EECE 340 Chapter 9, Fall 2011
American University of Beirut · Signals and Systems · 13 pages · Prof. Karim Kabalan
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Chapter 9
Sampling Theorem
Sampling
The Sampling Theorem
Signals bearing information are available either in continuous form
f(t)or in discrete form (digital form). Therefore, we would like to
determine the necessary conditions which allow us to change an
analog signal to a discrete signal without loss of information, and
how we recover the original signal by filtering, this link is known as
the "The sampling theorem".
?
Conditions
Filter
f t( )
f t( )
f nT
(
)
Definition
A real-valued band-limited (low-pass signals, the
bandwidth is limited) having no frequency
components above a frequency of W rad/s
[W=2πB; B is in Hz] is determined uniquely by its
values at uniform intervals that are spaced no
greater than (1/2B) seconds apart.
Physical Steps
Mathematical Steps
P t
T( )
t
τ / 2
−τ /2
T / 2
T / 2
f t( )
P t
T( )
2T
T
3T
t
P t
T( )
f t( )
f nT
f
S t
(
)
( )
=
×
Mathematical Details
� fs(t)=f(t).pT(t)
� PT(t) is a periodic function of period T. It
can be expressed in a Fourier series form.
t
jn
n
n
S
0
t
jn
n
n
T
0
0
P e
)t(
f
)t(
f
T
2
P e
)t(
P
ω
∞
+
−∞
=
ω
∞
+
−∞
=
∑
=
π
ω =
= ∑
The Fourier Transform of fs(t)
t
jn
n
n
S
0
t
jn
n
n
T
0
0
P e
)t(
f
)t(
f
T
2
P e
)t(
P
ω
∞
+
−∞
=
ω
∞
+
−∞
=
∑
=
π
ω =
∑
=
)
n
P F(
( )
F
e)t(
f
P
( )
F
dt
e
P e
)t(
f
dt
e)t(
f
( )
F
0
n
n
S
t)
n
(j
n
S
t
j
n
t
jn
n
j t
S
S
0
0
ω − ω
= ∑
ω
∫
= ∑
ω
∑
= ∫
= ∫
ω
∞
−∞
=
− ω− ω
∞
∞
−
∞
∞
−
− ω
∞
−∞
=
ω
∞
∞
−
− ω
∞
−∞
Case 1: T<1/2B
2W
2W
1
1
2(2 B)
1
1
2B
1
2
2B
1
2 T; T
T
2
0
0
0
0
0
0
⇒ ω >
⇒ ω <
π
⇒ ω <
<
ω
π
⇒
<
ω =
π
π ⇒
=
ω
F( )
ω
ω
W
−W
1
FS( )
ω
ω
W
−W
ω 0
−ω0
P0
P1
P−1
P2
2
ω0
−2 0ω
P−2
2W
2W
2W
2W
2W
Case 1: T<1/2B
� Accordingly, the 2-signals would not
interfere with each other. The original
signal f(t) can be recovered from its
sampled version by the use of an LPF of
bandwidth W rad/s.
� Notation: (1/2B) is called the Nyquist
interval , and 1/T is called the Nyquist
rate
Under sampling
Case 2: T>1/2B
� In this case,
Accordingly, f(t) can not be recovered from its
sampled version
ω0 < 2W
General notes
Aliasing: What if the signal f(t) is not
band-limited