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Module by: Richard Baraniuk. E-mail the author

Fiω=fte(iωt)d t F ω t f t ω t
ft=12πFiωeiωtd ω f t 1 2 ω F ω ω t
Both formulas are symmetrical except for the ±± sign and 12π 1 2 . Useful! Say ft Fiω f t F ω through CTFT, and Giω=fiω G ω f ω , that is: the same form as some time-domain signal f f . Then what is gt g t ?
gt=12πGiωeiωtd ω =12πfiωeiωtd ω g t 1 2 ω G ω ω t 1 2 ω f ω ω t
Let τ=ω τ ω , and i in fiω f ω doesn't matter, then:
gt=12πfτeiτtd τ =fτe(iτ(t))d τ =12πF(it) g t 1 2 τ f τ τ t τ f τ τ t 1 2 F t
In other words: gt g t takes the form of FT F F (reversed and scaled, Figure 1).

Example 1

Figure 1
Figure 1 (f1.png)

Example 2

CTFT of t :gt=1 t g t 1 (Figure 2).

Figure 2
Figure 2 (f2.png)

Direct approach:

Giω=1e(iωt)d t G ω t 1 ω t

Duality approach:

We know Figure 3.

Figure 3: ft=δt f t δ t and ω :Fiω=1 ω F ω 1 .
Figure 3 (f3.png)
So by duality we get Figure 4.
Figure 4
Figure 4 (f4.png)

Exercise 1: FT of a complex sinusoid

ft=ei ω 0 t f t ω 0 t

Exercise 2: FT of cosine

Figure 5
Figure 5 (f5.png)

Exercise 3: FT of sine

Figure 6
Figure 6 (f6.png)

Exercise 4: FT of a sinc

Figure 7
Figure 7 (f7.png)

Exercise 5: FT of unit step

Figure 8
Figure 8 (f8.png)

Uiω=πδω+1iω U ω δ ω 1 ω .

Figure 9
Figure 9 (f9.png)

See Lathi pp. 250-1 for derivation.

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