Digital Signal Octave Codes (0A)
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1 Digital Signal Periodic Conditions
2 Copyright (c) Young W. Lim. Permission is granted to copy, distribute and/or modify this document under the terms of the GNU Free Documentation License, Version 1.2 or any later version published by the Free Software Foundation; with no Invariant Sections, no Front-Cover Texts, and no Back-Cover Texts. A copy of the license is included in the section entitled "GNU Free Documentation License". Please send corrections (or suggestions) to youngwlim@hotmail.com. This document was produced by using OpenOffice and Octave.
3 Based on M.J. Roberts, Fundamentals of Signals and Systems S.K. Mitra, Digital Signal Processing : a computer-based approach 2 nd ed S.D. Stearns, Digital Signal Processing with Examples in MATLAB 3
4 Sampling and Normalized Frequency ω 0 t = 2 π f 0 t t = nt s T s : sampling period ω 0 nt s = 2 π f 0 n T s = 2 π T 0 n T s f 0 = 1 T 0 T 0 : signal period = 2 π n T s T 0 T s T 0 = f 0 f s normalization = 2 π n F 0 F 0 = f 0 T s = f 0 f s normalization 4
5 Analog and Digital Frequencies ω 0 t = 2 π f 0 t Analog Signal t = nt s t = nt s n ω 0 T s = 2 π n f 0 T s ω 0 T s = Ω 0 f 0 T s = F 0 Ω 0 n = 2π n F 0 Digital Signal 5
6 Multiplying by T s Normalization ω 0 t = 2 π f 0 t Analog Signal T s T s Normalization Ω 0 n = 2 π n F 0 Digital Signal 6
7 Normalization F 0 = f 0 T s f 0 T s Multiplied by T s = f 0 / f s f 0 / f s Divided by f s = T s / T 0 Ω 0 = 2 π F 0 7
8 Normalized Cyclic and Radian Frequencies Normalized Cyclic Frequency F 0 cycles/ sample = f 0 cycles/ second f s samples/ second Normalized Radian Frequency Ω 0 radians/sample = ω 0 radians/ second f s samples/ second 8
9 Periodic Relation e j(2 π(n+n 0 ) F 0 ) = e j(2 π n F 0 ) e j 2 π N 0 F 0 = 1 Digital Signal Period N 0 : the smallest integer Periodic Condition : integer m 2 π N 0 F 0 = 2 π m e j 2 π m = 1 N 0 = m F 0 = m T 0 T s Integer * Rational no : must be an Integer 9
10 Periodic Relation Integer N 0 = m F 0 = m T 0 T s Integer * Rational no : must be an Integer Rational numbers 10
11 Periodic Relation e j(2 π(n+ N 0 ) F 0 ) = e j(2 π n F 0 ) e j (2π f 0 )(t +T 0 ) = e j(2π f 0 )t Digital Signal Period N 0 : the smallest integer 2π N 0 F 0 = 2 π m Analog Signal Period T 0 : the smallest real number 2π f 0 T 0 = 2 π m N 0 = m F 0 = m T 0 T s T 0 = 1 f 0 Periodic Condition : some integers m Periodic Condition : for all integer m 11
12 Periodic Relation 2 π N 0 F 0 = 2 π m 2 π f 0 T 0 = 2 π m N 0 = m F 0 T 0 = 1 Integer N 0 Real T 0 Rational F 0 Real f f 0 0 = m p/q = m q p Minimum Integer N 0 Minimum Real T 0 N 0 = q m = p T 0 = 1 f 0 m = 1 12
13 N 0 = m F 0 Periodic Relation 2 π N 0 F 0 = 2 π m 2 π f 0 T 0 = 2 π m T 0 = 1 f 0 Integer N 0 Real T 0 given F 0 = m: multiples of 36 given m: all integers N 0 = m = 36 f 0 = T 0 = m = 1 2 N 0 = m = 72 2T 0 = m = 2 3 N 0 = m = 108 3T 0 = m = 3 13
14 Periodic Condition of a Sampled Signal 2 π F 0 n = 2 π m g(nt s ) = A cos(2 π f 0 T s n+θ) F 0 n = m Integers n, m F 0 = f 0 T s = f 0 / f s F 0 = m n F 0 = m n = f 0 f s Fundamental Frequency Sampling Frequency g[n] = A cos(2 π F 0 n + θ) Rational Number F 0 = m n M.J. Roberts, Fundamentals of Signals and Systems 14
15 A Cosine Waveform n= [0:29]; n= [0:29]; x= cos(2*pi*(n/10)); x= cos((2/10)*pi*n); n T s = n 1 10 F 0 = f 0 T s = f 0 f s = T s T 0 n T s = n 1 2 π f 0 nt s 2 π f 0 nt s = 2 π 1 n 1 10 = 2 π 1 10 n 1 T s = 0.1 f 0 = 1 (T 0 = 1) T s = 1 f 0 = 0.1 (T 0 =10) F 0 = f 0 T s = 0.1 F 0 = f 0 T s = 0.1 U of Rhode Island, ELE 436, FFT Tutorial 15
16 Many waveforms share the same sampled data x ` 3 U of Rhode Island, ELE 436, FFT Tutorial 30 16
17 Cosine Wave 1 n= [0:29]; x= cos(2*pi*n/10); ω 0 = 2π f 0 = 2π T 0 t = [0:29]/10; y = cos(2*pi*t); stem(t, y) hold on t2 = [0:290]/100; y2 = cos(2*pi*t2); plot(t2, y2) ω 0 = 2π f 0 = 2π T 0 t = [0:29]; y = cos(0.2*pi*t); stem(t, y) hold on t2 = [0:290]/10; y2 = cos(0.2*pi*t2); plot(t2, y2) U of Rhode Island, ELE 436, FFT Tutorial 17
18 Normalized Frequency subplot(2, 1, 1); t = [0:29]/10; y = cos(2*pi*t); stem(t, y) hold on t2 = [0:290]/100; y2 = cos(2*pi*t2); plot(t2, y2) axis([0, 10, -1, 1]); subplot(2, 1, 2) t = [0:29]; y = cos(0.2*pi*t); stem(t, y) hold on t2 = [0:290]/10; y2 = cos(0.2*pi*t2); plot(t2, y2) axis([0, 10, -1, 1]); f 0 = 1 T 0 = 1 f s = 10 T s = 0.1 f 0 = 0.1 T 0 = 10 f s = 1 T s = 1 U of Rhode Island, ELE 436, FFT Tutorial 18
19 Cosine Wave 1 t = [0:29]/10; y = cos(2*pi*t); stem(t, y) hold on t2 = [0:290]/100; y2 = cos(2*pi*t2); plot(t2, y2) f 0 = 1 T s = 0.1 F 0 = f 0 T s = 0.1 T 0 = 1 f 0 = 1 T 0 = 1 f s = 10 T s = 0.1 U of Rhode Island, ELE 436, FFT Tutorial 19
20 Cosine Wave 2 t = [0:29]; y = cos(0.2*pi*t); stem(t, y) hold on t2 = [0:290]/10; y2 = cos(0.2*pi*t2); plot(t2, y2) T 0 = 10 f 0 = 0.1 T 0 = 10 f s = 1 T s = 1 f 0 = 0.1 T s = 1 F 0 = f 0 T s = 0.1 U of Rhode Island, ELE 436, FFT Tutorial 20
21 Sampled Sinusoids g[n] = A e β n g[n] = A z n z = e β N 0 1 F 0 g[n] = A cos(2 π n/ N 0 + θ) m/ N 0 2 πm/ N 0 g[n] = A cos(2 π F 0 n + θ) = F 0 = 2 π F 0 g[n] = A cos(ω 0 n + θ) = Ω 0 /2 π = Ω 0 M.J. Roberts, Fundamentals of Signals and Systems 21
22 Sampling Period and Frequency g(t ) = A cos(2 π f 0 t+θ) g(nt s ) = A cos(2 π f 0 T s n+θ) g[n] = g(n T s ) F 0 = f 0 T s = f 0 / f s g[n] = A cos(2 π F 0 n + θ) g[n] = A cos(2 π F 0 n + θ) T s = 1 f s 1 T s = f s sampling period sampling frequency sampling rate M.J. Roberts, Fundamentals of Signals and Systems 22
23 Periodic Condition of a Sampled Signal 2 π F 0 n = 2 π m g(nt s ) = A cos(2 π f 0 T s n+θ) F 0 n = m Integers n, m F 0 = f 0 T s = f 0 / f s F 0 = m n F 0 = m n = f 0 f s Fundamental Frequency Sampling Frequency g[n] = A cos(2 π F 0 n + θ) Rational Number F 0 = m n M.J. Roberts, Fundamentals of Signals and Systems 23
24 Periodic Condition Examples g(t ) = A cos(2 π f 0 t+θ) g[t ] = 4 cos ( 72 π t 19 ) = 4 cos ( 2 π t ) g[n] = A cos(2 π F 0 n + θ) g[n] = 4 cos ( 72 π n 19 ) = 4 cos ( 2 π n ) T s = 1 g(t ) = 4 cos ( 2 π (t + T 0 ) ) T 0 = g[n] = 4 cos ( 2 π (n + N 0 ) ) N 0 = 19 Fundamental Period of Fundamental Period of g(t ) g[n] N 0 1 F 0 N 0 q = 1 F 0 q N 0 = F 0 M.J. Roberts, Fundamentals of Signals and Systems 24
25 Periodic Condition Examples g(t ) = 4 cos ( 2 π (t + T 0 ) ) T 0 = g[n] = 4 cos ( 2 π (n + N 0 ) ) N 0 = 19 Fundamental Period of Fundamental Period of g(t ) g[n] F 0 = = q the number of cycles in N 0 samples N the smallest integer : fundamental period 0 N 0 1 F 0 N 0 q = 1 F 0 q N 0 = F 0 M.J. Roberts, Fundamentals of Signals and Systems 25
26 Periodic Condition Examples F 0 = = q the number of cycles in N 0 samples N the smallest integer : fundamental period 0 When F 0 is not the reciprocal of an integer (q=1), a discrete-time sinusoid may not be immediately recognizable from its graph as a sinusoid. M.J. Roberts, Fundamentals of Signals and Systems 26
27 Periodic Condition Examples g[n] = 4 cos ( 2 π (n + N 0 ) ) (n + N 0 ) integer 1 19 N 0 = k integer N 0 integer N 0 = 19 Fundamental period of g[n] g(t ) = 4 cos ( 2 π (t + T 0 ) ) (t + T 0 ) integer T 0 = k integer T 0 integer T 0 = Fundamental period of g(t ) M.J. Roberts, Fundamentals of Signals and Systems 27
28 Periodic Condition Examples g[n] = 4 cos ( 2 π 1 19 n ) g[n] = 4 cos ( 2 π 2 19 n ) g[n] = 4 cos ( 2 π 3 19 n ) g[n] = 4 cos ( 2 π n ) clf n = [0:36]; t = [0:3600]/100; y1 = 4*cos(2*pi*(1/19)*n); y2 = 4*cos(2*pi*(2/19)*n); y3 = 4*cos(2*pi*(3/19)*n); y4 = 4*cos(2*pi*(36/19)*n); yt1 = 4*cos(2*pi*(1/19)*t); yt2 = 4*cos(2*pi*(2/19)*t); yt3 = 4*cos(2*pi*(3/19)*t); yt4 = 4*cos(2*pi*(36/19)*t); subplot(4,1,1); stem(n, y1); hold on; plot(t, yt1); subplot(4,1,2); stem(n, y2); hold on; plot(t, yt2); subplot(4,1,3); stem(n, y3); hold on; plot(t, yt3); subplot(4,1,4); stem(n, y4); hold on; plot(t, yt4); M.J. Roberts, Fundamentals of Signals and Systems 28
29 Periodic Condition Examples g[n] = 4 cos ( 2 π 1 19 n ) g[n] = 4 cos ( 2 π 2 19 n ) g[n] = 4 cos ( 2 π 3 19 n ) g[n] = 4 cos ( 2 π n ) N 0 = 19 T s = 1 1 cycle 2 cycles 3 cycles 36 cycles 29
30 Periodic Condition Examples g(t ) = A cos(2 π f 0 t+θ) g[n] = A cos(2 π F 0 n + θ) g 1 (t ) = 4 cos (2 π 1 t ) g 2 (t ) = 4 cos (2 π 2 t ) g 3 (t) = 4 cos (2 π 3 t ) t n T 1 t n T 2 t n T 3 g 1 [n] = 4 cos (2 π n T s1 ) g 2 [n] = 4 cos (2 π n T s 2 ) g 3 [n] = 4 cos (2 π nt s3 ) t n T 1 t n T 2 t n T 3 T 1 = 1 10 T 2 = 1 20 T 3 = 1 30 n = 0, 1, 2, 3, n = 0, 1, 2, 3, n = 0, 1, 2, 3, 1 t = 0, 0.1, 0.2, 0.3, 2 t = 0, 0.1, 0.2, 0.3, 3 t = 0, 0.1, 0.2, 0.3, { g 1 [n] } { g 2 [n] } { g 2 [n] } M.J. Roberts, Fundamentals of Signals and Systems 30
31 Periodic Condition Examples g(t ) = A cos(2 π f 0 t+θ) 2 π F 0 n = 2 π m g[n] = A cos(2 π F 0 n + θ) g[n] = 4 cos ( 72 π n 19 ) = 4 cos ( 2 π ( ) n ) n = m = m n = m n = f 0 f s smallest n = 19 = 4 cos( 2 π ( (n + N 0) ) ) smallest N 0 = 19 1/ N 0 = F F 0 0 = q N 0 = Ω 0 /2 π M.J. Roberts, Fundamentals of Signals and Systems 31
32 Periodic Condition Examples 4 cos (ω t 1 ) 4 cos (ω n 1 ) n 1 1 T s = 1 t 1 = 2t 2 n 1 = 2n 2 4 cos (2ω t 2 ) 4 cos (ω 2n 2 ) n 2 2 T s = 2 M.J. Roberts, Fundamentals of Signals and Systems 32
33 Periodic Condition Examples T s = 1 10 T s = 1 20 T s = 1 30 ω = 2π 1 ω = 2π 2 ω = 2π 3 clf n = [0:10]; t = [0:1000]/1000; y1 = 4*cos(2*pi*1*n/10); y2 = 4*cos(2*pi*2*n/20); y3 = 4*cos(2*pi*3*n/30); yt1 = 4*cos(2*pi*t); yt2 = 4*cos(2*pi*2*t); yt3 = 4*cos(2*pi*3*t); subplot(3,1,1); stem(n, y1); hold on; plot(t, yt1); subplot(3,1,2); stem(n/20, y2); hold on; plot(t, yt2); subplot(3,1,3); stem(n/30, y3); hold on; plot(t, yt3); M.J. Roberts, Fundamentals of Signals and Systems 33
34 References [1] [2] J.H. McClellan, et al., Signal Processing First, Pearson Prentice Hall, 2003 [3] M.J. Roberts, Fundamentals of Signals and Systems [4] S.J. Orfanidis, Introduction to Signal Processing [5] K. Shin, et al., Fundamentals of Signal Processing for Sound and Vibration Engineerings [6] A graphical interpretation of the DFT and FFT, by Steve Mann 34
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Copyright (c) 2016 2018 Young W. Lim. Permission is granted to copy, distribute and/or modify this document under the terms of the GNU Free Documentation License, Version 1.2 or any later version published
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Surface Integrals (6A) Surface Integral Stokes' Theorem Copright (c) 2012 Young W. Lim. Permission is granted to cop, distribute and/or modif this document under the terms of the GNU Free Documentation
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