmod),n-1), xlab=
expression(hat(epsilon)[i]),ylab=expression(hat(epsilon)[i+1]))
abline(h=0,v=0,col=grey(0.75))

Model to estimate the significance of correlation.

summary(lm(tail(residuals(lmod), n-1) ~ head(residuals(lmod), n-1)-1))

Ans: Serial correlation is not confirmed.

c. Fit a polynomial model with degree 10 and use backward elimination to reduce the degree of the model. Plot your fitted model on top of the data. Use this model to predict the temperature in 2020.

As there is no step or stepAIC function that is bespoke for polynomial terms, I don’t think I can easily use backward elimination method to reduce the degree of the model. Please refer to my codes below as I progressively create polynomial terms in decreasing fashion and leverage anova function to compare all of them collectively.

library(MASS)
lmod_poly_10<-lm(temp ~ poly(year,10), data=aatemp)
lmod_poly_9 <- lm(temp ~ poly(year,9), data=aatemp)
lmod_poly_8 <- lm(temp ~ poly(year,8), data=aatemp)
lmod_poly_7 <- lm(temp ~ poly(year,7), data=aatemp)
lmod_poly_6 <- lm(temp ~ poly(year,6), data=aatemp)
lmod_poly_5 <- lm(temp ~ poly(year,5), data=aatemp)
lmod_poly_4 <- lm(temp ~ poly(year,4), data=aatemp)
lmod_poly_3 <- lm(temp ~ poly(year,3), data=aatemp)
lmod_poly_2 <- lm(temp ~ poly(year,2), data=aatemp)
lmod_poly_1 <- lm(temp ~ poly(year,1), data=aatemp)
print(anova(lmod_poly_10,lmod_poly_9,lmod_poly_8,lmod_poly_7,lmod_poly_6, lmod_poly_5, lmod_poly_4, lmod_poly_3, lmod_poly_2, lmod_poly_1))
Analysis of Variance Table

Model  1: temp ~ poly(year, 10)
Model  2: temp ~ poly(year, 9)
Model  3: temp ~ poly(year, 8)
Model  4: temp ~ poly(year, 7)
Model  5: temp ~ poly(year, 6)
Model  6: temp ~ poly(year, 5)
Model  7: temp ~ poly(year, 4)
Model  8: temp ~ poly(year, 3)
Model  9: temp ~ poly(year, 2)
Model 10: temp ~ poly(year, 1)
   Res.Df    RSS Df Sum of Sq      F  Pr(>F)  
1     104 208.11                              
2     105 208.24 -1   -0.1207 0.0603 0.80652  
3     106 210.19 -1   -1.9583 0.9786 0.32483  
4     107 211.41 -1   -1.2124 0.6059 0.43812  
5     108 212.28 -1   -0.8784 0.4390 0.50908  
6     109 213.75 -1   -1.4700 0.7346 0.39337  
7     110 225.19 -1  -11.4404 5.7171 0.01860 *
8     111 231.14 -1   -5.9455 2.9711 0.08774 .
9     112 242.12 -1  -10.9776 5.4858 0.02108 *
10    113 242.94 -1   -0.8228 0.4112 0.52277  
---
Signif. codes:  0 ‘***’ 0.001 ‘**’ 0.01 ‘*’ 0.05 ‘.’ 0.1 ‘ ’ 1
# lmod_poly_10a <- lm(temp ~ year + I(year^2) + I(year^3) + I(year^4) + I(year^5) + I(year^6) + I(year^7) + I(year^8) + I(year^9) + I(year^10), data=aatemp)

# summary(lmod_poly_10)
# summary(lmod_poly_10a)

Since p-values for model 7 and mode 9 are significant. I picked out poly(year, 4) and poly(year, 2) to examine their other successful metrics to see which one to use.

summary(lmod_poly_4)

Call:
lm(formula = temp ~ poly(year, 4), data = aatemp)

Residuals:
    Min      1Q  Median      3Q     Max 
-4.0085 -0.9618 -0.0913  0.9926  3.7370 

Coefficients:
               Estimate Std. Error t value Pr(>|t|)    
(Intercept)     47.7426     0.1334 357.827  < 2e-16 ***
poly(year, 4)1   4.7616     1.4308   3.328  0.00119 ** 
poly(year, 4)2  -0.9071     1.4308  -0.634  0.52741    
poly(year, 4)3  -3.3132     1.4308  -2.316  0.02243 *  
poly(year, 4)4   2.4383     1.4308   1.704  0.09117 .  
---
Signif. codes:  0 ‘***’ 0.001 ‘**’ 0.01 ‘*’ 0.05 ‘.’ 0.1 ‘ ’ 1

Residual standard error: 1.431 on 110 degrees of freedom
Multiple R-squared:  0.1522,    Adjusted R-squared:  0.1213 
F-statistic: 4.936 on 4 and 110 DF,  p-value: 0.001068
# print(coef(summary(lmod_poly_4)))

step(object = lmod_poly_4, direction = "backward")
Start:  AIC=87.28
temp ~ poly(year, 4)

                Df Sum of Sq    RSS    AIC
<none>                       225.19 87.284
- poly(year, 4)  4    40.418 265.61 98.267

Call:
lm(formula = temp ~ poly(year, 4), data = aatemp)

Coefficients:
   (Intercept)  poly(year, 4)1  poly(year, 4)2  poly(year, 4)3  poly(year, 4)4  
       47.7426          4.7616         -0.9071         -3.3132          2.4383  
# print(coef(summary(lmod_poly_2)))
summary(lmod_poly_2)

Call:
lm(formula = temp ~ poly(year, 2), data = aatemp)

Residuals:
    Min      1Q  Median      3Q     Max 
-4.0412 -0.9538 -0.0624  0.9959  3.5820 

Coefficients:
               Estimate Std. Error t value Pr(>|t|)    
(Intercept)     47.7426     0.1371 348.218  < 2e-16 ***
poly(year, 2)1   4.7616     1.4703   3.239  0.00158 ** 
poly(year, 2)2  -0.9071     1.4703  -0.617  0.53851    
---
Signif. codes:  0 ‘***’ 0.001 ‘**’ 0.01 ‘*’ 0.05 ‘.’ 0.1 ‘ ’ 1

Residual standard error: 1.47 on 112 degrees of freedom
Multiple R-squared:  0.08846,   Adjusted R-squared:  0.07218 
F-statistic: 5.434 on 2 and 112 DF,  p-value: 0.005591
step(object = lmod_poly_2, direction = "backward")
Start:  AIC=91.62
temp ~ poly(year, 2)

                Df Sum of Sq    RSS    AIC
<none>                       242.12 91.616
- poly(year, 2)  2    23.495 265.61 98.267

Call:
lm(formula = temp ~ poly(year, 2), data = aatemp)

Coefficients:
   (Intercept)  poly(year, 2)1  poly(year, 2)2  
       47.7426          4.7616         -0.9071  

As polynomial with degree 4 has a lower AIC and a higher adjusted R-square at 12.13%, I conclude that I will go with degree 4 polynomial.

Here we plot the data along with the fitted model

# step(object = lmod_poly_10, direction = "backward")
# 
# final_lmod_poly_10 <- stepAIC(lmod_poly_10, direction = 'backward')
# 
# summary(final_lmod_poly_10)
# 
# final_lmod_poly_10 <- stepAIC(final_lmod_poly_10, direction = 'backward')

plot(temp~year)
points(year, fitted(lmod_poly_4),col="orange", pch=20)

Let’s predict the temperature in 2020.

predict(lmod_poly_4, new_data)
     1 
49.559 

Ans: So the predicted temperature in year 2020 is 49.559.

d. Suppose someone claims that the temperature was constant until 1930 and then began a linear trend. Fit a model corresponding to this claim. What does the fitted model say about this claim?

Inserting a vertical line when year = 1930.

plot(temp~year,aatemp,xlab="Year",ylab="Temperature", main="Annual Temperature distribution in Ann Arbor, MI")
abline(v=1930, lty=6)

# aatemp[which(aatemp$year == 1930), ]

constant<-function(x)ifelse(x<=1930, mean(aatemp[1:49,]$temp),0)
lienar_mod<-function(x)ifelse(x>1930, x-1930,0)
model<-lm(temp~constant(year)+lienar_mod(year),aatemp)
x<-seq(1854,2000,by=1)
additive_model<-model$coef[1]+model$coef[2]*constant(x)+model$coef[3]*lienar_mod(x)
lines(x,additive_model,lty=2)

summary(model)

Call:
lm(formula = temp ~ constant(year) + lienar_mod(year), data = aatemp)

Residuals:
    Min      1Q  Median      3Q     Max 
-3.5867 -0.9456 -0.0979  1.0233  3.9925 

Coefficients:
                  Estimate Std. Error t value Pr(>|t|)    
(Intercept)      48.748738   0.343152 142.062  < 2e-16 ***
constant(year)   -0.037279   0.008423  -4.426 2.24e-05 ***
lienar_mod(year) -0.012519   0.008248  -1.518    0.132    
---
Signif. codes:  0 ‘***’ 0.001 ‘**’ 0.01 ‘*’ 0.05 ‘.’ 0.1 ‘ ’ 1

Residual standard error: 1.381 on 112 degrees of freedom
Multiple R-squared:  0.1954,    Adjusted R-squared:  0.181 
F-statistic:  13.6 on 2 and 112 DF,  p-value: 5.167e-06

Ans: From the summary of the additive model (model), it does look like this particular claim is warranted as there is indications that the constant(year) portion of the linear model is statistical significant.

e. Make a cubic spline fit with six basis functions evenly spaced on the range. Plot the fit in comparison to the previous fits. Does this model fit better than the straight-line model?

Choosing knots given the goal to fit with a cubic spline with 6 basis functions

Visualizing the basis functions…

require(splines)
# Visualizing the basis functions
attr(bs(year ,df=6) ,"knots")
   25%    50%    75% 
1910.5 1939.0 1971.5 
dim(bs(year ,knots=c(1910.5, 1939.0, 1971.5) ))
[1] 115   6
bs_temp <- bs(year ,knots=c(1910.5, 1939.0, 1971.5) )
matplot(year, bs_temp, type="l", col=1, main="Visualizing basis functions")

Confirmed that the B-Spline Basis for polynomial Splines, called with bs(), has a dimension of 6. Recall that a cubic spline with three knots has seven degrees of freedom; these degrees of freedom are used up by an intercept, plus six basis functions. We could also use the df option to produce a spline with knots at uniform quantiles of the data. Since the requirement is for a cubic spline, we used the default degree of 3.

dim(bs(year ,df=6))
[1] 115   6

cs_fit <- lm(temp~bs(year ,df=6), data=aatemp)

yearlims =range(year)
year.grid=seq (from=yearlims [1], to=yearlims [2])

pred=predict (cs_fit ,newdata =list(year =year.grid),se=T)
plot(year ,temp ,col ="gray")
lines(year.grid ,pred$fit ,lwd =4)
lines(year.grid ,pred$fit +2* pred$se ,lty ="dashed")
lines(year.grid ,pred$fit -2* pred$se ,lty ="dashed")

# matplot(year, cbind(temp,cs_fit$fit), type="pl", ylab="year", pch=20,lty=1,col=1)
summary(cs_fit)

Call:
lm(formula = temp ~ bs(year, df = 6), data = aatemp)

Residuals:
    Min      1Q  Median      3Q     Max 
-3.6561 -0.9270 -0.1545  0.9551  3.2158 

Coefficients:
                  Estimate Std. Error t value Pr(>|t|)    
(Intercept)        47.8876     1.0083  47.493   <2e-16 ***
bs(year, df = 6)1  -0.2200     1.8374  -0.120   0.9049    
bs(year, df = 6)2  -2.3188     1.2635  -1.835   0.0692 .  
bs(year, df = 6)3   0.9948     1.2497   0.796   0.4278    
bs(year, df = 6)4   0.8136     1.2814   0.635   0.5268    
bs(year, df = 6)5  -1.1798     1.3381  -0.882   0.3799    
bs(year, df = 6)6   1.3563     1.2623   1.074   0.2850    
---
Signif. codes:  0 ‘***’ 0.001 ‘**’ 0.01 ‘*’ 0.05 ‘.’ 0.1 ‘ ’ 1

Residual standard error: 1.401 on 108 degrees of freedom
Multiple R-squared:  0.2017,    Adjusted R-squared:  0.1573 
F-statistic: 4.547 on 6 and 108 DF,  p-value: 0.0003774

Ans: No. This cubic spline model doesn’t fit better than the straight line model as its adjusted R-squared is lower at 15.73%.

---
title: "Ex 9.7.1"
output:
  html_notebook:
    code_folding: hide
  html_document:
    df_print: paged
    code_folding: hide
  pdf_document: default
---

The `aatemp` data come from the U.S. Historical Climatology Network. They are the annual mean temperatures (in degrees F) in Ann Arbor, Michigan going back about 150 years.

## a. Is there a linear trend?

```{r}
data(aatemp, package='faraway')
attach(aatemp)
```

```{r}
lmod<-lm(temp~year)
summary(lmod)
```

```{r}
# par(mfrow=c(2,2))
plot(lmod)
abline(h=0)
```

From the first diagnostic graph *(Residuals vs. fitted)* above, I do see that the trend is linear, and it isn't homoscedastic or is it non-linear.

In the Normal Q-Q plot, normal residuals should follow the line approximately. Here, the residuals look normal.

```{r}
par(mfrow=c(1,1))
plot(temp~year)
abline(coefficients(lmod))


```

*Ans*: So the trend is a linear trend.

## b. Observations in successive years may be correlated. Fit a model that estimates this correlation. Does this change your opinion about the trend?

```{r}
n <- length(residuals(lmod))
plot(tail(residuals(lmod),n-1) ~ head(residuals(lmod),n-1), xlab=
expression(hat(epsilon)[i]),ylab=expression(hat(epsilon)[i+1]))
abline(h=0,v=0,col=grey(0.75))
```

Model to estimate the significance of correlation.

```{r}
summary(lm(tail(residuals(lmod), n-1) ~ head(residuals(lmod), n-1)-1))
```

*Ans*: Serial correlation is not confirmed.

## c. Fit a polynomial model with degree 10 and use backward elimination to reduce the degree of the model. Plot your fitted model on top of the data. Use this model to predict the temperature in 2020.

As there is no step or stepAIC function that is bespoke for polynomial terms, I don't think I can easily use backward elimination method to reduce the degree of the model. Please refer to my codes below as I progressively create polynomial terms in decreasing fashion and leverage anova function to compare all of them collectively.

```{r}
library(MASS)
lmod_poly_10<-lm(temp ~ poly(year,10), data=aatemp)
lmod_poly_9 <- lm(temp ~ poly(year,9), data=aatemp)
lmod_poly_8 <- lm(temp ~ poly(year,8), data=aatemp)
lmod_poly_7 <- lm(temp ~ poly(year,7), data=aatemp)
lmod_poly_6 <- lm(temp ~ poly(year,6), data=aatemp)
lmod_poly_5 <- lm(temp ~ poly(year,5), data=aatemp)
lmod_poly_4 <- lm(temp ~ poly(year,4), data=aatemp)
lmod_poly_3 <- lm(temp ~ poly(year,3), data=aatemp)
lmod_poly_2 <- lm(temp ~ poly(year,2), data=aatemp)
lmod_poly_1 <- lm(temp ~ poly(year,1), data=aatemp)
print(anova(lmod_poly_10,lmod_poly_9,lmod_poly_8,lmod_poly_7,lmod_poly_6, lmod_poly_5, lmod_poly_4, lmod_poly_3, lmod_poly_2, lmod_poly_1))

# lmod_poly_10a <- lm(temp ~ year + I(year^2) + I(year^3) + I(year^4) + I(year^5) + I(year^6) + I(year^7) + I(year^8) + I(year^9) + I(year^10), data=aatemp)

# summary(lmod_poly_10)
# summary(lmod_poly_10a)
print(coef(summary(lmod_poly_4)))
```

Since p-values for model 7 and mode 9 are significant. I picked out poly(year, 4) and poly(year, 2) to examine their other successful metrics to see which one to use.

```{r}
summary(lmod_poly_4)
# print(coef(summary(lmod_poly_4)))

step(object = lmod_poly_4, direction = "backward")
```

```{r}
# print(coef(summary(lmod_poly_2)))
summary(lmod_poly_2)

step(object = lmod_poly_2, direction = "backward")
```

As polynomial with degree 4 has a lower AIC and a higher adjusted R-square at 12.13%, I conclude that I will go with degree 4 polynomial.

Here we plot the data along with the fitted model

```{r}
# step(object = lmod_poly_10, direction = "backward")
# 
# final_lmod_poly_10 <- stepAIC(lmod_poly_10, direction = 'backward')
# 
# summary(final_lmod_poly_10)
# 
# final_lmod_poly_10 <- stepAIC(final_lmod_poly_10, direction = 'backward')

plot(temp~year)
points(year, fitted(lmod_poly_4),col="orange", pch=20)
```

Let's predict the temperature in 2020.

```{r}
# str(aatemp)
# predict(lmod_poly_4, aatemp, interval="predict")


# predicted.intervals <- predict(lmod_poly_4,data.frame(x=t(c(1854:2020))),interval='predict',
#                                level=0.99)
# 
# summary(lmod_poly_4)
# X <- 2020
# temp_pred = coef(summary(lmod_poly_4))[[1]] + coef(summary(lmod_poly_4))[[2]]*X + coef(summary(lmod_poly_4))[[3]]*X + coef(summary(lmod_poly_4))[[4]]*X + coef(summary(lmod_poly_4))[[5]]*X
# temp_pred

new_data <- data.frame('year'=c(2020))
predict(lmod_poly_4, new_data)

```

*Ans*: So the predicted temperature in year 2020 is 49.559.

## d. Suppose someone claims that the temperature was constant until 1930 and then began a linear trend. Fit a model corresponding to this claim. What does the fitted model say about this claim?

```{r}

fit1<-lm(temp~year, aatemp,subset=(year<=1930))
fit2<-lm(temp~year, aatemp,subset=(year>1930))
plot(fit1)

```

```{r}
plot(fit2)
```

Inserting a vertical line when year = 1930.

```{r}
plot(temp~year,aatemp,xlab="Year",ylab="Temperature", main="Annual Temperature distribution in Ann Arbor, MI")
abline(v=1930, lty=6)

# aatemp[which(aatemp$year == 1930), ]

constant<-function(x)ifelse(x<=1930, mean(aatemp[1:49,]$temp),0)
lienar_mod<-function(x)ifelse(x>1930, x-1930,0)
model<-lm(temp~constant(year)+lienar_mod(year),aatemp)
x<-seq(1854,2000,by=1)
additive_model<-model$coef[1]+model$coef[2]*constant(x)+model$coef[3]*lienar_mod(x)
lines(x,additive_model,lty=2)
```

```{r}
summary(model)
```

*Ans*: From the summary of the additive model (*model*), it does look like this particular claim is warranted as there is indications that the constant(year) portion of the linear model is statistical significant.

## e. Make a cubic spline fit with six basis functions evenly spaced on the range. Plot the fit in comparison to the previous fits. Does this model fit better than the straight-line model?

Choosing knots given the goal to fit with a cubic spline with 6 basis functions

#### Visualizing the basis functions... 

```{r}
require(splines)
# Visualizing the basis functions
attr(bs(year ,df=6) ,"knots")

dim(bs(year ,knots=c(1910.5, 1939.0, 1971.5) ))

bs_temp <- bs(year ,knots=c(1910.5, 1939.0, 1971.5) )
matplot(year, bs_temp, type="l", col=1, main="Visualizing basis functions")
```

Confirmed that the B-Spline Basis for polynomial Splines, called with bs(), has a dimension of 6. Recall that a cubic spline with three knots has seven degrees of freedom; these degrees of freedom are used up by an intercept, plus six basis functions. We could also use the df option to produce a spline with knots at uniform quantiles of the data. Since the requirement is for a cubic spline, we used the default degree of 3.

```{r}
dim(bs(year ,df=6))

```

```{r}

cs_fit <- lm(temp~bs(year ,df=6), data=aatemp)

yearlims =range(year)
year.grid=seq (from=yearlims [1], to=yearlims [2])

pred=predict (cs_fit ,newdata =list(year =year.grid),se=T)
plot(year ,temp ,col ="gray")
lines(year.grid ,pred$fit ,lwd =4)
lines(year.grid ,pred$fit +2* pred$se ,lty ="dashed")
lines(year.grid ,pred$fit -2* pred$se ,lty ="dashed")

```

```{r}
# matplot(year, cbind(temp,cs_fit$fit), type="pl", ylab="year", pch=20,lty=1,col=1)
summary(cs_fit)
```

*Ans*: No. This cubic spline model doesn't fit better than the straight line model as its adjusted R-squared is lower at 15.73%.
