Fourier
Representation of Finite Duration sequence |
The Discrete
Fourier Transform (DFT) |
We now consider the
sequence such
that and.
Thus can
be take non-zero values only for.
Such sequences are known as finite length sequences,
and N is called the length of the sequence.
If a sequence has length M, we consider it
to be a length N sequence where.
In these cases last ( N - M ) sample values are zero.
To each finite length sequence of length N we can always
associate a periodic sequence defined
by |
 (6.16) |
Note that defined
by equation (6.16) will always be a periodic sequence
with period N, whether is
of finite length N or not. But when has
finite length N, we can recover the sequence from by
defining
|
 (6.17) |
This is because of has
finite length N , then there is no overlap
between terms and for
different values of. |
Recall that if
n = kN + r, where 
then n modulo N = r ,
i.e. we add or subtract multiple of N from n until
we get a number lying between 0 to N - 1.
We will use ((n))N to denote n modulo N.
Then for finite length sequences of length N equation
(6.16) can be written as |
 (6.18) |
We can extract from using
equation (6.17). Thus there is one-to- one correspondance
between finite length sequences of
length N , and periodic sequences of
period N. |
Given a finite length
sequence we
can associate a periodic sequence with
it.
This periodic sequence has discrete Fourier series
coefficients which
are also periodic with period N. From equations
(6.2) and (6.3) we see that we need values of for and
for 0 = k = N - 1.
Thus we define discrete Fourier transform of finite
length sequence as |
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where is
DFS coefficient of associated periodic sequence.
From we
can get by
the relation. |
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then from this we can
get using
synthesis equation (6.2) and finally using
equation (6.17). In equations (6.2) and (6.3) summation
interval is 0 to N - 1, we can write X [k ]
directly in terms of x[n], and x[n]
directly in terms of X[k] as |
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For convenience of
notation, we use the complex quantity |
 (6.19) |
with this notation,
DFT analysis and synthesis equations are written a
follows |
| Analysis equation: |
 (6.20) |
| Synthesis equation: |
 (6.21) |
If we use values of k and n outside
the interval 0 to N - 1 in equation (6.20) and (6.21),
then we will not get values zero, but we will get periodic
repetition of and respectively.
In defining DFT, we are concerned with values only
in interval 0 to N - 1. Since a sequence
of length M can also be considered a sequence
of length ,
we also specify the length of the sequence by saying
N-point-DFT, of sequence. |
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Sampling of
the Fourier transform: |
For sequence of
length N, we have two kinds of representations,
namely, discrete time Fourier transform and
discrete Fourier transform.
The DFT values can
be considered as samples of  |
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(as x[n] = 0 n < 0,
for n < 0, and n > N - 1) |
 (6.22) |
Thus is is
obtained by sampling at. |
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