06.06.2022 Views

B. P. Lathi, Zhi Ding - Modern Digital and Analog Communication Systems-Oxford University Press (2009)

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

9

RANDOM PROCESSES AND

SPECTRAL ANALYSIS

The notion of a random process is a natural extension of the random variable (RV).

Consider, for example, the temperature x of a certain city at noon. The temperature x

is an RV and takes on different values every day. To get the complete statistics of x, we

need to record values of x at noon over many days (a large number of trials). From this data,

we can determine P x (x), the PDF of the RV x (the temperature at noon).

But the temperature is also a function of time. At 1 p.m., for example, the temperature

may have an entirely different distribution from that of the temperature at noon. Still, the

two temperatures may be related, via a joint probability density function. Thus, this random

temperature x is a function of time and can be expressed as x(t). If the random variable is

defined for a time interval t E [t a , tb], then x(t) is a function of time and is random for every

instant t E [t a , tb]-An RV that is a function of time* is called a random process, or stochastic

process. Thus, a random process is a collection of an infinite number of RVs. Communication

signals as well as noises, typically random and varying with time, are well characterized by

random processes. For this reason, random process is the subject of this chapter before we

study the performance analysis of different communication systems.

9.1 FROM RANDOM VARIABLE TO

RANDOM PROCESS

To specify an RV x, we run multiple trials of the experiment and from the outcomes estimate

Px (x). Similarly, to specify the random process x(t), we do the same thing for each time instant

t. To continue with our example of the random process x(t), the temperature of the city, we

need to record daily temperatures for each value of t (for each time of the day). This can be

done by recording temperatures at every instant of the day, which gives a waveform x(t, {i),

where {i indicates the day for which the record was taken. We need to repeat this procedure

every day for a large number of days. The collection of all possible waveforms is known as the

ensemble ( corresponding to the sample space) of the random process x (t). A waveform in this

collection is a sample function (rather than a sample point) of the random process (Fig. 9.1 ).

* Actually, to qualify as a random process, x could be a function of any practical variable, such as distance. In fact, a

random process may also be a function of more than one variable.

456

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!