EECE 301 Note Set 13 FS Details

EECE 301 Note Set 13 FS Details - 1/21 EECE 301 Signals&...

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Unformatted text preview: 1/21 EECE 301 Signals & Systems Prof. Mark Fowler Note Set #13 • C-T Signals: Fourier Series (for Periodic Signals) • Reading Assignment: Section 3.2 & 3.3 of Kamen and Heck 2/21 Ch. 1 Intro C-T Signal Model Functions on Real Line D-T Signal Model Functions on Integers System Properties LTI Causal Etc Ch. 2 Diff Eqs C-T System Model Differential Equations D-T Signal Model Difference Equations Zero-State Response Zero-Input Response Characteristic Eq. Ch. 2 Convolution C-T System Model Convolution Integral D-T System Model Convolution Sum Ch. 3: CT Fourier Signal Models Fourier Series Periodic Signals Fourier Transform (CTFT) Non-Periodic Signals New System Model New Signal Models Ch. 5: CT Fourier System Models Frequency Response Based on Fourier Transform New System Model Ch. 4: DT Fourier Signal Models DTFT (for “Hand” Analysis) DFT & FFT (for Computer Analysis) New Signal Model Powerful Analysis Tool Ch. 6 & 8: Laplace Models for CT Signals & Systems Transfer Function New System Model Ch. 7: Z Trans. Models for DT Signals & Systems Transfer Function New System Model Ch. 5: DT Fourier System Models Freq. Response for DT Based on DTFT New System Model Course Flow Diagram The arrows here show conceptual flow between ideas. Note the parallel structure between the pink blocks (C-T Freq. Analysis) and the blue blocks (D-T Freq. Analysis). 3/21 3.2 & 3.3 Fourier Series In the last set of notes we looked at building signals using: ∑ − = = N N k t jk k e c t x ) ( ω N = finite integer We saw that these build periodic signals. Q: Can we get any periodic signal this way? A: No! There are some periodic signals that need an infinite number of terms: ∑ = + + = N k k k t k A A t x 1 ) cos( ) ( θ ω ∑ ∞ −∞ = = k t jk k e c t x ) ( ω Fourier Series (Complex Exp. Form) k are integers ∑ ∞ = + + = 1 ) cos( ) ( k k k t k A A t x θ ω k are integers Fourier Series (Trig. Form) These are two different forms of the same tool!! There is a 3 rd form that we’ll see later. Sect. 3.3 There is a related Form in Sect. 3.2 4/21 Q: Does this now let us get any periodic signal? A: No! Although Fourier thought so! Dirichlet showed that there are some that can’t be written in terms of a FS! But… those will never show up in practice! See top of p. 155 So we can write any practical periodic signal as a FS with infinite # of terms! So what??!! Here is what!! We can now break virtually any periodic signal into a sum of simple things… and we already understand how these simple things travel through an LTI system!...
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EECE 301 Note Set 13 FS Details - 1/21 EECE 301 Signals&...

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