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Mathematical Methods for Physicists: A concise introduction - Site Map

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INTRODUCTION TO PROBABILITY THEORY<br />

By analogy with those <strong>for</strong> discrete random variables the expected value or mean<br />

and the variance of a continuous random variable X with probability<br />

density function f …x† are de®ned, respectively, to be:<br />

E…X† ˆ ˆ<br />

Z 1<br />

1<br />

xf …x†dx;<br />

…14:40†<br />

Var…X† ˆ 2 ˆ E……X † 2 †ˆ<br />

Z 1<br />

1<br />

…x † 2 f …x†dx:<br />

…14:41†<br />

The Gaussian (or normal) distribution<br />

One of the most important examples of a continuous probability distribution is<br />

the Gaussian (or normal) distribution. The density function <strong>for</strong> this distribution is<br />

given by<br />

f …x† ˆ p 1<br />

<br />

e …x†2 =2 2 ; 1< x < 1; …14:42†<br />

2<br />

where and are the mean and standard deviation, respectively. The corresponding<br />

distribution function is<br />

F…x† ˆP…X x† ˆ p 1<br />

<br />

<br />

2<br />

Z x<br />

1<br />

e …u†2 =2 2 du:<br />

…14:43†<br />

The standard normal distribution has mean zero … ˆ 0† and standard deviation<br />

( ˆ 1)<br />

f …z† ˆp 1 e z2 =2 : …14:44†<br />

2<br />

Any normal distribution can be `standardized' by considering the substitution<br />

z ˆ…x †= in Eqs. (14.42) and (14.43). A graph of the density function (14.44),<br />

known as the standard normal curve, is shown in Fig. 14.7. We have also indicated<br />

the areas within 1, 2 and 3 standard deviations of the mean (that is between<br />

z ˆ1 and ‡1, 2 and ‡2, 3 and‡3):<br />

P…1 Z 1† ˆp<br />

1<br />

2<br />

P…2 Z 2† ˆp<br />

1<br />

2<br />

P…3 Z 3† ˆp<br />

1<br />

2<br />

502<br />

Z 1<br />

1<br />

Z 2<br />

2<br />

Z 3<br />

3<br />

e z2 =2 dz ˆ 0:6827;<br />

e z2 =2 dz ˆ 0:9545;<br />

e z2 =2 dz ˆ 0:9973:

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