COURSE OBJECTIVES By the end of this course, student will be able to • understand and use math models to represent basic signals and systems • understand the relationship between time an
Trang 1TON DUC THANG UNIVERSITY
FACULTY OF ELECTRICAL & ELECTRONICS
ENGINEERING
SIGNALS AND SYSTEMS
402067
Syllabus
Trang 2ACKNOWLEDGEMENT
The picture content of this slide is from Charles L Phillips, [2014],Signals, Systems, and Transforms, 5e Pearson
Trang 3COURSE OBJECTIVES
By the end of this course, student will be able to
• understand and use math models to represent basic signals and systems
• understand the relationship between time and frequency domain of basic systems’ math model
• transform signals and system models from time domain to frequency domain and vice versa
• understand the relationship between time and discrete-time models of system
Trang 4continuous-COURSE CONTENTS
• Introduce the mathematical tools for analysis signals and systems
• Provide a basis for applying the above techniques
in control and communication engineering
Trang 5COURSE CONTENTS
This course will cover the following topics:
• Continuous time signals and systems
• Fourier transform and its applications
• Linear time invariant systems
• Discrete time signals and systems
Simulation software: MATLAB
Trang 7REFERENCES
Textbook:
Charles L Phillips
Signals, Systems, and Transforms
5e Pearson Prentice Hall
Trang 8Other references please refer to the detail syllabus found in the library
Trang 9PREREQUISITE
ENGINEERING ANALYSIS - 402064
Trang 10GRADES
• 10%: writing test
• 20%: homework, quizzes, project
• 20%: midterm exam (writing test)
• 50%: final exam
(50% writing test + 50% multiple choices)
Trang 11MOODLE
ELEARNING COURSE Course key: piytg2ie
Trang 13CLASS POLICY
• MISSING 20% including classes, homework, quizzes, test will be banned from the final exam
Trang 14TON DUC THANG UNIVERSITY
FACULTY OF ELECTRICAL & ELECTRONICS
Trang 15ACKNOWLEDGEMENT
The picture content of this slide is from Charles L Phillips, [2014],Signals, Systems, and Transforms, 5e Pearson
Trang 16OUTLINE
1 Information vs signals
2 Mathematical representation of signals
3 Continuous time signals vs discrete time signals
4 Energy signals vs power signals
5 Linear systems
Trang 17OBJECTIVES
In this chapter, you will learn:
• the different between information and signals
• how to mathematical represent signals
• how to distinguish between continuous/discrete time signals, energy/power signals
• the definition of linear system, continuous/discrete time systems
Trang 181 WHAT IS A SIGNAL?
"A detectable physical quantity or impulse (as a voltage, current, or magnetic field strength) by which
messages or information can be transmitted."
"A signal is a function of independent variables that
carry some information."
"A signal is a physical quantity that varies with time, space or any other independent variable by which
information can be conveyed“
* Definitions of signal from Merrian-Webster dictionary
Trang 191 WHAT IS A SIGNAL?
Trang 202 REPRESENTING A SIGNAL
• Using mathematical model
• Signal = function of independent variables
Function of one independent variable: time
Trang 213 CONTINUOUS vs DISCRETE
TIME SIGNALS
Continuous time signals:
• Most signals in real world
Discrete time signals:
• Some signals like pixel…
• Digital signals
(sampled signals)
Trang 224 ENERGY vs POWER SIGNALS
• Energy of a signal x(t) is 𝐸𝑥 = |𝑥 𝑡 |−∞∞ 2𝑑𝑡
Signal x(t)
Energy of x(t)
Finite energy Infinite energy
x(t) is energy signal Finite power
x(t) is power signal
Trang 23ENERGY vs POWER SIGNALS
• Power of a signal x(t) is 𝑃𝑥 = lim
𝑇→∞
1 2𝑇 |𝑥 𝑡 |−𝑇𝑇 2𝑑𝑡
For periodic signal: 𝑃𝑥 = 1
𝑇 |𝑥 𝑡 |0𝑇 2𝑑𝑡
A signal can be a power signal, or an energy signal, or neither, but not both
Trang 24RECOGNIZING ENERGY vs POWER SIGNALS
Energy signals:
• Aperiodic and truncated
Trang 25RECOGNIZING ENERGY vs POWER SIGNALS
Energy signals:
• Approach zero asymptotically as t ∞
Trang 26RECOGNIZING ENERGY vs POWER SIGNALS
-1
Trang 27input (IP) and output (OP)
Trang 28WHAT IS A LINEAR SYSTEM?
• Linear system: mathematical model of the system is based on linear operators
• Which operator is linear?
is linear if with
Trang 29CONTINOUS-TIME SYSTEM
A continuous time system is one in which no sampled signals appear
Trang 30CONTINOUS-TIME SYSTEM
PROPERTIES
• Memory: OP y(t0) IP values other than x(t0)
• Invertibility: distinct IPs result in distinct OPs
Inverse of a system T is Ti
• Causality: OP at any time t0 IP only for t t0
All physical systems are causal
Trang 32DISCRETE-TIME SYSTEM
A discrete-time system operates on a time signal (IP signal) to produce another discrete-time signal (OP signal or response)
Trang 34SUMMARY
In this chapter, you have learned:
• the fundamentals of signal and how to mathematical represent signals
• the difference between continuous/discrete time signals, energy/power signals
• the definition of linear system, continuous/discrete time systems and their properties
Trang 35MATLAB TUTORIAL 1
MATLAB computing:
• Signals described in Math form
Trang 36HOMEWORK
• N/A
Trang 37PREP FOR NEXT TIME
[1] Chapter 2: Continuous-time signals and systems Section 2.1 to 2.7
Refer to the syllabus for more reading on references
Trang 38TON DUC THANG UNIVERSITY
FACULTY OF ELECTRICAL & ELECTRONICS
ENGINEERING
SIGNALS AND SYSTEMS
402067
Continuous-Time Signals & Systems
Trang 39ACKNOWLEDGEMENT
The picture content of this slide is from Charles L Phillips, [2014],Signals, Systems, and Transforms, 5e Pearson
Trang 40OUTLINE
1 Signal characteristics
2 Basic signal operations
3 Common signals in engineering
4 Continuous-time systems
Trang 41OBJECTIVES
In this chapter, you will learn:
• characteristics of signal
• basic operations on signal
• common signals that are used in engineering
• continuous-time systems and their properties
Trang 43SIGNAL CHARACTERISTICS
INTEGRAL
• Finite duration signal 𝑥(𝑡)
• Infinite duration signal 𝑥(𝑡)
Trang 44SIGNAL CHARACTERISTICS
AVERAGE
• Finite duration signal 𝑥(𝑡)
• Infinite duration signal 𝑥(𝑡)
Trang 45SIGNAL CHARACTERISTICS
ENERGY
• Finite duration signal 𝑥(𝑡)
• Infinite duration signal 𝑥(𝑡)
Recall: Energy signal:
Trang 46SIGNAL CHARACTERISTICS
AVERAGE POWER
• Finite duration signal 𝑥(𝑡)
• Infinite duration signal 𝑥(𝑡)
Trang 472 BASIC SIGNAL OPERATIONS
Trang 48BASIC SIGNAL OPERATIONS
AMPLITUDE SCALING
𝐴𝑥(𝑡): affecting the amplitude of the signal
• 0<A<1: Vertically squeezed
• A>1: Vertically expanded
• A<0: Vertically squeezed or expanded & inverted
Trang 49BASIC SIGNAL OPERATIONS
AMPLITUDE SHIFTING
𝐴 + 𝑥(𝑡): adding DC component to the signal
• A>0: Vertically move the signal up A units
• A<0: Vertically move the signal down A units
DIY: Sketch the following signals:
3 sin(1000 )
3 sin(1000 )
t t
Trang 50BASIC SIGNAL OPERATIONS
TIME SCALING
𝑥(A𝑡): time scaling by a factor of A
• If 0<A<1: signal is wider
• A>1: signal is squeezed
• A<0: squeezed or expanded and reflected
x(0.5t) x(2t)
-2 2 -1 1 -4 4
x(t)
x(-0.5t) x(t)
Trang 51BASIC SIGNAL OPERATIONS
TIME SHIFTING
𝑥(𝑡 - 𝑡0): shifting signal 𝑥(𝑡) by 𝑡0 to the right
Why to the right?
Trang 52BASIC SIGNAL OPERATIONS
Trang 53BASIC SIGNAL OPERATIONS
Trang 54BASIC SIGNAL OPERATIONS
COMPONENT ANALYZING
• Even signal:
if for any time t, we have 𝑥(−𝑡) = 𝑥(𝑡)
(has mirror symmetry w.r.t the vertical axis)
• Odd signal:
if for any time t, we have 𝑥 −𝑡 = −𝑥(𝑡)
(has mirror symmetry w.r.t the origin)
Note: (even function) (even function) = even function
(even function) (odd function) = odd function (odd function) (odd function) = even function
Trang 55BASIC SIGNAL OPERATIONS
Trang 56• Follows will be some common signals used in engineering
3 COMMON SIGNALS IN
ENGINEERING
Trang 57𝑥 𝑡 = 𝑎
Signal has constant value at all time
Practical example: DC voltage / current source
COMMON SIGNALS IN ENGINEERING
CONSTANT, DC SIGNAL
a
Trang 60Unit impulse function is related to Unit step function
Trang 61Also called Dirac delta function
Properties of unit impulse function:
COMMON SIGNALS IN ENGINEERING
CONSTANT, DC SIGNAL
Trang 62Properties of unit impulse function:
COMMON SIGNALS IN ENGINEERING
CONSTANT, DC SIGNAL
Trang 63COMMON SIGNALS IN ENGINEERING
SINUSOID
𝑥 𝑡 = 𝐴𝑐𝑜𝑠 𝑤0𝑡 + 𝜑 = 𝐴𝑐𝑜𝑠 2𝜋𝑓0𝑡 + 𝜑
A: amplitude or maximum value
𝑤0: mathematical frequency (rad/sec)
𝑓0: real or natural frequency (Hz)
𝜑: phase angle (rad)
T: period of the signal (sec)
AC signal is one-sided: V(t)= 𝐴𝑐𝑜𝑠 𝑤0𝑡 + 𝜑 𝑢 𝑡
Trang 64𝑥 𝑡 = 𝐶𝑒𝑎𝑡
Case 1: C and a are real
a>0: growing function a<0: decaying function
C is the y-intercept
COMMON SIGNALS IN ENGINEERING
EXPONENTIAL SIGNAL
Trang 65Case 2: C is complex and a is imaginary
Trang 66Case 3: C and a are complex
C = A𝑒𝑗∅ and a = 𝜎0 + j𝑤0
𝑥 𝑡 = 𝐶 𝑒𝑎𝑡 = 𝐴𝑒𝑗∅𝑒(𝜎0 +𝑗𝑤0) 𝑡 = 𝐴𝑒𝜎0 𝑡 𝑒𝑗(∅+𝑤0 𝑡)
= 𝐴𝑒𝜎0 𝑡 𝑐𝑜𝑠 ∅ + 𝑤0𝑡 + 𝑗𝐴𝑒𝜎0 𝑡 𝑠𝑖𝑛(∅ + 𝑤0𝑡)
Plot of the real part:
COMMON SIGNALS IN ENGINEERING
EXPONENTIAL SIGNAL
𝜎0 < 0
𝜎0 > 0
Trang 67Use rectangular function to represent a pulse:
𝑝 𝑡 = 𝐴 (𝑡 − 𝑐
𝑤 )
with c is center of the pulse
w is width of the pulse
A is height of the pulse
COMMON SIGNALS IN ENGINEERING
PULSE SIGNAL
c
w
A
Trang 68𝑥 𝑡 = 𝐴 ∧ (𝑡−𝑐
𝑊/2)
where A: height of the triangle signal
c: center of the triangle signal
W: width of the base
COMMON SIGNALS IN ENGINEERING
TRIANGLE SIGNAL
c
A
Trang 704 CONTINUOUS TIME SYSTEM
Recall: A general system
( ) [ ( )]
y t T x t
Trang 71CONTINUOUS TIME SYSTEM
INTERCONNECTING SYSTEM
Block diagram elements
Trang 72CONTINUOUS TIME SYSTEM
INTERCONNECTING SYSTEM
Basic connections of system
Trang 73CONTINUOUS TIME SYSTEM
FEEDBACK SYSTEM
Feedback control system
Trang 74CONTINUOUS TIME SYSTEM
Trang 76Recall:
• Time invariant system: time shift in input signal
results in the same time shift in the output signal
Example: Test for time invariance
CONTINUOUS TIME SYSTEM
TIME INVARIANCE
y t t T x t t
Trang 77CONTINUOUS TIME SYSTEM
STABILITY
Recall:
• BIBO Stability: a system is stable if the OP remains bounded for any bounded IP
Def: a signal x(t) is bounded if there exists a number
M such that 𝑥 𝑡 ≤ 𝑀 for all t
Trang 78SUMMARY
In this chapter, you have learned:
• the characteristics of signal
• the basic operations of signal
• the common signals in engineering
• the basic properties of continuous time systems
Trang 79MATLAB TUTORIAL 2
MATLAB computing:
• Elementary signals
Pages 1-2 to 1-25
Trang 80HOMEWORK
[1] page 102 to 113
2.1, 2.3, 2.4, 2.5, 2.6, 2.10, 2.11, 2.12, 2.14, 2,15, 2.16, 2.17, 2.18, 2.19, 2.20, 2.23, 2.24, 2.25, 2.26, 2.27, 2.30, 2.32, 2.34, 2.35
Trang 81PREP FOR NEXT TIME
[1] Chapter 4: Fourier Series
Trang 82TON DUC THANG UNIVERSITY
FACULTY OF ELECTRICAL & ELECTRONICS
Trang 83ACKNOWLEDGEMENT
The picture content of this slide is from Charles L Phillips, [2014],Signals, Systems, and Transforms, 5e Pearson
Trang 84OUTLINE
1 Fourier series
2 Convolution
3 Fourier transform of aperiodic signals
4 Fourier transform of periodic signals
Trang 85OBJECTIVES
In this chapter, you will learn:
• how to approximate periodic functions
• Fourier series and frequency spectra
• Convolution
• Fourier transform of different types of signals
Trang 861 HISTORY OF FOURIER SERIES
To predict astronomical
events, the idea of using
trigonometric sums was
Euler studied vibrating
strings
Fourier showed that periodic signals can be represented as the integrals of sinusoids that are not all harmonically related
Trang 87PERIODIC SIGNALS & FOURIER SERIES
• 𝑥(𝑡) is a periodic signal if 𝑥 𝑡 = 𝑥 𝑡 + 𝑇
Where T is the fundamental period
𝑤0 = 2𝜋𝑇 is the fundamental frequency
• Fourier series is of the form:
Trang 88PERIODIC SIGNALS & FOURIER SERIES
• Fourier series is of the form:
Trang 89• Forms of the Fourier series
PERIODIC SIGNALS & FOURIER SERIES
Trang 90FOURIER SERIES & FREQ SPECTRA
Example: Find Fourier series of a square wave
A method of displaying frequency content of a periodic signal is plotting the Fourier coefficients C k
Trang 91FOURIER SERIES & FREQ SPECTRA
Frequency content:
Trang 92PROPERTIES OF FOURIER SERIES
Assume 𝑥𝑝(𝑡) ↔ *𝐶𝑛+ and 𝑦𝑝(𝑡) ↔ *𝐷𝑛+ then
• Linearity: 𝐴𝑥𝑝 𝑡 + 𝐵𝑦𝑝 𝑡 ↔ 𝐴𝐶𝑛 + 𝐵𝐷𝑛
• Multiplication: 𝑥𝑝 𝑡 𝑦𝑝 𝑡 ↔ * ∞𝑘=−∞ 𝐶𝑘𝐷𝑛−𝑘+
• Time shifting: 𝑥𝑝 𝑡 − 𝜏 ↔ *𝐶𝑛𝑒−𝑗2𝜋𝑛𝑓𝑜 𝜏+
Trang 93PROPERTIES OF FOURIER SERIES
Assume 𝑥𝑝(𝑡) ↔ *𝐶𝑛+ and 𝑦𝑝(𝑡) ↔ *𝐷𝑛+ then
Trang 942 CONVOLUTION
• A function derived from two given functions by
integration
• Convolution expresses how the shape of one
function is modified by the other
• Convolution of functions 𝑥1 𝑡 and 𝑥2 𝑡 is 𝑥(𝑡)
defined as
𝑥 𝑡 ≝ 𝑥1 𝑡 ∗ 𝑥2 𝑡 = 𝑥∞ 1 𝑡 − 𝜏 𝑥2 𝜏 𝑑𝜏
−∞
Trang 95CONVOLUTION
Wikipedia: Convolution Wikimedia Foundation, Inc 22 July 2015 Web 13 May 2016
<https://en.wikipedia.org/wiki/Convolution>
Trang 993 FOURIER TRANSFORM
Example:
Find the Fourier transform of 𝑥 𝑡 = 𝑒−𝑎𝑡𝑢 𝑡 with
𝑎 > 0 , the magnitude spectrum and the phase spectrum?
• Fourier transform (frequency spectrum) of 𝑥(𝑡)
• Magnitude spectrum:
• Phase spectrum:
0
1 ( )w a t j t w t
Trang 103PROPERTIES OF F TRANSFORM
Assume then
• Frequency shifting:
• Multiplying by a sinusoid:
• Differentiation in frequency domain
• Differentiation in time domain
𝑥(𝑡) ↔ 𝑋(𝜔) and y(𝑡) ↔ Y(𝜔)
Trang 104PROPERTIES OF F TRANSFORM
Example:
• Find the frequency spectrum of
• Find the time function of signal 𝑥(𝑡) that has
frequency spectrum as follow:
𝑥(𝑡) = 𝑡 2 𝛱(𝑡 − 1
4 )
X(w) A
Trang 105PROPERTIES OF F TRANSFORM
Assume then
• Duality:
• Multiplication in time domain:
• Convolution in time domain:
𝑥 𝜏 𝑑𝜏 ↔ 1
𝑗𝜔
𝑡
𝑋(𝜔) + 𝜋𝑋(0)𝛿(𝜔)
Trang 1074 FOURIER TRANSFORM OF
PERIODIC FUNCTIONS
Recall:
• Periodic function of time 𝑥(𝑡) can be represented
by its Fourier series
with
• Take Fourier transform on both sides, we have
𝑥(𝑡) = 𝐶𝑛𝑒𝑗𝑛𝜔0 𝑡
∞ 𝑛=−∞
= 2𝜋 𝐶𝑛𝛿(𝜔 − 𝑛𝜔0)
∞ 𝑛=−∞
Trang 108• Periodic function can also be represented using
∞
𝛿 𝜔 − 𝑛𝜔0
4 FOURIER TRANSFORM OF
PERIODIC FUNCTIONS
Trang 109Example: Find the frequency spectrum of 𝑓(𝑡)
4 FOURIER TRANSFORM OF
PERIODIC FUNCTIONS
Trang 110APPLICATION OF F TRANSFORM
• Fourier transform are used in finding the frequency response of linear systems and the frequency
spectra of signals
• Finding the frequency response of linear systems
will be covered in the next chapters
Trang 111ENERGY AND POWER DENSITY SPECTRA
• Energy/Power spectral density functions are used
to determine the energy/power distribution of an energy/power signal, in the frequency spectrum
• Energy density spectrum of signal 𝑥(𝑡):
Then energy of signal 𝑥(𝑡) is
+∞
−∞
Trang 112• Power density spectrum of periodic signal 𝑥(𝑡):
with
Recall: spectrum of periodic signal x(t) is
Then power of signal 𝑥(𝑡) is
Trang 113SUMMARY
In this chapter, you have learned:
• how to represent periodic signals using Fourier series
• Fourier transform and frequency spectrum of various types of signal
• properties of frequency spectrum of signals and how to manipulate signals in frequency domain
Trang 116PREP FOR NEXT TIME
[1] Chapter 3: Continuous-Time Linear Time-Invariant Systems
Section 3.1 to 3.6
Refer to the syllabus for more reading on references
Trang 117TON DUC THANG UNIVERSITY
FACULTY OF ELECTRICAL & ELECTRONICS
Trang 118ACKNOWLEDGEMENT
The picture content of this slide is from Charles L Phillips, [2014],Signals, Systems, and Transforms, 5e Pearson
Trang 119OUTLINE
1 Linear time-invariant (LTI) systems
2 Impulse response of LTI systems
3 Recall of Convolution
4 Frequency response of LTI systems