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Bab 7 Sampling
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Bab 7 Sampling
Analisis dan Perancangan Sistem - Sampling...
Author:
Andy Primawan
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∗
T
x(t)
p( p(t) ∗
T p( p(t) ωs = 2π/T 2 π/T
p(t)
x(t)
P ( jω)
2π
x p (t)
×
T
x(t) −3ωs −2ωs −ωs
T
2ωs
3ωs
ω
X p ( jω)
t
0
ωs
0
p(t)
1
T
t
0 x(0)
ωs
−ωs −ωM 0 ωM
−2ωs
ω
2ωs
(ωs − ωM )
x p (t)
X p ( jω) t
−T 0 T
1
T
x p (t) = x(t) p(t),
−ωs
−2ωs
ωs
0
ω
2ωs
(ωs − ωM ) X p ( jω)
+∞
p(t) =
δ (t − nT ).
ω X ( jω )
1/T
n=−∞
ωM < (ωs −ωM ) X ( jω ) ωs < 2ωM x(t)
x(t) x(t)δ (t − t0 ) = x(t0 )δ (t − t0 ) x p (t) x(t)
x p (t) x(t)
T
x p (t)
+∞
x p (t) =
x(t)
x(nT )δ (t − nT ),
ωs > 2ωM
x p (t)
x p (t)
n=−∞
xr (t) X r ( jω) = X ( jω)
1 X p ( jω) = 2π
+∞
x(t)
X ( jθ)P ( j(ω − θ))dθ.
xr (t)
−∞
2π P ( jω) = T
+∞
δ (ω − kω s ).
k=−∞
X ( jω ) ∗ δ (ω − ω0 ) = X ( j(ω − ω0 )) X p ( jω) =
1 T
+∞
X ( j(ω − kω s )).
x(t)
k=−∞
X ( jω)
x(t)
1
x(t) x p (t)
−ωM ωM
ω
x p (t) ho (t)
x0 (t)
x(t) +∞
xr (t) =
t
0 x(0)
x(nT )
n=−∞
ωc T sin(ωc (t − nT )) . π ωc (t − nT )
x p (t)
t
−T 0 T
x(t)
h0 (t) 1 T
t
0
t
x(0)
x p (t)
x0 (t)
t
0 x(t) hr (t)
−T
x0 (t)
0
t
T
xr (t)
x0 (t)
H r ( jω) r(t) = x(t). r (t) = x(t) h0 (t) hr (t)
t
0
x(t) = cos 200πt + 3 cos 400πt 800
x p (t) xr (t) T =
x(nT ) = cos
t
0
200πn 400πn + 3 cos 800 800
x(nT ) = cos
x0 (t)
+∞
x p (t) =
cos
n=−∞
1 800
πn πn + 3 cos 4 2
πn πn n + 3 cos δ t − 4 2 800
xr (t) = x(nT )|n=
x(t)
xr (t) = cos
h(t) =
ωc T sin(ωc t) , πωc t
t T
800πt 800πt + 3 cos 4 2
xr (t) = cos 200πt + 3cos400πt
x(t) X ( jω ) = 0
|ω| > ωM
x(t) x(nT )
x(nT ) = cos
2πn 4πn + 3 cos 3 3
x(nT ) = cos
2πn 1 + 3cos 1 πn 3 3
n = 0, ±1, ±2,... x(nT ) = cos ωs > 2ωM
ωs =
2πn 2 x(nT ) = cos + 3 cos (2 − )πn 3 3
2πn 2 + 3 cos 2πn − πn 3 3
n
2π . T
2πn 2 x(nT ) = cos + 3 cos − πn 3 3
x(nT ) x(t) T
x(nT ) = 4 cos ωM
ωs − ωM x(t) 2ωM
+∞
x p (t) =
= cos
2πn 3
4cos
n=−∞
2ωM
2πn 3
δ t −
xr (t) = x(nT )|n= xr (t) = 4cos
2πn 2πn + 3 cos 3 3
n 300
t T
2πn.300 3
xr (t) = 4 cos 200πt 100
ωs < 2ωM x(t)
X ( jω )
X p ( jω)
200
x p (t)
100 300
xr (t)
400
x(t) ω0 (ωs −ω0 )
ωs /2 < ω0 < ω s ωs ωs = ω0
ω0 (ωs − ω0 ) x(t) = sin 200πt
(ω0 = 0)
200
x p (t) xr (t) T =
x(t) = cos 200πt + 3 cos 400πt 300
x(nT ) = sin x p (t) xr (t)
T =
1 300
200πn 400πn + 3 cos x(nT ) = cos 300 300
1 200 200πn 200
x(nT ) = sin πn n 0 x(nT ) = 0
x p (t) = 0 xr (t) = 0 100 200
Y c ( jω) = X c ( jω)H d (ejωt ).
200 H c ( jω) H d (ej Ω) H c ( jω) =
xc (t)
H d ej Ω
xc (t) xc (nT ) xc (nT )
H d (ejωT ), 0,
|ω| < ωs /2 |ω| > ωs /2
yc (t)
xd [n] H c ( jω) = jω . xd [n] = xc (nT ) xc (t)
xd [n]
ωc H c ( jω) =
yc (t)
jω, |ω| < ωc . 0, |ω| > ωc
ωs = 2ωc
yd [n] yd [n] = yc (nT )
jΩ
H d (e ) = j
Ω , T
|Ω| < π
|H c ( jω)| ωc
ωc
−ωc
ω
H c ( jω)
−ωc
π 2
π
−2
ωc
ω
|H c ( jω)|
jΩ
|H d (e )| ωc
1
π
−π
−2π
2π
ω
ω
ωc
−ωc H c ( jω)
∆ jΩ d (e )
H
ωc
−ωc
ω
π 2
−π
−2π
π
π
−2
2π
ω
|H d (ej Ω )| 1 π
−π
ω
H d (ej Ω )
π∆ T
yc = xc (t − ∆) −π
xc (t) ∆ Y c ( jω) = e−jω ∆ X c ( jω).
H c ( jω) =
e−jω ∆ , 0,
|ω| < ωc
.
ωc H c ( jω) ωc
ωs
ωs = 2ωc H d (ej Ω ) = e−j Ω∆/T , ∆
xd [n]
|Ω| < π , yd [n]
T
yd [n] = xd n −
∆ . T
∆
T
xc (t) yc (t) yd [n] yd [n] ∆
T
xd [n] H d (ej Ω ) xd [n]
= 1/2
− πT ∆
π
ω
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