Properties of the discrete-time Fourier transform Assignment Help

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Properties of the discrete-time Fourier transform (DTFT)

For DTFT Oppenheim & Schafer use symbol X (e jw ) while Proakis uses X(ω).

(1) Periodicity X(ω) is periodic with period 2π, i.e., X(ω+2π) = X(ω) for all ω. As e jn is periodic in ω with period 2π, it follows that X(ω) is periodic with the same period. Replacing ω with (ω+2π) gives

2025_Properties of the discrete-time Fourier transform.png

As a result, whereas in the continuous time case W varies from -∞  to ∞, in the discrete-time case we need to only consider values of ω over the range 0 to 2π (or, -π to π, or 2π-long interval).

(2) Linearity The discrete Fourier-transform is linear operation. If F{x1(n)} = X1(ω) and F{x2(n)} = X2(ω), then F{a1 x1(n) + a2 x2(n)} = a1 X1(ω)+ a2 X2(ω) for any constants a1 and a2.

(3) Time shifting Time shift results in the phase shift. If F{x(n)} = X(ω), then F{x(n-k)} = ejwk X(ω).

Proof We have

604_Properties of the discrete-time Fourier transform1.png

On the right hand side set n-k = m, such that n = m+k and limits n = - ∞ to ∞ change to m = - ∞ to + ∞ . Then

392_Properties of the discrete-time Fourier transform2.png

(4) Frequency shifting Multiplication in time domain by complex exponential results in the frequency shifting. Given F{x(n)} = X(ω), then F {e j w0 n x(n)} = X(ω-ω0).

Proof We have

2144_Properties of the discrete-time Fourier transform3.png

On the other hand, using the synthesis equation,

1210_Properties of the discrete-time Fourier transform4.png

Set ω-ω0 = λ such that ω = λ+ω0 and the limits ω = 0 to 2π change to λ = -ω0 to (-ω0+2π), which amounts to any interval of length 2π. Also = . Then

1806_Properties of the discrete-time Fourier transform5.png

(5) Time reversal corresponds to the frequency reversal. Given  F{x(n)} = X(ω), then F{x(-n)} =X(-ω).

Proof We have

1286_Properties of the discrete-time Fourier transform6.png

On right hand side set m = -n such that the limits n = -∞ to ∞ change to m = ∞ to - ∞ , and

856_Properties of the discrete-time Fourier transform7.png

As this is a summation the limits can be written in the reverse order, and we have

1835_Properties of the discrete-time Fourier transform8.png

(6) Differentiation in frequency 458_Properties of the discrete-time Fourier transform9.png

1941_1Properties of the discrete-time Fourier.png

we differentiate both the sides w.r.t. ω to get

1720_1Properties of the discrete-time Fourier1.png

(7) Convolution If y(n) represents convolution of the 2 discrete-time signals x(n) and h(n), i.e., y(n) = x(n)*h(n), then

Y (e jw ) = F{x(n)*h(n)} = X (e jw ) . H (e jw )

By the definition of Fourier transform

1238_1Properties of the discrete-time Fourier2.png

By interchanging the order of summation

1649_1Properties of the discrete-time Fourier3.png

 

The inner sum (I.S.) is taken care of, thus: Let (n-k) = λ. Then as n goes from - ∞ to ∞ , λ goes from - ∞ to ∞ as well. Further n = λ+k. Thus the inner sum becomes

2097_1Properties of the discrete-time Fourier4.png

 

 

The function H (e jw ) can be referred as frequency response of the system.

(8) Multiplication of 2 sequences Let y(n) be the product of the 2 sequences x1(n) and x2(nwith transforms X1 () and X 2(ejw ) , respectively. Then

 

641_1Properties of the discrete-time Fourier5.png

This is known as periodic convolution since X1 (e) andX 2 (e) are both periodic functions.

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