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B. P. Lathi, Zhi Ding - Modern Digital and Analog Communication Systems-Oxford University Press (2009)

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6.1 Sampling Theorem 263

Figure 6.9

(al Non-bandlimited

signal

spectrum and its

sampled

spectrum G(f) .

(bl Equivalent

low-pass signal

spectrum G a (f)

constructed from

uniform samples

of g(t) at

sampling

rate 2B.

(a)

Aliasing

B

2B

Aliasing

Equivalent low-pass signal G a (f)

(b)

-B 0

B

This theoretical rate of communication assumes a noise-free channel. In practice, channel

noise is unavoidable, and consequently, this rate will cause some detection errors. In

Chapter 14, we shall present the Shannon capacity which determines the theoretical error-free

communication rate in the presence of noise.

6. 1 .4 Nonideal Practical Sampling Analysis

Thus far, we have mainly focused on ideal uniform sampling that can use an ideal impulse

sampling pulse train to precisely extract the signal value g(kT s ) at the precise instant of t =

kT s . In practice, no physical device can carry out such a task. Consequently, we need to

consider the more practical implementation of sampling. This analysis is important to the

better understanding of errors that typically occur during practical AID conversion and their

effects on signal reconstruction.

Practical samplers take each signal sample over a short time interval T p

around t = kT s .

In other words, every T s seconds, the sampling device takes a short snapshot of duration T p

from the signal g(t) being sampled. This is just like taking a sequence of still photographs

of a sprinter during an 100-meter Olympic race. Much like a regular camera that generates a

still picture by averaging the picture scene over the window T p

, the practical sampler would

generate a sample value at t = kT s by averaging the values of signal g(t) over the window T p

,

that is,

g1 (kT s ) = -

1 T p/2

1 g(kT s + t) dt

T p -T p/2

(6.1 9a)

Depending on the actual device, this averaging may be weighted by a device-dependent

averaging function q(t) such that

g1 (kT s ) = -

1 T p/2

1 q(t)g (kT s + t) dt

T p -T p/2

(6.19b)

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