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B–5 Cumulative Distribution Functions and Probability Density Functions 691<br />

L is the largest integer such that x L … a, L … M, and M is the number of points in the<br />

discrete distribution. Here it is assumed that the discrete points x i are indexed so that<br />

they occur in ascending order of the index. That is, x 1 6 x 2 6 x 3 6 ... 6 x M .<br />

This theorem was illustrated in Fig. B–3, which is a plot of Eq. (B–20) for Example B–2.<br />

In electrical engineering problems, the CDFs or PDFs of waveforms are relatively<br />

easy to obtain by using the relative frequency approach, as described by Eqs. (B–14) and<br />

(B–15). For example, the PDFs for triangular and square waves are given in Fig. B–6.<br />

These are obtained by sweeping a narrow horizontal window, ¢ x volts wide, vertically<br />

across the waveforms and measuring the relative frequency of occurrence of voltages in the<br />

¢ x window. The time axis is divided into n intervals, and the waveform appears n ∆x times<br />

in these intervals in the ¢ x window. A rough idea of the PDF of a waveform can also be<br />

obtained by looking at the waveform on an analog oscilloscope. Using no horizontal sweep,<br />

the intensity of the presentation as a function of the voltage (y-axis) gives the PDF. (This<br />

assumes that the intensity of the image is proportional to the time that the waveform dwells<br />

in the window ¢ y units wide.) The PDF is proportional to the intensity as a function of y<br />

(the random variable).<br />

x (t)<br />

f (x)<br />

A<br />

f (x)<br />

x<br />

A<br />

1<br />

2A<br />

t<br />

A<br />

A<br />

x<br />

A<br />

x<br />

A<br />

(a) Triangular Waveform and Its Associated PDF<br />

x (t)<br />

f (x)<br />

A<br />

x<br />

A<br />

f (x)<br />

A<br />

t<br />

A<br />

Weights of<br />

d functions<br />

are 0.5<br />

x<br />

(b) Square Waveform and Its Associated PDF<br />

Figure B–6<br />

PDFs for triangular waves and square waves.

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