lecture notes on elementary probability [PDF]

G.Grimmett & D.Welsh. Introduction to probability theory. Oxford. P.King. Computer and communications systems perfor

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Mathematics 2Y Spring 1995 Probability Theory Contents x1. Basic concepts. Sample space, events, inclusion-exclusion principle,

probabilities. Examples. x2. Independence, conditioning, Baye's formula, law of total probability. Examples. x3. Discrete random variables. Expectation, variance, independence. Binomial, geometric and Poisson distributions and their relationships. Examples. x4. Probability generating functions. Compound randomness. Applications. x5. Continuous random variables. Distribution functions, density functions. Uniform, exponential and normal distributions. x6. Moment generating functions. Statement of Central Limit Theorem. Chebyshev's inequality and applications (including the weak law of large numbers). x7. Markov chains. Transition matrix, steady-state probability vectors, regularity, an ergodic theorem. x8. Birth and Death processes. Steady states. Application to telecom circuits. M/M/1 queue. If there is time we will go on to discuss reliability. Examples on the problem sheets will include some ideas associated with simulation.

Some recommended books

G.Grimmett & D.Welsh. Introduction to probability theory. Oxford. P.King. Computer and communications systems performance modelling. Prentice-Hall. H.F.Mattson Jr. Discrete Mathematics. Wiley. S.B.Maurer & A.A.Ralston. Discrete Algorithmic Mathematics. AddisonWesley. J.Pitman. Probability. Springer-Verlag. S.Ross. A rst course in probability theory. Collier-Macmillan.

2Y Probability, Spring 1995. AME x1.

2

Basic concepts

In this section of the course we will introduce some basic concepts of probability theory: sample spaces, events, inclusion-exclusion principle, probabilities. Think of modelling an experiment. There are a number of di erent possible outcomes to the experiment and we wish to assign a `likelihood' to each of these. We think of an experiment as being repeatable under identical conditions.

1.1. De nition

The set of all possible outcomes of our experiment is called the sample space. It is usually denoted .

1.2. Examples

a. Suppose we ip a coin. = fH; T g. b. Suppose that we roll a six-sided die. = f1; 2; 3; 4; 5; 6g c. Rolling a die twice, = f(i; j ) : i; j 2 f1; 2; 3; 4; 5; 6gg

1.3. De nition

Any subset of the sample space is called an event.

1.4. Example

If I roll a fair die, the event that I roll an even number (f2; 4; 6g  ) has probability one half. Discrete probability theory is concerned with the modelling of experiments which have a nite or countable number of possible outcomes. The simplest case is when there are a nite number of outcomes all of which are equally likely to happen. (For example rolling a fair die.) In general we assign a probability (`likelihood') pi to each element !i of the sample space. i.e. to each possible outcome of the experiment. The probability of the event A = f!1; !2 : : : !ng is then the sum of the probabilities corresponding to the outcomes which make up the event (p1 + p2 + : : : + pn).

1.5. Examples

a. For rolling a fair die we already calculated (without necessarily realising it) that 1 1 1 1 P(f2; 4; 6g) = P(f2g) + P(f4g) + P(f6g) = + + = 6 6 6 2

2Y Probability, Spring 1995. AME

3

b. Suppose that a certain component will fail during its nth minute of operation with probability 1=2n. The chance that the component fails within an hour is then

X1 60

n=1

2n

= (1 , 21 ) 60

1.6. IMPORTANT CHECK

When you set up your model be sure that all of the probabilities are nonnegative less than or equal to one and the sum of the probabilities is equal to one.

1.7. Notation

It is customary to use some notation from set-theory. The probability that both events A and B happen is written P(A \ B ). The probability that at least one of the events A and B happens is written P(A [ B ).

1.8. The principle of inclusion and exclusion

This principle looks rather daunting in full generality, so here rst is the statement for n = 2: for events A; B P(A

[ B ) = P(A) + P(B ) , P(A \ B )

If we take B to be the event A does not happen (in set-theoretic notation B = Ac), then this says 1 = P(A [ Ac) = P(A) + P(Ac ) i.e.

P(Ac ) = 1

, P(A)

In words this is just \the probability that A does not happen is one minus the probability that A does happen". Here then is the general form of the inclusion-exclusion principle: For events A ; A ; : : : ; An, 1

P(A1

2

[ A [ : : : [ An ) = 2

X

in

1

P(Ai )

X

,

i

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