604 Chapter 21Probability and statistics
Independent events
The possible outcomes of tossing a coin twice are {HH, HT, TH, TT}, each
with probability. The outcome of the second toss (event B) is independent of the
outcome of the first (event A), and the probability of event A andB is then the
product of the probabilities of A and B separately:
P(A and B) 1 = 1 P(A) 1 × 1 P(B) (independent events) (21.16)
EXAMPLE 21.4Find the probability of outcome 10 from two throws of a die.
Of the 36 possible outcomes, those equal to 10 are (5, 5), (4, 6), and (6, 4). The
second throw is independent of the first (or, for a single throw of two dice, the
outcome of each is independent of that of the other). Each outcome has probability
and because they are exclusive,
0 Exercises 9, 10
EXAMPLE 21.5Independent systems
In statistical thermodynamics the probabilityP(E)that a system is in a state with
energyEis a function of Eonly. Two noninteracting (independent) systems with
energiesE
1
andE
2
have combined energyE
1
1 + 1 E
2
and combined probability
P(E
1
1 + 1 E
2
) 1 = 1 P(E
1
) 1 × 1 P(E
2
) (21.17)
One function that satisfies this equation isP(E) 1 = 1 e
βE
, where βis a constant. We have
It can be shown that this function (multiplied by a constant) is the only one
that satisfies (21.17). In statistical thermodynamics the parameter βis inversely
proportional to the temperature,β 1 = 1 − 12 kT, where kis Boltzmann’s constant, and
the exponential probability function describes the Boltzmann distribution.
0 Exercise 11
21.5 The binomial distribution
The binomial distribution is the theoretical distribution that describes the results
of a given number of independent performances of an experiment that has only two
possible outcomes (see Section 21.3). We consider 4 tosses of a coin (or 4 observations
of the spin of an electron). Each toss (each ‘trial’) has two possible outcomes with
PE PE e e e PE E
EE EE
() () ( )
()
12 12
12 12
×= = =+
ββ β+
PP P P()()()()10 5 5 4 6 6 4 3
1
36
1
12
=+ + =×=and and and
1
6
1
6
1
36
×=
1
4