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Uniform Sampling of a Continuous-Time Bandlimited Signal

Module by: Phil Schniter

Summary: Covers methods involved in uniform sampling of a continuous-time bandlimited signal.

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Uniform Sampling

Say that xn xn is sampled from x c t x c t with uniform sampling interval TT:

n,n:xn= x c nT n n xn x c n T (1)

Let us define the continuous-time "impulse train"

pt=n=-δtnT p t n δ t nT (2)
where δt δ t denotes the Dirac delta function, defined by the properties:

unit area

-δtdt=1 t δ t 1 (3)

sifting property

-ftδtτdt=fτ t ft δ t τ fτ (4)

Using Fourier series, it can be shown that

pt=1Tk=-2πTkt p t 1 T k 2 T k t (5)

Figure 1: Signals used in sampling theorem.
Figure 1 (uni_sam.png)

Multiplying x c t x c t by the impulse train yields the "continuous-time sampled signal" x s t x s t which will help us to derive the sampling theorem. (See Figure 1)

x s t= x c tn=-δtnT= x c t1Tk=-2πTkt x s t x c t n δ t nT x c t 1 T k 2 T k t (6)

Taking the CTFT of xs t xs t,

Xs Ω=- xc t1Tk=-2πTkt-Ωtdt=1Tk=-- xc t-Ω2πTktdt Xs Ω t xc t 1 T k 2 T k t Ω t 1 T k t xc t Ω 2 T k t (7)
Xs Ω=1Tk=- Xc Ω2πTk Xs Ω 1 T k Xc Ω 2 T k (8)

Notice that Xs Ω Xs Ω is a summation of scaled and shifted copies of Xc Ω Xc Ω . When Xc Ω Xc Ω is bandlimited to πTrads T rad s the spectral copies do not overlap, and we say there is no "aliasing." Aliasing may result when Xc Ω Xc Ω is not bandlimited to πT T . (See Figure 2 and Figure 3) The frequency πTrads T rad s , i.e., 12THz 1 2 T Hz , is often called the Nyquist frequency.

Figure 2: Example of aliasing in Xs Ω Xs Ω
Figure 2 (aliasing.png)
Figure 3: Example of no aliasing in Xs Ω Xs Ω
Figure 3 (noaliasing.png)

We now investigate the relationship between the CTFT and the DTFT:

Xω=n=-xn-ωn=n=- xc nT-ωn=n=-- xc tδtnTdt-ωn=n=-- xc tδtnT-ωndt X ω n x n ω n n xc n T ω n n t xc t δ t n T ω n n t xc t δ t n T ω n (9)
where xc tδtnT-ωn xc t δ t n T ω n is nonzero ⇔ n=tT n t T
Xω=n=-- xc tδtnT-ωtTdt=- xc tn=--ωTtdt X ω n t xc t δ t n T ω t T t xc t n δ t n T ω T t (10)
where xc tn=-δtnT= xs t xc t n δ t n T xs t
Xω= X s ωT X ω X s ω T (11)
Plugging Equation 8 into Equation 11 yields:
Xω=1Tk=- Xc ω2πkT X ω 1 T k Xc ω 2 k T (12)

Notice that the DTFT of the sampled signal xn x n is a summation of scaled, stretched, and shifted copies of the CTFT of the continuous signal xc t xc t . As implied by Equation 11, the DTFT may show evidence of aliasing when xc t xc t is not bandlimited to the Nyquist frequency. (See Figure 4 and Figure 5)

Figure 4: Example of aliasing in Xω X ω .
Figure 4 (aliasing_scaling.png)
Figure 5: Example of no aliasing in Xω X ω .
Figure 5 (noaliasing_scaling.png)

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