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Leo Lam © 2010-2013
Signals and SystemsEE235
Leo Lam © 2010-2013
Fourier Transform:
2
• Fourier Formulas:• Inverse Fourier Transform:
• Fourier Transform:
Time domain toFrequency domain
Leo Lam © 2010-2013
Fourier Transform (delta function):
3
• Fourier Transform of
• Standard Fourier Transform pair notation
dtetF tj
)()(
( ) ( )f t t
1)()(
dttF
1)( t
Leo Lam © 2010-2013
Fourier Transform (rect function):
4
• Fourier Transform of
• Plot for T=1?
t-T/2 0 T/2
1
Define
-10 -8 -6 -4 -2 0 2 4 6 8 10-0.4
-0.2
0
0.2
0.4
0.6
0.8
1
Leo Lam © 2010-2013
Fourier Transform (rect function):
5
• Fourier Transform of
• Observation:– Wider pulse (in t) <-> taller narrower spectrum– Extreme case:
• <->
-10 -8 -6 -4 -2 0 2 4 6 8 10-0.4
-0.2
0
0.2
0.4
0.6
0.8
1
)2
()(T
sincTF
Peak=pulse width (example: width=1)
T
n2Zero-Crossings:
)(DC
Leo Lam © 2010-2013
Fourier Transform - Inverse relationship
6
• Inverse relationship between time/frequency
Leo Lam © 2010-2013
Fourier Transform - Inverse
7
• Inverse Fourier Transform (Synthesis)
• Example:
Leo Lam © 2010-2013
Fourier Transform - Inverse
8
• Inverse Fourier Transform (Synthesis)
• Example:
• Single frequency spike in w: exponential time signal with that frequency in t
A single spike in frequencyComplex exponential in time
Leo Lam © 2010-2013
Fourier Transform Properties
9
• A Fourier Transform “Pair”: f(t) F()• Re-usable!
Scaling
Additivity
Convolution
Time shift
time domain Fourier transform
Leo Lam © 2010-2013
How to do Fourier Transform
10
• Three ways (or use a combination) to do it:– Solve integral– Use FT Properties (“Spiky signals”)– Use Fourier Transform table (for known
signals)
Leo Lam © 2010-2013
FT Properties Example:
11
• Find FT for:
• We know the pair:
• So:
-8 0 8
G()
Leo Lam © 2010-2013
More Transform Pairs:
12
• More pairs:
time domain Fourier transform
21
aj 1
Leo Lam © 2010-2013
Periodic signals: Transform from Series
13
• Integral does not converge for periodic fns:
• We can get it from Fourier Series:• How? Find x(t) if• Using Inverse Fourier:
• So
)(2)( 0 X
tjtj edetx 0)(22
1)( 0
tje 0)(2 0
Leo Lam © 2010-2013
Periodic signals: Transform from Series
14
• We see this pair:
• More generally, if X(w) has equally spaced impulses:
• Then:
tje 0)(2 0
k
k kdX )(2)( 0
k
tjkk
tj eddeXtx 0)(2
1)(
Fourier Series!!!
Leo Lam © 2010-2013
Periodic signals: Transform from Series
15
• If we know Series, we know Transform
• Then:
• Example: • We know:
• We can write:
k
k kdX )(2)( 0
k
tjkkedtx 0)(
)8cos()( ttf 8,5.0,5.0 011 dd
)8()8()( F
Leo Lam © 2010-2013
Summary
• Fourier Transform Pairs• FT Properties
Leo Lam © 2010-2013
Duality of Fourier Transform
17
• Duality (very neat):
• Duality of the Fourier transform: If time domain signal f(t) has Fourier transform F(), then F(t) has Fourier transform 2 f(-)
• i.e. if:
• Then:
)(2
)(
0
0
0
0
tj
tj
e
ett
Changed sign
)(2)(
)()(
ftF
Ftf
Leo Lam © 2010-2013
Duality of Fourier Transform (Example)
18
• Using this pair:
• Find the FT of– Where T=5
2
TsincT
T
trect
)(5
5)( tF2
tsinctg
52
52)(
rectrectG
)(2)( fG
Leo Lam © 2010-2013
Duality of Fourier Transform (Example)
19
• Using this pair:
• Find the FT of
)(2)(
)(2)( )(
ueF
ueFa
a
jaatue at
10),(
jtatf
1)(
)(2)( fG