Figure 1.1 (a) Model of a communication system, and (b) signal processing functions.

Similar documents
Figure 3.1 Effect on frequency spectrum of increasing period T 0. Consider the amplitude spectrum of a periodic waveform as shown in Figure 3.2.

ω 0 = 2π/T 0 is called the fundamental angular frequency and ω 2 = 2ω 0 is called the

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

Frequency Response. Re ve jφ e jωt ( ) where v is the amplitude and φ is the phase of the sinusoidal signal v(t). ve jφ

LOPE3202: Communication Systems 10/18/2017 2

ECEN 420 LINEAR CONTROL SYSTEMS. Lecture 2 Laplace Transform I 1/52

Review of Fourier Transform

Lecture 1 Signals. notation and meaning. common signals. size of a signal. qualitative properties of signals. impulsive signals

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

MATHEMATICAL TOOLS FOR DIGITAL TRANSMISSION ANALYSIS

12. Introduction and Chapter Objectives

06/12/ rws/jMc- modif SuFY10 (MPF) - Textbook Section IX 1

Figure 1 A linear, time-invariant circuit. It s important to us that the circuit is both linear and time-invariant. To see why, let s us the notation

EA2.3 - Electronics 2 1

ELECTRONICS & COMMUNICATIONS DIGITAL COMMUNICATIONS

Circuit Analysis-III. Circuit Analysis-II Lecture # 3 Friday 06 th April, 18

Module 4. Signal Representation and Baseband Processing. Version 2 ECE IIT, Kharagpur

EE 230 Lecture 40. Data Converters. Amplitude Quantization. Quantization Noise

Direct-Sequence Spread-Spectrum

Digital Band-pass Modulation PROF. MICHAEL TSAI 2011/11/10

Review of Linear Time-Invariant Network Analysis

Chapter 1 Fundamental Concepts

Lecture 11 - AC Power

Three Phase Circuits

Sinusoidal Steady State Analysis (AC Analysis) Part II

PCM Reference Chapter 12.1, Communication Systems, Carlson. PCM.1

FBMC/OQAM transceivers for 5G mobile communication systems. François Rottenberg

Chapter 1 Fundamental Concepts

Chapter 10 Applications in Communications

1. SINGULARITY FUNCTIONS

A First Course in Digital Communications

Refresher course on Electrical fundamentals (Basics of A.C. Circuits) by B.M.Vyas

Module 4. Single-phase AC Circuits

Aspects of Continuous- and Discrete-Time Signals and Systems

Chapter 2: The Fourier Transform

Signal types. Signal characteristics: RMS, power, db Probability Density Function (PDF). Analogue-to-Digital Conversion (ADC).

Communication Signals (Haykin Sec. 2.4 and Ziemer Sec Sec. 2.4) KECE321 Communication Systems I

Laplace Transform Part 1: Introduction (I&N Chap 13)

2.161 Signal Processing: Continuous and Discrete Fall 2008

Sensors. Chapter Signal Conditioning

Chapter 7. Digital Control Systems

Signals and Systems Lecture Notes

EE 224 Signals and Systems I Review 1/10

8 PAM BER/SER Monte Carlo Simulation

Solutions to Problems in Chapter 4

System Identification & Parameter Estimation

NETWORK ANALYSIS WITH APPLICATIONS

Chapter 33. Alternating Current Circuits

Analog Digital Sampling & Discrete Time Discrete Values & Noise Digital-to-Analog Conversion Analog-to-Digital Conversion

3.2 Complex Sinusoids and Frequency Response of LTI Systems

Correlator I. Basics. Chapter Introduction. 8.2 Digitization Sampling. D. Anish Roshi

Fourier Transform for Continuous Functions

Fourier series. XE31EO2 - Pavel Máša. Electrical Circuits 2 Lecture1. XE31EO2 - Pavel Máša - Fourier Series

GATE EE Topic wise Questions SIGNALS & SYSTEMS

2.161 Signal Processing: Continuous and Discrete Fall 2008

Fourier Series and Transforms. Revision Lecture

EE538 Final Exam Fall :20 pm -5:20 pm PHYS 223 Dec. 17, Cover Sheet

The (Fast) Fourier Transform

CHAPTER 14. Based on the info about the scattering function we know that the multipath spread is T m =1ms, and the Doppler spread is B d =0.2 Hz.

CT Rectangular Function Pairs (5B)

Communication Theory Summary of Important Definitions and Results

Fourier Series. Spectral Analysis of Periodic Signals

EE (082) Ch. II: Intro. to Signals Lecture 2 Dr. Wajih Abu-Al-Saud

EE221 - Practice for the Midterm Exam

Chapter 5 Steady-State Sinusoidal Analysis

11. AC Circuit Power Analysis

Advanced Analog Building Blocks. Prof. Dr. Peter Fischer, Dr. Wei Shen, Dr. Albert Comerma, Dr. Johannes Schemmel, etc

Cast of Characters. Some Symbols, Functions, and Variables Used in the Book

Digital Modulation 1

April 24, 2012 (Tue) Lecture 19: Impulse Function and its Laplace Transform ( 6.5)

Basic Electronics. Introductory Lecture Course for. Technology and Instrumentation in Particle Physics Chicago, Illinois June 9-14, 2011

Chapter 3 Convolution Representation

Radar Systems Engineering Lecture 3 Review of Signals, Systems and Digital Signal Processing

Frequency Dependent Aspects of Op-amps

SIGNAL PROCESSING. B14 Option 4 lectures. Stephen Roberts

ECE 3084 QUIZ 2 SCHOOL OF ELECTRICAL AND COMPUTER ENGINEERING GEORGIA INSTITUTE OF TECHNOLOGY APRIL 2, Name:

Representation of Signals and Systems. Lecturer: David Shiung

EE/ME/AE324: Dynamical Systems. Chapter 7: Transform Solutions of Linear Models

8.1 Circuit Parameters

Pulse-Code Modulation (PCM) :

DESIGN OF CMOS ANALOG INTEGRATED CIRCUITS

ECE Circuit Theory. Final Examination. December 5, 2008

6.02 Fall 2012 Lecture #10

Signals and Spectra (1A) Young Won Lim 11/26/12

Chapter 5 Frequency Domain Analysis of Systems

3F1 Random Processes Examples Paper (for all 6 lectures)

Fourier Analysis and Power Spectral Density

Ver 3808 E1.10 Fourier Series and Transforms (2014) E1.10 Fourier Series and Transforms. Problem Sheet 1 (Lecture 1)

X b s t w t t dt b E ( ) t dt

Module 4. Single-phase AC Circuits. Version 2 EE IIT, Kharagpur 1

E2.5 Signals & Linear Systems. Tutorial Sheet 1 Introduction to Signals & Systems (Lectures 1 & 2)

University Question Paper Solution

Signals & Systems. Lecture 5 Continuous-Time Fourier Transform. Alp Ertürk

Generalized sources (Sect. 6.5). The Dirac delta generalized function. Definition Consider the sequence of functions for n 1, Remarks:

Chapter 5 Frequency Domain Analysis of Systems

2A1H Time-Frequency Analysis II

LTI Systems (Continuous & Discrete) - Basics

LECTURE 12 Sections Introduction to the Fourier series of periodic signals

Modeling Buck Converter by Using Fourier Analysis

EEE 188: Digital Control Systems

Transcription:

. Introduction to Signals and Operations Model of a Communication System [] Figure. (a) Model of a communication system, and (b) signal processing functions. Classification of Signals. Continuous-time and discrete-time signals [2] By the term continuous-time signal we mean a real or complex function of time s(t), where the independent variable t is continuous. If t is a discrete variable, i.e., s(t) is defined at discrete times, then the signal s(t) is a discrete-time signal. A discrete-time signal is often identified as a sequence of numbers, denoted by {s(n)}, where n is an integer. 2. Analogue and digital signals [2] If a continuous-time signal s(t) can take on any values in a continuous time interval, then s(t) is called an analogue signal. If a discrete-time signal can take on only a finite number of distinct values, {s(n)}, then the signal is called a digital signal. 3. Deterministic and random signals [2] Deterministic signals are those signals whose values are completely specified for any given time. Random signals are those signals that take random values at any given times. 4. Periodic and nonperiodic signals [2] A signal s(t) is a periodic signal if s(t) = s(t + n 0 ), where 0 is called the period and the integer n > 0. If s(t) s(t + 0 ) for all t and any 0, then s(t) is a nonperiodic or aperiodic signal..

5. Power and energy signals [2, 3] A complex signal s(t) is a power signal if the average normalised power P is finite, where /2 0 < P = lim s(t)s*(t)dt < (.) /2 and s*(t) is the complex conjugate of s(t). A complex signal s(t) is an energy signal if the normalised energy E is finite, where 0 < E = s(t)s*(t) dt = s(t) 2 dt < (.2) In communication systems, the received waveform is usually categorised into the desired part, containing the information signal, and the undesired part, called noise. Some Useful Functions. Unit impulse function [2] he unit impulse function, also known as the dirac delta function, δ(t), is defined by s(t) δ(t) dt = s(0) (.3) An alternative definition [4] is δ(t) dt = (.4a) and δ(t) =, t = 0 0, t 0 (.4b).2

Figure.2 Unit impulse function. 2. Unit step function [2] he unit step function u(t) is u(t) =, t > 0 0, t < 0 (.5) Figure.3 Unit step function. and the unit step function is related to the unit impulse function by u(t) = t δ(τ) dτ (.6) and du (t ) dt = δ(t) (.7) 3. Sampling function [4] A sampling function is denoted by Sa(x) = sin x x (.8) Figure.4 Sampling function. 4. Sinc function [4] A sinc function is denoted by sinc x = sin π x π x (.9) Hence, Sa(x) = sinc x ( π ) (.0).3

5. Rectangular function [4] A single rectangular pulse is denoted by Π( t )=, t 2 0, t > 2 (.) 6. riangular function [4] A triangular function is denoted by Λ( t )= t, t 0, t > (.2) Some Useful Operations [4]. ime average he time average operator is given by /2 <[.]> = lim [.]dt (.3) /2 If a waveform is periodic, the time average operator can be reduced to <[.]> = a + /2 0 [.]dt (.4) 0a /2 0 where 0 is the period of the waveform and a is an arbitrary real constant, which may be taken to be zero. Equation (.4) readily follows from (.3) because, referring to (.3), integrals over successive time intervals 0 seconds wide have identical area if the waveform is periodic. As these integrals are summed, the total area and are proportionally larger, resulting in a value for the time average that is the same as just integrating over one period and dividing by 0. In summary, (.3) may be used to evaluate the time average of any type of waveform..4

Equation (.4) is valid only for periodic waveforms. 2. Direct-current value he direct-current (dc) value of a waveform is given by /2 <s(t)> = lim s(t) dt (.5) /2 We can see that this is the time average of s(t). Over a finite interval of interest, the dc value is t 2 <s(t)> = t t s(t) dt (.6) 2 t 3. Power and energy he instantaneous power (incremental work divided by incremental time) is given by p(t) = v(t) i(t) (.7) where v(t) denotes voltage and i(t) denotes current. he average power is given by P = <p(t)> = <v(t) i(t)> (.8) he root mean square (rms) value of s(t) is given by S rms = < s 2 (t ) > (.9) If a load is resistive, the average power is given by P = <v 2 (t ) > R = <i 2 (t)>r = V 2 rms R 2 = I rms R = Vrms I rms (.20) where R is the value of the resistive load. When R = Ω, P becomes the normalised.5

power. he average normalised power of a real-valued signal s(t) is given by P = <s 2 /2 (t)> = lim s 2 (t)dt (.2) /2 he total normalised energy of a real-valued signal s(t) is given by /2 E = lim s 2 (t)dt (.22) /2 4. Decibel he decibel gain of a circuit is given by db = 0 log 0 P out P in (.23) If resistive loads are involved, (.23) can be reduced to db = 20 log V rms out 0 V rms in + 0 log R in 0 R load (.24) or db = 20 log 0 I rms out I rms in + 0 log 0 R load R in (.25) If normalised powers are used, db = 20 log V rms out 0 V rms in = 20 log I rms out 0 I rms in (.26) he decibel power level with respect to mw is given by.6

dbm = 0 log 0 actual power level in watts 0 3 (.27) he decibel power level with respect to W is given by dbw = 0 log 0 (actual power level in watts) he decibel power level with respect to a mv rms level is given by dbmv = 20 log V rms 0 0 3 (.28) 5. Complex number and phasor A complex number c is said to be a phasor if it is used to represent a sinusoidal waveform. hat is, s(t) = c cos [ω 0 t + c] = Re {c e jω 0 t } (.29) where the phasor c = c e jφ (.30) and φ = c. Other Useful Operations. Cross-correlation [5] he cross-correlation of two real-valued power waveforms s (t) and s 2 (t) is defined by /2 R (τ) = <s (t) s 2 (t+ τ)> = lim 2 s (t) s 2 (t+ τ) dt /2 (.3) If s (t) and s 2 (t) are periodic with the same period 0, then.7

R 2 (τ) = /2 0 s (t) s 2 (t+ τ) dt (.32) 0 /2 0 he cross-correlation of two real-valued energy waveforms s (t) and s 2 (t) is defined by R 2 (τ) = s (t) s 2 (t+ τ) dt (.33) Correlation is a useful operation to measure the similarity between two waveforms. o compute the correlation between waveforms, it is necessary to specify which waveform is being shifted. In general, R (τ) is not equal to R (τ), where 2 2 R 2 (τ) = <s 2 (t) s (t+ τ)>. he cross-correlation of two complex waveforms is R 2 (τ) = <s *(t) s 2 (t+ τ)>. 2. Auto-correlation [2, 4] he auto-correlation of a real-valued power waveform s (t) is defined by /2 R (τ) = <s (t) s (t+ τ)> = lim s (t) s (t+ τ) dt /2 (.34) If s (t) is periodic with fundamental period 0, then R (τ) = /2 0 s (t) s (t+ τ) dt (.35) 0 /2 0 he auto-correlation of a real-valued energy waveform s (t) is defined by R (τ) = s (t) s (t+ τ) dt (.36).8

he auto-correlation of a complex power waveform is R (τ) = <s *(t)s (t+ τ)>. 3. Convolution [4] he convolution of a waveform s (t) with a waveform s 2 (t) is given by s 3 (t) = s (t) * s 2 (t) = s (λ) s 2 (t-λ) dλ s 3 (t) = s (t) * s 2 (t) = s (λ) s 2 [-(λ-t)] dλ (.37a) (.37b) where * denotes the convolution operation. (.37b) is obtained by. ime reversal of s 2 (t) to obtain s 2 (-λ). 2. ime shifting of s 2 (-λ) to obtain s 2 [-(λ-t)]. 3. Multiplying s (λ ) and s 2 [-(λ-t)] to form the integrand s (λ) s 2 [-(λ-t)]. Example. Convolution of a rectangular waveform s (t) =, 0 < t < 0, elsewhere with an exponential waveform s 2 (t) = e -t/ u(t). Figure.5 Convolution between a rectangular waveform and an exponential waveform. References [] B. Sklar, Digital Communications, Prentice Hall, 998. [2] H. P. Hsu, Analog and Digital Communications, McGraw-Hill, 993. [3] J. D. Gibson, Modern Digital and Analog Communications, 2/e, Macmillan Publishing Company, 993. [4] L. W. Couch II, Digital and Analog Communication Systems, 5/e, Prentice Hall, 997. [5] H. aub, and D. L. Schilling, Principles of Communication Systems, 2/e, McGraw-Hill, 986..9

From other sources Source ADC Source encoder Cipher Channel encoder Multiplex Modulator Frequency spreader Multiple access... ransmitter Analogue signal Digital signals Synchroniser Channel... Receiver Sink DAC Source decoder Demodulator Decipher Channel decoder Demultiplex Frequency despreader Multiple access (a) o other destinations Essential ADC/ Source coding PCM DPCM DM Synthesis coding ransform coding Encryption Block cipher Stream cipher Channel coding Block Convolutional Synchronisation Carrier Subcarrier Symbol Frame Bit Multiplex/ Multiple access FDM/FDMA DM/DMA CDM/CDMA (b) Modem Coherent PSK Coherent FSK Coherent ASK CPM DPSK Noncoherent FSK Noncoherent ASK CPM Frequency spreading Direct sequence Frequency/ ime hopping Figure. (a) Model of a communication system, and (b) signal processing functions..0

δ ( t ) t 0 Figure.2 Unit impulse function. u ( t ) t 0 Figure.3 Unit step function. sin x x - 2π - π 0 π 2π Figure.4 Sampling function. x.

s ( λ ) - 0 2 s 2 ( λ ) - 0 2 s 2 (-( λ - t )) - 0 t 2 λ λ λ s ( t ) 3 0.63-0 2 t Figure.5 Convolution of a rectangular waveform and an exponential waveform..2