Signals in Natural Domain
Chapter 2 : Simple Operations and properties of Sequences
 
Periodic Signals:
An important class of signals that we encounter frequently is the class of periodic signals. We say that a signal {x[n] is periodic with period N, where N is a positive integer, if the signal is unchanged by the time shift of N ie.,
{x[n]}  =  {x[n + N]}
or   x[n] = x[ n + N ]   for all n.
Since   {x[n]}   is same as {x[n+N]} , it is also periodic so we get
{x[n]} = {x[n+N]} = {x[n+N+N]}  =  {x[n+2N]}
Generalizing this we get {x[n]} = {x[n+kN]}, where k is a positive integer. From this we see that  {x[n]} is periodic with 2N, 3N,... The fundamental period N0 is the smallest positive value N for which the signal is periodic.
The signal illustrated below is periodic with fundamental period N0 = 4
                         

FIGURE

 

By change of variable we can write {x[n]} = {x[n+N]} as   {x[m-N]} = {x[m]} and then arguing as before, we see that
{x[n]} = {x[n+kN]},

for all integer values of k positive, negative or zero. By definition, period of a signal is always a positive integer N.
Except for a all zero signal all periodic signals have infinite energy. They may have finite power. Let {x[n]} be periodic with period N, then the power Px is given by
                 $\displaystyle P-x=\lim\limits_{M\rightarrow
\infty}\frac{1}{(2M+1)}\sum\limits_{n=-M}^{M}\vert x[n]\vert^2$
                        
                             
where k  is largest integer such that   kN -1 ≤ M. Since the signal is periodic, sum over one period will be same for all terms. We see that k is approximately equal to  M/N (it is integer part of this) and for large M we get 2M/N  terms and limit   2M/(2M +1)  as M goes to infinite is one we get
                                 $\displaystyle P_x=\frac{1}{N}\sum\limits_{n=0}^{N-1}\vert x[n]\vert^2$