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Leo Lam © 2010-2012 Signals and Systems EE235. Leo Lam © 2010-2012 Today’s menu Happy May! Chocolates! Fourier Series Vote!

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Presentation on theme: "Leo Lam © 2010-2012 Signals and Systems EE235. Leo Lam © 2010-2012 Today’s menu Happy May! Chocolates! Fourier Series Vote!"— Presentation transcript:

1 Leo Lam © 2010-2012 Signals and Systems EE235

2 Leo Lam © 2010-2012 Today’s menu Happy May! Chocolates! Fourier Series Vote!

3 Fourier Series Leo Lam © 2010-2012 3 Fourier Series/Transform: Build signals out of complex exponentials Established “orthogonality” x(t) to X(j  ) Oppenheim Ch. 3.1-3.5 Schaum’s Ch. 5

4 Fourier Series: Orthogonality Leo Lam © 2010-2012 4 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 y a

5 Fourier Series: Orthogonality in signals Leo Lam © 2010-2012 5 Signals as a sum of orthogonal unit signals For a signal f(t) from t 1 to t 2 Orthonormal set of signals x 1 (t), x 2 (t), x 3 (t) … x N (t) of Does it equal f(t)?

6 Fourier Series: Signal representation Leo Lam © 2010-2012 6 For a signal f(t) from t 1 to t 2 Orthonormal set of signals x 1 (t), x 2 (t), x 3 (t) … x N (t) Let Error: of

7 Fourier Series: Signal representation Leo Lam © 2010-2012 7 For a signal f(t) from t 1 to t 2 Error: Let {x n } be a complete orthonormal basis Then: Summation series is an approximation Depends on the completeness of basis Does it equal f(t)? of Kind of!

8 Fourier Series: Parseval’s Theorem Leo Lam © 2010-2012 8 Compare to Pythagoras Theorem Parseval’s Theorem Generally: c a b Energy of vector Energy of each of orthogonal basis vectors All x n are orthonormal vectors with energy = 1

9 Fourier Series: Orthonormal basis Leo Lam © 2010-2012 9 x n (t) – orthonormal basis: –Trigonometric functions (sinusoids) –Exponentials –Wavelets, Walsh, Bessel, Legendre etc... Fourier Series functions

10 Trigonometric Fourier Series Leo Lam © 2010-2012 10 Set of sinusoids: fundamental frequency  0 Note a change in index

11 Trigonometric Fourier Series Leo Lam © 2010-2012 11 Orthogonality check: for m,n>0

12 Trigonometric Fourier Series Leo Lam © 2010-2012 12 Similarly: Also true: prove it to yourself at home:

13 Trigonometric Fourier Series Leo Lam © 2010-2012 13 Find coefficients: The average value of f(t) over one period (DC offset!)

14 Trigonometric Fourier Series Leo Lam © 2010-2012 14 Similarly for:

15 Compact Trigonometric Fourier Series Leo Lam © 2010-2012 15 Compact Trigonometric: Instead of having both cos and sin: Recall: Expand and equate to the LHS

16 Compact Trigonometric to e st Leo Lam © 2010-2012 16 In compact trig. form: Remember goal: Approx. f(t)  Sum of e st Re-writing: And finally:

17 Compact Trigonometric to e st Leo Lam © 2010-2012 17 Most common form Fourier Series Orthonormal:, Coefficient relationship: d n is complex: Angle of d n : Angle of d -n :

18 So for d n Leo Lam © 2010-2012 18 We want to write periodic signals as a series: And d n : Need T and  0, the rest is mechanical

19 Harmonic Series Leo Lam © 2010-2012 19 Building periodic signals with complex exp. Obvious case: sums of sines and cosines 1.Find fundamental frequency 2.Expand sinusoids into complex exponentials (“CE’s”) 3.Write CEs in terms of n times the fundamental frequency 4.Read off c n or d n

20 Harmonic Series Leo Lam © 2010-2012 20 Example: Expand: Fundamental freq.

21 Harmonic Series Leo Lam © 2010-2012 21 Example: Fundamental frequency: –   =GCF(1,2,5)=1 or Re-writing: d n = 0 for all other n

22 Harmonic Series Leo Lam © 2010-2012 22 Example (your turn): Write it in an exponential series: d 0 =-5, d 2 =d -2 =1, d 3 =1/2j, d -3 =-1/2j, d 4 =1

23 Leo Lam © 2010-2012 Summary Fourier series Periodic signals into sum of exp.


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