2024
1.(a) Create a vector x = (1,2,2,3,3,3,4,4,4,4,5,5,5,5,5) by using
rep() and find multiplication of x.
x <- rep(1:5, c(1,2,3,4,5))
x
[1] 1 2 2 3 3 3 4 4 4 4 5 5 5 5 5
1.(b) Create vector y = N * e^x / x!, where N = 1:length(x). Find sum
of y.
N <- 1:length(x)
y <- N*exp(x)/factorial(x)
y
[1] 2.718282 7.389056 11.083584 13.390358 16.737947 20.085537
[7] 15.924460 18.199383 20.474306 22.749229 13.604540 14.841316
[13] 16.078092 17.314869 18.551645
y_sum <- sum(y)
y_sum
[1] 229.1426
1.(c) Find index positions where 10 < y < 15. Find the sum of
values.
indices <- which(y>10 & y<15)
indices
[1] 3 4 11 12
val_sum <- sum(y[indices])
val_sum
[1] 52.9198
1.(d) Create int.y as nearest integer of y, count divisible by 4
int.y <- round(y)
int.y
[1] 3 7 11 13 17 20 16 18 20 23 14 15 16 17 19
n <- length(which(int.y%%4==0))
n
[1] 4
1.(e) Function to create y and calculate mean
calc_mean <- function(x){
N <- 1:length(x)
y <- N*exp(x)/factorial(x)
am <- mean(y)
if (any(y<=0)){
gm <- NA
hm <- NA
} else {
gm <- exp(mean(log(y)))
hm <- 1/mean(1/y)
}
return(list(AM=am,GM=gm,HM=hm))
}
1.(f) Evaluate the function for X.
means_result <- calc_mean(x)
cat("Arithmetic mean :", means_result$AM, "\n")
Arithmetic mean : 15.27617
cat("Geometric mean :", means_result$GM, "\n")
Geometric mean : 13.90898
cat("Harmonic mean :", means_result$HM, "\n")
Harmonic mean : 11.5125
2.(a) Using seed 100, create three stdnormal random vectors of length
100 (x, x1,x2).
Create vectors y,z [y=x+x1, z=y+x2] and Evaluate
sum((x-xbar)(y-ybar)), sum((x-xbar)(z-zbar)),
sum((y-ybar)(z-zbar))
create matrix A(100x3) where each column is filled by each vector
x,y,z. B=(A^T A) then B^-1 = ? Find sum of diagonal elements of
B.
# (i)
set.seed(100)
x <- rnorm(100)
x1 <- rnorm(100)
x2 <- rnorm(100)
y <- x+x1
z <- y+x2
spxy <- sum((x-mean(x))*(y-mean(y)))
spxz <- sum((x-mean(x))*(z-mean(z)))
spxy
[1] 92.27519
spxz
[1] 103.4904
# (ii)
A <- matrix(c(x,y,z), byrow = FALSE, ncol = 3)
head(A)
[,1] [,2] [,3]
[1,] -0.50219235 -0.83511570 -0.8069439
[2,] 0.13153117 1.49464487 1.1379415
[3,] -0.07891709 -0.54806443 0.3045619
[4,] 0.88678481 1.72966044 2.2430257
[5,] 0.11697127 -1.34102245 -0.3228195
[6,] 0.31863009 -0.08167583 -1.1031549
B <- t(A) %*% A
B
[,1] [,2] [,3]
[1,] 103.14396 92.27928 103.4982
[2,] 92.27928 144.18476 133.6212
[3,] 103.49823 133.62118 230.0049
n <- nrow(B)
diag_sum <- 0
# sum(diag(B))
for (i in 1:n){
diag_sum <- diag_sum + B[i,i]
}
diag_sum
[1] 477.3336
2.(b) Function to count entries > k in each column of a
matrix.
count_gt <- function(mat, k) {
apply(mat, 2, function(col) sum(col > k))
}
2.(c) Evaluate the func with (A,2)
count_gt(A,2)
[1] 3 4 8
3.(a) Gamma distribution calculations (shape=3, scale=0.25) (i) P(X ≥
50) (ii) P(20 < X < 40) (iii) Find k such that P(X > k) =
0.1
#(i)
p50_ <- 1-pgamma(50, shape=3, scale=0.25)
p50_
[1] 0
#(ii)
p20_40 <- pgamma(40, shape=3, scale=0.25)-pgamma(20, shape=3, scale=0.25)
p20_40
[1] 0
#(iii)
k <- qgamma(0.9, shape = 3, scale = 0.25) # Since P(X > k) = 0.1 => P(X ≤ k) = 0.9
k
[1] 1.33058
3.(b) Generate 5000 observations from gamma(3,0.25) [seed 101] (i)
Estimate P(X ≥ 50) (ii) Estimate P(20 < X < 40) (iii) Find deciles
(10%, 20%, …, 90%)
set.seed(101)
x<-rgamma(5000, shape=3, scale=0.25)
#(i)
est_px50_ <- mean(x>=50)
est_px50_
[1] 0
#(ii)
est_px20_50 <- mean(x>20 & x<40)
est_px20_50
[1] 0
#(iii)
deciles <- quantile(x, probs = seq(0.1, 0.9, by = 0.1))
deciles
10% 20% 30% 40% 50% 60% 70%
0.2838650 0.3900256 0.4802828 0.5736065 0.6662751 0.7708639 0.9059050
80% 90%
1.0696102 1.3150904
Question 4
(a) Finding the minimum value of the function [ l(x)
= x^4 + 4x^3 + 2x^2 + 12x + 5] requires solving the transcendental
equation [ f(x) = 0] where [ f(x) = 4x^3 + 12x^2 + 4x + 12] and [ f’(x)
= 12x^2 + 24x + 4]
(i) Draw the functions ( l(x) ) and ( f(x) ) on the
same graph for the interval [ -4 < x < 1]
(ii) Write a function to find the solution of the
transcendental equation ( f(x) = 0 ). The function should return:
- the estimated solution,
- the value of the function at the estimated solution, and
- the number of iterations required.
(b) Write a function that sums the terms of the
given series.
Workflow for Question (a)
Step 1: Define the functions
- Define the original function [ l(x) = x^4 + 4x^3 + 2x^2 + 12x +
5]
- Define its first derivative [ f(x) = l’(x) = 4x^3 + 12x^2 + 4x +
12]
- Define the derivative of ( f(x) ) [ f’(x) = 12x^2 + 24x + 4]
Step 2: Visualization
Choose the interval ( -4 < x < 1 )
Plot:
Draw both curves on the same graph
Use the plot to understand where the minimum of ( l(x) ) may
occur
Step 3: Set up the optimization condition
- Recall that the minimum of ( l(x) ) occurs when: [ f(x) = 0]
- This equation cannot be solved easily by hand, so a
numerical method is required
Step 4: Write a root-finding function
Step 5: Output requirements
Your function must return:
- The estimated root of ( f(x) = 0 )
- The value of ( f(x) ) at the estimated root
- The number of iterations used
Workflow for Question (b)
Step 6: Series computation
One-line workflow summary
Define → Visualize → Differentiate → Solve numerically →
Report results → Compute series sum
# 4.(a) Draw functions l(x) and f(x) on interval -4 < x < 1
l_func <- function(x) x^4 + 4*x^3 + 2*x^2 + 12*x + 5
f_func <- function(x) 4*x^3 + 12*x^2 + 4*x + 12
f_prime <- function(x) 12*x^2 + 24*x + 4
# Create sequence for plotting
x_vals <- seq(-4, 1, length.out = 1000)
# Plot both functions
plot(x_vals, l_func(x_vals), type = "l", col = "blue",
xlab = "x", ylab = "Function Value",
main = "Functions l(x) and f(x)",
ylim = range(c(l_func(x_vals), f_func(x_vals))))
lines(x_vals, f_func(x_vals), col = "red")
abline(h = 0, lty = 2, col = "gray")
legend("topright", legend = c("l(x)", "f(x)"),
col = c("blue", "red"), lty = 1)

cat("4.(a) Plot created.\n\n")
4.(a) Plot created.
# 4.(a)(ii) Function to solve transcendental equation using Newton's method
solve_transcendental <- function(x0 = 0, tol = 1e-10, max_iter = 1000) {
x <- x0
iterations <- 0
for(i in 1:max_iter) {
fx <- f_func(x)
fpx <- f_prime(x)
# Newton update: x_new = x - f(x)/f'(x)
x_new <- x - fx / fpx
# Check convergence
if(abs(x_new - x) < tol && abs(fx) < tol) {
break
}
x <- x_new
iterations <- i
}
return(list(
solution = x,
function_value = f_func(x),
iterations = iterations
))
}
# Find solution (try different starting points)
result <- solve_transcendental(x0 = -2)
cat("4.(a)(ii) Solution using Newton's method:\n")
4.(a)(ii) Solution using Newton's method:
cat("Estimated solution:", result$solution, "\n")
Estimated solution: -3
cat("Function value at estimate:", result$function_value, "\n")
Function value at estimate: -6.583178e-12
cat("Number of iterations:", result$iterations, "\n\n")
Number of iterations: 8
# 4.(b) Function to sum series for log(1+x)
log_series <- function(x, t0 = 1e-10, max_terms = 1000) {
# Check validity: -1 < x < 1
if(x <= -1 || x >= 1) {
stop("x must be in the interval (-1, 1)")
}
term <- x
sum_series <- term
n <- 1
while(abs(term) >= t0 && n < max_terms) {
n <- n + 1
term <- (-1)^(n-1) * x^n / n
sum_series <- sum_series + term
}
return(list(
x = x,
series_sum = sum_series,
true_value = log(1 + x),
terms_used = n,
absolute_error = abs(sum_series - log(1 + x))
))
}
# Test the function
cat("4.(b) Testing log series function:\n")
4.(b) Testing log series function:
test_values <- c(0.2, -0.3, 0.9)
for(val in test_values) {
result <- tryCatch({
log_series(val)
}, error = function(e) {
list(x = val, error = e$message)
})
if("error" %in% names(result)) {
cat("x =", val, ":", result$error, "\n")
} else {
cat("x =", val, ":\n")
cat("Series sum:", result$series_sum, "\n")
cat("True log(1+x):", result$true_value, "\n")
cat("Terms used:", result$terms_used, "\n")
cat("Absolute error:", result$absolute_error, "\n")
}
}
x = 0.2 :
Series sum: 0.1823216
True log(1+x): 0.1823216
Terms used: 13
Absolute error: 9.863138e-12
x = -0.3 :
Series sum: -0.3566749
True log(1+x): -0.3566749
Terms used: 17
Absolute error: 3.008227e-11
x = 0.9 :
Series sum: 0.6418539
True log(1+x): 0.6418539
Terms used: 170
Absolute error: 4.623013e-11
- Use iris dataset to compute:
- means of the numeric columns
- the means of the numeric columns by Species.
# (i) Means of numeric columns
numeric_cols <- iris[, 1:4]
col_means <- colMeans(numeric_cols)
cat("(i) Means of numeric columns:\n")
(i) Means of numeric columns:
cat("Sepal Length:", col_means[1], "\n")
Sepal Length: 5.843333
cat("Sepal Width:", col_means[2], "\n")
Sepal Width: 3.057333
cat("Petal Length:", col_means[3], "\n")
Petal Length: 3.758
cat("Petal Width:", col_means[4], "\n\n")
Petal Width: 1.199333
# (ii) Means by Species
cat("(ii) Means by Species:\n")
(ii) Means by Species:
species_means <- aggregate(. ~ Species, data = iris, FUN = mean)
print(species_means)
print(iris)
# 5. Iris dataset analysis
# (i) Overall means
cat("(i) Overall means of numeric columns:\n")
(i) Overall means of numeric columns:
cat("-------------------------------------\n")
-------------------------------------
overall <- colMeans(iris[1:4])
names(overall) <- c("Sepal.Length", "Sepal.Width", "Petal.Length", "Petal.Width")
print(overall)
Sepal.Length Sepal.Width Petal.Length Petal.Width
5.843333 3.057333 3.758000 1.199333
# (ii) Means by Species
cat("(ii) Means by Species:\n")
(ii) Means by Species:
cat("----------------------\n")
----------------------
species <- c("setosa", "versicolor", "virginica")
for(sp in species) {
cat(sp, ":\n")
subset_means <- colMeans(iris[iris$Species == sp, 1:4]) #iris[rows, columns]
print(subset_means)
}
setosa :
Sepal.Length Sepal.Width Petal.Length Petal.Width
5.006 3.428 1.462 0.246
versicolor :
Sepal.Length Sepal.Width Petal.Length Petal.Width
5.936 2.770 4.260 1.326
virginica :
Sepal.Length Sepal.Width Petal.Length Petal.Width
6.588 2.974 5.552 2.026
2023
1.(a) Make 3 vectors: (no loops)
Vector A: (3, 3.1, …, 6)
Vector B: (2, 2²/2, 2³/3, …, 2²⁵/25)
Vector C: Repeat (4,6,3) to get 10 total 4s Sum each vector.
#A
A <- seq(3,6,0.1)
A
[1] 3.0 3.1 3.2 3.3 3.4 3.5 3.6 3.7 3.8 3.9 4.0 4.1 4.2 4.3 4.4 4.5 4.6
[18] 4.7 4.8 4.9 5.0 5.1 5.2 5.3 5.4 5.5 5.6 5.7 5.8 5.9 6.0
#B
n <- 1:25
B <- (2^n) / n
B
[1] 2.000000e+00 2.000000e+00 2.666667e+00 4.000000e+00 6.400000e+00
[6] 1.066667e+01 1.828571e+01 3.200000e+01 5.688889e+01 1.024000e+02
[11] 1.861818e+02 3.413333e+02 6.301538e+02 1.170286e+03 2.184533e+03
[16] 4.096000e+03 7.710118e+03 1.456356e+04 2.759411e+04 5.242880e+04
[21] 9.986438e+04 1.906502e+05 3.647221e+05 6.990507e+05 1.342177e+06
#C
C <- rep(c(4,6,3), 10)
C
[1] 4 6 3 4 6 3 4 6 3 4 6 3 4 6 3 4 6 3 4 6 3 4 6 3 4 6 3 4 6 3
1.(b) Generate xVec, yVec with seed 50. Calculate: [No loops] xVec
<- sample(0:999, 250, replace=T) yVec <- sample(0:999, 250,
replace=T) x,y belongs to X,Y i) Sum(y − x) ii) Root over (Average of
x²) iii) Sum of exp(−y_(i+1))/((x_i)+10) for i=1 to n−1
set.seed(50)
xVec <- sample(0:999, 250, replace=T)
yVec <- sample(0:999, 250, replace=T)
#(i)
ans_i <- sum(yVec-xVec)
ans_i
[1] -12273
#(ii)
ans_ii <- sqrt(mean(xVec^2))
ans_ii
[1] 600.7198
#(iii)
n <- length(xVec)
# Use 2:n for y (i+1) and 1:(n-1) for x (i)
ans_iii <- sum(exp(-yVec[2:n]) / (xVec[1:(n-1)] + 10))
ans_iii
[1] 0.004409429
2.(a) With seed 209: Generate X ~ Binomial(20, 0.5) and ε ~ N(0, 3),
100 each. Compute Y = 20 + 1.5X + ε. Save as x, y.
set.seed(209)
x <- rbinom(100, 20, 0.5)
ε <- rnorm(100, 0, 3)
y <- 20 + 1.5*x + ε
2.(b) Write function: input x, y → output matrix[a, b]ᵀ (col
matrix…not transpose). b = (Σxy − (ΣxΣy)/n)/(Σx2-((Σx)2)/n) a
= ybar - b*xbar Store as mat1. & Compare to [20, 1.5]ᵀ which is the
matrix of regression parameters of (a).
# --- Part 2.(b) ---
# Define the function
get_coefficients <- function(x, y) {
n <- length(x)
# Calculate necessary sums
sum_x <- sum(x)
sum_y <- sum(y)
sum_xy <- sum(x * y)
sum_x_sq <- sum(x^2)
# Calculate slope b using the provided formula
# Numerator: Σxy - (ΣxΣy)/n
numerator <- sum_xy - (sum_x * sum_y) / n
# Denominator: Σx^2 - (Σx)^2/n
denominator <- sum_x_sq - (sum_x^2) / n
b <- numerator / denominator
# Calculate intercept a
# a = ybar - b * xbar
a <- mean(y) - b * mean(x)
# Return as a column matrix (2 rows, 1 column)
return(matrix(c(a, b), nrow = 2, ncol = 1))
}
# Store the result as mat1
mat1 <- get_coefficients(x, y)
# Define the theoretical parameters [20, 1.5] for comparison
theoretical <- matrix(c(20, 1.5), nrow = 2, ncol = 1)
# Display the results
print("Estimated Matrix (mat1):")
[1] "Estimated Matrix (mat1):"
print(mat1)
[,1]
[1,] 20.695560
[2,] 1.457999
print("Theoretical Matrix:")
[1] "Theoretical Matrix:"
print(theoretical)
[,1]
[1,] 20.0
[2,] 1.5
print("Difference (Estimated - Theoretical):")
[1] "Difference (Estimated - Theoretical):"
print(mat1 - theoretical)
[,1]
[1,] 0.69556007
[2,] -0.04200109
2.(c) Create D = [1(column full of ones), x] and a column matrix M of
1000 rows using vector y. Compute (DᵀD)⁻¹DᵀM → store as mat2. Compare to
[20, 1.5]ᵀ.
D <- cbind(1, x) # First column = 1, second column = X
M <- matrix(rep(y, length.out = 1000), ncol = 1)
# Calculate (D^T D)^{-1} D^T M
# But D is 100x2, M is 1000x1 - dimensions don't match!
# This seems like an error. Let me assume M should be based on y (100x1)
M_correct <- matrix(y, ncol = 1) # 100x1 matrix
mat2 <- solve(t(D) %*% D) %*% t(D) %*% M_correct
cat("Estimated parameters (mat2):\n")
Estimated parameters (mat2):
print(mat2)
[,1]
20.695560
x 1.457999
cat("Difference from true parameters:\n")
Difference from true parameters:
print(mat2 - matrix(c(20, 1.5), nrow = 2, ncol = 1))
[,1]
0.69556007
x -0.04200109
2.(d) X <- matrix(c(0.63, 0.75, 1.53, -1.70, -0.93, 1.23, 0.80,
1.11, 2.84), nrow = 3, byrow = TRUE) Replace: Row 2 with (0.47, 2.33,
87) Row1Col3=63, Row3Col3=75 Find column means and SDs.
x <- matrix(c(0.63, 0.75, 1.53,
-1.70, -0.93, 1.23,
0.80, 1.11, 2.84), nrow = 3, byrow = TRUE)
x[2,] <- c(0.47, 2.33, 87)
x[1,3] = 63
x[3,3] = 75
x
[,1] [,2] [,3]
[1,] 0.63 0.75 63
[2,] 0.47 2.33 87
[3,] 0.80 1.11 75
col_means <- apply(x, 2, mean)
col_means
[1] 0.6333333 1.3966667 75.0000000
col_sds <- apply(x, 2, sd)
col_sds
[1] 0.1650253 0.8280902 12.0000000
- X ~ Poisson(λ=2.7). Find:
- P(X > 3)
- P(2 < X < 8)
- Smallest k: P(X ≤ k) ≥ 0.5
#(i)
px3_ <- 1-ppois(3,2.7)
px3_
[1] 0.2859078
#(ii)
px2_8 <- sum(dpois(3:7,2.7))
px2_8
[1] 0.4997543
#(iii)
k <- qpois(0.5, 2.7)
k
[1] 3
- Generate 3000 obs from Poisson(λ=1.5) with seed 101. Estimate:
- P(X > 3)
- P(2 < X < 8)
- p(x<=3)
set.seed(101)
sim_x <- rpois(3000, 1.5)
# (i) Estimate P(X > 3)
prob_i <- mean(sim_x > 3)
print(paste("Estimate for P(X > 3):", prob_i))
[1] "Estimate for P(X > 3): 0.071"
# (ii) Estimate P(2 < X < 8)
prob_ii <- mean(sim_x > 2 & sim_x < 8)
print(paste("Estimate for P(2 < X < 8):", prob_ii))
[1] "Estimate for P(2 < X < 8): 0.193666666666667"
# (iii) Estimate P(X <= 3)
prob_iii <- mean(sim_x <= 3)
print(paste("Estimate for P(X <= 3):", prob_iii))
[1] "Estimate for P(X <= 3): 0.929"
- X ~ Exponential(mean=1). Find:
- P(0.5 < X < 1.5)
- k such that P(X < k) = 0.8
px0.5_1.5 <- pexp(1.5, rate=1)-pexp(0.5, rate=1) #rate = 1/mean = 1/lambda
px0.5_1.5
[1] 0.3834005
k <- qexp(0.8, rate=1)
k
[1] 1.609438
- Generate 5000 obs from Exp(1) with seed 102. Estimate:
- P(0.5 < X < 1.5)
- P(X > 1.61)
set.seed(102)
# Note: Since mean = 1, rate = 1/mean = 1
sim_x_exp <- rexp(5000, rate = 1)
# (i) Estimate P(0.5 < X < 1.5)
prob_i_exp <- mean(sim_x_exp > 0.5 & sim_x_exp < 1.5)
print(paste("Estimate for P(0.5 < X < 1.5):", prob_i_exp))
[1] "Estimate for P(0.5 < X < 1.5): 0.3832"
# (ii) Estimate P(X > 1.61)
prob_ii_exp <- mean(sim_x_exp > 1.61)
print(paste("Estimate for P(X > 1.61):", prob_ii_exp))
[1] "Estimate for P(X > 1.61): 0.1924"
- Write function: Add two vectors by truncating longer to match
shorter length.
trunc_add <- function(v1, v2) {
n <- min(length(v1), length(v2))
return(v1[1:n] + v2[1:n])
}
- Write A.sort (sorts ascending) and own.med (finds median using
A.sort). With seed 200, generate 500 obs from N(10,10), find median
using own.med.
# 1. Define Functions
A.sort <- function(x) {
return(sort(x)) # Uses R's built-in sort (ascending)
}
own.med <- function(x) {
sorted_x <- A.sort(x)
n <- length(sorted_x)
if (n %% 2 == 1) {
return(sorted_x[(n + 1) / 2])
} else {
return(mean(sorted_x[c(n / 2, n / 2 + 1)]))
}
}
# 2. Generate Data and Test
set.seed(200)
# Assuming N(10, 10) means mean=10, sd=10 based on previous context
data <- rnorm(500, mean = 10, sd = 10)
result <- own.med(data)
print(paste("Median:", result))
[1] "Median: 10.1536202073796"
- Plot f(x)=x³−2x²−4. Use Newton-Raphson to solve f(x)=0. Function
inputs: x0, tolerance t0. Outputs: root, f(root), iteration count.
# 1. Define the function f(x) and its derivative df(x)
f <- function(x) x^3 - 2*x^2 - 4
df <- function(x) 3*x^2 - 4*x
# 2. Plot f(x)
curve(f, from = -2, to = 4, main = "Plot of f(x)")
abline(h = 0, col = "red") # Shows the x-axis

# 3. Newton-Raphson Function
newton_solve <- function(x0, t0) {
iter <- 0
x <- x0
while (abs(f(x)) > t0) {
x <- x - f(x) / df(x)
iter <- iter + 1
}
return(list(root = x, value = f(x), iterations = iter))
}
# Example Usage (Guessing 2)
newton_solve(2, 0.0001)
$root
[1] 2.594318
$value
[1] 4.882565e-05
$iterations
[1] 4
- In birthwt dataset: treat low, race, smoke, ht, ui as categorical.
Find mean of numeric columns.
# Load data
library(MASS)
data(birthwt)
birthwt$low <- factor(birthwt$low) #Factor converts numeric/text data into categories (groups).
birthwt$race <- factor(birthwt$race)
birthwt$smoke <- factor(birthwt$smoke)
birthwt$ht <- factor(birthwt$ht)
birthwt$ui <- factor(birthwt$ui)
numeric_cols <- c("age", "lwt", "bwt", "ptl", "ftv")
numeric_means <- colMeans(birthwt[numeric_cols])
cat("(a) Means of numeric columns:\n")
(a) Means of numeric columns:
print(numeric_means)
age lwt bwt ptl ftv
23.2380952 129.8148148 2944.5873016 0.1957672 0.7936508
- Write function: For bwt variable, compute mean and SD for each race
group.
bwt_stats_by_race <- function(data) {
races <- levels(data$race)
results <- data.frame()
for(r in races) {
bwt_values <- data$bwt[data$race == r]
mean_val <- mean(bwt_values)
sd_val <- sd(bwt_values)
results <- rbind(results, data.frame(Race = r, Mean = mean_val, SD = sd_val))
}
return(results)
}
cat("\n(b) BWT statistics by race:\n")
(b) BWT statistics by race:
print(bwt_stats_by_race(birthwt))
---
title: "Final Year Solve 24-23"
output: html_notebook
---
# 2024

1.(a) Create a vector x = (1,2,2,3,3,3,4,4,4,4,5,5,5,5,5) by using rep() and find multiplication of x.
```{r}
x <- rep(1:5, c(1,2,3,4,5))
x
```
1.(b) Create vector y = N * e^x / x!, where N = 1:length(x). Find sum of y.
```{r}
N <- 1:length(x)
y <- N*exp(x)/factorial(x)
y
y_sum <- sum(y)
y_sum
```
1.(c) Find index positions where 10 < y < 15. Find the sum of values.
```{r}
indices <- which(y>10 & y<15)
indices
val_sum <- sum(y[indices])
val_sum
```
1.(d) Create int.y as nearest integer of y, count divisible by 4
```{r}
int.y <- round(y)
int.y
n <- length(which(int.y%%4==0))
n
```
1.(e) Function to create y and calculate mean
```{r}
calc_mean <- function(x){
  N <- 1:length(x)
  y <- N*exp(x)/factorial(x)
  am <- mean(y)
  if (any(y<=0)){
    gm <- NA
    hm <- NA
  } else {
    gm <- exp(mean(log(y)))
    hm <- 1/mean(1/y)
  }
  return(list(AM=am,GM=gm,HM=hm))
}

```
1.(f) Evaluate the function for X. 
```{r}
means_result <- calc_mean(x)
cat("Arithmetic mean :", means_result$AM, "\n")
cat("Geometric mean  :", means_result$GM, "\n")
cat("Harmonic mean   :", means_result$HM, "\n")
```
2.(a) Using seed 100, create three stdnormal random vectors of length 100 (x, x1,x2).

(i) Create vectors y,z [y=x+x1, z=y+x2] and 
Evaluate sum((x-xbar)(y-ybar)), sum((x-xbar)(z-zbar)), sum((y-ybar)(z-zbar))

(ii) create matrix A(100x3) where each column is filled by each vector x,y,z. B=(A^T A) then B^-1 = ? Find sum of diagonal elements of B.
```{r}
# (i)
set.seed(100)
x <- rnorm(100)
x1 <- rnorm(100)
x2 <- rnorm(100)

y <- x+x1
z <- y+x2
spxy <- sum((x-mean(x))*(y-mean(y)))
spxz <- sum((x-mean(x))*(z-mean(z)))
spxy
spxz
# (ii)
A <- matrix(c(x,y,z), byrow = FALSE, ncol = 3)
head(A)
B <- t(A) %*% A
B
n <- nrow(B)
diag_sum <- 0
# sum(diag(B))
for (i in 1:n){
    diag_sum <- diag_sum + B[i,i]
}
diag_sum
```
2.(b) Function to count entries > k in each column of a matrix.
```{r}
count_gt <- function(mat, k) {
  apply(mat, 2, function(col) sum(col > k))
}
```
2.(c) Evaluate the func with (A,2)
```{r}
count_gt(A,2)
```
3.(a) Gamma distribution calculations (shape=3, scale=0.25)
(i) P(X ≥ 50)
(ii) P(20 < X < 40)
(iii) Find k such that P(X > k) = 0.1
```{r}
#(i)
p50_ <- 1-pgamma(50, shape=3, scale=0.25)
p50_
#(ii)
p20_40 <- pgamma(40, shape=3, scale=0.25)-pgamma(20, shape=3, scale=0.25)
p20_40
#(iii)
k <- qgamma(0.9, shape = 3, scale = 0.25)  # Since P(X > k) = 0.1 => P(X ≤ k) = 0.9
k
```
3.(b) Generate 5000 observations from gamma(3,0.25) [seed 101]
(i) Estimate P(X ≥ 50)
(ii) Estimate P(20 < X < 40)
(iii) Find deciles (10%, 20%, ..., 90%)
```{r}
set.seed(101)
x<-rgamma(5000, shape=3, scale=0.25)
#(i)
est_px50_ <- mean(x>=50)
est_px50_
#(ii)
est_px20_50 <- mean(x>20 & x<40)
est_px20_50
#(iii)
deciles <- quantile(x, probs = seq(0.1, 0.9, by = 0.1))
deciles
```
---

### **Question 4**

**(a)** Finding the minimum value of the function
[
l(x) = x^4 + 4x^3 + 2x^2 + 12x + 5
]
requires solving the transcendental equation
[
f(x) = 0
]
where
[
f(x) = 4x^3 + 12x^2 + 4x + 12
]
and
[
f'(x) = 12x^2 + 24x + 4
]

**(i)** Draw the functions ( l(x) ) and ( f(x) ) on the same graph for the interval
[
-4 < x < 1
]

**(ii)** Write a function to find the solution of the transcendental equation ( f(x) = 0 ).
The function should return:

* the estimated solution,
* the value of the function at the estimated solution, and
* the number of iterations required.

---

**(b)** Write a function that sums the terms of the given series.

---

---

## Workflow for Question (a)

### **Step 1: Define the functions**

* Define the original function
  [
  l(x) = x^4 + 4x^3 + 2x^2 + 12x + 5
  ]
* Define its first derivative
  [
  f(x) = l'(x) = 4x^3 + 12x^2 + 4x + 12
  ]
* Define the derivative of ( f(x) )
  [
  f'(x) = 12x^2 + 24x + 4
  ]

---

### **Step 2: Visualization**

* Choose the interval ( -4 < x < 1 )
* Plot:

  * ( l(x) )
  * ( f(x) )
* Draw both curves on the **same graph**
* Use the plot to understand where the minimum of ( l(x) ) may occur

---

### **Step 3: Set up the optimization condition**

* Recall that the minimum of ( l(x) ) occurs when:
  [
  f(x) = 0
  ]
* This equation cannot be solved easily by hand, so a **numerical method** is required

---

### **Step 4: Write a root-finding function**

* Write a function that numerically solves:
  [
  f(x) = 0
  ]
* The function should:

  1. Start from an initial guess
  2. Iteratively update the estimate
  3. Stop when convergence is reached

---

### **Step 5: Output requirements**

Your function must return:

* The **estimated root** of ( f(x) = 0 )
* The **value of ( f(x) )** at the estimated root
* The **number of iterations** used

---

## Workflow for Question (b)

### **Step 6: Series computation**

* Identify the given series
* Write a function that:

  * Computes the sum of the series
  * Uses a specified number of terms or a stopping rule
* Return the final sum

---

## One-line workflow summary

> **Define → Visualize → Differentiate → Solve numerically → Report results → Compute series sum**

---
```{r}
# 4.(a) Draw functions l(x) and f(x) on interval -4 < x < 1
l_func <- function(x) x^4 + 4*x^3 + 2*x^2 + 12*x + 5
f_func <- function(x) 4*x^3 + 12*x^2 + 4*x + 12
f_prime <- function(x) 12*x^2 + 24*x + 4

# Create sequence for plotting
x_vals <- seq(-4, 1, length.out = 1000)

# Plot both functions
plot(x_vals, l_func(x_vals), type = "l", col = "blue", 
     xlab = "x", ylab = "Function Value",
     main = "Functions l(x) and f(x)",
     ylim = range(c(l_func(x_vals), f_func(x_vals))))
lines(x_vals, f_func(x_vals), col = "red")
abline(h = 0, lty = 2, col = "gray")
legend("topright", legend = c("l(x)", "f(x)"), 
       col = c("blue", "red"), lty = 1)
cat("4.(a) Plot created.\n\n")

# 4.(a)(ii) Function to solve transcendental equation using Newton's method
solve_transcendental <- function(x0 = 0, tol = 1e-10, max_iter = 1000) {
  x <- x0
  iterations <- 0
  
  for(i in 1:max_iter) {
    fx <- f_func(x)
    fpx <- f_prime(x)
    
    # Newton update: x_new = x - f(x)/f'(x)
    x_new <- x - fx / fpx
    
    # Check convergence
    if(abs(x_new - x) < tol && abs(fx) < tol) {
      break
    }
    
    x <- x_new
    iterations <- i
  }
  
  return(list(
    solution = x,
    function_value = f_func(x),
    iterations = iterations
  ))
}

# Find solution (try different starting points)
result <- solve_transcendental(x0 = -2)
cat("4.(a)(ii) Solution using Newton's method:\n")
cat("Estimated solution:", result$solution, "\n")
cat("Function value at estimate:", result$function_value, "\n")
cat("Number of iterations:", result$iterations, "\n\n")

# 4.(b) Function to sum series for log(1+x)
log_series <- function(x, t0 = 1e-10, max_terms = 1000) {
  # Check validity: -1 < x < 1
  if(x <= -1 || x >= 1) {
    stop("x must be in the interval (-1, 1)")
  }
  
  term <- x
  sum_series <- term
  n <- 1
  
  while(abs(term) >= t0 && n < max_terms) {
    n <- n + 1
    term <- (-1)^(n-1) * x^n / n
    sum_series <- sum_series + term
  }
  
  return(list(
    x = x,
    series_sum = sum_series,
    true_value = log(1 + x),
    terms_used = n,
    absolute_error = abs(sum_series - log(1 + x))
  ))
}

# Test the function
cat("4.(b) Testing log series function:\n")
test_values <- c(0.2, -0.3, 0.9)

for(val in test_values) {
  result <- tryCatch({
    log_series(val)
  }, error = function(e) {
    list(x = val, error = e$message)
  })
  
  if("error" %in% names(result)) {
    cat("x =", val, ":", result$error, "\n")
  } else {
    cat("x =", val, ":\n")
    cat("Series sum:", result$series_sum, "\n")
    cat("True log(1+x):", result$true_value, "\n")
    cat("Terms used:", result$terms_used, "\n")
    cat("Absolute error:", result$absolute_error, "\n")
  }
}
```
5. Use iris dataset to compute:
(i) means of the numeric columns
(ii) the means of the numeric columns by Species.
```{r}
# (i) Means of numeric columns
numeric_cols <- iris[, 1:4]
col_means <- colMeans(numeric_cols)
cat("(i) Means of numeric columns:\n")
cat("Sepal Length:", col_means[1], "\n")
cat("Sepal Width:", col_means[2], "\n")
cat("Petal Length:", col_means[3], "\n")
cat("Petal Width:", col_means[4], "\n\n")

# (ii) Means by Species
cat("(ii) Means by Species:\n")
species_means <- aggregate(. ~ Species, data = iris, FUN = mean)
print(species_means)
```
```{r}
print(iris)
```

```{r}
# 5. Iris dataset analysis
# (i) Overall means
cat("(i) Overall means of numeric columns:\n")
cat("-------------------------------------\n")
overall <- colMeans(iris[1:4])
names(overall) <- c("Sepal.Length", "Sepal.Width", "Petal.Length", "Petal.Width")
print(overall)

# (ii) Means by Species
cat("(ii) Means by Species:\n")
cat("----------------------\n")
species <- c("setosa", "versicolor", "virginica")

for(sp in species) {
  cat(sp, ":\n")
  subset_means <- colMeans(iris[iris$Species == sp, 1:4]) #iris[rows, columns]
  print(subset_means)
}
```
# 2023

1.(a) Make 3 vectors: (no loops)

Vector A: (3, 3.1, ..., 6)

Vector B: (2, 2²/2, 2³/3, …, 2²⁵/25)

Vector C: Repeat (4,6,3) to get 10 total 4s
Sum each vector.
```{r}
#A
A <- seq(3,6,0.1)
A
#B
n <- 1:25
B <- (2^n) / n
B
#C
C <- rep(c(4,6,3), 10)
C
```
1.(b) Generate xVec, yVec with seed 50. Calculate: [No loops]
xVec <- sample(0:999, 250, replace=T)
yVec <- sample(0:999, 250, replace=T)
x,y belongs to X,Y
i) Sum(y − x)
ii) Root over (Average of x²)
iii) Sum of exp(−y_(i+1))/((x_i)+10) for i=1 to n−1
```{r}
set.seed(50)
xVec <- sample(0:999, 250, replace=T)
yVec <- sample(0:999, 250, replace=T)
#(i)
ans_i <- sum(yVec-xVec)
ans_i
#(ii)
ans_ii <- sqrt(mean(xVec^2))
ans_ii
#(iii)
n <- length(xVec)
# Use 2:n for y (i+1) and 1:(n-1) for x (i)
ans_iii <- sum(exp(-yVec[2:n]) / (xVec[1:(n-1)] + 10))
ans_iii
```
2.(a) With seed 209:
Generate X ~ Binomial(20, 0.5) and ε ~ N(0, 3), 100 each.
Compute Y = 20 + 1.5X + ε. Save as x, y.
```{r}
set.seed(209)
x <- rbinom(100, 20, 0.5)
ε <- rnorm(100, 0, 3)
y <- 20 + 1.5*x + ε
```
2.(b) 
Write function: input x, y → output matrix[a, b]ᵀ
(col matrix...not transpose).
b = (Σxy − (ΣxΣy)/n)/(Σx^2-((Σx)^2)/n)
a = ybar - b*xbar
Store as mat1. & Compare to [20, 1.5]ᵀ 
which is the matrix of regression parameters of (a).
```{r}
# --- Part 2.(b) ---
# Define the function
get_coefficients <- function(x, y) {
  n <- length(x)
  # Calculate necessary sums
  sum_x <- sum(x)
  sum_y <- sum(y)
  sum_xy <- sum(x * y)
  sum_x_sq <- sum(x^2)
  # Calculate slope b using the provided formula
  # Numerator: Σxy - (ΣxΣy)/n
  numerator <- sum_xy - (sum_x * sum_y) / n
  # Denominator: Σx^2 - (Σx)^2/n
  denominator <- sum_x_sq - (sum_x^2) / n
  b <- numerator / denominator
  # Calculate intercept a
  # a = ybar - b * xbar
  a <- mean(y) - b * mean(x)
  # Return as a column matrix (2 rows, 1 column)
  return(matrix(c(a, b), nrow = 2, ncol = 1))
}

# Store the result as mat1
mat1 <- get_coefficients(x, y)

# Define the theoretical parameters [20, 1.5] for comparison
theoretical <- matrix(c(20, 1.5), nrow = 2, ncol = 1)

# Display the results
print("Estimated Matrix (mat1):")
print(mat1)

print("Theoretical Matrix:")
print(theoretical)

print("Difference (Estimated - Theoretical):")
print(mat1 - theoretical)
```
2.(c) Create D = [1(column full of ones), x] and a column matrix M of 1000 rows using vector y. Compute (DᵀD)⁻¹DᵀM → store as mat2. Compare to [20, 1.5]ᵀ.
```{r}
D <- cbind(1, x)  # First column = 1, second column = X
M <- matrix(rep(y, length.out = 1000), ncol = 1)

# Calculate (D^T D)^{-1} D^T M
# But D is 100x2, M is 1000x1 - dimensions don't match!
# This seems like an error. Let me assume M should be based on y (100x1)
M_correct <- matrix(y, ncol = 1)  # 100x1 matrix

mat2 <- solve(t(D) %*% D) %*% t(D) %*% M_correct
cat("Estimated parameters (mat2):\n")
print(mat2)
cat("Difference from true parameters:\n")
print(mat2 - matrix(c(20, 1.5), nrow = 2, ncol = 1))
```
2.(d) 
X <- matrix(c(0.63, 0.75, 1.53,
                    -1.70, -0.93, 1.23,
                     0.80, 1.11, 2.84), nrow = 3, byrow = TRUE)
Replace:
Row 2 with (0.47, 2.33, 87)
Row1Col3=63, 
Row3Col3=75
Find column means and SDs.
```{r}
x <- matrix(c(0.63, 0.75, 1.53,
                    -1.70, -0.93, 1.23,
                     0.80, 1.11, 2.84), nrow = 3, byrow = TRUE)
x[2,] <- c(0.47, 2.33, 87)
x[1,3] = 63
x[3,3] = 75
x
col_means <- apply(x, 2, mean)
col_means
col_sds <- apply(x, 2, sd)
col_sds
```
3.
(a) X ~ Poisson(λ=2.7). Find:
i) P(X > 3)
ii) P(2 < X < 8)
iii) Smallest k: P(X ≤ k) ≥ 0.5
```{r}
#(i)
px3_ <- 1-ppois(3,2.7)
px3_
#(ii)
px2_8 <- sum(dpois(3:7,2.7))
px2_8
#(iii)
k <- qpois(0.5, 2.7)
k
```
(b) Generate 3000 obs from Poisson(λ=1.5) with seed 101. 
Estimate: 
i) P(X > 3)
ii) P(2 < X < 8)
iii) p(x<=3)
```{r}
set.seed(101)
sim_x <- rpois(3000, 1.5)

# (i) Estimate P(X > 3)
prob_i <- mean(sim_x > 3)
print(paste("Estimate for P(X > 3):", prob_i))
# (ii) Estimate P(2 < X < 8)
prob_ii <- mean(sim_x > 2 & sim_x < 8)
print(paste("Estimate for P(2 < X < 8):", prob_ii))
# (iii) Estimate P(X <= 3)
prob_iii <- mean(sim_x <= 3)
print(paste("Estimate for P(X <= 3):", prob_iii))
```
(c) X ~ Exponential(mean=1). Find:
i) P(0.5 < X < 1.5)
ii) k such that P(X < k) = 0.8
```{r}
px0.5_1.5 <- pexp(1.5, rate=1)-pexp(0.5, rate=1) #rate = 1/mean = 1/lambda
px0.5_1.5
k <- qexp(0.8, rate=1)
k
```
(d) Generate 5000 obs from Exp(1) with seed 102. 
Estimate:
i) P(0.5 < X < 1.5)
ii) P(X > 1.61)
```{r}
set.seed(102)
# Note: Since mean = 1, rate = 1/mean = 1
sim_x_exp <- rexp(5000, rate = 1)
# (i) Estimate P(0.5 < X < 1.5)
prob_i_exp <- mean(sim_x_exp > 0.5 & sim_x_exp < 1.5)
print(paste("Estimate for P(0.5 < X < 1.5):", prob_i_exp))
# (ii) Estimate P(X > 1.61)
prob_ii_exp <- mean(sim_x_exp > 1.61)
print(paste("Estimate for P(X > 1.61):", prob_ii_exp))
```
4.
(a) Write function: Add two vectors by truncating longer to match shorter length.
```{r}
trunc_add <- function(v1, v2) {
  n <- min(length(v1), length(v2))
  return(v1[1:n] + v2[1:n])
}
```
(b) Write A.sort (sorts ascending) and own.med (finds median using A.sort).
With seed 200, generate 500 obs from N(10,10), find median using own.med.
```{r}
# 1. Define Functions
A.sort <- function(x) {
  return(sort(x)) # Uses R's built-in sort (ascending)
}

own.med <- function(x) {
  sorted_x <- A.sort(x)
  n <- length(sorted_x)
  if (n %% 2 == 1) {
    return(sorted_x[(n + 1) / 2])
  } else {
    return(mean(sorted_x[c(n / 2, n / 2 + 1)]))
  }
}

# 2. Generate Data and Test
set.seed(200)
# Assuming N(10, 10) means mean=10, sd=10 based on previous context
data <- rnorm(500, mean = 10, sd = 10) 
result <- own.med(data)
print(paste("Median:", result))
```
(c) Plot f(x)=x³−2x²−4. Use Newton-Raphson to solve f(x)=0.
Function inputs: x0, tolerance t0.
Outputs: root, f(root), iteration count.
```{r}
# 1. Define the function f(x) and its derivative df(x)
f <- function(x) x^3 - 2*x^2 - 4
df <- function(x) 3*x^2 - 4*x

# 2. Plot f(x)
curve(f, from = -2, to = 4, main = "Plot of f(x)")
abline(h = 0, col = "red") # Shows the x-axis

# 3. Newton-Raphson Function
newton_solve <- function(x0, t0) {
  iter <- 0
  x <- x0
  while (abs(f(x)) > t0) {
    x <- x - f(x) / df(x)
    iter <- iter + 1
  }
  return(list(root = x, value = f(x), iterations = iter))
}

# Example Usage (Guessing 2)
newton_solve(2, 0.0001)
```
5.
(a) In birthwt dataset: treat low, race, smoke, ht, ui as categorical. Find mean of numeric columns.
```{r}
# Load data
library(MASS)
data(birthwt)

birthwt$low <- factor(birthwt$low) #Factor converts numeric/text data into categories (groups).
birthwt$race <- factor(birthwt$race)
birthwt$smoke <- factor(birthwt$smoke)
birthwt$ht <- factor(birthwt$ht)
birthwt$ui <- factor(birthwt$ui)

numeric_cols <- c("age", "lwt", "bwt", "ptl", "ftv")
numeric_means <- colMeans(birthwt[numeric_cols])

cat("(a) Means of numeric columns:\n")
print(numeric_means)

```
(b) Write function: For bwt variable, compute mean and SD for each race group.
```{r}
bwt_stats_by_race <- function(data) {
  races <- levels(data$race)
  results <- data.frame()
  
  for(r in races) {
    bwt_values <- data$bwt[data$race == r]
    mean_val <- mean(bwt_values)
    sd_val <- sd(bwt_values)
    results <- rbind(results, data.frame(Race = r, Mean = mean_val, SD = sd_val))
  }
  
  return(results)
}

cat("\n(b) BWT statistics by race:\n")
print(bwt_stats_by_race(birthwt))
```
