Recall CTFS (renormalize a bit)
Define
Δω=2πT=
ω
0
Δ
ω
2
T
ω
0
.
d
n
=T
c
n
=∫−T2T2fte(−i)(Δωn)td
t
d
n
T
c
n
t
T
2
T
2
f
t
Δ
ω
n
t
(1)
ft=12π∑n∈z
d
n
ei(Δωn)tΔω
f
t
1
2
n
n
z
d
n
Δ
ω
n
t
Δ
ω
(2)
As
T→∞
T
, Equation 1 becomes
d
n
=∫−∞∞fte(−i)(Δωn)td
t
d
n
t
f
t
Δ
ω
n
t
, where
Δω→0
Δ
ω
0
so
Δωn
Δ
ω
n
can approximate any real number.
Let
(ω=Δωn)∈R
ω
Δ
ω
n
and
Fiω=
d
n
F
ω
d
n
.
Fiω=∫−∞∞fte−(iωt)d
t
F
ω
t
f
t
ω
t
(3)
Then Equation 2 becomes
ft=12π∑n∈Z
d
n
ei(Δωn)tΔω
f
t
1
2
n
n
d
n
Δ
ω
n
t
Δ
ω
where
∑n∈ZΔω
n
n
Δ
ω
is a Reimann integral,
d
n
d
n
is
Fiω
F
ω
, and
Δωn
Δ
ω
n
is ωω.
ft=12π∫−∞∞Fiωeiωtd
ω
f
t
1
2
ω
F
ω
ω
t
(4)
Recall FS
ft=∑n∈z
c
n
ei
ω
0
nt
f
t
n
n
z
c
n
ω
0
n
t
builds up periodic or finite length
signal from sum of harmonic sinusoids with
frequencies that are multiples of
ω
0
=2πT
ω
0
2
T
.
CTFT
ft=12π∫−∞∞Fiωeiωtd
ω
f
t
1
2
ω
F
ω
ω
t
builds up arbitrary signal from sum of sinusoids of
all frequencies
ω∈R
ω
R
.
Table 1: CTFT
| analysis |
synthesis |
|
Fiω=∫−∞∞fte−(iωt)d
t
F
ω
t
f
t
ω
t
|
ft=12π∫−∞∞Fiωeiωtd
ω
f
t
1
2
ω
F
ω
ω
t
|
Totally symmetrical, except for
12π
1
2
goes with
ⅆω
ⅆ
ω
.
Alternate normalizations:
-
1
2
2π
1
2
2
in both above equations.
-
Don't use
radsec
rad
sec
frequency
ω
ω
but rather
Hz
Hz
frequency
γ
γ
(substitute
ω=2πγ
ω
2
γ
in above).
Then all
12π
1
2
's go away.