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Sec. 2–1 Properties of Signals and Noise 37<br />

It is seen that this operator is a linear operator, since, from Eq. (2–1), the average of the<br />

sum of two quantities is the same as the sum of their averages: †<br />

8a 1 w 1 (t) + a 2 w 2 (t)9 = a 1 8w 1 (t)9 + a 2 8w 2 (t)9<br />

(2–2)<br />

Equation (2–1) can be reduced to a simpler form given by Eq. (2–4) if the operator is operating<br />

on a periodic waveform.<br />

DEFINITION.<br />

A waveform w(t) is periodic with period T 0 if<br />

w(t) = w(t + T 0 ) for all t<br />

where T 0 is the smallest positive number that satisfies this relationship. ‡<br />

(2–3)<br />

For example, a sinusoidal waveform of frequency f 0 = 1/T 0 hertz is periodic, since it<br />

satisfies Eq. (2–3). From this definition, it is clear that a periodic waveform will have significant<br />

values over an infinite time interval (-q, q) . Consequently, physical waveforms<br />

cannot be truly periodic, but they can have periodic values over a finite time interval. That<br />

is, Eq. (2–3) can be satisfied for t over some finite interval, but not for all values of t.<br />

THEOREM.<br />

reduced to<br />

If the waveform involved is periodic, the time average operator can be<br />

8[ #<br />

1 ]9 =<br />

T 0 L<br />

T 0 /2+a<br />

-T 0 /2+a<br />

[ # ] dt<br />

(2–4)<br />

where T 0 is the period of the waveform and a is an arbitrary real constant, which may<br />

be taken to be zero.<br />

Equation (2–4) readily follows from Eq. (2–1) because, referring to Eq. (2–1), integrals<br />

over successive time intervals T 0 seconds wide have identical areas, since the waveshape is<br />

periodic with period T 0 . As these integrals are summed, the total area and T are proportionally<br />

larger, resulting in a value for the time average that is the same as just integrating over one<br />

period and dividing by the width of that interval, T 0 .<br />

In summary, Eq. (2–1) may be used to evaluate the time average of any type of waveform,<br />

whether or not it is periodic. Equation (2–4) is valid only for periodic waveforms.<br />

DC Value<br />

DEFINITION. The DC (direct “current”) value of a waveform w(t) is given by its time<br />

average, 8w(t)9.<br />

Thus,<br />

1<br />

W dc = lim<br />

T: q T L<br />

T/2<br />

-T/2<br />

w(t) dt<br />

(2–5)<br />

† See Eq. (2–130) for the definition of linearity.<br />

‡ Nonperiodic waveforms are called aperiodic waveforms by some authors.

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