Mathematical Methods for Physics and Engineering : A Comprehensive Guide

(lu) #1

PROBABILITY


Stirling’s approximation for largexgives


x!≈


2 πx

(x

e

)x

implying that


lnx!≈ln


2 πx+xlnx−x,

which, on substituting into (30.115), yields


lnf(x)≈−λ+xlnλ−(xlnx−x)−ln


2 πx.

Since we expect the Poisson distribution to peak aroundx=λ, we substitute


=x−λto obtain


lnf(x)≈−λ+(λ+)

{
lnλ−ln

[
λ

(
1+


λ

)]}
+(λ+)−ln


2 π(λ+).

Using the expansion ln(1 +z)=z−z^2 /2+···, we find


lnf(x)≈−(λ+)

(

λ


^2
2 λ^2

)
−ln


2 πλ−

(

λ


^2
2 λ^2

)

≈−

^2
2 λ

−ln


2 πλ,

when only the dominant terms are retained, after using the fact thatis of the


order of the standard deviation ofx,i.e.oforderλ^1 /^2. On exponentiating this


result we obtain


f(x)≈

1

2 πλ

exp

[

(x−λ)^2
2 λ

]
,

which is the Gaussian distribution withμ=λandσ^2 =λ.


The larger the value ofλ, the better is the Gaussian approximation to the

Poisson distribution; the approximation is reasonable even forλ= 5, butλ≥ 10


is safer. As in the case of the Gaussian approximation to the binomial distribution,


a continuity correction is necessary since the Poisson distribution is discrete.


E-mail messages are received by an author at an average rate of one per hour. Find the
probability that in a day the author receives 24 messages or more.

We first define the random variable


X= number of messages received in a day.

ThusE[X]=1×24 = 24, and soX∼Po(24). Sinceλ>10 we may approximate the
Poisson distribution byX∼N(24, 24). Now the standard variable is


Z=

X− 24



24


,


and, using the continuity correction, we find


Pr(X> 23 .5) = Pr

(


Z>


23. 5 − 24



24


)


=Pr(Z>− 0 .102) = Pr(Z< 0 .102) = 0. 54 .
Free download pdf