Foundations of Signal Processing Tables

Size: px
Start display at page:

Download "Foundations of Signal Processing Tables"

Transcription

1 Foundations of Signal Processing Tables Martin Vetterli École Polytechnique Fédérale de Lausanne and University of California, Berkeley Jelena Kovačević Carnegie Mellon University Vivek K Goyal Massachusetts Institute of Technology August 8, 2012 Copyright (c) 2012 Martin Vetterli, Jelena Kovačević, and Vivek K Goyal. These materials are protected by copyright under the Attribution-NonCommercial-NoDerivs 3.0 Unported License from Creative Commons.

2 iisignal Processing: Foundations Cover photograph by Christiane Grimm, Geneva, Switzerland. Experimental set up by Prof. Libero Zuppiroli and Philippe Bugnon, Laboratory of Optoelectronics Molecular Materials, EPFL, Lausanne, Switzerland. The photograph captures an experiment first described by Isaac Newton in Opticks in 1730, explaining how the white light can be split into its color components and then resynthesized. It is a physical implementation of a white light decomposition into its Fourier components the colors of the rainbow, followed by a synthesis to recover the original. This experiment graphically summarizes the major theme of the book many signals can be split into essential components, and the signal s characteristics can be better understood by looking at its components; the process called analysis. These components can be used for processing the signal; more importantly, the signal can be perfectly recovered from those same components, through the process called synthesis.

3 Fundamental subspaces associated with matrix A The four fundamental subspaces associated with a real matrix A R M N. The matrix determines an orthogonal decomposition of R N into the row space of A and the null space of A; and an orthogonal decomposition of R M into the column space (range) of A and the left null space of A. The column and row spaces of A have the same dimension, which equals the rank of A. (Figure inspired by the cover of G. Strang. Introduction to Linear Algebra. 4th edition, 2009.) R N A R M row space R(A T ) column space R(A) A T 0 A T A 0 null space N(A) left null space N(A T ) R(A T ) N(A) dim(r(a T )) + dim(n(a)) = N R(A) N(A T ) dim(r(a)) + dim(n(a T )) = M Space Symbol Definition Dimension Column space (range) R(A) y C M y = Ax for some x C N } rank(a) Left null space N(A ) y C M A y = 0} M rank(a) dim(r(a))+dim(n(a )) = M Row space R(A ) x C N x = A y for some y C M } rank(a) Null space (kernel) N(A) x C N Ax = 0} N rank(a) dim(r(a ))+dim(n(a)) = N

4 Discrete-time processing concepts Concept Notation Infinite-length sequences Finite-length sequences Shift δ n 1 linear circular Sequence x n n Z n 0,1,...,N 1} vector LSI system h n n Z n 0,1,...,N 1} filter, impulse response operator Convolution h x x k h n k k Z k=0 x k h N,(n k) mod N Eigensequence v e jωn e j(2π/n)kn satisfies h v λ = λv λ h v ω = H(e jω )v ω h v k = H k v k invariant space S λ S ω = αe jωn } S k = αe j(2π/n)kn } α C,ω R α C,k Z Frequency response λ λ ω = H(e jω ) λ k = H k eigenvalue h ne jωn h ne j(2π/n)kn Fourier transform X DTFT DFT spectrum X(e jω ) = n Zx ne jωn X k = n Z n=0 x ne j(2π/n)kn n=0

5 Multirate discrete-time processing concepts Concept Expression Sampling factor 2 Input x n,x(z),x(e jω ) Downsampling by 2 y n = x 2n y = D 2 x [ ] Y(z) = (1/2) X(z 1/2 )+X( z 1/2 ) [ ] Y(e jω ) = (1/2) X(e jω/2 )+X(e j(ω 2π)/2 ) x Upsampling by 2 y n = n/2, n even; y = U 2 x Y(z) = X(z 2 ) Y(e jω ) = X(e j2ω ) Filtering with h y = D 2 H x [ ] & downsampling by 2 Y(z) = (1/2) 1 H(z 1/2 )X(z 1/2 )+H( z 1/2 )X( z 1/2 ) 2 [ ] Y(e jω ) = (1/2) H(e jω/2 )X(e jω/2 )+H(e j(ω 2π)/2 )X(e j(ω 2π)/2 ) Upsampling by 2 y = GU 2 x & filtering with g Y(z) = G(z)X(z 2 ) Y(e jω ) = G(e jω )X(e j2ω ) Sampling factor N Input x n,x(z),x(e jω ) Downsampling by N y n = x Nn y = D N x Upsampling by N y n = Y(z) = (1/N) X(ω k N z1/n ) k=0 Y(e jω ) = (1/N) X(e j(ω 2πk/N) ) k=0 x n/n, n/n Z; y = U N x Y(z) = X(z N ) Y(e jω ) = X(e jnω )

6 Kronecker delta sequence properties Kronecker delta sequence Normalization δ n = 1 Sifting n Z n0 nδ n = n Zx δ n0 nx n = x n0 n Z Shifting x n n δ n n0 = x n n0 Sampling x nδ n = x 0 δ n Restriction x nδ n = 1 0} x Dirac delta function properties Dirac delta function Normalization δ(t) dt = 1 Sifting x(t 0 t) δ(t) dt = x(t) δ(t 0 t) dt = x(t 0 ) Shifting x(t) t δ(t t 0 ) = x(t t 0 ) Sampling x(t) δ(t) = x(0) δ(t) Scaling δ(t/a) = a δ(t) for any nonzero a R

7 Ideal filters with unit-norm impulse response Ideal filters Time domain DTFT domain Ideal lowpass filter Ideal Nth-band filter Ideal halfband lowpass filter ω0 2π sinc(ω 0n/2) (1/ N) sinc(πn/n) (1/ 2) sinc(πn/2) 2π/ω0, 0, N, 0, 2, 0, ω ω 0 /2; otherwise. ω π/n; otherwise. ω π/2; otherwise. Unit-norm box and sinc functions/sequences Functions on the real line x(t), t R, x = 1 1/ t 0, t t 0 /2; Box ω0 Sinc 2π sinc(ω 0t/2) Periodic functions x(t), t [ T/2,T/2), x = 1 1/ t 0, t t 0 /2; Box k0 sinc(πk 0 t/t) Sinc T sinc(πt/t) Infinite-length sequences x n, n Z, x = 1 Box Sinc 1/ n 0, n (n 0 1)/2; ω0 2π sinc(ω 0n/2) Finite-length sequences x n, n 0,1,...,N 1}, x = 1 1/ n 0, n N/2 (n 0 1)/2; Box k0 sinc(πnk 0 /N) Sinc N sinc(πn/n) FT X(ω), ω R, X = 2π t0 sinc(ωt 0 /2) 2π/ω0, ω ω 0 /2; FS X k, k Z, X = 1/ T t0 T sinc(πkt 0/T) 1/ k 0 T, k (k 0 1)/2; DTFT X(e jω ), ω [ π,π), X = 2π sinc(ωn 0 /2) n0 sinc(ω/2) 2π/ω0, ω ω 0 /2; DFT X k, k 0,1,...,N 1}, X = N sinc(πn 0 k/n) n0 sinc(πk/n) N/k0, k N/2 (k 0 1)/2;

8 Energy and power concepts for sequences Deterministic sequences Energy spectral density A(e jω ) = X(e jω ) 2 WSS discrete-time stochastic processes Power spectral density A(e jω ) = E[x nx n k ]e jωk k Z Energy Power E = 1 π A(e jω )dω P = 1 π A(e jω )dω 2π π 2π π E = a 0 = n Z x n 2 P = a 0 = E[ x n 2 ] Orthogonality concepts for sequences Deterministic sequences WSS discrete-time stochastic processes Time c x,y,k = x n, y n k n = 0 c x,y,k = E[x nyn k ] = 0 Frequency C x,y(e jω ) = X(e jω )Y (e jω ) = 0 C x,y(e jω ) = 0

9 Deterministic discrete-time autocorrelation/crosscorrelation properties Domain Autocorrelation/Crosscorrelation Properties Sequences x n, y n Time a n k Z x kx k n a n = a n c n k Z x kyk n c x,y,n = c y,x, n DTFT A(e jω ) X(e jω ) 2 A(e jω ) = A (e jω ) C(e jω ) X(e jω )Y (e jω ) C x,y(e jω ) = C y,x (ejω ) z-transform A(z) X(z)X (z 1 ) A(z) = A (z 1 ) C(z) X(z)Y (z 1 ) C x,y(z) = C y,x (z 1 ) DFT A k X k 2 A k = A k mod N C k X k Yk C k = Cy,x, k mod N Real sequences x n, y n Time a n k Z x kx k n a n = a n c n k Z x ky k n c x,y,n = c y,x, n DTFT A(e jω ) X(e jω ) 2 A(e jω ) = A(e jω ) C(e jω ) X(e jω )Y(e jω ) C x,y(e jω ) = C y,x(e jω ) z-transform A(z) X(z)X(z 1 ) A(z) = A(z 1 ) C(z) X(z)Y(z 1 ) C x,y(z) = C y,x(z 1 ) DFT A k X k 2 A k = A k mod N C k X k Y k C k = C y,x, k mod N Vector of sequences [x 0,n ] T x 1,n Time A n a 0,n c 0,1,n c 1,0,n a 1,n [ ] [ ] DTFT A(e jω ) A 0 (e jω ) C 0,1 (e jω ) C 1,0 (e jω ) A 1 (e jω ) [ ] z-transform A(z) A 0 (z) C 0,1 (z) C 1,0 (z) A 1 (z) DFT A k A 0,k C 0,1,k C 1,0,k A 1,k [ ] A n = A n A n = A T n A(e jω ) = A (e jω ) A(e jω ) = A T (e jω ) A(z) = A (z 1 ) A(z) = A T (z 1 ) A k = A k mod N A k = A T k mod N

10 Discrete/continuous Fourier transform summary Transform Forward/Inverse Duality/Periodicity X(ω) = x(t)e jωt dt Fourier transform x(t) = 1 X(ω)e jωt dω 2π Fourier series X k = 1 T/2 x(t)e j(2π/t)kt dt T T/2 x(t) = X k e j(2π/t)kt k Z dual with DTFT x(t+t) = x(t) Discrete-time Fourier transform Discrete Fourier transform X(e jω ) = x ne jωn n Z x n = 1 π X(e jω )e jωn dω 2π π X k = x ne j(2π/n)kn n=0 x n = 1 X k e j(2π/n)kn N k=0 dual with Fourier series X(e j(ω+2π) ) = X(e jω )

11 Discrete Fourier transform (DFT) properties DFT properties Time domain DFT domain Basic properties Linearity αx n +βy n αx k +βy k Circular shift in time x (n n0 ) mod N W kn 0 N X k Circular shift in frequency W k 0n N x n X (k k0 ) mod N Circular time reversal x n mod N X k mod N Circular convolution in time (h x) n H k X k Circular convolution in frequency h nx n 1 N (H X) k Circular deterministic autocorrelation a n = x k x (k n) mod N A k = X k 2 k=0 N 1 Circular deterministic crosscorrelation c n = x k y(k n) mod N C k = X k Yk k=0 Parseval s equality x 2 = x n 2 = 1 X k 2 = 1 N N X 2 n=0 k=0 Related sequences Conjugate x n X k mod N Conjugate, time reversed x n mod N Xk Real part R(x n) (X k +X k mod N )/2 Imaginary part I(x n) (X k X k mod N )/(2j) Conjugate-symmetric part (x n +x n mod N )/2 R(X k) Conjugate-antisymmetric part (x n x n mod N )/(2j) I(X k) Symmetries for real x X conjugate symmetric X k = X k mod N Real part of X even R(X k ) = R(X k mod N ) Imaginary part of X odd I(X k ) = I(X k mod N ) Magnitude of X even X k = X k mod N Phase of X odd argx k = argx k mod N Common transform pairs Kronecker delta sequence δ n 1 Shifted Kronecker delta sequence δ (n n0 ) mod N W kn 0 N Constant sequence 1 Nδ k s Geometric sequence α n (1 αwn kn )/(1 αwk N ) Periodic sinc sequence k0 sinc(πnk 0 /N) N k, k0 N 2 k 0 1 ; 2 (ideal lowpass filter) N sinc(πn/n) 1 Box sequence n0, n N 2 n 0 1 ; sinc(πn 2 0 k/n) n0 sinc(πk/n)

12 Fourier series properties FS properties Time domain FS domain Basic properties Linearity αx(t)+βy(t) αx k +βy k Shift in time x(t t 0 ) e j(2π/t)kt 0 X k Shift in frequency e j(2π/t)k0t x(t) X(k k 0 ) Time reversal x( t) X k Differentiation d n x(t)/dt n t (j2πk/t) n X k Integration x(τ)dτ (T/(j2πk))X k, X 0 = 0 T/2 Circular convolution in time (h x)(t) T H k X k Convolution in frequency h(t)x(t) (H X) k T/2 Circular deterministic autocorrelation a(t) = x(τ)x (τ t)dτ A k = T X k 2 T/2 T/2 Circular deterministic crosscorrelation c(t) = x(τ)y (τ t)dτ C k = T X k Yk T/2 T/2 Parseval s equality x 2 = T/2 x(t) 2 dt = T X k 2 = T X 2 k Z Related functions Conjugate x (t) X k Conjugate, time reversed x ( t) Xk Real part R(x(t)) (X k +X k )/2 Imaginary part I(x(t)) (X k X k )/(2j) Conjugate-symmetric part (x(t)+x ( t))/2 R(X k ) Conjugate-antisymmetric part (x(t) x ( t))/(2j) I(X k ) Symmetries for real x X conjugate symmetric X k = X k Real part of X even R(X k ) = R(X k ) Imaginary part of X odd I(X k ) = I(X k ) Magnitude of X even X k = X k Phase of X odd argx k = argx k Common transform pairs Dirac comb Periodic sinc function (ideal lowpass filter) Box function (one period) Square wave (one period with T = 1) Triangle wave (one period with T = 1) Sawtooth wave (one period with T = 1) δ(t nt) 1/T n Z k0 sinc(πk 0 t/t) T sinc(πt/t) 1/ t0, t t 0 /2; 0, t 0 /2 < t T/2. 1, t [ 1/2,0); 1, t [0,1/2). 1 t, t 1/2. 2 2t, t 1/2. 1/ k0 T, k (k 0 1)/2; t0 T sinc(πkt 0/T) 2j/(πk), k odd; 0, k even. 1/4, k = 0; 1/(πk) 2, k odd; 0, k 0 even. 0, k = 0; j( 1) k /(πk), k 0.

13 z-transform properties z-transform properties Time domain z domain ROC ROC properties General seq. 0 r 1 < z < r 2 Finite-length seq. all z, except possibly 0, Right-sided seq. z > largest pole Left-sided seq. z < smallest pole BIBO stable z = 1 Basic properties Linearity αx n +βy n αx(z)+βy(z) ROC x ROC y Shift in time x n n0 z n 0 X(z) ROC x Scaling in time N 1 1 Downsampling x Nn X(WN k N ) (ROC x) 1/N k=0 xn/n, n/n Z; Upsampling X(z N ) (ROC x) N Scaling in z α n x n X(α 1 z) α ROC x Time reversal x n X(z 1 ) 1/ROC x Differentiation n k x n ( 1) k z k k X(z)/ z k ROC x m k = n k x n = ( 1) k k X(z)/ z k z=1 n Z Convolution in time (h x) n H(z)X(z) ROC h ROC x Deterministic autocorrelation a n = k Zx k x k n A(z) = X(z)X (z 1 ) ROC x 1/ROC x Deterministic crosscorrelation c n = k Zx k y k n C(z) = X(z)Y (z 1 ) 1/ROC x ROC y Related sequences Conjugate x n X (z ) ROC x Conjugate, time reversed x n X (z 1 ) 1/ROC x Real part R(x n) (X(z)+X (z ))/2 ROC x Imaginary part I(x n) (X(z) X (z ))/(2j) ROC x Symmetries for real x X conjugate symmetric X(z) = X (z ) Common transform pairs Kronecker delta sequence δ n 1 all z Shifted Kronecker delta sequence δ n n0 z n 0 all z, except possibly 0, Geometric sequence α n u n 1/(1 αz 1 ) z > α α n u n 1 z < α Arithmetic-geometric sequence nα n u n (αz 1 )/(1 αz 1 ) 2 z > α nα n u n 1 z < α

14 DTFT: Discrete-time Fourier transform properties DTFT properties Time domain DTFT domain Basic properties Linearity αx n +βy n αx(e jω )+βy(e jω ) Shift in time x n n0 e jωn 0 X(e jω ) Shift in frequency e jω0n x n X(e j(ω ω0) ) Scaling in time N 1 1 Downsampling x Nn X(e j(ω 2πk)/N ) N k=0 Upsampling x n/n, n = ln; 0, otherwise X(e jnω ) Time reversal x n X(e jω ) Differentiation in freq. ( jn) k k X(e jω ) x n ω k Moments m k = n k x n = ( j) k X(ejω ) ω n Z ω=0 Convolution in time (h x) n H(e jω )X(e jω ) 1 Circular convolution in frequency h nx n 2π (H X)(ejω ) Deterministic autocorrelation a n = x k x k n A(e jω ) = X(e jω ) 2 k Z Deterministic crosscorrelation c n = k Zx k yk n C(e jω ) = X(e jω )Y (e jω ) Parseval s equality x 2 = x n 2 = 1 π X(e jω ) 2 dω = 1 2π n Z π 2π X 2 Related sequences Conjugate x n X (e jω ) Conjugate, time reversed x n X (e jω ) Real part R(x n) (X(e jω )+X (e jω ))/2 Imaginary part I(x n) (X(e jω ) X (e jω ))/(2j) Conjugate-symmetric part (x n +x n)/2 R(X(e jω )) Conjugate-antisymmetric part (x n x n )/(2j) I(X(ejω )) Symmetries for real x X conjugate symmetric X(e jω ) = X (e jω ) Real part of X even R(X(e jω )) = R(X(e jω )) Imaginary part of X odd I(X(e jω )) = I(X(e jω )) Magnitude of X even X(e jω ) = X(e jω ) Phase of X odd argx(e jω ) = argx(e jω ) Common transform pairs Kronecker delta sequence δ n 1 Shifted Kronecker delta sequence δ n n0 e jωn 0 Constant sequence 1 2π δ(ω 2πk) k= Geometric sequence α n u n 1/(1 αe jω ), α < 1 Arithmetic-geometric sequence nα n u n αe jω /(1 αe jω ) 2, α < 1 Sinc sequence ω0 (ideal lowpass filter) 2π sinc(ω 2π/ω0, ω ω 0 /2; 0n/2) 1/ n0, n (n Box sequence 0 1)/2; sinc(ωn 0 /2) n0 sinc(ω/2)

15 Fourier transform properties FT properties Time domain FT domain Basic properties Linearity αx(t) + βy(t) αx(ω) + βy(ω) Shift in time x(t t 0 ) e jωt 0 X(ω) Shift in frequency e jω0t x(t) X(ω ω 0 ) Scaling in time and frequency x(αt) (1/α)X (ω/α) Time reversal x( t) X( ω) Differentiation in time d n x(t)/dt n (jω) n X(ω) Differentiation in frequency ( jt) n x(t) t d n X(ω)/dω n Integration in time x(τ)dτ X(ω)/jω, X(0) = 0 Moments m k = t k x(t)dt = (j) kdk X(ω) dω k ω=0 Convolution in time (h x)(t) H(ω) X(ω) Convolution in frequency 1 h(t) x(t) (H X)(ω) 2π Deterministic autocorrelation a(t) = x(τ)x (τ t)dτ A(ω) = X(ω) 2 Deterministic crosscorrelation c(t) = x(τ)y (τ t)dτ C(ω) = X(ω)Y (ω) Parseval s equality x 2 = x(t) 2 dt = 1 X(ω) 2 dω = 1 2π 2π X 2 Related functions Conjugate x (t) X ( ω) Conjugate, time reversed x ( t) X (ω) Real part R(x(t)) (X(ω) +X ( ω))/2 Imaginary part I(x(t)) (X(ω) X ( ω))/(2j) Conjugate-symmetric part (x(t)+x ( t))/2 R(X(ω)) Conjugate-antisymmetric part (x(t) x ( t))/(2j) I(X(ω)) Symmetries for real x X conjugate symmetric Real part of X even Imaginary part of X odd Magnitude of X even Phase of X odd X(ω) = X ( ω) R(X(ω)) = R(X( ω)) I(X(ω)) = I(X( ω)) X(ω) = X( ω) argx(ω) = argx( ω) Common transform pairs Dirac delta function δ(t) 1 Shifted Dirac delta function δ(t t 0 ) e jω 0t Dirac comb n Zδ(t nt) (2π/T) δ(ω (2π/T)k) k Z Constant function 1 2π δ(ω) Exponential function e α t (2α)/(ω 2 +α 2 ) Gaussian function e αt2 π/αe ω 2 /α Sinc function ω0 (ideal lowpass filter) 2π sinc(ω 2π/ω0, ω ω 0 /2; 0t/2) 1/ t0, t t Box function 0 /2; t0 sinc(ωt 0 /2) 1 t, t < 1; Triangle function (sinc(ω/2))

Mathematical Foundations of Signal Processing

Mathematical Foundations of Signal Processing Mathematical Foundations of Signal Processing Module 4: Continuous-Time Systems and Signals Benjamín Béjar Haro Mihailo Kolundžija Reza Parhizkar Adam Scholefield October 24, 2016 Continuous Time Signals

More information

Review of Discrete-Time System

Review of Discrete-Time System Review of Discrete-Time System Electrical & Computer Engineering University of Maryland, College Park Acknowledgment: ENEE630 slides were based on class notes developed by Profs. K.J. Ray Liu and Min Wu.

More information

Discrete Time Signals and Systems Time-frequency Analysis. Gloria Menegaz

Discrete Time Signals and Systems Time-frequency Analysis. Gloria Menegaz Discrete Time Signals and Systems Time-frequency Analysis Gloria Menegaz Time-frequency Analysis Fourier transform (1D and 2D) Reference textbook: Discrete time signal processing, A.W. Oppenheim and R.W.

More information

The World of Fourier and Wavelets: Theory, Algorithms and Applications 1

The World of Fourier and Wavelets: Theory, Algorithms and Applications 1 The World of Fourier and Wavelets: Theory, Algorithms and Applications 1 C. Grimm Martin Vetterli École Polytechnique Fédérale de Lausanne and University of California, Berkeley Jelena Kovačević Carnegie

More information

ELEN 4810 Midterm Exam

ELEN 4810 Midterm Exam ELEN 4810 Midterm Exam Wednesday, October 26, 2016, 10:10-11:25 AM. One sheet of handwritten notes is allowed. No electronics of any kind are allowed. Please record your answers in the exam booklet. Raise

More information

Signals & Systems Handout #4

Signals & Systems Handout #4 Signals & Systems Handout #4 H-4. Elementary Discrete-Domain Functions (Sequences): Discrete-domain functions are defined for n Z. H-4.. Sequence Notation: We use the following notation to indicate the

More information

ECE 301. Division 2, Fall 2006 Instructor: Mimi Boutin Midterm Examination 3

ECE 301. Division 2, Fall 2006 Instructor: Mimi Boutin Midterm Examination 3 ECE 30 Division 2, Fall 2006 Instructor: Mimi Boutin Midterm Examination 3 Instructions:. Wait for the BEGIN signal before opening this booklet. In the meantime, read the instructions below and fill out

More information

EE 438 Essential Definitions and Relations

EE 438 Essential Definitions and Relations May 2004 EE 438 Essential Definitions and Relations CT Metrics. Energy E x = x(t) 2 dt 2. Power P x = lim T 2T T / 2 T / 2 x(t) 2 dt 3. root mean squared value x rms = P x 4. Area A x = x(t) dt 5. Average

More information

Discrete Time Fourier Transform

Discrete Time Fourier Transform Discrete Time Fourier Transform Recall that we wrote the sampled signal x s (t) = x(kt)δ(t kt). We calculate its Fourier Transform. We do the following: Ex. Find the Continuous Time Fourier Transform of

More information

Fourier transform representation of CT aperiodic signals Section 4.1

Fourier transform representation of CT aperiodic signals Section 4.1 Fourier transform representation of CT aperiodic signals Section 4. A large class of aperiodic CT signals can be represented by the CT Fourier transform (CTFT). The (CT) Fourier transform (or spectrum)

More information

EC Signals and Systems

EC Signals and Systems UNIT I CLASSIFICATION OF SIGNALS AND SYSTEMS Continuous time signals (CT signals), discrete time signals (DT signals) Step, Ramp, Pulse, Impulse, Exponential 1. Define Unit Impulse Signal [M/J 1], [M/J

More information

DISCRETE FOURIER TRANSFORM

DISCRETE FOURIER TRANSFORM DISCRETE FOURIER TRANSFORM 1. Introduction The sampled discrete-time fourier transform (DTFT) of a finite length, discrete-time signal is known as the discrete Fourier transform (DFT). The DFT contains

More information

Discrete Time Fourier Transform (DTFT)

Discrete Time Fourier Transform (DTFT) Discrete Time Fourier Transform (DTFT) 1 Discrete Time Fourier Transform (DTFT) The DTFT is the Fourier transform of choice for analyzing infinite-length signals and systems Useful for conceptual, pencil-and-paper

More information

Fourier series for continuous and discrete time signals

Fourier series for continuous and discrete time signals 8-9 Signals and Systems Fall 5 Fourier series for continuous and discrete time signals The road to Fourier : Two weeks ago you saw that if we give a complex exponential as an input to a system, the output

More information

ECSE 512 Digital Signal Processing I Fall 2010 FINAL EXAMINATION

ECSE 512 Digital Signal Processing I Fall 2010 FINAL EXAMINATION FINAL EXAMINATION 9:00 am 12:00 pm, December 20, 2010 Duration: 180 minutes Examiner: Prof. M. Vu Assoc. Examiner: Prof. B. Champagne There are 6 questions for a total of 120 points. This is a closed book

More information

Fourier Series. Spectral Analysis of Periodic Signals

Fourier Series. Spectral Analysis of Periodic Signals Fourier Series. Spectral Analysis of Periodic Signals he response of continuous-time linear invariant systems to the complex exponential with unitary magnitude response of a continuous-time LI system at

More information

Complex symmetry Signals and Systems Fall 2015

Complex symmetry Signals and Systems Fall 2015 18-90 Signals and Systems Fall 015 Complex symmetry 1. Complex symmetry This section deals with the complex symmetry property. As an example I will use the DTFT for a aperiodic discrete-time signal. The

More information

ECE 301 Division 1, Fall 2006 Instructor: Mimi Boutin Final Examination

ECE 301 Division 1, Fall 2006 Instructor: Mimi Boutin Final Examination ECE 30 Division, all 2006 Instructor: Mimi Boutin inal Examination Instructions:. Wait for the BEGIN signal before opening this booklet. In the meantime, read the instructions below and fill out the requested

More information

Discrete-Time Fourier Transform (DTFT)

Discrete-Time Fourier Transform (DTFT) Discrete-Time Fourier Transform (DTFT) 1 Preliminaries Definition: The Discrete-Time Fourier Transform (DTFT) of a signal x[n] is defined to be X(e jω ) x[n]e jωn. (1) In other words, the DTFT of x[n]

More information

EE 224 Signals and Systems I Review 1/10

EE 224 Signals and Systems I Review 1/10 EE 224 Signals and Systems I Review 1/10 Class Contents Signals and Systems Continuous-Time and Discrete-Time Time-Domain and Frequency Domain (all these dimensions are tightly coupled) SIGNALS SYSTEMS

More information

Table 1: Properties of the Continuous-Time Fourier Series. Property Periodic Signal Fourier Series Coefficients

Table 1: Properties of the Continuous-Time Fourier Series. Property Periodic Signal Fourier Series Coefficients able : Properties of the Continuous-ime Fourier Series x(t = a k e jkω0t = a k = x(te jkω0t dt = a k e jk(/t x(te jk(/t dt Property Periodic Signal Fourier Series Coefficients x(t y(t } Periodic with period

More information

University of Connecticut Lecture Notes for ME5507 Fall 2014 Engineering Analysis I Part III: Fourier Analysis

University of Connecticut Lecture Notes for ME5507 Fall 2014 Engineering Analysis I Part III: Fourier Analysis University of Connecticut Lecture Notes for ME557 Fall 24 Engineering Analysis I Part III: Fourier Analysis Xu Chen Assistant Professor United Technologies Engineering Build, Rm. 382 Department of Mechanical

More information

Chapter 5. Fourier Analysis for Discrete-Time Signals and Systems Chapter

Chapter 5. Fourier Analysis for Discrete-Time Signals and Systems Chapter Chapter 5. Fourier Analysis for Discrete-Time Signals and Systems Chapter Objec@ves 1. Learn techniques for represen3ng discrete-)me periodic signals using orthogonal sets of periodic basis func3ons. 2.

More information

Chap 2. Discrete-Time Signals and Systems

Chap 2. Discrete-Time Signals and Systems Digital Signal Processing Chap 2. Discrete-Time Signals and Systems Chang-Su Kim Discrete-Time Signals CT Signal DT Signal Representation 0 4 1 1 1 2 3 Functional representation 1, n 1,3 x[ n] 4, n 2 0,

More information

Signals and Systems Spring 2004 Lecture #9

Signals and Systems Spring 2004 Lecture #9 Signals and Systems Spring 2004 Lecture #9 (3/4/04). The convolution Property of the CTFT 2. Frequency Response and LTI Systems Revisited 3. Multiplication Property and Parseval s Relation 4. The DT Fourier

More information

! Circular Convolution. " Linear convolution with circular convolution. ! Discrete Fourier Transform. " Linear convolution through circular

! Circular Convolution.  Linear convolution with circular convolution. ! Discrete Fourier Transform.  Linear convolution through circular Previously ESE 531: Digital Signal Processing Lec 22: April 18, 2017 Fast Fourier Transform (con t)! Circular Convolution " Linear convolution with circular convolution! Discrete Fourier Transform " Linear

More information

Digital Signal Processing Lecture 10 - Discrete Fourier Transform

Digital Signal Processing Lecture 10 - Discrete Fourier Transform Digital Signal Processing - Discrete Fourier Transform Electrical Engineering and Computer Science University of Tennessee, Knoxville November 12, 2015 Overview 1 2 3 4 Review - 1 Introduction Discrete-time

More information

1.3 Frequency Analysis A Review of Complex Numbers

1.3 Frequency Analysis A Review of Complex Numbers 3 CHAPTER. ANALYSIS OF DISCRETE-TIME LINEAR TIME-INVARIANT SYSTEMS I y z R θ x R Figure.8. A complex number z can be represented in Cartesian coordinates x, y or polar coordinates R, θ..3 Frequency Analysis.3.

More information

Table 1: Properties of the Continuous-Time Fourier Series. Property Periodic Signal Fourier Series Coefficients

Table 1: Properties of the Continuous-Time Fourier Series. Property Periodic Signal Fourier Series Coefficients able : Properties of the Continuous-ime Fourier Series x(t = e jkω0t = = x(te jkω0t dt = e jk(/t x(te jk(/t dt Property Periodic Signal Fourier Series Coefficients x(t y(t } Periodic with period and fundamental

More information

ECE 301 Division 1, Fall 2008 Instructor: Mimi Boutin Final Examination Instructions:

ECE 301 Division 1, Fall 2008 Instructor: Mimi Boutin Final Examination Instructions: ECE 30 Division, all 2008 Instructor: Mimi Boutin inal Examination Instructions:. Wait for the BEGIN signal before opening this booklet. In the meantime, read the instructions below and fill out the requested

More information

7.16 Discrete Fourier Transform

7.16 Discrete Fourier Transform 38 Signals, Systems, Transforms and Digital Signal Processing with MATLAB i.e. F ( e jω) = F [f[n]] is periodic with period 2π and its base period is given by Example 7.17 Let x[n] = 1. We have Π B (Ω)

More information

! Introduction. ! Discrete Time Signals & Systems. ! Z-Transform. ! Inverse Z-Transform. ! Sampling of Continuous Time Signals

! Introduction. ! Discrete Time Signals & Systems. ! Z-Transform. ! Inverse Z-Transform. ! Sampling of Continuous Time Signals ESE 531: Digital Signal Processing Lec 25: April 24, 2018 Review Course Content! Introduction! Discrete Time Signals & Systems! Discrete Time Fourier Transform! Z-Transform! Inverse Z-Transform! Sampling

More information

EEE4001F EXAM DIGITAL SIGNAL PROCESSING. University of Cape Town Department of Electrical Engineering PART A. June hours.

EEE4001F EXAM DIGITAL SIGNAL PROCESSING. University of Cape Town Department of Electrical Engineering PART A. June hours. EEE400F EXAM DIGITAL SIGNAL PROCESSING PART A Basic digital signal processing theory.. A sequencex[n] has a zero-phase DTFT X(e jω ) given below: X(e jω ) University of Cape Town Department of Electrical

More information

LECTURE 12 Sections Introduction to the Fourier series of periodic signals

LECTURE 12 Sections Introduction to the Fourier series of periodic signals Signals and Systems I Wednesday, February 11, 29 LECURE 12 Sections 3.1-3.3 Introduction to the Fourier series of periodic signals Chapter 3: Fourier Series of periodic signals 3. Introduction 3.1 Historical

More information

Aspects of Continuous- and Discrete-Time Signals and Systems

Aspects of Continuous- and Discrete-Time Signals and Systems Aspects of Continuous- and Discrete-Time Signals and Systems C.S. Ramalingam Department of Electrical Engineering IIT Madras C.S. Ramalingam (EE Dept., IIT Madras) Networks and Systems 1 / 45 Scaling the

More information

Lecture 19: Discrete Fourier Series

Lecture 19: Discrete Fourier Series EE518 Digital Signal Processing University of Washington Autumn 2001 Dept. of Electrical Engineering Lecture 19: Discrete Fourier Series Dec 5, 2001 Prof: J. Bilmes TA: Mingzhou

More information

ECE 301 Division 1 Final Exam Solutions, 12/12/2011, 3:20-5:20pm in PHYS 114.

ECE 301 Division 1 Final Exam Solutions, 12/12/2011, 3:20-5:20pm in PHYS 114. ECE 301 Division 1 Final Exam Solutions, 12/12/2011, 3:20-5:20pm in PHYS 114. The exam for both sections of ECE 301 is conducted in the same room, but the problems are completely different. Your ID will

More information

x[n] = x a (nt ) x a (t)e jωt dt while the discrete time signal x[n] has the discrete-time Fourier transform x[n]e jωn

x[n] = x a (nt ) x a (t)e jωt dt while the discrete time signal x[n] has the discrete-time Fourier transform x[n]e jωn Sampling Let x a (t) be a continuous time signal. The signal is sampled by taking the signal value at intervals of time T to get The signal x(t) has a Fourier transform x[n] = x a (nt ) X a (Ω) = x a (t)e

More information

Your solutions for time-domain waveforms should all be expressed as real-valued functions.

Your solutions for time-domain waveforms should all be expressed as real-valued functions. ECE-486 Test 2, Feb 23, 2017 2 Hours; Closed book; Allowed calculator models: (a) Casio fx-115 models (b) HP33s and HP 35s (c) TI-30X and TI-36X models. Calculators not included in this list are not permitted.

More information

University Question Paper Solution

University Question Paper Solution Unit 1: Introduction University Question Paper Solution 1. Determine whether the following systems are: i) Memoryless, ii) Stable iii) Causal iv) Linear and v) Time-invariant. i) y(n)= nx(n) ii) y(t)=

More information

Homework: 4.50 & 4.51 of the attachment Tutorial Problems: 7.41, 7.44, 7.47, Signals & Systems Sampling P1

Homework: 4.50 & 4.51 of the attachment Tutorial Problems: 7.41, 7.44, 7.47, Signals & Systems Sampling P1 Homework: 4.50 & 4.51 of the attachment Tutorial Problems: 7.41, 7.44, 7.47, 7.49 Signals & Systems Sampling P1 Undersampling & Aliasing Undersampling: insufficient sampling frequency ω s < 2ω M Perfect

More information

MEDE2500 Tutorial Nov-7

MEDE2500 Tutorial Nov-7 (updated 2016-Nov-4,7:40pm) MEDE2500 (2016-2017) Tutorial 3 MEDE2500 Tutorial 3 2016-Nov-7 Content 1. The Dirac Delta Function, singularity functions, even and odd functions 2. The sampling process and

More information

Solutions. Number of Problems: 10

Solutions. Number of Problems: 10 Final Exam February 9th, 2 Signals & Systems (5-575-) Prof. R. D Andrea Solutions Exam Duration: 5 minutes Number of Problems: Permitted aids: One double-sided A4 sheet. Questions can be answered in English

More information

Lecture Notes on Fundamentals of Audio-Video Signal Processing

Lecture Notes on Fundamentals of Audio-Video Signal Processing Marco Tagliasacchi Lecture Notes on Fundamentals of Audio-Video Signal Processing November 12, 2007 Politecnico di Milano Contents Part I Fundamentals of Digital Signal Processing 1 Introduction to the

More information

Signal and systems. Linear Systems. Luigi Palopoli. Signal and systems p. 1/5

Signal and systems. Linear Systems. Luigi Palopoli. Signal and systems p. 1/5 Signal and systems p. 1/5 Signal and systems Linear Systems Luigi Palopoli palopoli@dit.unitn.it Wrap-Up Signal and systems p. 2/5 Signal and systems p. 3/5 Fourier Series We have see that is a signal

More information

ECE503: Digital Signal Processing Lecture 5

ECE503: Digital Signal Processing Lecture 5 ECE53: Digital Signal Processing Lecture 5 D. Richard Brown III WPI 3-February-22 WPI D. Richard Brown III 3-February-22 / 32 Lecture 5 Topics. Magnitude and phase characterization of transfer functions

More information

ECE 301. Division 3, Fall 2007 Instructor: Mimi Boutin Midterm Examination 3

ECE 301. Division 3, Fall 2007 Instructor: Mimi Boutin Midterm Examination 3 ECE 30 Division 3, all 2007 Instructor: Mimi Boutin Midterm Examination 3 Instructions:. Wait for the BEGIN signal before opening this booklet. In the meantime, read the instructions below and fill out

More information

Frequency-Domain C/S of LTI Systems

Frequency-Domain C/S of LTI Systems Frequency-Domain C/S of LTI Systems x(n) LTI y(n) LTI: Linear Time-Invariant system h(n), the impulse response of an LTI systems describes the time domain c/s. H(ω), the frequency response describes the

More information

Question Paper Code : AEC11T02

Question Paper Code : AEC11T02 Hall Ticket No Question Paper Code : AEC11T02 VARDHAMAN COLLEGE OF ENGINEERING (AUTONOMOUS) Affiliated to JNTUH, Hyderabad Four Year B. Tech III Semester Tutorial Question Bank 2013-14 (Regulations: VCE-R11)

More information

Shift-Variance and Nonstationarity of Generalized Sampling-Reconstruction Processes

Shift-Variance and Nonstationarity of Generalized Sampling-Reconstruction Processes Shift-Variance and Nonstationarity of Generalized Sampling-Reconstruction Processes Runyi Yu Eastern Mediterranean University Gazimagusa, North Cyprus Web: faraday.ee.emu.edu.tr/yu Emails: runyi.yu@emu.edu.tr

More information

Z-TRANSFORMS. Solution: Using the definition (5.1.2), we find: for case (b). y(n)= h(n) x(n) Y(z)= H(z)X(z) (convolution) (5.1.

Z-TRANSFORMS. Solution: Using the definition (5.1.2), we find: for case (b). y(n)= h(n) x(n) Y(z)= H(z)X(z) (convolution) (5.1. 84 5. Z-TRANSFORMS 5 z-transforms Solution: Using the definition (5..2), we find: for case (a), and H(z) h 0 + h z + h 2 z 2 + h 3 z 3 2 + 3z + 5z 2 + 2z 3 H(z) h 0 + h z + h 2 z 2 + h 3 z 3 + h 4 z 4

More information

ECE-700 Review. Phil Schniter. January 5, x c (t)e jωt dt, x[n]z n, Denoting a transform pair by x[n] X(z), some useful properties are

ECE-700 Review. Phil Schniter. January 5, x c (t)e jωt dt, x[n]z n, Denoting a transform pair by x[n] X(z), some useful properties are ECE-7 Review Phil Schniter January 5, 7 ransforms Using x c (t) to denote a continuous-time signal at time t R, Laplace ransform: X c (s) x c (t)e st dt, s C Continuous-ime Fourier ransform (CF): ote that:

More information

Homework 4. May An LTI system has an input, x(t) and output y(t) related through the equation y(t) = t e (t t ) x(t 2)dt

Homework 4. May An LTI system has an input, x(t) and output y(t) related through the equation y(t) = t e (t t ) x(t 2)dt Homework 4 May 2017 1. An LTI system has an input, x(t) and output y(t) related through the equation y(t) = t e (t t ) x(t 2)dt Determine the impulse response of the system. Rewriting as y(t) = t e (t

More information

Chapter 6: Applications of Fourier Representation Houshou Chen

Chapter 6: Applications of Fourier Representation Houshou Chen Chapter 6: Applications of Fourier Representation Houshou Chen Dept. of Electrical Engineering, National Chung Hsing University E-mail: houshou@ee.nchu.edu.tw H.S. Chen Chapter6: Applications of Fourier

More information

EDISP (NWL2) (English) Digital Signal Processing Transform, FT, DFT. March 11, 2015

EDISP (NWL2) (English) Digital Signal Processing Transform, FT, DFT. March 11, 2015 EDISP (NWL2) (English) Digital Signal Processing Transform, FT, DFT March 11, 2015 Transform concept We want to analyze the signal represent it as built of some building blocks (well known signals), possibly

More information

Representing a Signal

Representing a Signal The Fourier Series Representing a Signal The convolution method for finding the response of a system to an excitation takes advantage of the linearity and timeinvariance of the system and represents the

More information

Multirate signal processing

Multirate signal processing Multirate signal processing Discrete-time systems with different sampling rates at various parts of the system are called multirate systems. The need for such systems arises in many applications, including

More information

Homework 7 Solution EE235, Spring Find the Fourier transform of the following signals using tables: te t u(t) h(t) = sin(2πt)e t u(t) (2)

Homework 7 Solution EE235, Spring Find the Fourier transform of the following signals using tables: te t u(t) h(t) = sin(2πt)e t u(t) (2) Homework 7 Solution EE35, Spring. Find the Fourier transform of the following signals using tables: (a) te t u(t) h(t) H(jω) te t u(t) ( + jω) (b) sin(πt)e t u(t) h(t) sin(πt)e t u(t) () h(t) ( ejπt e

More information

Discrete Fourier Transform

Discrete Fourier Transform Discrete Fourier Transform Virtually all practical signals have finite length (e.g., sensor data, audio records, digital images, stock values, etc). Rather than considering such signals to be zero-padded

More information

2.1 Basic Concepts Basic operations on signals Classication of signals

2.1 Basic Concepts Basic operations on signals Classication of signals Haberle³me Sistemlerine Giri³ (ELE 361) 9 Eylül 2017 TOBB Ekonomi ve Teknoloji Üniversitesi, Güz 2017-18 Dr. A. Melda Yüksel Turgut & Tolga Girici Lecture Notes Chapter 2 Signals and Linear Systems 2.1

More information

Discrete-Time Signals and Systems

Discrete-Time Signals and Systems ECE 46 Lec Viewgraph of 35 Discrete-Time Signals and Systems Sequences: x { x[ n] }, < n

More information

A.1 THE SAMPLED TIME DOMAIN AND THE Z TRANSFORM. 0 δ(t)dt = 1, (A.1) δ(t)dt =

A.1 THE SAMPLED TIME DOMAIN AND THE Z TRANSFORM. 0 δ(t)dt = 1, (A.1) δ(t)dt = APPENDIX A THE Z TRANSFORM One of the most useful techniques in engineering or scientific analysis is transforming a problem from the time domain to the frequency domain ( 3). Using a Fourier or Laplace

More information

Interchange of Filtering and Downsampling/Upsampling

Interchange of Filtering and Downsampling/Upsampling Interchange of Filtering and Downsampling/Upsampling Downsampling and upsampling are linear systems, but not LTI systems. They cannot be implemented by difference equations, and so we cannot apply z-transform

More information

Multimedia Signals and Systems - Audio and Video. Signal, Image, Video Processing Review-Introduction, MP3 and MPEG2

Multimedia Signals and Systems - Audio and Video. Signal, Image, Video Processing Review-Introduction, MP3 and MPEG2 Multimedia Signals and Systems - Audio and Video Signal, Image, Video Processing Review-Introduction, MP3 and MPEG2 Kunio Takaya Electrical and Computer Engineering University of Saskatchewan December

More information

Digital Signal Processing. Midterm 1 Solution

Digital Signal Processing. Midterm 1 Solution EE 123 University of California, Berkeley Anant Sahai February 15, 27 Digital Signal Processing Instructions Midterm 1 Solution Total time allowed for the exam is 8 minutes Some useful formulas: Discrete

More information

Lecture 2 OKAN UNIVERSITY FACULTY OF ENGINEERING AND ARCHITECTURE

Lecture 2 OKAN UNIVERSITY FACULTY OF ENGINEERING AND ARCHITECTURE OKAN UNIVERSITY FACULTY OF ENGINEERING AND ARCHITECTURE EEE 43 DIGITAL SIGNAL PROCESSING (DSP) 2 DIFFERENCE EQUATIONS AND THE Z- TRANSFORM FALL 22 Yrd. Doç. Dr. Didem Kivanc Tureli didemk@ieee.org didem.kivanc@okan.edu.tr

More information

Digital Signal Processing Lecture 3 - Discrete-Time Systems

Digital Signal Processing Lecture 3 - Discrete-Time Systems Digital Signal Processing - Discrete-Time Systems Electrical Engineering and Computer Science University of Tennessee, Knoxville August 25, 2015 Overview 1 2 3 4 5 6 7 8 Introduction Three components of

More information

BME 50500: Image and Signal Processing in Biomedicine. Lecture 2: Discrete Fourier Transform CCNY

BME 50500: Image and Signal Processing in Biomedicine. Lecture 2: Discrete Fourier Transform CCNY 1 Lucas Parra, CCNY BME 50500: Image and Signal Processing in Biomedicine Lecture 2: Discrete Fourier Transform Lucas C. Parra Biomedical Engineering Department CCNY http://bme.ccny.cuny.edu/faculty/parra/teaching/signal-and-image/

More information

UNIVERSITY OF OSLO. Please make sure that your copy of the problem set is complete before you attempt to answer anything.

UNIVERSITY OF OSLO. Please make sure that your copy of the problem set is complete before you attempt to answer anything. UNIVERSITY OF OSLO Faculty of mathematics and natural sciences Examination in INF3470/4470 Digital signal processing Day of examination: December 9th, 011 Examination hours: 14.30 18.30 This problem set

More information

2007 Final Exam for Random Processes. x(t)

2007 Final Exam for Random Processes. x(t) 2007 Final Exam for Random Processes x(t ϕ n (τ y n (t. (a (8 pt. Let {ϕ n (τ} n and {λ n } n satisfy that and ϕ n (τϕ m(τdτ δ[n m] R xx (t sϕ n (sds λ n ϕ n (t, where R xx (τ is the autocorrelation function

More information

DSP-I DSP-I DSP-I DSP-I

DSP-I DSP-I DSP-I DSP-I NOTES FOR 8-79 LECTURES 3 and 4 Introduction to Discrete-Time Fourier Transforms (DTFTs Distributed: September 8, 2005 Notes: This handout contains in brief outline form the lecture notes used for 8-79

More information

Digital Signal Processing. Midterm 2 Solutions

Digital Signal Processing. Midterm 2 Solutions EE 123 University of California, Berkeley Anant Sahai arch 15, 2007 Digital Signal Processing Instructions idterm 2 Solutions Total time allowed for the exam is 80 minutes Please write your name and SID

More information

Chap 4. Sampling of Continuous-Time Signals

Chap 4. Sampling of Continuous-Time Signals Digital Signal Processing Chap 4. Sampling of Continuous-Time Signals Chang-Su Kim Digital Processing of Continuous-Time Signals Digital processing of a CT signal involves three basic steps 1. Conversion

More information

A system that is both linear and time-invariant is called linear time-invariant (LTI).

A system that is both linear and time-invariant is called linear time-invariant (LTI). The Cooper Union Department of Electrical Engineering ECE111 Signal Processing & Systems Analysis Lecture Notes: Time, Frequency & Transform Domains February 28, 2012 Signals & Systems Signals are mapped

More information

ENSC327 Communications Systems 2: Fourier Representations. School of Engineering Science Simon Fraser University

ENSC327 Communications Systems 2: Fourier Representations. School of Engineering Science Simon Fraser University ENSC37 Communications Systems : Fourier Representations School o Engineering Science Simon Fraser University Outline Chap..5: Signal Classiications Fourier Transorm Dirac Delta Function Unit Impulse Fourier

More information

Discrete-time Fourier transform (DTFT) representation of DT aperiodic signals Section The (DT) Fourier transform (or spectrum) of x[n] is

Discrete-time Fourier transform (DTFT) representation of DT aperiodic signals Section The (DT) Fourier transform (or spectrum) of x[n] is Discrete-time Fourier transform (DTFT) representation of DT aperiodic signals Section 5. 3 The (DT) Fourier transform (or spectrum) of x[n] is X ( e jω) = n= x[n]e jωn x[n] can be reconstructed from its

More information

Signals & Systems. Lecture 4 Fourier Series Properties & Discrete-Time Fourier Series. Alp Ertürk

Signals & Systems. Lecture 4 Fourier Series Properties & Discrete-Time Fourier Series. Alp Ertürk Signals & Systems Lecture 4 Fourier Series Properties & Discrete-Time Fourier Series Alp Ertürk alp.erturk@kocaeli.edu.tr Fourier Series Representation of Continuous-Time Periodic Signals Synthesis equation:

More information

ECE 301 Fall 2010 Division 2 Homework 10 Solutions. { 1, if 2n t < 2n + 1, for any integer n, x(t) = 0, if 2n 1 t < 2n, for any integer n.

ECE 301 Fall 2010 Division 2 Homework 10 Solutions. { 1, if 2n t < 2n + 1, for any integer n, x(t) = 0, if 2n 1 t < 2n, for any integer n. ECE 3 Fall Division Homework Solutions Problem. Reconstruction of a continuous-time signal from its samples. Consider the following periodic signal, depicted below: {, if n t < n +, for any integer n,

More information

Signals and Systems Profs. Byron Yu and Pulkit Grover Fall Midterm 2 Solutions

Signals and Systems Profs. Byron Yu and Pulkit Grover Fall Midterm 2 Solutions 8-90 Signals and Systems Profs. Byron Yu and Pulkit Grover Fall 08 Midterm Solutions Name: Andrew ID: Problem Score Max 8 5 3 6 4 7 5 8 6 7 6 8 6 9 0 0 Total 00 Midterm Solutions. (8 points) Indicate whether

More information

ELC 4351: Digital Signal Processing

ELC 4351: Digital Signal Processing ELC 4351: Digital Signal Processing Liang Dong Electrical and Computer Engineering Baylor University liang dong@baylor.edu October 18, 2016 Liang Dong (Baylor University) Frequency-domain Analysis of LTI

More information

ENSC327 Communications Systems 2: Fourier Representations. Jie Liang School of Engineering Science Simon Fraser University

ENSC327 Communications Systems 2: Fourier Representations. Jie Liang School of Engineering Science Simon Fraser University ENSC327 Communications Systems 2: Fourier Representations Jie Liang School of Engineering Science Simon Fraser University 1 Outline Chap 2.1 2.5: Signal Classifications Fourier Transform Dirac Delta Function

More information

ELEN E4810: Digital Signal Processing Topic 11: Continuous Signals. 1. Sampling and Reconstruction 2. Quantization

ELEN E4810: Digital Signal Processing Topic 11: Continuous Signals. 1. Sampling and Reconstruction 2. Quantization ELEN E4810: Digital Signal Processing Topic 11: Continuous Signals 1. Sampling and Reconstruction 2. Quantization 1 1. Sampling & Reconstruction DSP must interact with an analog world: A to D D to A x(t)

More information

Overview. Signals as functions (1D, 2D) 1D Fourier Transform. 2D Fourier Transforms. Discrete Fourier Transform (DFT) Discrete Cosine Transform (DCT)

Overview. Signals as functions (1D, 2D) 1D Fourier Transform. 2D Fourier Transforms. Discrete Fourier Transform (DFT) Discrete Cosine Transform (DCT) Fourier Transform Overview Signals as functions (1D, 2D) Tools 1D Fourier Transform Summary of definition and properties in the different cases CTFT, CTFS, DTFS, DTFT DFT 2D Fourier Transforms Generalities

More information

Fourier Series and Fourier Transforms

Fourier Series and Fourier Transforms Fourier Series and Fourier Transforms EECS2 (6.082), MIT Fall 2006 Lectures 2 and 3 Fourier Series From your differential equations course, 18.03, you know Fourier s expression representing a T -periodic

More information

Very useful for designing and analyzing signal processing systems

Very useful for designing and analyzing signal processing systems z-transform z-transform The z-transform generalizes the Discrete-Time Fourier Transform (DTFT) for analyzing infinite-length signals and systems Very useful for designing and analyzing signal processing

More information

Signals and Systems I Have Known and Loved. (Lecture notes for CSE 3451) Andrew W. Eckford

Signals and Systems I Have Known and Loved. (Lecture notes for CSE 3451) Andrew W. Eckford Signals and Systems I Have Known and Loved (Lecture notes for CSE 3451) Andrew W. Eckford Department of Electrical Engineering and Computer Science York University, Toronto, Ontario, Canada Version: December

More information

Lecture 10. Digital Signal Processing. Chapter 7. Discrete Fourier transform DFT. Mikael Swartling Nedelko Grbic Bengt Mandersson. rev.

Lecture 10. Digital Signal Processing. Chapter 7. Discrete Fourier transform DFT. Mikael Swartling Nedelko Grbic Bengt Mandersson. rev. Lecture 10 Digital Signal Processing Chapter 7 Discrete Fourier transform DFT Mikael Swartling Nedelko Grbic Bengt Mandersson rev. 016 Department of Electrical and Information Technology Lund University

More information

GATE EE Topic wise Questions SIGNALS & SYSTEMS

GATE EE Topic wise Questions SIGNALS & SYSTEMS www.gatehelp.com GATE EE Topic wise Questions YEAR 010 ONE MARK Question. 1 For the system /( s + 1), the approximate time taken for a step response to reach 98% of the final value is (A) 1 s (B) s (C)

More information

X. Chen More on Sampling

X. Chen More on Sampling X. Chen More on Sampling 9 More on Sampling 9.1 Notations denotes the sampling time in second. Ω s = 2π/ and Ω s /2 are, respectively, the sampling frequency and Nyquist frequency in rad/sec. Ω and ω denote,

More information

Like bilateral Laplace transforms, ROC must be used to determine a unique inverse z-transform.

Like bilateral Laplace transforms, ROC must be used to determine a unique inverse z-transform. Inversion of the z-transform Focus on rational z-transform of z 1. Apply partial fraction expansion. Like bilateral Laplace transforms, ROC must be used to determine a unique inverse z-transform. Let X(z)

More information

Review of Fundamentals of Digital Signal Processing

Review of Fundamentals of Digital Signal Processing Chapter 2 Review of Fundamentals of Digital Signal Processing 2.1 (a) This system is not linear (the constant term makes it non linear) but is shift-invariant (b) This system is linear but not shift-invariant

More information

Signal Processing Signal and System Classifications. Chapter 13

Signal Processing Signal and System Classifications. Chapter 13 Chapter 3 Signal Processing 3.. Signal and System Classifications In general, electrical signals can represent either current or voltage, and may be classified into two main categories: energy signals

More information

1 Signals and systems

1 Signals and systems 978--52-5688-4 - Introduction to Orthogonal Transforms: With Applications in Data Processing and Analysis Signals and systems In the first two chapters we will consider some basic concepts and ideas as

More information

The Johns Hopkins University Department of Electrical and Computer Engineering Introduction to Linear Systems Fall 2002.

The Johns Hopkins University Department of Electrical and Computer Engineering Introduction to Linear Systems Fall 2002. The Johns Hopkins University Department of Electrical and Computer Engineering 505.460 Introduction to Linear Systems Fall 2002 Final exam Name: You are allowed to use: 1. Table 3.1 (page 206) & Table

More information

Chapter 13 Z Transform

Chapter 13 Z Transform Chapter 13 Z Transform 1. -transform 2. Inverse -transform 3. Properties of -transform 4. Solution to Difference Equation 5. Calculating output using -transform 6. DTFT and -transform 7. Stability Analysis

More information

Discrete Fourier Transform

Discrete Fourier Transform Discrete Fourier Transform Valentina Hubeika, Jan Černocký DCGM FIT BUT Brno, {ihubeika,cernocky}@fit.vutbr.cz Diskrete Fourier transform (DFT) We have just one problem with DFS that needs to be solved.

More information

Review of Linear Time-Invariant Network Analysis

Review of Linear Time-Invariant Network Analysis D1 APPENDIX D Review of Linear Time-Invariant Network Analysis Consider a network with input x(t) and output y(t) as shown in Figure D-1. If an input x 1 (t) produces an output y 1 (t), and an input x

More information

LAST Name FOURIER FIRST Name Jean Baptiste Joseph Lab Time 365/24/7

LAST Name FOURIER FIRST Name Jean Baptiste Joseph Lab Time 365/24/7 EECS 20N: Structure and Interpretation of Signals and Systems Final Exam Sol. Department of Electrical Engineering and Computer Sciences 13 December 2005 UNIVERSITY OF CALIFORNIA BERKELEY LAST Name FOURIER

More information

NAME: 11 December 2013 Digital Signal Processing I Final Exam Fall Cover Sheet

NAME: 11 December 2013 Digital Signal Processing I Final Exam Fall Cover Sheet NAME: December Digital Signal Processing I Final Exam Fall Cover Sheet Test Duration: minutes. Open Book but Closed Notes. Three 8.5 x crib sheets allowed Calculators NOT allowed. This test contains four

More information

Lecture 11: Two Channel Filter Bank

Lecture 11: Two Channel Filter Bank WAVELETS AND MULTIRATE DIGITAL SIGNAL PROCESSING Lecture 11: Two Channel Filter Bank Prof.V.M.Gadre, EE, IIT Bombay 1 Introduction In the previous lecture we studied Z domain analysis of two channel filter

More information