q Chapter 2 Signals and Spectra This chapter

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q Chapter 2. Signals and Spectra Ø This chapter reviews one of the two

q Chapter 2. Signals and Spectra Ø This chapter reviews one of the two pre-requisites for communications research. v. Signals and Systems v. Probability, Random Variables, and Random Processes Ø We use linear, particularly LTI, systems to develop theory for communications. Ø Outline v 2. 1 Line Spectra and Fourier Series v 2. 2 Fourier Transform and Continuous Spectra v 2. 3 Time and Frequency Relations v 2. 4 Convolution v 2. 5 Impulses and Transforms in the Limit v 2. 6 Discrete Time Signals and the Discrete Fourier Transform 1

o Communication Engineering 통신공학 Step 1. Given a communication medium, we first analyze the

o Communication Engineering 통신공학 Step 1. Given a communication medium, we first analyze the channel and build a mathematical model. 주어진 통신 매체에 따라 Channel 을 분석하고 모형을 만든다. Step 2. Using the model, we design the pair of a transmitter and a receiver that best exploits the channel characteristic. Channel 에 가장 효과적 신호처리를 할 수 있도록 Transmitter 와 Receiver를 설계한다. ex) Modulation (변조)과 Demodulation (복조) Encoding 과 Decoding Multiplexing 과 Demultiplexing 2

o Mathematical Tool for Signal Processing: Fourier Analysis time domain frequency domain analysis, synthesis,

o Mathematical Tool for Signal Processing: Fourier Analysis time domain frequency domain analysis, synthesis, design q 2. 1 Line Spectra and Fourier Series o Linear Time-Invariant system 3

 Line spectrum of periodic signals Amplitude A phase 복소지수 (Complex exponential)에 의한 sinusoidal

Line spectrum of periodic signals Amplitude A phase 복소지수 (Complex exponential)에 의한 sinusoidal wave정현파 신호 의 표현 복소수? Euler’s theorem/identity 6

 Phasor를 이용한 정현파 신호의 표현 허수축 실수축 Phasor representation is useful when sinusoidal

Phasor를 이용한 정현파 신호의 표현 허수축 실수축 Phasor representation is useful when sinusoidal signal is processed by real-in real-out LTI systems. 8

A 1 Line Spectrum Phase Amplitude 90 5 3 0 10 40 2 0

A 1 Line Spectrum Phase Amplitude 90 5 3 0 10 40 2 0 35 10 35 Frequency content “왜 Phase는 Amplitude보다 덜 중요한가? (phase time delay ) “모든 주기적 신호는 정현파 신호의 선형적 결합으로 표현될 수 있다. ” 10

o Periodic Signals (주기 신호) Rectangular pulse train Figure 2. 1 -7 11

o Periodic Signals (주기 신호) Rectangular pulse train Figure 2. 1 -7 11

o Fourier Series 어떠한 periodic signal 정현파 신호의 선형적 집합 Where Phasor표현 two-sided line

o Fourier Series 어떠한 periodic signal 정현파 신호의 선형적 집합 Where Phasor표현 two-sided line spectrum 12

주기함수의 주파수 특성 (Spectrum of periodic signals) 1. harmonics of fundamental frequency . 2.

주기함수의 주파수 특성 (Spectrum of periodic signals) 1. harmonics of fundamental frequency . 2. 3. 실함수 는 13

Spectrum of rectangular pulse train with ƒ 0 = 1/4 (a) Amplitude (b) Phase

Spectrum of rectangular pulse train with ƒ 0 = 1/4 (a) Amplitude (b) Phase Figure 2. 1 -8 14

trigonometric Fourier series for real signals 매우 중요한 함수 15

trigonometric Fourier series for real signals 매우 중요한 함수 15

Fourier-series reconstruction of a rectangular pulse train Figure 2. 1 -9 16

Fourier-series reconstruction of a rectangular pulse train Figure 2. 1 -9 16

Fourier-series reconstruction of a rectangular pulse train Figure 2. 1 -9 c 17

Fourier-series reconstruction of a rectangular pulse train Figure 2. 1 -9 c 17

Gibbs phenomenon at a step discontinuity Figure 2. 1 -10 18

Gibbs phenomenon at a step discontinuity Figure 2. 1 -10 18

Average Power of Periodic Signal 19

Average Power of Periodic Signal 19

Ø Parseval’s Power Theorem 20

Ø Parseval’s Power Theorem 20

q 2. 2 Fourier Transforms and Continuous Spectra Ø Fourier Transform 비주기 신호 or

q 2. 2 Fourier Transforms and Continuous Spectra Ø Fourier Transform 비주기 신호 or Energy signal Definition called the analysis equation. 21

Ø Inverse Fourier Transform called the synthesis equation. 22

Ø Inverse Fourier Transform called the synthesis equation. 22

Ex 1 Rectangular pulse 23

Ex 1 Rectangular pulse 23

Rectangular pulse spectrum V(ƒ) = A sinc ƒ Figure 2. 2 -2 24

Rectangular pulse spectrum V(ƒ) = A sinc ƒ Figure 2. 2 -2 24

Ø Rayleigh’s Energy Theorem Generally Also called Parseval’s relation/theorem. 25

Ø Rayleigh’s Energy Theorem Generally Also called Parseval’s relation/theorem. 25

Ø Duality Theorem 26

Ø Duality Theorem 26

q 2. 3 Time and Frequency Relations Ø Superposition Property useful tool for linear

q 2. 3 Time and Frequency Relations Ø Superposition Property useful tool for linear systems Ø Time Delay linear phase Ø Time Scale Change Slow Playback Fast Playback Low Tone High Tone 27

Ø Frequency Translation/Shift and Modulation 28

Ø Frequency Translation/Shift and Modulation 28

continued (a) RF pulse (b) Amplitude spectrum Figure 2. 3 -3 29

continued (a) RF pulse (b) Amplitude spectrum Figure 2. 3 -3 29

Ø Differentiation and Integration Principle of FM demodulator differentiator In general Example. Triangular pulse

Ø Differentiation and Integration Principle of FM demodulator differentiator In general Example. Triangular pulse 30

q 2. 4 Convolution Ø Convolution Integral Graphical interpretation of convolution Figure 2. 4

q 2. 4 Convolution Ø Convolution Integral Graphical interpretation of convolution Figure 2. 4 -1 31

Result of the convolution in Fig. 2. 4 -1 Figure 2. 4 -2 In

Result of the convolution in Fig. 2. 4 -1 Figure 2. 4 -2 In general, convolution is a complicated operation in the TD. 32

Ø Convolution Theorems 33

Ø Convolution Theorems 33

q 2. 5 Impulses and Transforms in the Limit Ø Dirac delta function Thus

q 2. 5 Impulses and Transforms in the Limit Ø Dirac delta function Thus 34

Two functions that become impulses as 0 Figure 2. 5 -2 35

Two functions that become impulses as 0 Figure 2. 5 -2 35

Properties 36

Properties 36

Ø 실제적 함수 (Practical Impulses) 37

Ø 실제적 함수 (Practical Impulses) 37

Ø Fourier Transform of Power Signals infinite energy 38

Ø Fourier Transform of Power Signals infinite energy 38

Ø From Fourier Series , Other periodic signals 39

Ø From Fourier Series , Other periodic signals 39

q 2. 6 Discrete Time Signals and Discrete Fourier Transform Ø DT signal Ø

q 2. 6 Discrete Time Signals and Discrete Fourier Transform Ø DT signal Ø DT periodic signal and DFTS v. Analysis equation v. Synthesis equation Ø DFT, IDFT v. Periodic extension and Fourier Series Ø DTFT v. Analysis equation v. Synthesis equation 40

Ø Convolution using the DFT v. Q. We are given a convolution sum of

Ø Convolution using the DFT v. Q. We are given a convolution sum of two finite-length DT signals. Each signal has support N_1, N_2. Find the finitelength (at most N_1+N_2 -1) output of the convolution using DFT. v. A. Choose N>= N_1+N_2 -1. Compute DFT(x) and DFT(h). Perform entry-by-entry multiplication. Apply the inverse DFT. Done. 41

q HW #1 (Due on Next Tuesday 9/22. Please turn in handwritten solutions. )

q HW #1 (Due on Next Tuesday 9/22. Please turn in handwritten solutions. ) Ø 2. 7 Questions v 3 v 4 v 6 v 2. 1 -9, 13 v 2. 2 -7, 10 v 2. 3 -8, 14 v 2. 4 -8, 15 v 2. 5 -10 v 2. 6 -4, 6 42