Graphics Programs Reference
In-Depth Information
Matched Filter Response to LFM Waveforms
171
2
v
c
f
d
=
------
f
0
(3.108)
and since
, we get
γ
1
=
2
vc
⁄
f
d
=
(
γ
1
)
f
0
(3.109)
Using the approximation
and Eq. (3.109), Eq. (3.107) is rewritten as
γ
≈
1
()
e
j
2π
f
d
t
0
(
)
s
r
≈
st t
0
(
)
(3.110)
where
j
2π
f
0
t
st t
0
(
)
=
e
s
1
(
t
)
(3.111)
0
is given in Eq. (3.101). The matched filter response is given by the con-
volution integral
s
1
()
∞
∫
s
o
()
=
h
()
s
r
(
tu
)
du
(3.112)
∞
s
∗
For a non-causal matched filter the impulse response
h
()
is equal to
()
t
; it
follows that
∞
∫
s
∗
s
o
()
=
(
s
r
u
(
tu
)
d
(3.113)
∞
Substituting Eq. (3.111) into Eq. (3.113), and performing some algebraic
manipulations, we get
∞
∫
s
∗
()
e
j
2π
f
d
tu
0
(
+
)
s
o
()
=
st
(
+
u t
0
)
d
(3.114)
∞
Finally, making the change of variable
yields
t
'
=
tu
+
∞
∫
)
e
j
2π
f
d
t
'
(
t
0
)
s
∗
t
'
s
o
()
=
(
t
)
st
'
(
t
0
d
t
'
(3.115)
∞
It is customary to set
. It follows that
t
0
=
0
∞
∫
)
e
j
2π
f
d
t
'
st
()
s
∗
t
'
s
o
(
tf
d
;
)
=
(
t
d
t
'
(3.116)
∞
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