The mathematics of uncertainty β from conditional chance to Bayes' reasoning
The theory of probability was developed to analyse situations where the outcome of an experiment is uncertain. In Class XI, we studied the axiomatic approach to probability and concepts like sample space, events, and probability of events.
In this chapter, we take this forward and study conditional probability, which asks: what is the probability of an event given that another event has already occurred? This leads to important results like the multiplication theorem, the theorem of total probability, and the celebrated Bayes' theorem.
The conditional probability of an event E, given the occurrence of the event F, is defined as:
0 β€ P(E|F) β€ 1 | P(E'|F) = 1 β P(E|F)
P((E βͺ F)|G) = P(E|G) + P(F|G) β P((E β© F)|G)
If {Eβ, Eβ, ..., Eβ} is a partition of the sample space S (meaning the Eα΅’ are pairwise disjoint and their union is S), and each Eα΅’ has nonzero probability, then for any event A associated with S:
This theorem allows us to compute P(A) by considering all possible "causes" Eα΅’ that could lead to event A, weighting each conditional probability P(A|Eα΅’) by the probability P(Eα΅’) of that cause.
The multiplication theorem provides a way to compute the probability of the intersection of events:
For three events E, F, G:
To find the probability that both E and F occur, we can first find the probability that E occurs, and then multiply by the probability that F occurs given that E has already occurred. This is particularly useful for sequential experiments.
Two events E and F are said to be independent if the occurrence of one does not affect the probability of occurrence of the other. Mathematically:
Mutually exclusive: E β© F = β
(cannot both occur).
Independent: P(E β© F) = P(E)Β·P(F) (occurrence of one doesn't affect the other).
These are very different concepts!
Events Eβ, Eβ, ..., Eβ are independent if P(Eα΅’β β© ... β© Eα΅’β) = P(Eα΅’β)Β·...Β·P(Eα΅’β) for every subset. Pairwise independence is weaker than full independence.
If Eβ, Eβ, ..., Eβ are events which constitute a partition of sample space S (i.e., they are pairwise disjoint and Eβ βͺ Eβ βͺ ... βͺ Eβ = S), and A is any event with nonzero probability, then:
Numerator: probability of "cause Eα΅’ AND effect A" β the joint probability that Eα΅’ is the cause and A is the observed effect.
Denominator: the total probability of A β obtained from the theorem of total probability, serving as a normalising constant.
Result: the posterior probability P(Eα΅’|A) β the probability that Eα΅’ is the cause, given that we have observed effect A.
The great Dutch scientist Christiaan Huygens (1629β1695), became acquainted with the correspondence between Pascal and Fermat and published the first book on probability, De Ratiociniis in Ludo Aleae, containing solutions of many interesting problems on probability in games of chance.
The next great work on probability theory is by Jacob Bernoulli (1654β1705), in the form of a great book, Ars Conjectandi, published posthumously in 1713. To him is due the discovery of one of the most important probability distributions β the Binomial distribution.
The next remarkable work on probability lies in 1933. A. N. Kolmogorov (1903β1987) is credited with the axiomatic theory of probability. His book, Foundations of Probability, published in 1933, introduces probability as a set function and is considered a classic.