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DISCRETE FOURIER TRANSFORM 1. Introduction The sampled discrete-time fourier transform (DTFT) of a finite length, discrete-time signal is known as the discrete Fourier transform (DFT). The DFT contains a finite number of samples equal to the number of samples N in the given signal. Computationally efficient algorithms for implementing the DFT go by the generic name of fast Fourier transforms (FFTs). This chapter describes the DFT and its properties, and its relationship to DTFT. 2. Definition of DFT and its Inverse Lest us consider a discrete time signal x (n) having a finite duration, say in the range 0 ≤ n ≤N -1. The DTFT of the signal is N-1 X ( ) = x (n)e -jwn (1) n-0 Let us sample X using a total of N equally spaced samples in the range : (0,2), so the sampling interval is 2 That is, we sample X() using the frequencies. N = k = 2 k , 0 ≤ k ≤N-1. N-1 Thus X (k) = x (n)e -jwn (2) n-0 N-1 X (k) = x (n)e - j2 kn (2) n-0 N The result is, by definition the DFT. That is , Equation (0.2) is known as N-point DFT analysis equation. Fig 0.1 shows the Fourier transform of a discrete time signal and its DFT samples.
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Page 1: vtu notes

DISCRETE FOURIER TRANSFORM

1. Introduction

The sampled discrete-time fourier transform (DTFT) of a finite length, discrete-time signal isknown as the discrete Fourier transform (DFT). The DFT contains a finite number of samplesequal to the number of samples N in the given signal. Computationally efficient algorithms forimplementing the DFT go by the generic name of fast Fourier transforms (FFTs). This chapterdescribes the DFT and its properties, and its relationship to DTFT.

2. Definition of DFT and its Inverse

Lest us consider a discrete time signal x (n) having a finite duration, say in the range 0 ≤ n ≤N-1.The DTFT of the signal is

N-1

X ( ) = x (n)e-jwn (1)

n-0

Let us sample X using a total of N equally spaced samples in the range : (0,2), so thesampling interval is 2 That is, we sample X() using the frequencies.

N= k = 2k , 0 ≤ k ≤N-1.

N-1

Thus X (k) = x (n)e-jwn (2)

n-0

N-1

X (k) = x (n)e- j2kn (2)

n-0N

The result is, by definition the DFT.

That is ,

Equation (0.2) is known as N-point DFT analysis equation. Fig 0.1 shows the Fourier transformof a discrete – time signal and its DFT samples.

Page 2: vtu notes

x(w)

0 2 w

Fig.1 Sampling of X(w) to get x(k)

While working with DFT, it is customary to introduce a complex quantityWN = e-j2 /N

Also, it is very common to represent the DFT operation

N=1

X(k) = DFT ( x(n)) = x(n) WNkn, 0≤n≤N-1

n=0

The complex quantity Wn is periodic with a period equal to N. That is,WN

a+N = e-j+2/N(a+N) = e-j2 /N n = WNa where a is any integer.

Figs. 0.2(a) and (b) shows the sequence for 0≤n≤N-1 in the z-plane for N being even andodd respectively.

6 55 7 4 6

4 0 0

3 1 3 1

2 2

(a) (b)

Fig.2 The Sequence for even N (b) The sequence for odd N.

The sequence WkN

N for 0 ≤ n ≤ N-1 lies on a circle of unit radius in the complex planeand the phases are equally spaced, beginning at zero.

The formula given in the lemma to follow is a useful tool in deriving and analyzingvarious DFT oriented results.

Page 3: vtu notes

2.1. Lemma

N-1

Wkn = N (k) = { N, k = 0(3)

n-0 N 0, k ≠ 0

Proof :N-1

an = 1 - aN : a≠ 1n-0 1 - a

We know thatApplying the above result to the left side of equation (3.3), we get

N-1

(WkN) n = 1- Wk

NN = 1- e-j2 k

NN

n= 01- Wk

NN 1- e-j2 k

NN : k ≠ 0

= 1 - 1

1- e- j2 kN

N

= 0, k ≠ 0

when k = 0, the left side of equation (3.3) becomes

N-1 N-1

WN0xn = 1 = N

n= 0 n =0

N-1 N, k = 0Hence, we may write WN

0xn = 0, k ≠ 0n=0

= N (k), 0≤ k≤ N-1

2.2 Inverse DFT

The DFT values (X(k), 0≤ k≤ N-1), uniquely define the sequence x(n) through the inverse DFTformula (IDFT) :

N-1

x (n) = IDFT (X(k) = 1 X(k) WN-kn , 0≤ k≤ N-1

N k=0

The above equation is known as the synthesis equation.

Page 4: vtu notes

N-1 N-1 N-1

Proof : 1 X(k) WN-kn = 1 [ x(m) WN

km] = WN-kn

N k=0 N k=0 m=0

N-1 N-1 N-1

= 1 x(m) [ WN-(n-m)k]

N k=0 m=0

It can be shown that

N-1

WN(n-m)k = N , n = m

0, n ≠ mHence,

N-1

1 x(m) N (n-m)

N

= 1 x Nx (m) ( sifting property)N m=n

= x(n)

2.3 Periodicity of X (k) and x (n)

The N-point DFT and N-point IDFT are implicit period N. Even though x (n) and X (k) aresequences of length – N each, they can be shown to be periodic with a period N because theexponentials WN

±kn in the defining equations of DFT and IDFT are periodic with a period N. Forthis reason, x (n) and X (k) are called implicit periodic sequences. We reiterate the fact that forfinite length sequences in DFT and IDFT analysis periodicity means implicit periodicity. Thiscan be proved as follows :

N-1

X (k) = x(n) WNkn

N-p=0

X (k+N) = x(n) WN(k+N)n

Since, WNNn = e-j2nNn = 1, we get

N-1

X (k+N) = x(n) WN-kn

n=0= X (k)

Page 5: vtu notes

N-1

Similarly, x (n) X (k) WN-kn

k=0

N-1

x (n+N) = 1 X(k) WN-k(n+N)

N k=0

N-1

= 1 X(k) WN-kn WN

-kn

N k=0

Since, WN-kn = e-j2/N kN = e-j2k = 1, we get

N-1

x(n+N) = 1 X(k) WN-kn

= x (n)

Since, DFT and its inverse are both periodic with period N, it is sufficient to compute theresults for one period (0 to N-1). We want to emphasize that both x (n) and X (k) have a startingindex of zero.

A very important implication of x (n), being periodic is, if we wish to find DFT of aperiodic signal, we extract one period of the periodic signal and then compute its DFT.

Example 1 Compute the 8 – point DFt of the sequence x (n) given below :

x (n) = (1,1,1,1,0,0,0,0)

SolutionThe complex basis functions, W for 0 n 7 lie on a circle of unit radius as shown in Fig. Ex.3

W86

W85 W87

W84 1.0 Re(z)

W83 W81

W82

Fig. 3 Sequence W80 for 0≤ n ≤ 8.

Page 6: vtu notes

Since N = 8 we get W = e –j2/8

Thus,W8

0 = 1

W81 = e -j/4 = 1 – j 1

2 2W8

2 = e -j/2 = – j

W83 = e -j3/4 = 1 – j 1

2 2W8

4 = -W80 = -1

By definition, the DFT of x (n) is

X ( k) = DFTI (x (n))

= W8kn

= 1+1 x W8k + W8

-2k + W83k .

= 1 + W8k + W8

2k + W83k k = 0, 1…7

X(0) = 1+1+1+1 = 4X(1) = 1+ W8

1 + W82 + W8

3 = 1 – j2.414

X(2) = 1+ W82 + W8

4+ W86 = 0

X(3) = 1+ W83 + W8

6+ W81 = 1 – j0.414

X(4) = 1 + W84 + W8

0+ W84 = 0

X(5) = 1+ W85 + W8

2 + W87 = 1+j0.414

X(6) = 1+ W86 + W8

4 + W82 = 0.

X(7) = 1+ W87 + W8

6 + W85 = 1+j2.414

Please note the periodic property : WNa = WN

a+N where a is any integer.

Example 2 : Compute the DFT of the sequence defined by x (n) = (-1) n fora. = N= 3b. N = 4,c. N odd,d. N even.

SolutionX (k) = DFT (x-n)

N-1

= (-1)n WNnk

n-0

Page 7: vtu notes

N-1

(-1)n [WNk] n

n=0= 1 – (1)N for WN

k ≠-1

1+ WNk

a. N = 3

X(k) = 2 = 2 0≤ k ≤ 21+ WN

k 1+ cos (2k/3) – j sin ((2k/3)

b. N = 4 X (k) = 0 for W4k ≠-1 or k≠ 2

With k = 2 we getN-1

X(2) (-1)n W42n

n=0= 1 - W4

2 + W44 - W4

6

= 1 – (-1) + (-1)2– (-1)2 = 4

Hence, X (k) = 48(k-2)

c. We know that

W42n – e-j2 / N k

If N = 2k, we get WNk= -1.

Since N is odd no k exists. This means to say that WNk -1 for all k from 0 to N-1.

Therefore,X(k) = 2 0≤ k ≤ N-1

1+ WNk

d. N even WNk = - 1, if k = N/2.

X ( k) = 0 for k ≠ N/2

With k = 2, we getN-1

And x (N/2) = [- WNk] n

n=0N-1

= [1] = Nn=0

Hence X (k) = N (k-N/2)

Page 8: vtu notes

Example 3. Compute the inverse DFT of the sequence,

X(k) = (2,1+j,0,1 –j)

Solution

x (n) = IDFT (X(k))N-1

1 x(n) WN-kn , 0 ≤ n ≤N -1

N n=0

Please note that :

WN-kn = [ WN

kn]*

Since, N = 4, we get

N-1

x (n) = 1 X(k) W4-kn , 0 ≤ n ≤3

4 n=0

= 1 [X(0) W4-0xn + X(1) W4

-n + X (2) W4-2n + X (3) W4

-3n]4

= 1 [2 + (1+j) W4-n +0 + (1-j) + X (3) W4

-3n]4

Hence, x (0) = 1 [2 + (1+j) +(1-j)] = 14

x (1) = 1 [2 + (1+j) W4-1 +(1-j) W4

-3] = 14

x (2) = 1 [2 + (1+j) W4-2 +(1-j) W4

-6] = 14

Because of periodicity, W4-6 = W4

-2

Hence, x (2) = 1 [2 + (1+j) (-1) + (1-j) (-1)] = 04

x (3) = 1 [2 + (1+j) W4-3 +(1-j) W4

-9] = 14

Because of periodicity, W4-9 = W4

-5 = W4-1

Page 9: vtu notes

Hence, x (3) = 1 [2 + (1+j) W4-3 +(1-j) W4

-1]4

= 1 [2 + (1+j) (-j) (-j) + (1-j) ] = 14

Hence, x(n) = (1,0,0,1)

3. Matrix Relation for Computing DFT

The defining relation for DFT of a finite length sequence x (n) is

N-1

X (k) = x(n) Wnkn , 0.1, …… N-1

n=0

Let us evaluate X (k) for different values of k in the range (0, N-1) as given below :X (0) = WN

0 x (0) + WN0 x (1) + …… + WN

0 x (N-1)

X (1) = WN0 x (0) + WN

1 x (1) + …… + WN(N-1) x (N-1)

X (2) = WN0 x (0) + WN

2 x (1) + …… + WN2(N-1) x (N-1)

X (N-1) = WN0 x (0) + WN

(N-1)x (1) + ….. =+ WN(N-1) (N-1) x (N-1)

Putting the N DFT equations in N unknowns in the matrix form, we getX = WNx

Here X and x are (N x 1) matrices, and Wn is an (N x N) square matrix called the DFT matrix.The full matrix form is described by

X(0) WN0 WN

0 WN0 WN

0 x(0)

X(1) WN0 WN

1 WN2 WN

(N-1) x(1)

X(2) = WN0 WN

2 WN4 WN

kn x(2)

: : : : : :X(N-1) WN

0 WNN-1 WN

2(N-1) WN(N-1)(N-1) x(N-1)

The elements WNkn of WN are called complex basis functions or twiddle factors.

Example : Compute the 4-point DFT of the sequence, x(n) = (1,2,1,0).

SolutionWith N = 4, W4 = e-j2 /4 = -j.We know that

Page 10: vtu notes

X = WN x

X(0) W40 W4

0 W40 W4

0 x(0)

X(1) W40 W4

1 W42 W4

3 x(1)

X(2) = W40 W4

2 W44 W4

6 x(2)

X(3) W40 W4

3 W46 W4

0 x(3)

Exploiting the periodic property WN0 = WN

n+N where a is any integer the above matrix relationbecomes.

X(0) W40 W4

0 W40 W4

0 x(0)

X(1) W40 W4

1 W42 W43 x(1)

X(2) = W40 W4

2 W40 W4

2 x(2)

X(3) W40 W4

3 W42 W4

1 x(3)

X(0) 1 1 1 1 1X(1) 1 -j -1 j 2X(2) = 1 -1 1 -1 1X(3) 1 j -1 -j 0

Hence,X(k) = (4, -j2, 0, j2)

4. Matrix Relation for Computing IDFT

We know that x = WN1X

Premultiplying both the sides of the above equation by we get

WN-1-X = WN

-1 WNx

WN-1X = x

Or x = WN-1X

In the above equation (.8) x = WN-1 is called IDFT matrix.

The defining equation for finding IDFT of a sequence X (k) is

Page 11: vtu notes

N-1

X (n) = 1 X(k) W , 0≤ n ≤ N-1N k=0

N-1

= 1 X (k) [WNkn ]*

N k=0

The first set of N IDFT equation in N unknowns may be expressed in the matrix form as

x = 1 W*NX

N

Where W*N denotes the complex conjugate of WN. Comparision of equation (3.8) and (3.9)leads us to conclude that

WN-1 = 1/N W*N

This very important result shows that W-1N requires only conjugation of Wn multiplied by 1/N.

an obvious computational advantage. The matrix relations (.7) and (.9) together define DFT as alinear transformation.

5. Using the DFT to Find the IDFT

We know thatN-1

x* (n) = 1 X(k) WN-kn , n= 0,1 …. N-1

N k=0

Taking complex conjugates on both the sides of the above equation, we get

N-1

x*(n) = 1 X(k) WN-kn *

N k=0

Page 12: vtu notes

N-1

x*(n) = 1 X*(k) WN-kn * (10)

N k =0

The right – hand side of equation (3.10) is recognized as the DFT of X* (k), so we can rewriteequation (3.10) as follows :

x*(n) = 1 DFT (X*(k))N

Taking complex conjugates on both the sides of equation (11), we get

x*(n) = 1 [DFT (X*(k))]N

The above results suggests the DFT algorithm itself can be used to find IDFT. In practice, this isindeed what is done.

6. Properties of DFTIn the following section, we shall discuss some of the important properties of the DFt. They arestrikingly similar to other frequency domain transforms, but must always be used in keeping withimplied periodicity for both DFT and IDFT in time and frequency domains.

6.1 Linearity

DFT (ax1(n) + bx2(n)j = aX1(k) + bX2(k), k = 0, N =1

If X1(k) and X2(k) are the DFTs of the sequence x1 (n) and x2 (n), respectively, both of lengths

N.

Proof :

N-1

We know that DFT [x(n)] = x(n) WNkn

n=0

Letting x (n) = ax1(n) + bx2(n) we getN-1

DFT = ax1(n) + bx2(n) = (ax1(n) +bx2 (n)] WNkn

n=0N-1

= a x1(n) WNkn + b x1(n) WN

kn

n=0

Page 13: vtu notes

= aX1 (k) + bX2(k), 0 ≤ k≤ N-1

Sometimes we represent the linearity property as given belowDFT

ax1 (n) + bx2(n) aX1 (k) + bX2(k)

Example : Find the 4- point DFT of the sequenceX(n) = cos ( n) + sin ( n)

4 4Use linearity property.

Solution

Given N = 4,WN = e j2 /n W = e j /2

We know that, W40 = 1

Hence, W40 = 1

W41 = e = -j

W43 = e = -1

x1 (n) = cos ( /4 n )Let

x2 (n) = sin ( /4 n )

andThen, the values of x (n) and x2 (n) for 0 <n <3 tabulated below :

N x1 (n) = cos ( /4 n ) x2 (n) = sin ( /4 n )

0 1 01 1 1

2 22 0 13 -1 1

2 2

X1 (k) = DFT (x1 (n))

3

x1 (n) W4kn, k = 0,1,2,3

n=0

X1 (k) = 1 + 1 W4k +0 – 1 W4

3k

Page 14: vtu notes

2 2Hence, X1 (0) = 1 + 1 – 1 = 1

2 2X1 (1) = 1 + 1 W4

1 – 1 W43 = 1 –j1.414

2 2X1 (2) = 1 + 1 W4

2 – 1 W46

2 2= 1 + 1 W4

2 – 1 W24 = 1

2 2X1 (3) = 1 + 1 W4

3 – 1 W49

2 2= 1 + 1 W4

3 – 1 W41

2 2Similarly, X2 (k) = DFT (x2 (n))

3

x2 (n) W4kn

n=0

X2 (k) = 1 W4k + W4

2k + 1 W43k

2 2Hence, X2 (0) = 1 + 1 + 1 = 2.414

2 2X2 (1) = 1 W4

1 + W42 + 1 W4

3 = -1

2 2X2 (2) = 1 W4

2 + W40 + 1 W4

9

2 2= 1 W4

3 + W46 + 1 W4

9 = -0.414

2 2

X2 (3) = 1 W43 + W4

6 + 1 W49

2 2= 1 W4

3 + W42 + 1 W4

1 = -1

2 2

Finally, applying the linearity property, we getX (k) = DFT ( x1(n) + x2(n))

= X1(k) + X2(k)= ( X1(0) + X2(0), X1(1) + X2(1). X1(2), X2(2), X1(3) + X2 (3) )= (3.414. – j1.414.0.586. j1.414)

k=0

Page 15: vtu notes

It may be noted that the arrow, explicitly represents the position index of k = 0 or n = 0 of agiven sequence. The absence of this arrow also implicitly means that the first element in asequence always has the index k = 0 or n = 0.

Example Compute DFT (x(n)) of the sequence given below using the linearity property.x (n) = cosh an, 0 ≤ n ≤ N-1

SolutionGiven x(n) = cosh an, 0 ≤ n ≤ N-1

Then the N point DFT of the sequence x (n) is

X (k) = DFT [x(n)] = DFT ( cosh an)

= DFT 1 ean + 1 e-an

2 2Applying linearity property, we get

X (k) = 1 DFT [e an ] + 1 DFT [e -an ], 0 ≤ n ≤ N-12 2

We know from Example 3.5, thatDFT (b N ) = b N -1 , 0 ≤ k ≤ N-1

b WNk -1

Hence, X (k) = 1 e a(N) - 1 + e a(N) - 12 e a(N) WN

k -1 e -a WNk - 1

= WN-kn ( e a(N-1) + e -a(N-1) - e -a + e –a ] - e –aN- e –aN +2

2[1- WNk (ea – ea ) + WN

k ]= 1 – cosh Na + WN

k [cosh ( N-1)a – cosh a] , 0 ≤ k ≤ N-1

1- 2 WNk cosha + WN

k

6.2 Circular time shift

If DFT [x(n)] = X (k).Then DFt [x(n-m))] = X(k), 0 ≤ n ≤ N-1

Proof :

N=1

x (n) = 1 [ X (k) WN-kn

N k=0

Page 16: vtu notes

N=1

x (n-m) = 1 [ X (k) WNk(n-m)

N k=0

Since, the time shift is circular, we can write the above equation asN=1

x (n-m) = 1 [ X (k) WNkm ] WN

-kn

N k=0 x (n-m)N = IDFt [ X(k) WN

km]

or DFT [x(n-m) N ] = WNkm X (k)

In terms of the transform pair, we can write the above equation is

DFT

x (n-m)N WNkm X (k)

Example Find the 4- point DFT of the sequence, x(n) = (1, -1, 1, -1) Also, using time shiftproperty, find the DFT of the sequence, y(n) = x (n-2)4.

Solution

Given N = 4We know that

W40= 1, W4

1= -j

W42 = -1, W4

3 = jHence, X (k) = DFT (x (n) )

3

= x(n) W4kn , 0 ≤ k≤ 3

n=0= 1 W4

0k x – 1 x W4k +1 x W4

2k - 1 x W43k

= 1- W41+W4

2k - W43k

X(0) = 1 -1 +1 -1 = 0X(1) = 1 - W4

1+ W42- W4

3 = 0

X(2) = 1 - W42 + W4

4 - W46

= 1- W42+ W4

0 - W42 = 4

X(3) = 1 - W43 + W4

6- W49

= 1- W43 + W4

2- W41= 0

Given y (n) = x(n-2) 4

Applying circular time shift property, we getY(k) = W4

2k X (k), k = 0,1,2,3

Y(0) = W40 X(0) = 0

Page 17: vtu notes

Y(1) = W42 X (1) = 0

Y(2) = W44 = W4

0 x(2) = 4

Y(3) = W46x (3) = W4

2 x (3) = 0Hence, Y(k) = (0,0,4,0)

k-0

Example Suppose x(n) is a sequence defined on 0 -7 only as ( 0,1,2,3,4,5,6,7),a. Illustrate x(n-2) isb. If DFT (x(n)) = X (k), what is the DFT (x (n-2)s)

Solutiona. GivenTo generate x (n-2) move the last 2 samples of x (n) to the beginning.That is, x (n-2) = (6,7,0,1,2,3,4,5)

s(n-2)g7

56 4

2 31

0 1 2 3 4 5 6 7 n

It should be noted that x (n-2) is implicity periodic with a period N = 8.b. Let y(n)=x(n-2) 8

Applying circular time shift property, we get

Y(k) = W32k X(k)

Example : Let X (k) donate a 6-point DFT of a length – 6 real sequence, x(n). The sequence isshown in Fig. Ex 3.17, without computing the IDFT, determine the length -6 sequence, y(n)

whose 6-point DFT is given by, Y (k) = W32k X(k)

1 2 3 x(n)0

4 5-1

Fig. Sequence x(n)

Page 18: vtu notes

SolutionWe may write

W32k = e-j2/3nx2k

= e-j2/3nx2k

Hence, W32k = W64k

It is given in the problem that

Y(k) = W3 j2k X(k)

Y(k) = W64k X(k)

We know that DFT (x(n=m) N = WNmk X(k)

IDFT WNmk X(k) = x(n-m) NHence, y(n) = x(n-4)6Since, x(n) = (1,-1,2,3,0,0)We get x(n-4) is by moving the last 4 samples of x(n) to the beginning

y(n) = x(n-4) 6= (2,3,0,0,1-1)

Circular frequency shift ( Multiplication by exponential in time-domain)If DFT (x(n)) = X (k), then DFT = X (k-1) N.

Proof :

N-1

X (k) = DFT (x (n)) = x(n) WNkn, 0 ≤ k ≤ N-1n=0

N-1

X(k-1) =x(n) WN(k-1)n

Since, the shift is frequency is circular, we may write the above equation as

N-1

X(k-1)8 = { x(n) WN-ln } WNkn

n=0

Hence, DFT {x(n) WN-ln } = X (k=1)N

Example Compute the 4-point DFT of the sequence x (n) = (1,0,1,0), Also, find y (n) if Y (k) =X (k-2) 4.

Page 19: vtu notes

SolutionGiven N = 4.

Also W40 = 1, W4l =-j, W42 =-1, W43 =j,

The DFT of the sequence, x (n) is3

X(k) = x(n) W4kn , 0 ≤ k≤ 3

= 1x W40k + 0+1 x W42k =0

= 1 +W42k

X(0) = 1+1= 2X(1) = 1+W24 = 0

X(2) = 1+W04 = 2

X(3) = 1+W24 = 0

X(0) = 1+1= 2X(k) = X(k-2))4

Given Y(k) = X(k-2) 4

We know that, DFT (WN-ln x (n)) = X(k-l)N

That is, y(n) = WN-ln x (n) DFT Y(k) = X(k-1)N

Hence, y(n) = W4-2n x (n)

y(0) = W4-0 x (0) = 1

y(1) = W4-2 x (1) = 0

y (2) = W4-4 x (2)

= W4-0 x (2) = 1x 1 =1

y(3) = W4-6 x (3) = W4-2 x (3) = 0

That is, y(n) = (1,0,1,0)n=0

Page 20: vtu notes

Circular convolutionUnlike DFT convolution in DFT in circular consider two sequence x(n) and y(n) the

circular convolution of x(n) and y(n) in given by

Let f (n) = x (n) x y(n)

N-1

x(n+N) = 1 x(n-m) Nh(m) 0 ≤ n ≤ N-1m=0N-1

= x(m) h(n-m) nn=0

Point to be noted here in that x(n) and y(n) should be of same length

Example :

Let x (n) = 1,1,1 y (n) = 1,-2,2Retain x (n) as it is and circularly fold y (n) i.e. y(n) = 1,2,-2.

N x(m) y(n-m)N f(n)

0 1,1,1 1,2,-2 1 x 1+1x2+1x-2 = 11 1,1,1 -2,1,2 1 x -2 + 1x1 + 1x2 = 12 1,1,1 2,-2,1 1 x 2, +1x-2 + 1x1 = 1

h (n) = 1,1,1

Page 21: vtu notes

SummaryN-1

1) x (k) = x(n) e-jwn

n=0N-1

= x(n) Wnkn

n=0

N-1

2) x (n) = 1 x(n) Wnkn 0≤ n≤ N-1

N k=0

3) Periodicity of Wnkn

W6

8

W5

8W

78

W4

8W

08

=W4

6W

N= W

N+N

-W7

8= W

38

W1

8= -W

58

W2

8

= W8

84) DFT { ax1(n) + bx2(n) } = ax1 (k) + bx2(k)

5) DFT {x(n-m)N} = WNmk x (k)

6) DFT {Wn-lnx(n) } = x(k-l)N

7) X (k) = Xy (N-k)

8) DFT {x(N-n)} = x(N-k)

9) DFT { xe (n) } = 1 DFT {x(n) + 1 DFT { x(-n)N)}

2= 1 x (k) + 1 x (-k) N

2 210) DFT { x1 (n) x2(n) } = 1 x 1(k) x2 (k)

N


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