Mathematical Methods for Physics and Engineering : A Comprehensive Guide

(lu) #1

PROBABILITY


The above results may be extended. For example, if the random variables

Xi,i=1, 2 ,...,n, are distributed asXi∼N(μi,σ^2 i) then the random variable


Z=



iciXi(where theciare constants) is distributed asZ∼N(


iciμi,


ic

2

2
i).

30.9.2 The log-normal distribution

If the random variableXfollows a Gaussian distribution then the variable


Y=eXis described by alog-normaldistribution. Clearly, ifXcan take values


in the range−∞to∞,thenYwill lie between 0 and∞. The probability density


function forYis found using the result (30.58). It is


g(y)=f(x(y))





dx
dy




∣=

1
σ


2 π

1
y

exp

[

(lny−μ)^2
2 σ^2

]
.

We note that μandσ^2 are not the mean and variance of the log-normal


distribution, but rather the parameters of the corresponding Gaussian distribution


forX. The mean and variance ofY, however, can be found straightforwardly


using the MGF ofX, which readsMX(t)=E[etX]=exp(μt+^12 σ^2 t^2 ). Thus, the


mean ofYis given by


E[Y]=E[eX]=MX(1) = exp(μ+^12 σ^2 ),

and the variance ofYreads


V[Y]=E[Y^2 ]−(E[Y])^2 =E[e^2 X]−(E[eX])^2

=MX(2)−[MX(1)]^2 =exp(2μ+σ^2 )[exp(σ^2 )−1].

In figure 30.15, we plot some examples of the log-normal distribution for various


values of the parametersμandσ^2.


30.9.3 The exponential and gamma distributions

The exponential distribution with positive parameterλis given by


f(x)=

{
λe−λx forx> 0 ,

0forx≤ 0

(30.116)

and satisfies


∫∞
−∞f(x)dx= 1 as required. The exponential distribution occurs nat-
urally if we consider the distribution of the length of intervals between successive


events in a Poisson process or, equivalently, the distribution of the interval (i.e.


the waiting time) before the first event. If the average number of events per unit


interval isλthen on average there areλxevents in intervalx, so that from the


Poisson distribution the probability that there will be no events in this interval is


given by


Pr(no events in intervalx)=e−λx.
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