Read X and the City: Modeling Aspects of Urban Life Online
Authors: John A. Adam
Nothing that
we can approximate the logarithm of the factorial
M
! for a large positive integer
M
by a “quick and dirty” method as follows:
From this it follows directly that
M
! ≈
M
M
e
−
M
. This result is sometimes known as the weak form of
Stirling’s approximation
. Returning to equation (A4.3) and applying it to the two terms on the right of equation (A4.4), it follows that
Since
n
N
,
Therefore
We have neglected the term in
n
2
since
N
is large. Hence
Therefore, combining the approximations (A4.2) and (A4.5), we have
The expected number of tails in
N
tosses is
λ
=
Np
. Thus equation (A4.6) can be written in terms of the expectation
λ
as
This is the Poisson distribution for the probability of exactly
n
tails occurring in
N
tosses of the coin, when
p
1. And instead of heads and tails, we can think of customers arriving at the post office, or gaps in traffic, as applied in
Chapters 3
and
9
, respectively.
We can think of this in another way. Note that
This result can be interpreted as the sums of the probabilities of all possible outcomes occurring; in other words, we have a probability distribution.
We state without proof a rather formal expression of a general problem to which this method applies:
Any local maxima or minima of a function
z
=
f
(
x
,
y
) that is subject to the constraint
g
(
x
,
y
) = 0 will be among those points (
x
0
,
y
0
) for which the point (
x
0
,
y
0
,
λ
0
) is a solution to the system of equations