For example, the sinusoidal signal where for all t Î Time
is a periodic signal with period 2p /w 0. A finite signal in time is a signal whose domain is a subset [a,b] Ì Time, for some finite a and b. For example, the signal g where for all t Î [0, 2p /w 0] Ì Time,
is a finite signal with duration 2p /w 0.
A finite signal with duration p can be used to define a periodic signal with period p. All that is needed is to periodically repeat the finite signal. Formally, given a finite signal g: [a,b] ® Reals, we can define a signal g': Reals ® Reals with an augmented domain by
In other words, g'(t) is simply g(t) inside its domain, and zero elsewhere. Then with the examples above,
where p = b - a. That is, the periodic signal is just a sum of all versions of g(t) that have been shifted in time by multiples of p. Thus, a periodic signal can be defined in terms of a finite signal, which represents one period, and a finite signal can be defined in terms of a periodic signal (by taking one period).
We will see that any periodic signal, and hence any finite signal, can be described as a sum of sinusoidal signals. This result, known as the Fourier series, is one of the fundamental tools in electrical engineering.