Leo Lam © 2010-2013 Signals and Systems EE235. Courtesy of Phillip Leo Lam © 2010-2013.
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Transcript of Leo Lam © 2010-2013 Signals and Systems EE235. Courtesy of Phillip Leo Lam © 2010-2013.
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Leo Lam © 2010-2013
Signals and Systems
EE235
![Page 2: Leo Lam © 2010-2013 Signals and Systems EE235. Courtesy of Phillip Leo Lam © 2010-2013.](https://reader038.fdocuments.us/reader038/viewer/2022103015/551a84f4550346e0158b4b8b/html5/thumbnails/2.jpg)
Leo Lam © 2010-2013
Courtesy of Phillip
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Leo Lam © 2010-2013
Today’s menu
• Fourier Series
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Leo Lam © 2010-2013
Fourier Series
4
• Fourier Series/Transform: Build signals out of complex exponentials
• Established “orthogonality”• x(t) to X(jw)• Oppenheim Ch. 3.1-3.5• Schaum’s Ch. 5
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Leo Lam © 2010-2013
Fourier Series: Orthogonality
5
• Vectors as a sum of orthogonal unit vectors• Signals as a sum of orthogonal unit signals
• How much of x and of y to add?
• x and y are orthonormal (orthogonal and normalized with unit of 1)
x
y a = 2x + y
of x
of ya
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Leo Lam © 2010-2013
Fourier Series: Orthogonality in signals
6
• Signals as a sum of orthogonal unit signals• For a signal f(t) from t1 to t2
• Orthonormal set of signals x1(t), x2(t), x3(t) … xN(t)
of
of
of
Does it equal f(t)?
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Leo Lam © 2010-2013
Fourier Series: Signal representation
7
• For a signal f(t) from t1 to t2
• Orthonormal set of signals x1(t), x2(t), x3(t) … xN(t)
• Let
• Error:
of
of
of
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Leo Lam © 2010-2013
Fourier Series: Signal representation
8
• For a signal f(t) from t1 to t2
• Error:
• Let {xn} be a complete orthonormal basis • Then:
• Summation series is an approximation• Depends on the completeness of basis
Does it equal f(t)?
of
of
of Kind of!
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Leo Lam © 2010-2013
Fourier Series: Parseval’s Theorem
9
• Compare to Pythagoras Theorem
• Parseval’s Theorem
• Generally:
c
a
b
Energy of vector Energy of
each oforthogonalbasis vectors
All xn are orthonormal vectors with energy = 1
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Leo Lam © 2010-2013
Fourier Series: Orthonormal basis
10
• xn(t) – orthonormal basis:– Trigonometric functions (sinusoids)– Exponentials– Wavelets, Walsh, Bessel, Legendre etc...
Fourier Series functions
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Leo Lam © 2010-2013
Trigonometric Fourier Series
11
• Set of sinusoids: fundamental frequency w0
Note a change in index
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Leo Lam © 2010-2013
Trigonometric Fourier Series
12
• Orthogonality check:
for m,n>0
))cos()(cos(2
1)cos()cos( yxyxyx
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Leo Lam © 2010-2013
Trigonometric Fourier Series
13
• Similarly:
Also true: prove it to yourself at home:
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Leo Lam © 2010-2013
Trigonometric Fourier Series
14
• Find coefficients:
The average value of f(t) over one period (DC offset!)
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Leo Lam © 2010-2013
Trigonometric Fourier Series
15
• Similarly for:
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Leo Lam © 2010-2013
Compact Trigonometric Fourier Series
16
• Compact Trigonometric:• Instead of having both cos and sin:• Recall:
Expand and equate to the LHS
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Leo Lam © 2010-2013
Compact Trigonometric to est
17
• In compact trig. form:
• Remember goal: Approx. f(t)Sum of est
• Re-writing:
• And finally:
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Leo Lam © 2010-2013
Compact Trigonometric to est
18
• Most common form Fourier Series• Orthonormal: ,• Coefficient relationship:
• dn is complex:
• Angle of dn:
• Angle of d-n:
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Leo Lam © 2010-2013
So for dn
19
• We want to write periodic signals as a series:
• And dn:
• Need T and w0 , the rest is mechanical
00 0( ) 2 /jn t
nn
x t d e T
T
tjnn dtetfT
d 0)(1
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Leo Lam © 2010-2013
Harmonic Series
20
• Building periodic signals with complex exp.
• Obvious case: sums of sines and cosines1. Find fundamental frequency2. Expand sinusoids into complex exponentials (“CE’s”)3. Write CEs in terms of n times the fundamental frequency4. Read off cn or dn
00 0( ) 2 /jn t
nn
x t d e T
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Leo Lam © 2010-2013
Harmonic Series
21
• Example:
• Expand:
0( ) 1 cos(5 .6) 5, 2 / 5x t t T
Fundamental freq.
0 0
(.6) (.6)0 0 0
( .6) ( .6)
0
1( ) 1 ( )
21 1
2 2
j j
j t j t
t j t j t
x t e e
e e e e e
0 1d 0.61 0.5 jd e
0.61 0.5 jd e