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 f d t 0
(
–
)
s r
st t 0
(
–
)
(3.110)
where
–
j 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 f d tu 0
(
+
–
)
s o
()
=
st
(
+
u t 0
–
) d
(3.114)
–
Finally, making the change of variable
yields
t '
=
tu
+
) e j 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 f d t '
st () s t '
s o
(
tf d
;
)
=
(
–
t
d
t '
(3.116)
–
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