Introduction

This project is intended to extend and supplement what we talked about last week in discussing Linear Regression.

In some of the sections you will be asked to write R code to solve a particular problem. In some you will be asked to answer questions in your own words.

Summary and Exercises

Single Variable Regression

We are trying to fit a straight line to a scatter plot. This means finding the equation of the line that comes closest to all the points. More specifically, the problem becomes, given \(X = \{x_1,x_1,\ldots,x_n\}\) and \(Y = \{y_1, y_2,\dots,y_n\}\) find \(\beta_0\) and \(beta_1\) such that \[ Y_i = \beta_0 + \beta_1 X_i + \epsilon_i\] where, \(\sum_{i}^{n}\epsilon_i = 0\) and \(\sigma^2 = \sum_{i}^{n}\epsilon_i ^2\) is as minimized. This is called least squares regression.

Given estimates of \(\beta_0\) and \(\beta_1\) called \(\hat{\beta_0}\) and \(\hat{\beta_1}\) we define: \[\hat{y_i} = \hat{\beta_0} + \hat{\beta_1}x_i\] The \(\hat{y_i}\) are called the predicted values.

The residuals, \(e_i\), are the differences between the predicted values and the actual values.\[e_i = y_i - \hat{y_i}\]

Note: the residuals are estimates of the \(\epsilon_i\) in the model.

Examining Residual variance.

Please work through this document before continuing with this project.

Section I Working with Simulated scatter plots.

There are four data sets in Project3 data folder the files section, problem1.csv, problem2.csv, problem3.csv, and problem4.csv These data are some of the groups from this data. You will need to load the files into your project using read_csv.

You will also need to read in the file `bdims.csv’ to do the problems in Section II.

read.csv("problem1.csv")
read.csv("problem2.csv")
read.csv("problem3.csv")
read.csv("problem4.csv")
read.csv("bdims.csv")

For each of the four files:

  1. plot the scatter plot of x and y (x on the horizontal axis.)
  2. fit a regression model using lm report the coefficients, and plot the regression line over the scatter plot.
  3. Plot the residuals versus x. Record any observations you have in this document.
  4. Calculate the correlation between x and y.
  5. Does the calculation indicate a strong linear relationship between x and y?
  6. Normalize the x and y data, this means calculating the z-score for each \(x_i\) and \(y_i\), it is possible to do this with one line of R code.

Hint the z-score of a vector of data, x, is the vector \(z\) given by \(z = \frac{x - \bar{x}}{s_x}\) where \(s_x\) is the standard deviation of \(x\).

  1. Using lm calculate the regression coefficients. What do you notice?
  2. Calculate Total Variation and \(R^2\)
  3. Assess your results.

#Problem1.csv

  1. plot the scatter plot of x and y (x on the horizontal axis.)
ggplot(data = problem1) +
  geom_point(mapping = aes(x = x, y = y))

  1. fit a regression model using lm report the coefficients, and plot the regression line over the scatter plot.
fit_1p <- lm(problem1$x ~ problem1$y, data = problem1)
summary(fit_1p)

Call:
lm(formula = problem1$x ~ problem1$y, data = problem1)

Residuals:
    Min      1Q  Median      3Q     Max 
-31.914  -6.822  -0.336   7.087  27.507 

Coefficients:
            Estimate Std. Error t value Pr(>|t|)    
(Intercept)  16.4901     1.4702   11.22   <2e-16 ***
problem1$y   -1.0063     0.0571  -17.63   <2e-16 ***
---
Signif. codes:  0 ‘***’ 0.001 ‘**’ 0.01 ‘*’ 0.05 ‘.’ 0.1 ‘ ’ 1

Residual standard error: 12.71 on 73 degrees of freedom
Multiple R-squared:  0.8097,    Adjusted R-squared:  0.8071 
F-statistic: 310.7 on 1 and 73 DF,  p-value: < 2.2e-16
problem1 %>%
  ggplot(aes(x = x, y = y)) +
  geom_point(mapping = aes(x = x, y = y)) +
  geom_smooth(method = "lm")
`geom_smooth()` using formula 'y ~ x'

  1. Plot the residuals versus x. Record any observations you have in this document.

The residuals are kind of all over the place. I can sort of see a trend upwards but it’s not very clear.

problem1 %>%
  ggplot() +
  geom_point(aes(x = x, y = fit_1p$residuals))

  1. Calculate the correlation between x and y.
cor(problem1$x, problem1$y)
[1] -0.8998508
  1. Does the calculation indicate a strong linear relationship between x and y?

The value is close to -1 so that indicates a strong and negative relationship between the 2. That makes sense considering that the scatterplot shows a downward trend.

  1. Normalize the x and y data, this means calculating the z-score for each \(x_i\) and \(y_i\), it is possible to do this with one line of R code.

Z = (x - mean)/standard deviation so I can calculate it by defining mean and sd for x and y.

x_bar_1p = mean(problem1$x)
sdx_1p = sd(problem1$x)
zx_1p <- (problem1$x - x_bar_1p)/sdx_1p
zx_1p
 [1] -1.06655437 -0.30351828  0.32490658 -1.28335543  0.25308878  0.06425960  0.12728719
 [8]  1.30271002 -1.35941370  1.47455475 -0.81903006 -1.25951702 -0.78663149  0.31791252
[15]  0.20323426 -0.32076528 -1.05639122 -0.70898864  1.42547764  0.25768106 -0.62947252
[22] -1.04417572 -0.20230084 -1.86963827 -0.52229236 -0.81480237  1.35287053  1.18354475
[29] -0.05223762 -1.26585894  1.05651518  1.00082777  0.85942119  0.86943717 -0.37145882
[36]  0.83411652  1.51215814  0.07352452 -1.08633148  0.93470495  0.92643594 -0.32396455
[43]  1.96642596 -0.87580927  0.42709513 -2.55233483 -0.15497024  1.31895858 -0.48933977
[50] -0.99500819  0.85842236 -0.89273311  0.33436394 -1.95032820 -1.57891539 -0.48706602
[57] -1.15040059  1.58258475  1.07570144 -0.86503576  0.68365704  1.07654433  0.32205583
[64]  0.43111754  1.36851131 -0.51817888 -0.44748811  1.11862436 -1.43937449  0.24216270
[71] -0.00578463  0.56235135  1.19737196  0.33467551  0.29417334
y_bar_1p = mean(problem1$y)
sdy_1p = sd(problem1$y)
zy_1p <- (problem1$y - y_bar_1p)/sdy_1p
zy_1p
 [1]  1.32183109  0.85678665 -0.09191802  0.71123718 -0.27807998  0.76808027 -0.25612720
 [8] -0.82522234  1.80487316 -0.92999073  0.75086145  1.24951035  0.31392153 -0.05951540
[15] -0.57165411 -0.08774540  0.50727757  0.35366250 -0.76572130 -0.39067126  0.55151613
[22]  0.74107760  0.45279473  2.12564480  0.39133553  1.03622035 -1.37709409 -0.54966027
[29]  0.34698756  1.62524228 -0.64226077 -0.77852258 -1.62753629 -1.07321545  0.57652277
[36] -0.93984133 -1.46150543 -0.23648526  1.74335915 -1.14944317 -1.01783066  0.31751458
[43] -1.63823568  0.89217938 -0.38429645  1.61137305  0.33022206 -0.91925677  0.23434865
[50]  1.22410311 -1.10038263  0.99873474 -0.58588528  0.96665337  1.96969441  0.77830471
[57]  1.11665915 -0.70284402 -1.69793010  0.85425273 -1.70481171 -0.27276224 -0.67448592
[64] -0.97025011 -1.60994011 -0.05508548 -0.49750072 -1.43863526  1.23852347  0.22739851
[71]  0.21521336 -1.05787695 -1.34812077  0.61640280 -0.05197951
  1. Using lm calculate the regression coefficients. What do you notice?

The coefficients are 16.4901 and -1.0063. The slope is negative which makes sense considering the downward direction of the datapoints.

fit_1p <- lm(problem1$x ~ problem1$y, data = problem1)
summary(fit_1p)

Call:
lm(formula = problem1$x ~ problem1$y, data = problem1)

Residuals:
    Min      1Q  Median      3Q     Max 
-31.914  -6.822  -0.336   7.087  27.507 

Coefficients:
            Estimate Std. Error t value Pr(>|t|)    
(Intercept)  16.4901     1.4702   11.22   <2e-16 ***
problem1$y   -1.0063     0.0571  -17.63   <2e-16 ***
---
Signif. codes:  0 ‘***’ 0.001 ‘**’ 0.01 ‘*’ 0.05 ‘.’ 0.1 ‘ ’ 1

Residual standard error: 12.71 on 73 degrees of freedom
Multiple R-squared:  0.8097,    Adjusted R-squared:  0.8071 
F-statistic: 310.7 on 1 and 73 DF,  p-value: < 2.2e-16
  1. Calculate Total Variation and \(R^2\)

R^2 is Rsq_1p

Rsq_1p = (cor(problem1$x, problem1$y))^2
Rsq_1p
[1] 0.8097315
res_var_1p = sum(residuals(fit_1p)^2)
y_hat_1p = predict(fit_1p)
reg_var_1p = sum((y_hat_1p - x_bar_1p)^2)
tot_var_1p = sum((problem1$x - x_bar_1p)^2)
tot_var_1p
[1] 62022.72
res_var_1p + reg_var_1p
[1] 62022.72
  1. Assess your results.

When I calculated total variability (tot_var_1p) I found that it was the same as residual variability + regression variability (res_var_1p + reg_var_1p) as it should be.

The R^2 is 0.81 and since that is close to +1 that means that there is a strong and positive linear relationship.

#Problem2.csv

  1. plot the scatter plot of x and y (x on the horizontal axis.)
ggplot(data = problem2) +
  geom_point(mapping = aes(x = x, y = y))

  1. fit a regression model using lm report the coefficients, and plot the regression line over the scatter plot.
fit_2p <- lm(problem2$x ~ problem2$y, data = problem2)
summary(fit_2p)

Call:
lm(formula = problem2$x ~ problem2$y, data = problem2)

Residuals:
   Min     1Q Median     3Q    Max 
 -45.0  -22.5    0.0   22.5   45.0 

Coefficients:
             Estimate Std. Error t value Pr(>|t|)    
(Intercept) 4.500e+01  1.191e+01   3.778 0.000975 ***
problem2$y  1.474e-15  1.170e+00   0.000 1.000000    
---
Signif. codes:  0 ‘***’ 0.001 ‘**’ 0.01 ‘*’ 0.05 ‘.’ 0.1 ‘ ’ 1

Residual standard error: 28.19 on 23 degrees of freedom
Multiple R-squared:  4.419e-32, Adjusted R-squared:  -0.04348 
F-statistic: 1.016e-30 on 1 and 23 DF,  p-value: 1
problem2 %>%
  ggplot(aes(x = x, y = y)) +
  geom_point(mapping = aes(x = x, y = y)) +
  geom_smooth(method = "lm")
`geom_smooth()` using formula 'y ~ x'

  1. Plot the residuals versus x. Record any observations you have in this document.

The residuals are all lined up together in what looks like a strong positive linear trend.

problem2 %>%
  ggplot() +
  geom_point(aes(x = x, y = fit_2p$residuals))

  1. Calculate the correlation between x and y.
cor(problem2$x, problem2$y)
[1] 2.961786e-16
  1. Does the calculation indicate a strong linear relationship between x and y?

The value is very far from +1 and -1 which does not indicate a strong linear relationship between x and y. This makes sense considering the non-linear shape of the graph.

  1. Normalize the x and y data, this means calculating the z-score for each \(x_i\) and \(y_i\), it is possible to do this with one line of R code.
x_bar_2p = mean(problem2$x)
sdx_2p = sd(problem2$x)
zx_2p <- (problem2$x - x_bar_2p)/sdx_2p
zx_2p
 [1] -1.6304789 -1.4946057 -1.3587324 -1.2228592 -1.0869860 -0.9511127 -0.8152395 -0.6793662
 [9] -0.5434930 -0.4076197 -0.2717465 -0.1358732  0.0000000  0.1358732  0.2717465  0.4076197
[17]  0.5434930  0.6793662  0.8152395  0.9511127  1.0869860  1.2228592  1.3587324  1.4946057
[25]  1.6304789
y_bar_2p = mean(problem2$y)
sdy_2p = sd(problem2$y)
zy_2p <- (problem2$y - y_bar_2p)/sdy_2p
zy_2p
 [1] -1.82326297 -1.43330628 -1.05002186 -0.67996781 -0.32947586 -0.00454302  0.28927102
 [8]  0.54693901  0.76405220  0.93689570  1.06251212  1.13875214  1.16431125  1.13875214
[15]  1.06251212  0.93689570  0.76405220  0.54693901  0.28927102 -0.00454302 -0.32947586
[22] -0.67996781 -1.05002186 -1.43330628 -1.82326297
  1. Using lm calculate the regression coefficients. What do you notice?

The coefficients are 45 and 1.47E-15. The slope is very big compared to the intercept.

fit_2p <- lm(problem2$x ~ problem2$y, data = problem2)
summary(fit_2p)

Call:
lm(formula = problem2$x ~ problem2$y, data = problem2)

Residuals:
   Min     1Q Median     3Q    Max 
 -45.0  -22.5    0.0   22.5   45.0 

Coefficients:
             Estimate Std. Error t value Pr(>|t|)    
(Intercept) 4.500e+01  1.191e+01   3.778 0.000975 ***
problem2$y  1.474e-15  1.170e+00   0.000 1.000000    
---
Signif. codes:  0 ‘***’ 0.001 ‘**’ 0.01 ‘*’ 0.05 ‘.’ 0.1 ‘ ’ 1

Residual standard error: 28.19 on 23 degrees of freedom
Multiple R-squared:  4.419e-32, Adjusted R-squared:  -0.04348 
F-statistic: 1.016e-30 on 1 and 23 DF,  p-value: 1
  1. Calculate Total Variation and \(R^2\)
Rsq_2p = (cor(problem2$x, problem2$y))^2
Rsq_2p
[1] 8.772177e-32
res_var_2p = sum(residuals(fit_2p)^2)
y_hat_2p = predict(fit_2p)
reg_var_2p = sum((y_hat_2p - x_bar_2p)^2)
tot_var_2p = sum((problem2$x - x_bar_2p)^2)
tot_var_2p
[1] 18281.25
res_var_2p + reg_var_2p
[1] 18281.25
  1. Assess your results.

When I calculated total variability I found that it was the same as residual variability + regression variability as it should be.

R^2 is very far from -1 and +1 which indicates that there is not a strong linear relationship.

#Problem3.csv

  1. plot the scatter plot of x and y (x on the horizontal axis.)
ggplot(data = problem3) +
  geom_point(mapping = aes(x = x, y = y))

  1. fit a regression model using lm report the coefficients, and plot the regression line over the scatter plot.
fit_3p <- lm(problem3$x ~ problem3$y, data = problem3)
summary(fit_3p)
Warning in summary.lm(fit_3p) :
  essentially perfect fit: summary may be unreliable

Call:
lm(formula = problem3$x ~ problem3$y, data = problem3)

Residuals:
       Min         1Q     Median         3Q        Max 
-4.956e-16 -2.600e-19  8.510e-18  1.609e-17  5.663e-17 

Coefficients:
              Estimate Std. Error    t value Pr(>|t|)    
(Intercept) -1.256e-16  1.896e-17 -6.626e+00 2.76e-08 ***
problem3$y   1.000e+00  3.405e-17  2.937e+16  < 2e-16 ***
---
Signif. codes:  0 ‘***’ 0.001 ‘**’ 0.01 ‘*’ 0.05 ‘.’ 0.1 ‘ ’ 1

Residual standard error: 7.402e-17 on 48 degrees of freedom
Multiple R-squared:      1, Adjusted R-squared:      1 
F-statistic: 8.625e+32 on 1 and 48 DF,  p-value: < 2.2e-16
problem3 %>%
  ggplot(aes(x = x, y = y)) +
  geom_point(mapping = aes(x = x, y = y)) +
  geom_smooth(method = "lm")
`geom_smooth()` using formula 'y ~ x'

  1. Plot the residuals versus x. Record any observations you have in this document.

The residuals are mostly within the same range and even the one residual by itself is still only a decimal place off.

problem3 %>%
  ggplot() +
  geom_point(aes(x = x, y = fit_3p$residuals))

  1. Calculate the correlation between x and y.
cor(problem3$x, problem3$y)
[1] 1
  1. Does the calculation indicate a strong linear relationship between x and y?

The calculation indicates a perfectly linear relationship between x and y. Something close to perfect was expected since the regression line perfectly lines up with the data points.

  1. Normalize the x and y data, this means calculating the z-score for each \(x_i\) and \(y_i\), it is possible to do this with one line of R code.
x_bar_3p = mean(problem3$x)
sdx_3p = sd(problem3$x)
zx_3p <- (problem3$x - x_bar_3p)/sdx_3p
zx_3p
 [1] -0.64367687 -0.13217104 -0.31421737  1.54035206 -1.09617799 -1.26906610  1.61058719
 [8] -0.06966477 -0.30227491 -0.94638054 -1.32007917  0.62367295  0.36714280  1.68395548
[15]  0.44967462 -1.28543292 -0.97257415  0.03623611 -1.48835200 -0.07304894 -0.65436527
[22]  1.52717692  0.81045348 -0.96943009  0.03878028  0.72809531 -0.01046365  1.58105824
[29]  0.79984929 -0.21573390 -1.11550789 -0.72138597  1.28637026 -0.09070372  0.10859138
[36]  0.73347587  0.95368194 -0.99417389  1.24073076  1.55423858  0.40017189  0.12270416
[43] -0.88347228 -1.48866105  1.33128210 -1.06272869 -1.42134764  1.52950490 -0.55126207
[50] -0.96543368
y_bar_3p = mean(problem3$y)
sdy_3p = sd(problem3$y)
zy_3p <- (problem3$y - y_bar_3p)/sdy_3p
zy_3p
 [1] -0.64367687 -0.13217104 -0.31421737  1.54035206 -1.09617799 -1.26906610  1.61058719
 [8] -0.06966477 -0.30227491 -0.94638054 -1.32007917  0.62367295  0.36714280  1.68395548
[15]  0.44967462 -1.28543292 -0.97257415  0.03623611 -1.48835200 -0.07304894 -0.65436527
[22]  1.52717692  0.81045348 -0.96943009  0.03878028  0.72809531 -0.01046365  1.58105824
[29]  0.79984929 -0.21573390 -1.11550789 -0.72138597  1.28637026 -0.09070372  0.10859138
[36]  0.73347587  0.95368194 -0.99417389  1.24073076  1.55423858  0.40017189  0.12270416
[43] -0.88347228 -1.48866105  1.33128210 -1.06272869 -1.42134764  1.52950490 -0.55126207
[50] -0.96543368
  1. Using lm calculate the regression coefficients. What do you notice?

RStudio tells us that the summary is unreliable because the fit is essentially perfect. This confirms the belief that the relationship is perfectly linear because the correlation = 1.

fit_3p <- lm(problem3$x ~ problem3$y, data = problem3)
summary(fit_3p)
Warning in summary.lm(fit_3p) :
  essentially perfect fit: summary may be unreliable

Call:
lm(formula = problem3$x ~ problem3$y, data = problem3)

Residuals:
       Min         1Q     Median         3Q        Max 
-4.956e-16 -2.600e-19  8.510e-18  1.609e-17  5.663e-17 

Coefficients:
              Estimate Std. Error    t value Pr(>|t|)    
(Intercept) -1.256e-16  1.896e-17 -6.626e+00 2.76e-08 ***
problem3$y   1.000e+00  3.405e-17  2.937e+16  < 2e-16 ***
---
Signif. codes:  0 ‘***’ 0.001 ‘**’ 0.01 ‘*’ 0.05 ‘.’ 0.1 ‘ ’ 1

Residual standard error: 7.402e-17 on 48 degrees of freedom
Multiple R-squared:      1, Adjusted R-squared:      1 
F-statistic: 8.625e+32 on 1 and 48 DF,  p-value: < 2.2e-16
  1. Calculate Total Variation and \(R^2\)
Rsq_3p = (cor(problem3$x, problem3$y))^2
Rsq_3p
[1] 1
res_var_3p = sum(residuals(fit_3p)^2)
y_hat_3p = predict(fit_3p)
reg_var_3p = sum((y_hat_3p - x_bar_3p)^2)
tot_var_3p = sum((problem3$x - x_bar_3p)^2)
tot_var_3p
[1] 4.725709
res_var_3p + reg_var_3p
[1] 4.725709
  1. Assess your results.

When I calculated total variability I found that it was the same as residual variability + regression variability as it should be.

R^2 being 1 indicates that the relationship between x and y is perfectly linear. This was expected because of the result of the correlation function.

#Problem4.csv

  1. plot the scatter plot of x and y (x on the horizontal axis.)
ggplot(data = problem4) +
  geom_point(mapping = aes(x = x, y = y))

  1. fit a regression model using lm report the coefficients, and plot the regression line over the scatter plot.
fit_4p <- lm(problem4$x ~ problem4$y, data = problem4)
summary(fit_4p)

Call:
lm(formula = problem4$x ~ problem4$y, data = problem4)

Residuals:
    Min      1Q  Median      3Q     Max 
-2.1522 -1.1929  0.3144  1.0636  2.0662 

Coefficients:
            Estimate Std. Error t value Pr(>|t|)    
(Intercept)  0.09574    0.37736   0.254 0.800720    
problem4$y   1.31191    0.31788   4.127 0.000133 ***
---
Signif. codes:  0 ‘***’ 0.001 ‘**’ 0.01 ‘*’ 0.05 ‘.’ 0.1 ‘ ’ 1

Residual standard error: 1.337 on 52 degrees of freedom
Multiple R-squared:  0.2467,    Adjusted R-squared:  0.2322 
F-statistic: 17.03 on 1 and 52 DF,  p-value: 0.0001332
problem4 %>%
  ggplot(aes(x = x, y = y)) +
  geom_point(mapping = aes(x = x, y = y)) +
  geom_smooth(method = "lm")
`geom_smooth()` using formula 'y ~ x'

  1. Plot the residuals versus x. Record any observations you have in this document.

In comparison to the scatterplot, the residuals seem to be fitting to more of a trend than the data points.

problem4 %>%
  ggplot() +
  geom_point(aes(x = x, y = fit_4p$residuals))

  1. Calculate the correlation between x and y.
cor(problem4$x, problem4$y)
[1] 0.4967192
  1. Does the calculation indicate a strong linear relationship between x and y?

The calculation indicate a linear relationship between x and y but not a really strong one because 0.5 isn’t that close to 1. Compared to problem 2 though, this is much stronger.

  1. Normalize the x and y data, this means calculating the z-score for each \(x_i\) and \(y_i\), it is possible to do this with one line of R code.
x_bar_4p = mean(problem4$x)
sdx_4p = sd(problem4$x)
zx_4p <- (problem4$x - x_bar_4p)/sdx_4p
zx_4p
 [1] -1.286867588 -1.222223502 -1.446498546  1.432376147  0.595256714 -1.300990643
 [7]  0.001945231 -0.099751562 -0.382574167  1.634972846 -1.034031243  1.052969972
[13] -1.387510163 -0.299913621 -1.149362530 -0.978475404  1.144420615  0.746607313
[19] -0.736381889  0.009825397 -1.339462233 -0.452455817  1.563262859  0.434745861
[25]  0.565466075 -0.588058784 -0.282748541  1.651280588  1.189400303  1.511961511
[31]  1.049267867  0.950589137 -0.734200015  0.884971691  1.619289227 -0.649920524
[37] -0.303512614  1.048699280 -1.358993675 -0.420311190 -0.161859863 -1.098357984
[43]  0.295492485  1.566385979  1.629733477 -1.033699324  0.164212800 -0.352805222
[49]  0.603288532 -0.729562537 -0.956559433 -0.956559433 -0.301386930 -0.301386930
y_bar_4p = mean(problem4$y)
sdy_4p = sd(problem4$y)
zy_4p <- (problem4$y - y_bar_4p)/sdy_4p
zy_4p
 [1] -0.078542927 -0.110099044 -0.073330393  0.806389528  0.531980985  0.057160582
 [7]  1.290626050  0.990944093 -1.678594019  0.736640568 -0.249329080  0.773633206
[13] -0.088568439  1.322161404 -0.163184169 -0.121919435  0.595839764  0.255259297
[19] -1.750083769  1.052321485  0.032954962 -1.947898625  0.580866315  0.454077556
[25]  0.152211980 -1.748859732  1.095404765  0.759919557  0.917114336  0.904547705
[31]  0.668965741 -0.003743964 -1.492614008  0.358973324  0.776127811 -1.801120850
[37] -1.736803107  0.689425718 -0.017377795 -1.848648573  0.973880866  0.052300990
[43]  1.328938034  0.671689188  0.555642675  0.009841240  1.136730520 -2.012416343
[49]  0.277280058 -1.876912762 -0.976160401 -1.076364791  0.152468506 -0.109746585
  1. Using lm calculate the regression coefficients. What do you notice?

The slope is positive 0.096 and the intercept is 1.31. The positive nature of the slope makes it seem like the linear relationship is positive.

fit_4p <- lm(problem4$x ~ problem4$y, data = problem4)
summary(fit_4p)

Call:
lm(formula = problem4$x ~ problem4$y, data = problem4)

Residuals:
    Min      1Q  Median      3Q     Max 
-2.1522 -1.1929  0.3144  1.0636  2.0662 

Coefficients:
            Estimate Std. Error t value Pr(>|t|)    
(Intercept)  0.09574    0.37736   0.254 0.800720    
problem4$y   1.31191    0.31788   4.127 0.000133 ***
---
Signif. codes:  0 ‘***’ 0.001 ‘**’ 0.01 ‘*’ 0.05 ‘.’ 0.1 ‘ ’ 1

Residual standard error: 1.337 on 52 degrees of freedom
Multiple R-squared:  0.2467,    Adjusted R-squared:  0.2322 
F-statistic: 17.03 on 1 and 52 DF,  p-value: 0.0001332
  1. Calculate Total Variation and \(R^2\)
Rsq_4p = (cor(problem4$x, problem4$y))^2
Rsq_4p
[1] 0.24673
res_var_4p = sum(residuals(fit_4p)^2)
y_hat_4p = predict(fit_4p)
reg_var_4p = sum((y_hat_4p - x_bar_4p)^2)
tot_var_4p = sum((problem4$x - x_bar_4p)^2)
tot_var_4p
[1] 123.4709
res_var_4p + reg_var_4p
[1] 123.4709
  1. Assess your results.

When I calculated total variability I found that it was the same as residual variability + regression variability as it should be.

The R^2 is 0.25 and since that is not that close to +1 that means that the relationship is only somewhat strong and positive.

Section II Body measurement study

Anthropological researchers collected body measurements from 507 individuals (247 men and 260 women.) The data are contained in the file bdims.csv. A description of the variables can be found here

Using R Perform the following tasks, give the most complete specific answers you can given the data.

  1. Describe the relationship between shoulder girth and height.

I can see by making a scatter plot of sho_gi vs. hgt that as shoulder girth increases, so does height. Although the difference varies, we can see a clear linear trend upwards (positive trend).

ggplot(data = bdims) +
  geom_point(mapping = aes(x = sho_gi, y = hgt))
  1. How would the relationship change if shoulder girth were measured in inches while the units of height remained in centimeters?

The relationship shouldn’t change if we correctly transform the shoulder girth data from inches to centimeters so that the 2 variables could be compared.

  1. Write the equation of the regression line for predicting height. How would you find the coefficients without using lm?

y = 0.6036442x + 105.8324618

You would need to find m and b using coef as I did to get the m and b in the above equation.

m = sho_gi_hgt$coef[[2]]
b = sho_gi_hgt$coef[[1]]
c(m,b)
  1. Interpret the slope and intercept in this context.

In this context, the slope (m) is beta_1 and the intercept (b) is beta_0. So the slope and intercept are used to represent the relationship between x and y. This means that we can use x and the equation to predict y although there may be some error. The relationship means that for every increase in shoulder girth cm (x) we (using the model) predict an additional 105.8324618 cm in height (y). 105.8324618 is the b intercept.

  1. Calculate \(R^2\) of the regression line for predicting height from shoulder girth

R^2 is equal to the square of the correlation coefficient. Therefore if I square the correlation between x (sho_gi) and y (hgt), I should get R^2 (R_sq_s).

R_sq_s = (cor(bdims$sho_gi, bdims$hgt))^2
R_sq_s
  1. A randomly selected student from your class has a shoulder girth of 100cm. Predict the height of this student using this model.

If x (shoulder girth) is 100 cm, then y (height) is 166.1969 cm.

(m*100)+b
  1. If the selected student is actually 160 cm tall, calculate the residual and explain it’s meaning.

The difference between the model-calculated height and the actual height is -6.1969 cm. The negative residual means that this model overestimated the height (which we already knew since 166 > 160).

160-166.1969
  1. A one year old has has a shoulder girth of 56 cm. Would it be appropriate to use this linear model to predict the height of this child?

You could try but since the dataset says that the data was collected from “physically active men and women”, the model is therefore going to be more representative of adults not babies. Since babies grow very much in a short amount of time (compared to adults), a specific model for baby growth is necessitated. Therefore, trying to calculate a one year old’s height from shoulder girth using this model would only be useful for comparison purposes, to see how the model’s answer compares to the height of the one year old.

Murders and Poverty

murders %>%
  ggplot(aes(x = perc_pov, y = annual_murders_per_mil)) +
  geom_point()
summary(lm(annual_murders_per_mil~ perc_pov, data = murders))

Just referring to the plot and the summary above:

  1. Write out the linear model

y = 2.559x + -29.901

  1. Interpret the intercept

The intercept -29.901 is how much is subtracted from annual murders with each increase in percent poverty. That seems strange considering the positive linear nature of the scatterplot. However a bigger intercept may be necessary considering that the datapoints look sparse.

  1. Interpret the slope

The slope 2.559 is the adjustment to percent poverty (x).

  1. Interpret \(R^2\)

R^2 (R_sq_m in code below) is 0.705. That means that 70% of the variability in annual murders can be traced back to the model or explained by percent poverty.

  1. Calculate the correlation coefficient
cor(murders$perc_pov, murders$annual_murders_per_mil)
[1] 0.8397782
R_sq_m = (cor(murders$perc_pov, murders$annual_murders_per_mil))^2
R_sq_m
[1] 0.7052275
---
title: "Project 3 Regression"
author: "Tara Bhat"
output: html_notebook
---

```{r, include = FALSE}
library(tidyverse)
library(openintro)
```

## Introduction

This project is intended to extend and supplement what we talked about last week in discussing Linear Regression.

In some of the sections you will be asked to write R code to solve a particular problem. In some you will be asked to answer questions in your own words. 

 

## Summary and Exercises

### Single Variable Regression

We are trying to fit a straight line to a scatter plot. This means finding the equation of the line that comes closest to all the points. More specifically, the problem becomes, given $X = \{x_1,x_1,\ldots,x_n\}$ and $Y = \{y_1, y_2,\dots,y_n\}$ find $\beta_0$ and $beta_1$ such that
$$ Y_i = \beta_0 + \beta_1 X_i + \epsilon_i$$
where, $\sum_{i}^{n}\epsilon_i = 0$ and $\sigma^2 = \sum_{i}^{n}\epsilon_i ^2$ is as minimized. This is called *least squares* regression.

Given estimates of $\beta_0$ and $\beta_1$ called $\hat{\beta_0}$ and $\hat{\beta_1}$ we define: $$\hat{y_i} = \hat{\beta_0} + \hat{\beta_1}x_i$$
The $\hat{y_i}$ are called the predicted values.

The residuals, $e_i$, are the differences between the predicted values and the actual values.$$e_i = y_i - \hat{y_i}$$

Note: the residuals are *estimates* of the $\epsilon_i$ in the model.


## Examining Residual variance.

Please work through this [document](http://rpubs.com/ProfCelia/794919) before continuing with this project.


## Section I Working with Simulated scatter plots.


There are four data sets in Project3 data folder the files section, `problem1.csv`, `problem2.csv`, `problem3.csv`, and `problem4.csv`
These data are some of the  groups from [this](https://www.openintro.org/data/index.php?data=simulated_scatter) data. You will need to load the files into your project using `read_csv`.

You will also need to read in the file `bdims.csv' to do the problems in Section II.

```{r}
read.csv("problem1.csv")
read.csv("problem2.csv")
read.csv("problem3.csv")
read.csv("problem4.csv")
read.csv("bdims.csv")
```


### For each of the four files:

1. plot the scatter plot of `x` and `y` (`x` on the horizontal axis.)
2. fit a regression model using `lm` report the coefficients, and plot the regression line over the scatter plot.
3. Plot the residuals versus `x`.
Record any observations you have in this document.
4. Calculate the correlation between `x` and `y`.
5. Does the calculation indicate a strong linear relationship between `x` and `y`?
6. Normalize the `x` and `y` data, this means calculating the z-score for each $x_i$ and $y_i$, it is possible to do this with one line of R code.

**Hint** the z-score of a vector of data, x, is the vector $z$ given by  $z = \frac{x - \bar{x}}{s_x}$ where $s_x$ is the standard deviation of $x$.

7. Using `lm` calculate the regression coefficients. What do you notice?
8. Calculate Total Variation and $R^2$ 
9. Assess your results.


#Problem1.csv

1. plot the scatter plot of `x` and `y` (`x` on the horizontal axis.)

```{r}
ggplot(data = problem1) +
  geom_point(mapping = aes(x = x, y = y))
```

2. fit a regression model using `lm` report the coefficients, and plot the regression line over the scatter plot.


```{r}
fit_1p <- lm(problem1$x ~ problem1$y, data = problem1)
summary(fit_1p)
problem1 %>%
  ggplot(aes(x = x, y = y)) +
  geom_point(mapping = aes(x = x, y = y)) +
  geom_smooth(method = "lm")
```

3. Plot the residuals versus `x`.
Record any observations you have in this document.

The residuals are kind of all over the place. I can sort of see a trend upwards but it's not very clear.

```{r}
problem1 %>%
  ggplot() +
  geom_point(aes(x = x, y = fit_1p$residuals))
```


4. Calculate the correlation between `x` and `y`.

```{r}
cor(problem1$x, problem1$y)
```


5. Does the calculation indicate a strong linear relationship between `x` and `y`?

The value is close to -1 so that indicates a strong and negative relationship between the 2. That makes sense considering that the scatterplot shows a downward trend.

6. Normalize the `x` and `y` data, this means calculating the z-score for each $x_i$ and $y_i$, it is possible to do this with one line of R code.

Z = (x - mean)/standard deviation so I can calculate it by defining mean and sd for x and y.

```{r}
x_bar_1p = mean(problem1$x)
sdx_1p = sd(problem1$x)
zx_1p <- (problem1$x - x_bar_1p)/sdx_1p
zx_1p
```

```{r}
y_bar_1p = mean(problem1$y)
sdy_1p = sd(problem1$y)
zy_1p <- (problem1$y - y_bar_1p)/sdy_1p
zy_1p
```



7. Using `lm` calculate the regression coefficients. What do you notice?

The coefficients are 16.4901 and -1.0063. The slope is negative which makes sense considering the downward direction of the datapoints.

```{r}
fit_1p <- lm(problem1$x ~ problem1$y, data = problem1)
summary(fit_1p)
```


8. Calculate Total Variation and $R^2$ 

R^2 is Rsq_1p
```{r}
Rsq_1p = (cor(problem1$x, problem1$y))^2
Rsq_1p

res_var_1p = sum(residuals(fit_1p)^2)
y_hat_1p = predict(fit_1p)
reg_var_1p = sum((y_hat_1p - x_bar_1p)^2)
tot_var_1p = sum((problem1$x - x_bar_1p)^2)
tot_var_1p
res_var_1p + reg_var_1p
```


9. Assess your results.

When I calculated total variability (tot_var_1p) I found that it was the same as residual variability + regression variability (res_var_1p + reg_var_1p) as it should be. 

The R^2 is 0.81 and since that is close to +1 that means that there is a strong and positive linear relationship.



#Problem2.csv

1. plot the scatter plot of `x` and `y` (`x` on the horizontal axis.)

```{r}
ggplot(data = problem2) +
  geom_point(mapping = aes(x = x, y = y))
```


2. fit a regression model using `lm` report the coefficients, and plot the regression line over the scatter plot.

```{r}
fit_2p <- lm(problem2$x ~ problem2$y, data = problem2)
summary(fit_2p)
problem2 %>%
  ggplot(aes(x = x, y = y)) +
  geom_point(mapping = aes(x = x, y = y)) +
  geom_smooth(method = "lm")
```


3. Plot the residuals versus `x`.
Record any observations you have in this document.

The residuals are all lined up together in what looks like a strong positive linear trend.


```{r}
problem2 %>%
  ggplot() +
  geom_point(aes(x = x, y = fit_2p$residuals))
```


4. Calculate the correlation between `x` and `y`.

```{r}
cor(problem2$x, problem2$y)
```


5. Does the calculation indicate a strong linear relationship between `x` and `y`?

The value is very far from +1 and -1 which does not indicate a strong linear relationship between x and y. This makes sense considering the non-linear shape of the graph.

6. Normalize the `x` and `y` data, this means calculating the z-score for each $x_i$ and $y_i$, it is possible to do this with one line of R code.

```{r}
x_bar_2p = mean(problem2$x)
sdx_2p = sd(problem2$x)
zx_2p <- (problem2$x - x_bar_2p)/sdx_2p
zx_2p
```

```{r}
y_bar_2p = mean(problem2$y)
sdy_2p = sd(problem2$y)
zy_2p <- (problem2$y - y_bar_2p)/sdy_2p
zy_2p
```


7. Using `lm` calculate the regression coefficients. What do you notice?

The coefficients are 45 and 1.47E-15. The slope is very big compared to the intercept.


```{r}
fit_2p <- lm(problem2$x ~ problem2$y, data = problem2)
summary(fit_2p)
```

 

8. Calculate Total Variation and $R^2$ 

```{r}
Rsq_2p = (cor(problem2$x, problem2$y))^2
Rsq_2p

res_var_2p = sum(residuals(fit_2p)^2)
y_hat_2p = predict(fit_2p)
reg_var_2p = sum((y_hat_2p - x_bar_2p)^2)
tot_var_2p = sum((problem2$x - x_bar_2p)^2)
tot_var_2p
res_var_2p + reg_var_2p
```


9. Assess your results.

When I calculated total variability I found that it was the same as residual variability + regression variability as it should be. 

R^2 is very far from -1 and +1 which indicates that there is not a strong linear relationship.


#Problem3.csv

1. plot the scatter plot of `x` and `y` (`x` on the horizontal axis.)

```{r}
ggplot(data = problem3) +
  geom_point(mapping = aes(x = x, y = y))
```


2. fit a regression model using `lm` report the coefficients, and plot the regression line over the scatter plot.

```{r}
fit_3p <- lm(problem3$x ~ problem3$y, data = problem3)
summary(fit_3p)
problem3 %>%
  ggplot(aes(x = x, y = y)) +
  geom_point(mapping = aes(x = x, y = y)) +
  geom_smooth(method = "lm")
```


3. Plot the residuals versus `x`.
Record any observations you have in this document.

The residuals are mostly within the same range and even the one residual by itself is still only a decimal place off.

```{r}
problem3 %>%
  ggplot() +
  geom_point(aes(x = x, y = fit_3p$residuals))
```


4. Calculate the correlation between `x` and `y`.

```{r}
cor(problem3$x, problem3$y)
```


5. Does the calculation indicate a strong linear relationship between `x` and `y`?

The calculation indicates a perfectly linear relationship between x and y. Something close to perfect was expected since the regression line perfectly lines up with the data points.

6. Normalize the `x` and `y` data, this means calculating the z-score for each $x_i$ and $y_i$, it is possible to do this with one line of R code.

```{r}
x_bar_3p = mean(problem3$x)
sdx_3p = sd(problem3$x)
zx_3p <- (problem3$x - x_bar_3p)/sdx_3p
zx_3p
```

```{r}
y_bar_3p = mean(problem3$y)
sdy_3p = sd(problem3$y)
zy_3p <- (problem3$y - y_bar_3p)/sdy_3p
zy_3p
```



7. Using `lm` calculate the regression coefficients. What do you notice?

RStudio tells us that the summary is unreliable because the fit is essentially perfect. This confirms the belief that the relationship is perfectly linear because the correlation = 1.

```{r}
fit_3p <- lm(problem3$x ~ problem3$y, data = problem3)
summary(fit_3p)
```


8. Calculate Total Variation and $R^2$ 

```{r}
Rsq_3p = (cor(problem3$x, problem3$y))^2
Rsq_3p

res_var_3p = sum(residuals(fit_3p)^2)
y_hat_3p = predict(fit_3p)
reg_var_3p = sum((y_hat_3p - x_bar_3p)^2)
tot_var_3p = sum((problem3$x - x_bar_3p)^2)
tot_var_3p
res_var_3p + reg_var_3p
```


9. Assess your results.

When I calculated total variability I found that it was the same as residual variability + regression variability as it should be. 

R^2 being 1 indicates that the relationship between x and y is perfectly linear. This was expected because of the result of the correlation function.


#Problem4.csv

1. plot the scatter plot of `x` and `y` (`x` on the horizontal axis.)

```{r}
ggplot(data = problem4) +
  geom_point(mapping = aes(x = x, y = y))
```


2. fit a regression model using `lm` report the coefficients, and plot the regression line over the scatter plot.

```{r}
fit_4p <- lm(problem4$x ~ problem4$y, data = problem4)
summary(fit_4p)
problem4 %>%
  ggplot(aes(x = x, y = y)) +
  geom_point(mapping = aes(x = x, y = y)) +
  geom_smooth(method = "lm")
```


3. Plot the residuals versus `x`.
Record any observations you have in this document.

In comparison to the scatterplot, the residuals seem to be fitting to more of a trend than the data points. 

```{r}
problem4 %>%
  ggplot() +
  geom_point(aes(x = x, y = fit_4p$residuals))
```


4. Calculate the correlation between `x` and `y`.

```{r}
cor(problem4$x, problem4$y)
```


5. Does the calculation indicate a strong linear relationship between `x` and `y`?

The calculation indicate a linear relationship between x and y but not a really strong one because 0.5 isn't that close to 1. Compared to problem 2 though, this is much stronger.

6. Normalize the `x` and `y` data, this means calculating the z-score for each $x_i$ and $y_i$, it is possible to do this with one line of R code.

```{r}
x_bar_4p = mean(problem4$x)
sdx_4p = sd(problem4$x)
zx_4p <- (problem4$x - x_bar_4p)/sdx_4p
zx_4p
```

```{r}
y_bar_4p = mean(problem4$y)
sdy_4p = sd(problem4$y)
zy_4p <- (problem4$y - y_bar_4p)/sdy_4p
zy_4p
```


7. Using `lm` calculate the regression coefficients. What do you notice?

The slope is positive 0.096 and the intercept is 1.31. The positive nature of the slope makes it seem like the linear relationship is positive. 

```{r}
fit_4p <- lm(problem4$x ~ problem4$y, data = problem4)
summary(fit_4p)
```



8. Calculate Total Variation and $R^2$ 

```{r}
Rsq_4p = (cor(problem4$x, problem4$y))^2
Rsq_4p

res_var_4p = sum(residuals(fit_4p)^2)
y_hat_4p = predict(fit_4p)
reg_var_4p = sum((y_hat_4p - x_bar_4p)^2)
tot_var_4p = sum((problem4$x - x_bar_4p)^2)
tot_var_4p
res_var_4p + reg_var_4p
```


9. Assess your results.

When I calculated total variability I found that it was the same as residual variability + regression variability as it should be. 

The R^2 is 0.25 and since that is not that close to +1 that means that the relationship is only somewhat strong and positive.



## Section II Body measurement study


Anthropological researchers collected body measurements from 507 individuals (247 men and 260 women.) The data are contained in the file `bdims.csv`. A description of the variables can be found [here](https://www.openintro.org/data/index.php?data=bdims)
 
Using R Perform the following tasks, give the most complete specific answers you can given the data.


1. Describe the relationship between shoulder girth and height.

I can see by making a scatter plot of sho_gi vs. hgt that as shoulder girth increases, so does height. Although the difference varies, we can see a clear linear trend upwards (positive trend).

```{r}
ggplot(data = bdims) +
  geom_point(mapping = aes(x = sho_gi, y = hgt))
```


2. How would the relationship change if shoulder girth were measured in inches while the units of height remained in centimeters?

The relationship shouldn’t change if we correctly transform the shoulder girth data from inches to centimeters so that the 2 variables could be compared. 


3. Write the equation of the regression line for predicting height. How would you find the coefficients **without** using `lm`?

y = 0.6036442x + 105.8324618

You would need to find m and b using coef as I did to get the m and b in the above equation.
```{r}
m = sho_gi_hgt$coef[[2]]
b = sho_gi_hgt$coef[[1]]
c(m,b)
```


4. Interpret the slope and intercept in this context.

In this context, the slope (m) is beta_1 and the intercept (b) is beta_0. So the slope and intercept are used to represent the relationship between x and y. This means that we can use x and the equation to predict y although there may be some error. The relationship means that for every increase in shoulder girth cm (x) we (using the model) predict an additional 105.8324618 cm in height (y). 105.8324618 is the b intercept. 


5. Calculate $R^2$ of the regression line for predicting height from shoulder girth

R^2 is equal to the square of the correlation coefficient. Therefore if I square the correlation between x (sho_gi) and y (hgt), I should get R^2 (R_sq_s).

```{r}
R_sq_s = (cor(bdims$sho_gi, bdims$hgt))^2
R_sq_s
```


6. A randomly selected student from your class has a shoulder girth of 100cm. Predict the height of this student using this model.

If x (shoulder girth) is 100 cm, then y (height) is 166.1969 cm.
```{r}
(m*100)+b
```


7. If the selected student is actually 160 cm tall, calculate the residual and explain it's meaning.

The difference between the model-calculated height and the actual height is -6.1969 cm. The negative residual means that this model overestimated the height (which we already knew since 166 > 160). 

```{r}
160-166.1969
```


8. A one year old has has a shoulder girth of 56 cm. Would it be appropriate to use this linear model to predict the height of this child?

You could try but since the dataset says that the data was collected from “physically active men and women”, the model is therefore going to be more representative of adults not babies. Since babies grow very much in a short amount of time (compared to adults), a specific model for baby growth is necessitated. Therefore, trying to calculate a one year old’s height from shoulder girth using this model would only be useful for comparison purposes, to see how the model’s answer compares to the height of the one year old.


### Murders and Poverty

```{r}
murders %>%
  ggplot(aes(x = perc_pov, y = annual_murders_per_mil)) +
  geom_point()
```

```{r}
summary(lm(annual_murders_per_mil~ perc_pov, data = murders))
```

Just referring to the plot and the summary above:

a. Write out the linear model

y = 2.559x + -29.901


b. Interpret the intercept

The intercept -29.901 is how much is subtracted from annual murders with each increase in percent poverty. That seems strange considering the positive linear nature of the scatterplot. However a bigger intercept may be necessary considering that the datapoints look sparse.


c. Interpret the slope

The slope 2.559 is the adjustment to percent poverty (x).


d. Interpret $R^2$

R^2 (R_sq_m in code below) is 0.705. That means that 70% of the variability in annual murders can be traced back to the model or explained by percent poverty.


e. Calculate the correlation coefficient
```{r}
cor(murders$perc_pov, murders$annual_murders_per_mil)
R_sq_m = (cor(murders$perc_pov, murders$annual_murders_per_mil))^2
R_sq_m
```




