Basic functions of simulating probability distributions

R comes with a set of pseuodo-random number generators that allow you to simulate from well-known probability distributions like:Binomial, Poisson, Exponential, Uniform,Normal, Gamma, Weibull, Log-normal, Beta, Chi-Squared, logistic, Pareto ect.

In base R you may find a number of popular (for some of us) probability distributions. See below.

Distribution Function(arguments)

beta - beta(shape1, shape2, ncp)

binomial - binom(size, prob)

chi-squared - chisq(df, ncp)

exponential - exp(rate)

gamma - gamma(shape, scale)

logistic - logis(location, scale)

normal - norm(mean, sd)

Poisson - pois(lambda)

Student’s t - t(df, ncp)

uniform - unif(min, max)

Placing a prefix (one of the: “d”, “p”, “q”,“r”) for the distribution function will change it’s behavior in the following ways:

dxxx(x,) returns the density or the value on the y-axis of a probability distribution for a discrete value of x

pxxx(q,) returns the cumulative density function (CDF) or the area under the curve to the left of an x value on a probability distribution curve

qxxx(p,) returns the quantile value, i.e. the standardized z value for x

rxxx(n,) returns a random simulation of size n

Binomial(n,p)

rbinom: generate random Binomial variables with a given n (sample size) and p (probability of success)

dbinom: evaluate the Binomial probability density (with a given n,p) at a point x (or vector of points)

pbinom: evaluate the cumulative distribution function for a Binomial distribution

qbinom: returns the quatile value for a given probability

Example Binomial

rbinom(20,2,3/4) # simulate 20 observations from B(2,1/3)
 [1] 1 2 2 1 2 2 2 1 1 2 2 2 2 2 2 1 1 2 0 2
# let us observe the frequencies of 0,1 and 2 from different sample size 
table(rbinom(100,2,3/4))/100

   0    1    2 
0.08 0.35 0.57 
table(rbinom(100,2,3/4))/100

   0    1    2 
0.10 0.34 0.56 
table(rbinom(1000,2,3/4))/1000

    0     1     2 
0.060 0.369 0.571 
table(rbinom(1000,2,3/4))/1000

    0     1     2 
0.061 0.349 0.590 

Cumulative Density Function (CDF) returns the probability P(X<x) for a given value of x from [0,n], for a Binomial distribution.

# CDF 
pbinom(0,2,1/3) # P(X<0) 
[1] 0.4444444
pbinom(1,2,1/3) # P(X<1)
[1] 0.8888889
pbinom(2,2,1/3) # P(X<2)
[1] 1
# PDF
dbinom(0,2,1/3) # calculate P(X=0)
[1] 0.4444444
dbinom(1,2,1/3) # calculate P(X=1)
[1] 0.4444444
dbinom(2,2,1/3) # calculate P(X=2)
[1] 0.1111111

Graphically we have this output:

library(ggplot2)
var.X <- rbinom(100, 10, 0.3)

ggplot() +
  geom_histogram( aes(var.X), binwidth = 1, fill = "white", color = "black" )

Why we use set.seed()?

The seed argument in set.seed is a single value, interpreted as an integer (as defined in help(set.seed()).

The seed in set.seed produces random values which are unique to that seed (and will be same irrespective of the computer you run and hence ensures reproducibility).

So the random values generated by set.seed(1) and set.seed(123) will not be the same but the random values generated by R in your computer using set.seed(1) and by R in my computer using the same seed are the same.

set.seed(512)
x <- seq(0,100,by=1) # create a sequence from 0 to 100 with step=1 
y <- dbinom(x,100,0.6) # Calculate probabilities for X~B(100,0.6) # a vector of values
y
  [1] 1.606938e-40 2.410407e-38 1.789727e-36 8.769664e-35 3.189965e-33
  [6] 9.187099e-32 2.181936e-30 4.395043e-29 7.663856e-28 1.175125e-26
 [11] 1.604045e-25 1.968601e-24 2.190068e-23 2.223762e-22 2.072864e-21
 [16] 1.782663e-20 1.420559e-19 1.052885e-18 7.282455e-18 4.714432e-17
 [21] 2.864017e-16 1.636581e-15 8.815222e-15 4.484265e-14 2.158053e-13
 [26] 9.840720e-13 4.258004e-12 1.750513e-11 6.845755e-11 2.549454e-10
 [31] 9.050560e-10 3.065512e-09 9.915016e-09 3.064641e-08 9.058719e-08
 [36] 2.562323e-07 6.939626e-07 1.800552e-06 4.477688e-06 1.067756e-05
 [41] 2.442492e-05 5.361569e-05 1.129759e-04 2.285792e-04 4.441709e-04
 [46] 8.291190e-04 1.487007e-03 2.562714e-03 4.244495e-03 6.756543e-03
 [51] 1.033751e-02 1.520222e-02 2.148776e-02 2.919091e-02 3.811036e-02
 [56] 4.781118e-02 5.762955e-02 6.672895e-02 7.420719e-02 7.923819e-02
 [61] 8.121914e-02 7.988768e-02 7.537790e-02 6.819905e-02 5.914136e-02
 [66] 4.913282e-02 3.908293e-02 2.974969e-02 2.165603e-02 1.506506e-02
 [71] 1.000750e-02 6.342785e-03 3.832099e-03 2.204769e-03 1.206664e-03
 [76] 6.274654e-04 3.096047e-04 1.447502e-04 6.402414e-05 2.674426e-05
 [81] 1.053055e-05 3.900205e-06 1.355559e-06 4.409650e-07 1.338644e-07
 [86] 3.779700e-08 9.888749e-09 2.386939e-09 5.289241e-10 1.069734e-10
 [91] 1.961179e-11 3.232713e-12 4.743655e-13 6.120845e-14 6.837114e-15
 [96] 6.477266e-16 5.060364e-17 3.130122e-18 1.437301e-19 4.355457e-21
[101] 6.533186e-23
which(y==max(y)) # which is the value of x with the highest probability
[1] 61
# you may also use: dbinom(0:100,100,0.6) to calculate the probabilities
plot(x,y,main="Binomial density B(100,0.6)",col="red",xlab="Observations",ylab="Probability") # pdf
abline(v=which(y==max(y)),col="blue")
text(80,0.08,"Highest probability",col="green")

dbinom(60,100,0.6) # calculate P(X=60)
[1] 0.08121914
dbinom(61,100,0.6) # calculate P(X=61)
[1] 0.07988768

Exercise

Try to change the number of simulations above and observe the behavior of the pdf.

Example Binomial

# Calculate P(X=27) when X~B(100,0.25)
dbinom(27, size=100, prob=0.25)
[1] 0.08064075
#F(x)=P(X<x) pbinom(x,n,p)
pbinom(25,100,0.6)# will give as output P(X<=25)= when X~B(100,0.6)
[1] 1.255514e-12
pbinom(60,100,0.6)# will give as output P(X<=60)= when X~B(100,0.6)
[1] 0.5379247
# Find x such that F(x)= a given value
# P(X<x)=0.5, qbinom(F(x),n,p) 
qbinom(0.5,100,0.6) # output x such as F(x)=0.5 when X~B(100,0.6)
[1] 60

Example Binomial

A bank issues credit cards to customers.Based on the past data, the bank has found out that 75% of all accounts pay on time the bill. If a sample of 25 accounts is selected at random from the current database, construct the Binomial Probability Distribution of accounts paying on time.

We have p=0.75 (pays on time), n=25 individuals, We need to calculate P(X=x) when x=0,1,2,3,4,5,…,25

i=seq(0,25)
prob_binom=dbinom(i, size=25, prob=0.75)# creates a vector with calculated probabilities
prob_binom
 [1] 8.881784e-16 6.661338e-14 2.398082e-12 5.515588e-11 9.100720e-10
 [6] 1.146691e-08 1.146691e-07 9.337339e-07 6.302704e-06 3.571532e-05
[11] 1.714335e-04 7.013190e-04 2.454617e-03 7.363850e-03 1.893561e-02
[16] 4.165835e-02 7.810941e-02 1.240561e-01 1.654082e-01 1.828195e-01
[21] 1.645376e-01 1.175268e-01 6.410555e-02 2.508478e-02 6.271195e-03
[26] 7.525435e-04

Graphically we have:

plot(i,prob_binom,type="l",col="red",lwd=2,main="Density distribution of n clients paying on time",xlab="nr of clients paying on time",ylab="probability of paying on time")
abline(v=which(prob_binom==max(prob_binom)),col="blue")
text(10,0.15,"Highest probability",col="green")


which(prob_binom== max(prob_binom))# x-20 has the highest probability of paying on time. based on the information above the highest probability of individuals paying on time is 20 individuals with a probability = 0.1828195.
[1] 20
prob_binom[20] # P(X=20)
[1] 0.1828195
# just to check the probabilities based also in the graph below
prob_binom[18:21]
[1] 0.1240561 0.1654082 0.1828195 0.1645376

Exercise Try to change the number of individuals, what you observe?

The histogram for increased number of simulations for Binomial distribution

Central Limit Theorem

par(mfrow=c(1,3))
hist(rbinom(15,15,0.6),main="N=15 simulation")
hist(rbinom(150,15,0.6),main="N=150 simulation")
hist(rbinom(1500,15,0.6),main="N=1500 simulation")

Example Binomial

Suppose the probability a client will buy a product in a store is 0.35. What is the distribution of the probabilities of buying a product if in the store in one day arrive 15 clients? We have, X = 0,1,2,..,15 n = 15, and p = 0.35

j=seq(0,15)
Vect=dbinom(j,15,0.35)# 
barplot(Vect,main="probability 15 clients buy",xlab="Nr of clients buying",ylab="Probability of buying")


plot(j,Vect,type="h",lwd=3,col="red",main="Probability that in 15 clients x will buy",xlab="Nr of clients buying",ylab="Probability of buying")


plot(j,Vect,type="l",lwd=3,col="red",main="Probability that in 15 clients x will buy",xlab="Nr of clients buying",ylab="Probability of buying")

Poisson distribution

How we simulate and plot, calculate probabilities and find quantiles from a Poisson distribution.

Example Poisson

rpois(20,5)# simulate 20 values from a Poisson distribution a=5
 [1] 4 4 3 4 5 9 8 6 6 1 3 1 7 4 3 6 3 2 4 4
# Simulation graphs -Histogram
hist(rpois(50,5),col="red",xlab="Values",ylab="Frequencies", main="Histogram of P(5) for 50 simulations") 

hist(rpois(1000,5),col="red",xlab="Values",ylab="Frequencies", main="Histogram of P(5) for 10^3 simulations") 


# probability density function for the simulations above 
plot(density(rpois(1000,5)),col="blue",lwd=2,main="PDF of P(5) for n=10^3 simulations")


# CDF for P(5), F(x)=P(X<x)
ppois(2,5)# calculates P(X<=2) when X~P(5), including x=2
[1] 0.124652
# Calculates probability of X=x, P(X=x)
dpois(0,5)# P(X=0) when X~P(5)
[1] 0.006737947
dpois(1,5) # P(X=1) when X~P(5)
[1] 0.03368973
dpois(0,5)+dpois(1,5) # P(X=0)+P(X=1)=exp(-5)+exp(-5)*5^1
[1] 0.04042768
# Finds the value of x for wich we have F(x)=p , qpois(p,a)
qpois(0.03368973,5) # finds x such that P(X<x)=F(x)=0.5 when X~P(5)
[1] 1

Exercise Poisson

Try to change the value of a=20 and a=0.5 what you observe for the same number of observations?

Example- Poisson

The random variable X has a Poisson distribution with lambda=15. Calculate the probabilities: P(X=20) ; P(X>20); P(10<X<15) ;

la=15 # declare object lambda

# Calculate  P(X=20)
dpois(20,15) 
[1] 0.04181031
# Calculate P(X>20)
1-ppois(20,15)
[1] 0.08297091
# Calculate P(10<X<15), Attention! for discrete distribution = is important
ppois(14,15)-ppois(9,15)
[1] 0.3958

If we increase the simulation number how will the histogram change? Poisson approximation to Normal distribution

par(mfrow=c(1,4))
hist(rpois(15,3),main="N=15 simulation")
hist(rpois(150,3),main="N=150 simulation")
hist(rpois(1500,3),main="N=1500 simulation")
hist(rpois(15000,3),main="N=15000 simulation")

Check parameter estimation.

We know that the parameter of a Poisson distribution is estimated as te mean of the sample. Let us check!

mean(rpois(10,3))
[1] 3.5
mean(rpois(100,3))
[1] 3.01
mean(rpois(1000,3))
[1] 3.118

Observe, the simulation have a mean value very close to the parameter a=3, especially this is observed with the increasing number of simulations. This confirms the fact that: Parameter estimation in probability distributions is closely related with the sample size, the larger the sample the more accurate the estimation. (Central Limit Theorem and Law of Large Numbers)

Graphically the Poisson distribution.

set.seed(34)
pois=rpois(150,3)# simulate 150 values from P(3)
table(pois)
pois
 0  1  2  3  4  5  6  7  8  9 
 9 19 33 27 26 24  4  5  2  1 
hist(pois, main="150 Simulation")
lines(table(pois),col="red",type="l")

barplot(table(pois)/150)

Example Poisson

Suppose you get approximately 16 calls a day from your co-workers. Simulate a 365 day call and visualize it. How can you interpret the histogram below?

set.seed(123)
call <- rpois(n = 365, lambda = 16)
which(call==max(call))
[1] 202
call[202]
[1] 29
ggplot() +
  geom_histogram(aes(call), binwidth = 1, fill = "white", color = "black" )

Continuous distributions

Example Sampling

A service center has observed that during one day it can offer {0,1,2,3} services with probabilities respectively : 0.6; 0.2; 0.15; 0.05 a. Simulate number of services for a period of 10 days, 50 days, 100 days (plot it)

Sim.10<-sample(c(0,1,2,3), size=10, replace=TRUE, prob=c(.6,.2,.15,.05))
Sim.50<-sample(c(0,1,2,3), size=50, replace=TRUE, prob=c(.6,.2,.15,.05))
Sim.100<-sample(c(0,1,2,3), size=100, replace=TRUE, prob=c(.6,.2,.15,.05))

# Histograms
par(mfrow=c(1,3))
hist(Sim.10)
hist(Sim.50)
hist(Sim.100)

Create a normal density function in R

The probability density function of normal distribution is: f(x)=exp((-(x-mu)^2)/2s^2)/ssqrt(2*pi).

f.norm<-function(x){
  exp(-(x-64)^2/2*9^2)/9*sqrt(2*pi)
}

# calculate  P(X<40)
integrate(f.norm,-Inf,40)
0 with absolute error < 0
# Calculate P(X>70)
integrate(f.norm,70,Inf)
0 with absolute error < 0
# Calculate P(40<X<70)
integrate(f.norm,-Inf,70)
0.07757019 with absolute error < 8.2e-05
# Probability density function for N(0,1)
f.1<-function(x){
  (1/sqrt(2*pi))*exp(-x^2/2)
}

# Density plot for a normal distribution 
curve(f.1,xlim=c(-10,10),main="Normal Density plot", xlab="X values", ylab="Probabilities")

curve(f.1,xlim=c(-3,3),main="Normal Density plot", xlab="X values", ylab="Probabilities")

Normal distribution N(m,s2)

rnorm: generate random Normal variables with a given mean and standard deviation

pnorm: evaluate the cumulative distribution function for a Normal distribution

qnorm: return the quantile for a given value of x

Example Normal

rnorm(4) # simulate 4 observations from X~N(0,1)
[1] -1.0396804 -0.1843089  0.9672673 -0.1082801
rnorm(4,mean=3) #  simulate 4 observations from X~N(3,1)
[1] 2.301579 2.724055 4.114649 3.550044
rnorm(4,mean=3,sd=3) #  simulate 4 observations from X~N(3,9) (sd=3)
[1] 6.710027 3.417294 4.230825 1.324629

Example- Normal Distribution

Below are some examples of simulating, finding probabilities and quantiles.

pnorm(1, mean = 0, sd = 1, lower.tail = TRUE, log.p = FALSE) # P(X<1)
[1] 0.8413447
qnorm(0.8413, mean = 0, sd = 1, lower.tail = TRUE, log.p = FALSE) # find x so P(X<x)=0.8413
[1] 0.9998151
# 
pnorm(0, mean = 0, sd = 1, lower.tail = TRUE, log.p = FALSE) # P(X<0)
[1] 0.5
qnorm(0.5, mean = 0, sd = 1, lower.tail = TRUE, log.p = FALSE) # find x so P(X<x)=0.5
[1] 0
rnorm(10, mean = 0, sd = 1)# simulate 10 values from a normal dist mu=0, sd=1
 [1]  0.6053707 -0.5063335 -1.4205655  0.1279930  1.9458512  0.8009143
 [7]  1.1652534  0.3588557 -0.6085572 -0.2022409
rnorm(10, mean = 0, sd = 1)# simulate 10 values from a normal dist mu=0, sd=1
 [1] -0.2732481 -0.4686998  0.7041673 -1.1973635  0.8663661  0.8641525
 [7] -1.1986224  0.6394920  2.4302267 -0.5572155
rnorm(10, mean = 0, sd = 1)# simulate 10 values from a normal dist mu=0, sd=1
 [1]  0.84490424 -0.78220185  1.11071142  0.24982472  1.65191539
 [6] -1.45897073 -0.05129789 -0.52692518 -0.19726487 -0.62957874
# Every simulation is different
summary(rnorm(10, mean = 0, sd = 1))# summary desc statistics
     Min.   1st Qu.    Median      Mean   3rd Qu.      Max. 
-1.186207 -0.700819  0.090291 -0.004632  0.567289  1.484031 
summary(rnorm(100, mean = 0, sd = 1))# summary desc statistics
    Min.  1st Qu.   Median     Mean  3rd Qu.     Max. 
-2.80977 -0.83166 -0.02167 -0.10858  0.63131  2.08672 
summary(rnorm(1000, mean = 0, sd = 1))# summary desc statistics
    Min.  1st Qu.   Median     Mean  3rd Qu.     Max. 
-2.69533 -0.65303  0.05172  0.03393  0.68304  3.39037 
summary(rnorm(10000, mean = 0, sd = 1))# summary desc statistics
     Min.   1st Qu.    Median      Mean   3rd Qu.      Max. 
-3.845320 -0.665178 -0.012122 -0.000968  0.687333  3.847768 
# increasing the number of simulations will converge the values of mean and sd to theoretical values mu=0 and sd=1

Graphically: Histogram and QQ-Plot

y <- rnorm(200,mean=-2,sd=4) #simulate 200 observations from N(2,16)

hist(y,col="red",xlab="Observation",ylab="Frequence", main="Histogram N(2,16)") 


qqnorm(y,col="red") # plot empirical vs theoretical N(2,16)
# add y=x for a better view of the fit
qqline(y,col="blue",lwd=2) 

Exercise Try to increase the number of observations and observe QQ-plot.

Histogram and density plot for normal distribution.

set.seed(34)
N <- rnorm(1000, mean=50, sd=8)# simulate n=1000 from N(50,25)
hist(N, probability=TRUE,col="red",main="Normal distribution")
N.1 <- seq(min(N), max(N), length=100)
lines(N.1, dnorm(N.1, mean=50, sd=8))

Standardized values and histogram/ density plot

Z=(N-mean(N))/sd(N)# standardize simulations (N)
hist(Z, probability=TRUE,col="red",main="Standardized density plot")
N.2 <- seq(min(Z), max(Z), length=100)
lines(N.2, dnorm(N.2),col="black",lwd=2)

Normal distribution Simulation example

set.seed(512)
x=rnorm(100,0,1)# real observations
plot(density(x),main=" Simulated vs Real",lwd=2,xlim=c(-7,7),ylim=c(0,0.45))

x1=rnorm(100,0.5,1.5)# simulate 100 observations from N(0.5,1.5)
lines(density(x1),col="red",lwd=2)# plot x1

x2=rnorm(100,1,1)#simulate 100 observations from N(1,1)
lines(density(x2),col="blue",lwd=2)# plot x2

x3=rnorm(100,3,3)#simulate 100 observations from N(3,3)
lines(density(x3),col="green",lwd=2)# plot x3

legend(-6,0.4,c("reale","Sim 1","Sim 2","Sim 3"),fill=c("black","blue","red","green"),box.col="white")


# We can also plot a scatterplot to check the fitting
plot(x,x1,col="red",pch="R",ylim=c(-4,10),lwd=4,ylab="X2,X3",xlab="Real",main="Real vs Simulations")
points(x,x2,col="blue",pch="O")
points(x,x3,col="green",pch="X3")
legend(-3,8,c("real~1","real~2","real~3"),fill=c("blue","red","green"),box.col="white")

Exercise Try to graph the empirical rules for a normal distribution.

Exponential distribution E(a)

Simulations: Simulate 20 observations from exponential distribution with rate a=2

rexp(20,2)
 [1] 0.236461562 1.185195289 0.306916572 0.853144883 0.517788602
 [6] 0.356570007 0.223254350 0.112111269 0.126689595 0.128251989
[11] 0.595154632 0.295709382 0.244065052 0.410756204 0.275743932
[16] 0.341076302 0.039352908 0.556349813 0.005826933 0.752978405
# Histogram
hist(rexp(100,2), breaks = 100, col="red",xlab="vlerat X",main = "Histogram of exponential distribution")    
text(1,6,"X~E(2)")
text(1,5,"100 observations")

#
hist(rexp(1000,5),col="red",xlab="Simulations",ylab="Frequency", main="Histogram of Exp(5) for 10^3 simulations")

plot(density(rexp(1000,5)),col="blue",lwd=2,main="Probability Density  Function ")

Calculate probabilities

# Cumulative function F(x) for X~E(a)
pexp(2,5)# calculates F(2)=P(X<2) for X~E(5)
[1] 0.9999546
Exp=function(x,a=5){a*exp(-a*x)}# p.d.f for exponential distribution of unknown parameter a (by default a=5)

# P(X<2)<-integrate(Exp,0,2)
F.exp=integrate(Exp,0,2) # same as: pexp(x,a)=F(x) for X~E(a)

# qexp(p,a) will find x such as F(x)=P(X<x)=p for X~E(a)
qexp(0.9999546,5) # Finds x such as F(x)=0.98168; Look pexp() above.
[1] 2

Example Exponential

Remember from the Poisson example above,lambda=15,Let suppose the time from two arrivals is exponential with intensity 15 arrival per hour (60minutes. Estimate the parameter of exponential distribution in minutes. 15 arrivals/60 minutes=0.25 arrivals/min =rate Find the probability that time between two arrivals is:

  1. less than 10 minutes.

  2. more than 5 minutes and less than 10 minutes

  3. more than 30 minutes

library(ggplot2)
max.x<-qexp(0.999, rate=0.25)# finds the maximum value of x for which exist P(X<x)=0.999 very close to 1
x.value <- seq(0, max.x, length=100)# construct a sequence of x
qplot(x.value, dexp(x.value, rate=0.2), geom="line", ylab="f(x)", xlab="x",main="Density plot for exponential distribution")+
geom_vline(xintercept=c(5,10,30),col="red",lwd=1)

# we added the vertical lines to observe the probabilities

# calculate probabilities
pexp(10,0.25)
[1] 0.917915
pexp(10,0.25)- pexp(5,0.25)
[1] 0.2044198
1-pexp(30,0.25)
[1] 0.0005530844

Uniform distribution

Use runif() to sample from a continuous uniform distribution.

runif(n, min=0, max=1)# simulate n values from Uniform (0,1) punif(): To calculate the cdf qunif(): to find the quantile for a given value of probability

u <- runif(100000, min = 0, max = 1)
punif(0.5,0.1)# Calculate P(X<0.5)
[1] 0.4444444
qunif(0.4444444,0.1)# Find x such as P(X<x)=0.444
[1] 0.5
# plot to visualize
ggplot() + 
  geom_histogram(aes(u), binwidth = 0.05, boundary = 0, fill = "white", colour = "black")

Eralda Gjika (Dhamo)

---
title: "Simulation and Probability Distributions in R"
subtitle: "Discrete and Continuous random Variables"
author: "Eralda Gjika (Dhamo)"
date: "18 January 2021"
output: html_notebook
---


## Basic functions of simulating probability distributions

R comes with a set of pseuodo-random number generators that allow you to simulate from well-known probability distributions like:Binomial, Poisson, Exponential, Uniform,Normal, Gamma, Weibull, Log-normal, Beta, Chi-Squared, logistic, Pareto ect. 

In base R you may find a number of popular (for some of us) probability distributions. See below.

### Distribution		Function(arguments)

beta	-	beta(shape1, shape2, ncp)

binomial	-	binom(size, prob)

chi-squared	-	chisq(df, ncp)

exponential	-	exp(rate)

gamma	-	gamma(shape, scale)

logistic	-	logis(location, scale)

normal	-	norm(mean, sd)

Poisson	-	pois(lambda)

Student's t	-	t(df, ncp)

uniform	-	unif(min, max)

Placing a prefix (one of the: "d", "p", "q","r") for the distribution function will change it's behavior in the following ways:

dxxx(x,) returns the density or the value on the y-axis of a probability distribution for a discrete value of x

pxxx(q,) returns the cumulative density function (CDF) or the area under the curve to the left of an x value on a probability distribution curve

qxxx(p,) returns the quantile value, i.e. the standardized z value for x

rxxx(n,) returns a random simulation of size n


## Binomial(n,p)
rbinom: generate random Binomial variables with a given n (sample size) and p (probability of success)

dbinom: evaluate the Binomial probability density (with a given n,p) at a point x (or vector of points)

pbinom: evaluate the cumulative distribution function for a Binomial distribution

qbinom: returns the quatile value for a given probability 

### Example Binomial 
```{r}
rbinom(20,2,3/4) # simulate 20 observations from B(2,1/3)
# let us observe the frequencies of 0,1 and 2 from different sample size 
table(rbinom(100,2,3/4))/100
table(rbinom(100,2,3/4))/100
table(rbinom(1000,2,3/4))/1000
table(rbinom(1000,2,3/4))/1000
```
Cumulative Density Function (CDF) returns the probability P(X<x) for a given value of x from [0,n], for a Binomial distribution. 
```{r}
# CDF 
pbinom(0,2,1/3) # P(X<0) 
pbinom(1,2,1/3) # P(X<1)
pbinom(2,2,1/3) # P(X<2)
# PDF
dbinom(0,2,1/3) # calculate P(X=0)
dbinom(1,2,1/3) # calculate P(X=1)
dbinom(2,2,1/3) # calculate P(X=2)
```
Graphically we have this output:
```{r}
library(ggplot2)
var.X <- rbinom(100, 10, 0.3)

ggplot() +
  geom_histogram( aes(var.X), binwidth = 1, fill = "white", color = "black" )
```


## Why we use set.seed()?

The seed argument in set.seed is a single value, interpreted as an integer (as defined in help(set.seed()). 

The seed in set.seed produces random values which are unique to that seed (and will be same irrespective of the computer you run and hence ensures reproducibility). 

So the random values generated by set.seed(1) and set.seed(123) will not be the same but the random values generated by R in your computer using set.seed(1) and by R in my computer using the same seed are the same.

```{r}
set.seed(512)
x <- seq(0,100,by=1) # create a sequence from 0 to 100 with step=1 
y <- dbinom(x,100,0.6) # Calculate probabilities for X~B(100,0.6) # a vector of values
y
which(y==max(y)) # which is the value of x with the highest probability
# you may also use: dbinom(0:100,100,0.6) to calculate the probabilities
plot(x,y,main="Binomial density B(100,0.6)",col="red",xlab="Observations",ylab="Probability") # pdf
abline(v=which(y==max(y)),col="blue")
text(80,0.08,"Highest probability",col="green")
dbinom(60,100,0.6) # calculate P(X=60)
dbinom(61,100,0.6) # calculate P(X=61)
```
#### Exercise
Try to change the number of simulations above and observe the behavior of the pdf.

### Example Binomial
```{r}
# Calculate P(X=27) when X~B(100,0.25)
dbinom(27, size=100, prob=0.25)
#F(x)=P(X<x) pbinom(x,n,p)
pbinom(25,100,0.6)# will give as output P(X<=25)= when X~B(100,0.6)
pbinom(60,100,0.6)# will give as output P(X<=60)= when X~B(100,0.6)
# Find x such that F(x)= a given value
# P(X<x)=0.5, qbinom(F(x),n,p) 
qbinom(0.5,100,0.6) # output x such as F(x)=0.5 when X~B(100,0.6)
```

### Example Binomial 
A bank issues credit cards to customers.Based on the past data, the bank has found out that 75% of all accounts pay on time the bill. 
If a sample of 25 accounts is selected at random from the current database, construct the Binomial Probability Distribution of accounts paying on time.

We have p=0.75 (pays on time), n=25 individuals, We need to calculate P(X=x) when x=0,1,2,3,4,5,...,25
```{r}
i=seq(0,25)
prob_binom=dbinom(i, size=25, prob=0.75)# creates a vector with calculated probabilities
prob_binom
```
Graphically we have:
```{r}
plot(i,prob_binom,type="l",col="red",lwd=2,main="Density distribution of n clients paying on time",xlab="nr of clients paying on time",ylab="probability of paying on time")
abline(v=which(prob_binom==max(prob_binom)),col="blue")
text(10,0.15,"Highest probability",col="green")

which(prob_binom== max(prob_binom))# x-20 has the highest probability of paying on time. based on the information above the highest probability of individuals paying on time is 20 individuals with a probability = 0.1828195.

prob_binom[20] # P(X=20)
# just to check the probabilities based also in the graph below
prob_binom[18:21]
```

Exercise
Try to change the number of individuals, what you observe?

#### The histogram for increased number of simulations for Binomial distribution
Central Limit Theorem 
```{r}
par(mfrow=c(1,3))
hist(rbinom(15,15,0.6),main="N=15 simulation")
hist(rbinom(150,15,0.6),main="N=150 simulation")
hist(rbinom(1500,15,0.6),main="N=1500 simulation")
```
### Example Binomial
Suppose the probability a client will buy a product in a store is 0.35. What is the distribution of the probabilities of buying a product if in the store in one day arrive 15 clients? 
We have, X = 0,1,2,..,15 n = 15, and p = 0.35

```{r}
j=seq(0,15)
Vect=dbinom(j,15,0.35)# 
barplot(Vect,main="probability 15 clients buy",xlab="Nr of clients buying",ylab="Probability of buying")

plot(j,Vect,type="h",lwd=3,col="red",main="Probability that in 15 clients x will buy",xlab="Nr of clients buying",ylab="Probability of buying")

plot(j,Vect,type="l",lwd=3,col="red",main="Probability that in 15 clients x will buy",xlab="Nr of clients buying",ylab="Probability of buying")

```

## Poisson distribution
How we simulate and plot, calculate probabilities and find quantiles from a Poisson distribution. 

### Example Poisson
```{r}
rpois(20,5)# simulate 20 values from a Poisson distribution a=5

# Simulation graphs -Histogram
hist(rpois(50,5),col="red",xlab="Values",ylab="Frequencies", main="Histogram of P(5) for 50 simulations") 
hist(rpois(1000,5),col="red",xlab="Values",ylab="Frequencies", main="Histogram of P(5) for 10^3 simulations") 

# probability density function for the simulations above 
plot(density(rpois(1000,5)),col="blue",lwd=2,main="PDF of P(5) for n=10^3 simulations")

# CDF for P(5), F(x)=P(X<x)
ppois(2,5)# calculates P(X<=2) when X~P(5), including x=2

# Calculates probability of X=x, P(X=x)
dpois(0,5)# P(X=0) when X~P(5)
dpois(1,5) # P(X=1) when X~P(5)
dpois(0,5)+dpois(1,5) # P(X=0)+P(X=1)=exp(-5)+exp(-5)*5^1

# Finds the value of x for wich we have F(x)=p , qpois(p,a)
qpois(0.03368973,5) # finds x such that P(X<x)=F(x)=0.5 when X~P(5)
```
### Exercise Poisson
Try to change the value of a=20 and a=0.5 what you observe for the same number of observations?

### Example- Poisson
 The random variable X has a Poisson distribution with lambda=15. Calculate the probabilities:
  P(X=20) ; P(X>20); P(10<X<15) ; 
```{r}
la=15 # declare object lambda

# Calculate  P(X=20)
dpois(20,15) 

# Calculate P(X>20)
1-ppois(20,15)

# Calculate P(10<X<15), Attention! for discrete distribution = is important
ppois(14,15)-ppois(9,15)
```

 If we increase the simulation number how will the histogram change?
 Poisson approximation to Normal distribution

```{r}
par(mfrow=c(1,4))
hist(rpois(15,3),main="N=15 simulation")
hist(rpois(150,3),main="N=150 simulation")
hist(rpois(1500,3),main="N=1500 simulation")
hist(rpois(15000,3),main="N=15000 simulation")
```

#### Check parameter estimation. 
We know that the parameter of a Poisson distribution is estimated as te mean of the sample. Let us check!
```{r}
mean(rpois(10,3))
mean(rpois(100,3))
mean(rpois(1000,3))
```
Observe, the simulation have a mean value very close to the parameter a=3, especially this is observed with the increasing number of simulations. 
This confirms the fact that: Parameter estimation in probability distributions is closely related with the sample size, the larger the sample the more accurate the estimation. (Central Limit Theorem and Law of Large Numbers)

Graphically the Poisson distribution.
```{r}
set.seed(34)
pois=rpois(150,3)# simulate 150 values from P(3)
table(pois)
hist(pois, main="150 Simulation")
lines(table(pois),col="red",type="l")
barplot(table(pois)/150)
```
### Example Poisson
Suppose you get approximately 16 calls a day from your co-workers. Simulate a 365 day call and visualize it. How can you interpret the histogram below?

```{r}
set.seed(123)
call <- rpois(n = 365, lambda = 16)
which(call==max(call))
call[202]

ggplot() +
  geom_histogram(aes(call), binwidth = 1, fill = "white", color = "black" )
```
# Continuous distributions

### Example Sampling
A service center has observed that during one day it can offer {0,1,2,3} services with probabilities respectively : 0.6; 0.2; 0.15; 0.05
a. Simulate number of services for a period of 10 days, 50 days, 100 days (plot it)

```{r}
Sim.10<-sample(c(0,1,2,3), size=10, replace=TRUE, prob=c(.6,.2,.15,.05))
Sim.50<-sample(c(0,1,2,3), size=50, replace=TRUE, prob=c(.6,.2,.15,.05))
Sim.100<-sample(c(0,1,2,3), size=100, replace=TRUE, prob=c(.6,.2,.15,.05))

# Histograms
par(mfrow=c(1,3))
hist(Sim.10)
hist(Sim.50)
hist(Sim.100)
```
### Create a normal density function in R
The probability density function of normal distribution is:  f(x)=exp((-(x-mu)^2)/2*s^2)/s*sqrt(2*pi).

```{r}
f.norm<-function(x){
  exp(-(x-64)^2/2*9^2)/9*sqrt(2*pi)
}

# calculate  P(X<40)
integrate(f.norm,-Inf,40)

# Calculate P(X>70)
integrate(f.norm,70,Inf)

# Calculate P(40<X<70)
integrate(f.norm,-Inf,70)

# Probability density function for N(0,1)
f.1<-function(x){
  (1/sqrt(2*pi))*exp(-x^2/2)
}

# Density plot for a normal distribution 
curve(f.1,xlim=c(-10,10),main="Normal Density plot", xlab="X values", ylab="Probabilities")
curve(f.1,xlim=c(-3,3),main="Normal Density plot", xlab="X values", ylab="Probabilities")
```
## Normal distribution N(m,s2)

rnorm: generate random Normal variables with a given mean and standard deviation

pnorm: evaluate the cumulative distribution function for a Normal distribution

qnorm: return the quantile for a given value of x

### Example Normal 
```{r}
rnorm(4) # simulate 4 observations from X~N(0,1)
rnorm(4,mean=3) #  simulate 4 observations from X~N(3,1)
rnorm(4,mean=3,sd=3) #  simulate 4 observations from X~N(3,9) (sd=3)
```
### Example- Normal Distribution
Below are some examples of simulating, finding probabilities and quantiles.
```{r}
pnorm(1, mean = 0, sd = 1, lower.tail = TRUE, log.p = FALSE) # P(X<1)
qnorm(0.8413, mean = 0, sd = 1, lower.tail = TRUE, log.p = FALSE) # find x so P(X<x)=0.8413
# 
pnorm(0, mean = 0, sd = 1, lower.tail = TRUE, log.p = FALSE) # P(X<0)
qnorm(0.5, mean = 0, sd = 1, lower.tail = TRUE, log.p = FALSE) # find x so P(X<x)=0.5

rnorm(10, mean = 0, sd = 1)# simulate 10 values from a normal dist mu=0, sd=1
rnorm(10, mean = 0, sd = 1)# simulate 10 values from a normal dist mu=0, sd=1
rnorm(10, mean = 0, sd = 1)# simulate 10 values from a normal dist mu=0, sd=1

# Every simulation is different
summary(rnorm(10, mean = 0, sd = 1))# summary desc statistics
summary(rnorm(100, mean = 0, sd = 1))# summary desc statistics
summary(rnorm(1000, mean = 0, sd = 1))# summary desc statistics
summary(rnorm(10000, mean = 0, sd = 1))# summary desc statistics
# increasing the number of simulations will converge the values of mean and sd to theoretical values mu=0 and sd=1
```
Graphically: Histogram and QQ-Plot
```{r}
y <- rnorm(200,mean=-2,sd=4) #simulate 200 observations from N(2,16)

hist(y,col="red",xlab="Observation",ylab="Frequence", main="Histogram N(2,16)") 

qqnorm(y,col="red") # plot empirical vs theoretical N(2,16)
# add y=x for a better view of the fit
qqline(y,col="blue",lwd=2) 
```
Exercise
Try to increase the number of observations and observe QQ-plot.

Histogram and density plot for normal distribution.
```{r}
set.seed(34)
N <- rnorm(1000, mean=50, sd=8)# simulate n=1000 from N(50,25)
hist(N, probability=TRUE,col="red",main="Normal distribution")
N.1 <- seq(min(N), max(N), length=100)
lines(N.1, dnorm(N.1, mean=50, sd=8))
```
Standardized values and histogram/ density plot

```{r}
Z=(N-mean(N))/sd(N)# standardize simulations (N)
hist(Z, probability=TRUE,col="red",main="Standardized density plot")
N.2 <- seq(min(Z), max(Z), length=100)
lines(N.2, dnorm(N.2),col="black",lwd=2)
```
Normal distribution Simulation example
```{r}
set.seed(512)
x=rnorm(100,0,1)# real observations
plot(density(x),main=" Simulated vs Real",lwd=2,xlim=c(-7,7),ylim=c(0,0.45))

x1=rnorm(100,0.5,1.5)# simulate 100 observations from N(0.5,1.5)
lines(density(x1),col="red",lwd=2)# plot x1

x2=rnorm(100,1,1)#simulate 100 observations from N(1,1)
lines(density(x2),col="blue",lwd=2)# plot x2

x3=rnorm(100,3,3)#simulate 100 observations from N(3,3)
lines(density(x3),col="green",lwd=2)# plot x3

legend(-6,0.4,c("reale","Sim 1","Sim 2","Sim 3"),fill=c("black","blue","red","green"),box.col="white")

# We can also use scatterplot to check the fitting
plot(x,x1,col="red",pch="R",ylim=c(-4,10),lwd=4,ylab="X2,X3",xlab="Real",main="Real vs Simulations")
points(x,x2,col="blue",pch="O")
points(x,x3,col="green",pch="X3")
legend(-3,8,c("real~1","real~2","real~3"),fill=c("blue","red","green"),box.col="white")
```

Exercise
Try to graph the empirical rules for a normal distribution. 

# Exponential distribution E(a)                   
Simulations:
Simulate 20 observations from exponential distribution with rate a=2
```{r}
rexp(20,2)
# Histogram
hist(rexp(100,2), breaks = 100, col="red",xlab="vlerat X",main = "Histogram of exponential distribution")    
text(1,6,"X~E(2)")
text(1,5,"100 observations")
#
hist(rexp(1000,5),col="red",xlab="Simulations",ylab="Frequency", main="Histogram of Exp(5) for 10^3 simulations")
plot(density(rexp(1000,5)),col="blue",lwd=2,main="Probability Density  Function ")
```
Calculate probabilities
```{r}
# Cumulative function F(x) for X~E(a)
pexp(2,5)# calculates F(2)=P(X<2) for X~E(5)

Exp=function(x,a=5){a*exp(-a*x)}# p.d.f for exponential distribution of unknown parameter a (by default a=5)

# P(X<2)<-integrate(Exp,0,2)
F.exp=integrate(Exp,0,2) # same as: pexp(x,a)=F(x) for X~E(a)

# qexp(p,a) will find x such as F(x)=P(X<x)=p for X~E(a)
qexp(0.9999546,5) # Finds x such as F(x)=0.98168; Look pexp() above.
```
### Example Exponential
Remember from the Poisson example above,lambda=15,Let suppose the time from two arrivals is exponential with intensity 15 arrival per hour (60minutes. Estimate the parameter of exponential distribution in minutes. 
15 arrivals/60 minutes=0.25 arrivals/min =rate
Find the probability that time between two arrivals is:

a) less than 10 minutes.

b) more than 5 minutes and less than 10 minutes

c) more than 30 minutes

```{r}
library(ggplot2)
max.x<-qexp(0.999, rate=0.25)# finds the maximum value of x for which exist P(X<x)=0.999 very close to 1
x.value <- seq(0, max.x, length=100)# construct a sequence of x
qplot(x.value, dexp(x.value, rate=0.2), geom="line", ylab="f(x)", xlab="x",main="Density plot for exponential distribution")+
geom_vline(xintercept=c(5,10,30),col="red",lwd=1)
# we added the vertical lines to observe the probabilities

# calculate probabilities
pexp(10,0.25)
pexp(10,0.25)- pexp(5,0.25)
1-pexp(30,0.25)
```
## Uniform distribution

Use runif() to sample from a continuous uniform distribution.

runif(n, min=0, max=1)# simulate n values from Uniform (0,1)
punif(): To calculate the cdf
qunif(): to find the quantile for a given value of probability

```{r}
u <- runif(100000, min = 0, max = 1)
punif(0.5,0.1)# Calculate P(X<0.5)
qunif(0.4444444,0.1)# Find x such as P(X<x)=0.444

# plot to visualize
ggplot() + 
  geom_histogram(aes(u), binwidth = 0.05, boundary = 0, fill = "white", colour = "black")
```

### Eralda Gjika (Dhamo)
## January 2021


Reference:

http://pages.cs.wisc.edu/~st471-1/Rnotes/Density.html

https://bookdown.org/rdpeng/rprogdatascience/simulation.html

http://www.columbia.edu/~cjd11/charles_dimaggio/DIRE/styled-4/styled-6/code/

https://stat.ethz.ch/R-manual/R-devel/library/stats/html/NegBinomial.html

https://psyteachr.github.io/msc-data-skills/sim.html
