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Hertz. In practice, this approximation is widely accepted since it accounts for
most of the signal energy.
τ
frequency
–
f 0
f 0
–
(
1 τ
)
f 0
+
(
1 τ
)
Figure 3.3. Amplitude spectrum for a single pulse, or a
train of non-coherent pulses.
Now consider the coherent gated CW waveform
given by
f 3
()
f 3
()
=
f 2
(
tnT
–
)
(3.23)
n
=
–
Clearly
is periodic, where
is the period (recall that
is the
f 3
()
T
f r
=
1
T
PRF). Using the complex exponential Fourier series we can rewrite
as
f 3
()
j nt
T
--------------
f 3
()
=
F n e
(3.24)
n
=
–
where the Fourier series coefficients
are given by
F n
A τ
T
n τπ
T
F n
=
------
Sinc
---------
(3.25)
It follows that the FT of
is
f 3
()
 
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