Robert_V._Hogg,_Joseph_W._McKean,_Allen_T._Craig

(Jacob Rumans) #1
72 Probability and Distributions

us to interchange the order of differentiation and integration (or summation in the
discrete case). That is, ifXis continuous,

M′(t)=

dM(t)
dt

=

d
dt

∫∞

−∞

etxf(x)dx=

∫∞

−∞

d
dt

etxf(x)dx=

∫∞

−∞

xetxf(x)dx.

Likewise, ifXis a discrete random variable,


M′(t)=
dM(t)
dt

=


x

xetxp(x).

Upon settingt=0,wehaveineithercase


M′(0) =E(X)=μ.

The second derivative ofM(t)is


M′′(t)=

∫∞

−∞

x^2 etxf(x)dx or


x

x^2 etxp(x),

so thatM′′(0) =E(X^2 ). Accordingly, Var(X)equals


σ^2 =E(X^2 )−μ^2 =M′′(0)−[M′(0)]^2.

For example, ifM(t)=(1−t)−^1 ,t<1, as in the illustration above, then
M′(t)=(1−t)−^2 and M′′(t)=2(1−t)−^3.

Hence
μ=M′(0) = 1


and
σ^2 =M′′(0)−μ^2 =2−1=1.
Of course, we could have computedμandσ^2 from the pdf by


μ=

∫∞

−∞

xf(x)dx and σ^2 =

∫∞

−∞

x^2 f(x)dx−μ^2 ,

respectively. Sometimes one way is easier than the other.
In general, ifmis a positive integer and ifM(m)(t)meansthemth derivative of
M(t), we have, by repeated differentiation with respect tot,


M(m)(0) =E(Xm).

Now


E(Xm)=

∫∞

−∞

xmf(x)dx or


x

xmp(x),

and the integrals (or sums) of this sort are, in mechanics, calledmoments.Since
M(t) generates the values ofE(Xm),m=1, 2 , 3 ,...,it is called the moment-
generating function (mgf). In fact, we sometimes callE(Xm)themth momentof
the distribution, or themth moment ofX.
The next two examples concern random variables whose distributions do not
have mgfs.

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