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Introduction to System Theory
Vijaya Laxmi
Dept. of EEE
BIT, Mesra
1Vijaya Laxmi, Dept. of EEE, BIT, Mesra
Course Objectives
The course enables the students :
• To outline the fundamentals of common signals, systems, and recall
the list of electrical and non-electrical components.
• To summarize different transform methods, state-space techniques
and different stability conditions of linear time-invariant systemand different stability conditions of linear time-invariant system
using Routh-Hurwitz criteria.
• To analyze the transient and steady-state performance of first order
and second order systems when subjected to different signals and
also the absolute stability using above criterion.
• Actualize the electrical, mechanical, hydraulic and thermal systems
using differential equations, transfer functions and state variables.
2Vijaya Laxmi, Dept. of EEE, BIT, Mesra
Syllabus:EE 3201 INTRODUCTION TO SYSTEM THEORY
• MODULE – I: Introduction to Signals and Systems: Definition, Basis of classification,
Representation of common signals and their properties, System modeling. (4)
• MODULE – II: Analogous System: Introduction, D Alembert's Principle, Force-voltage
and force-current analogies, Electrical analogue of mechanical, Hydraulic and thermal
systems. (5)
• MODULE – III: Fourier Transform Method: Introduction, Fourier transform pair,
Amplitude spectrum and phase spectrum of signals, Sinusoidal transfer function. (3)
• MODULE – IV: Laplace Transform Method: Introduction, Laplace transform pair, Laplace
transformation of common functions, Gate function, Step function and impulse
function, Laplace theorems shifting, initial value, final value and convolution theorems,
Inverse Laplace transform by partial fraction expansion and convolution integralInverse Laplace transform by partial fraction expansion and convolution integral
method. (12)
• MODULE – V: System Analysis: System Analysis by Laplace Transform method, System
response. Natural, forced, transient and steady state responses. Transfer function and
characteristic equation, Superposition integral, Concept of poles and zeros, Nature of
system response from poles and zeros. (6)
• MODULE – VI: System Stability: Concept of stability, Types, Necessary and sufficient
conditions, Routh-Hurwitz stability criterion, Limitations and its applications to closed
loop systems. (4)
• MODULE – VII: State-Space Concept: Introduction, Definition: State, State variable, State
vector and state space, State space representation, Derivation of State model from
transfer function, Bush form and diagonal canonical form of state model, Non-
uniqueness of state model, Derivation of transfer function from state model, Transition
matrix and its properties, Solution of time invariant state equation. (6)3Vijaya Laxmi, Dept. of EEE, BIT, Mesra
Books
• Text Books:
1. Analysis of Linear Systems – D.K.Cheng. Narosa Publishing
House, Indian Student Edition, 8th Reprint, 1994
2. Control System Engineering – Nagrath & Gopal, New Age
International Pvt. Ltd. New Delhi, 2nd Edition
3. Control System – A. Anand Kumar3. Control System – A. Anand Kumar
• Reference Books:
1. Networks and Systems – D. Roy Choudhury, New Age
International Pvt. Ltd. New Delhi
2. Signal and Systems- Haykin
3. Signal and Systems- B.P. Lathi
4. Signals and Systems - Basu & Natarajan
4Vijaya Laxmi, Dept. of EEE, BIT, Mesra
Course Outcomes
After the completion of this course, students will be able to:
• Describe characteristics of different signals and systems
• Interpret the transform domains like Laplace equations,
concept of poles and zeros, Fourier equations and time-
domain state-space techniques
• Solve mathematical model of electrical and non-electrical
components with the knowledge of system science, related
mathematics of simple engineering problems and concept ofmathematics of simple engineering problems and concept of
analogous quantities
• Relate Laplace equations, Fourier equations and time-domain
state-space techniques to solve any given linear ordinary
differential equations and analyze transient and steady-state
performance of a first order and second order linear time-
invariant system using standard test signals
• Evaluate and formulate electrical or non-electrical linear time
invariant systems for desired transient behaviour, steady state
error and stability.
5Vijaya Laxmi, Dept. of EEE, BIT, Mesra
Module I
Introduction to Signals and SystemsIntroduction to Signals and Systems
6Vijaya Laxmi, Dept. of EEE, BIT, Mesra
Objectives: Module I
• To introduce introduce common signals and systems needed
in almost all electrical and other engineering fields and
scientific disciplines as well.
• The mathematical description and representation of signals
and systems and their classification.and systems and their classification.
• Define several basic properties of signals and systems.
7Vijaya Laxmi, Dept. of EEE, BIT, Mesra
Signal
• It is a function representing a physical quantity or
variable, and typically it contains information about
the behavior or nature of the phenomenon.
• Example: In RLC circuit the signal may be the voltageExample: In RLC circuit the signal may be the voltage
across the capacitor or current flowing through the
inductor or resistor.
• Mathematically, a signal may be represented as a
function of an independent variable ‘t’ and denoted
by x(t).
8Vijaya Laxmi, Dept. of EEE, BIT, Mesra
Classification of Signals
• Continuous-time and Discrete-time Signals
• Analog and Digital Signals
• Real and Complex Signals
• Deterministic and Random Signals• Deterministic and Random Signals
• Even and odd signals
• Periodic and Nonperiodic Signals
9Vijaya Laxmi, Dept. of EEE, BIT, Mesra
Continuous-time and Discrete-time Signals
• A signal x(t) is called continuous-time signal, if t is a
continuous variable.
• A signal x(t) is called discrete-time signal, if t is a discrete
variable, i.e., x(t) is defined at discrete times, often called
sequence of numbers and denoted by x[n], where n=integer.sequence of numbers and denoted by x[n], where n=integer.
• Discrete-time signal may be also obtained by sampling a
continuous-time signal x(t) such as
       
,...,...,,,
],...[],...1[],0[
,....,...,,,
210
210
n
n
xxxx
or
nxxx
or
txtxtxtx )(][.,. nn txnxxei 
For uniform sampling,
 sn nTxnxx  ][
Where Ts is the sampling interval
10Vijaya Laxmi, Dept. of EEE, BIT, Mesra
Continuous-time signal Discrete-time signal
11Vijaya Laxmi, Dept. of EEE, BIT, Mesra
Analog and Digital Signal
• If a continuous-time signal x(t) can take on any value
in the continuous interval (a,b), where a may be -∞
and b may be +∞, then the continuous-time signal is
called analog signal.
• If the discrete-time signal x[n] can take on only a
finite number of distinct values, then it is called a
digital signal.
12Vijaya Laxmi, Dept. of EEE, BIT, Mesra
Real and Complex Signal
• A signal x(t) is a real signal, if its value is a real
number, and signal x(t) is a complex signal if its value
is a complex number.
13Vijaya Laxmi, Dept. of EEE, BIT, Mesra
Deterministic and Random Signal
• Deterministic signals are those signals, whose values
are completely specified for any given time. Thus, a
deterministic signal can be modeled by a known
function of time t.
• Random signals are those signals that take random
values at any given time and must be characterized
statistically.
14Vijaya Laxmi, Dept. of EEE, BIT, Mesra
Even and Odd signals
• A signal x(t) or x[n] is referred to as an even signal if
   
   nxnx
txtx


• A signal x(t) or x[n] is referred to as an odd signal if
   
   nxnx
txtx


15Vijaya Laxmi, Dept. of EEE, BIT, Mesra
Even signalsEven signals
Odd Signals
16Vijaya Laxmi, Dept. of EEE, BIT, Mesra
Periodic and Nonperiodic signals
• A continuous-time signal x(t) is said to be periodic with
period T, if there is a positive nonzero value of T for
which
• Any continuous-time signal which is not periodic is called
a nonperiodic (aperiodic) signal.
    tallfortxTtx 
a nonperiodic (aperiodic) signal.
• A discrete-time signal x[n] is said to be periodic with
period N, if there is a positive nonzero value of N for
which
• Any discrete-time signal which is not periodic is called a
nonperiodic (aperiodic) signal.
    nallfornxNnx 
17Vijaya Laxmi, Dept. of EEE, BIT, Mesra
Periodic Signals
18Vijaya Laxmi, Dept. of EEE, BIT, Mesra
Basic continuous-time signals
• Unit step function
• Ramp function
• Unit impulse function
• Complex exponential signals• Complex exponential signals
• Real exponential signals
• Sinusoidal signals
19Vijaya Laxmi, Dept. of EEE, BIT, Mesra
Unit step function
• The unit step function u(t) is defined as
• It is discontinuous at t=0.






00
01
)(
t
t
tu
• It is discontinuous at t=0.
• The shifted unit step function u(t-t0) is defined as






0
0
0
0
1
)(
tt
tt
ttu
20Vijaya Laxmi, Dept. of EEE, BIT, Mesra
Gate function
• It can be written as sum of two step functions.
     tftftf      
   
   
      btUatUKtfhence
btKUtfand
atKUtfwhere
tftftf




,
,
2
1
21
     tbUatKUtf  .
It can also be represented as the product of two step functions as
21Vijaya Laxmi, Dept. of EEE, BIT, Mesra
Ramp function
• A ramp function is described as
 
  0;
0;0


ttKr
ttf
 
  atatKr
attfand


;
;0
22Vijaya Laxmi, Dept. of EEE, BIT, Mesra
Impulse function
• Consider a pulse function as
• The area of pulse =TX1/T=1.
• It can be represented mathematically as
      TtUtU
T
Ltt
T


1
0

23Vijaya Laxmi, Dept. of EEE, BIT, Mesra
Problem
• Express the half sine wave function using step
functions.
24Vijaya Laxmi, Dept. of EEE, BIT, Mesra
Solution
• The sine wave can be represented as
   
     
2/,0
2/,2/
0,0
0,
2
1
Tt
TtTtUtSinVtvand
t
tttUSinVtv
m
m






2/,0 Tt 
     
      
    2/
2/
21
TtUtUtSinV
TtUtSinttUSinV
tvtvtv
m
m





25Vijaya Laxmi, Dept. of EEE, BIT, Mesra
Problem
• Express the triangular wave using ramp functions.
26Vijaya Laxmi, Dept. of EEE, BIT, Mesra
Solution
• We have,
     
    TtTTtrT
TttrTtv


2/;22//2
2/0;/2
    TtfortvwhileTtforTtrBut  0,02/,
             TtrTTtrTtrTtv
Hence
 /22//4/2
,
27Vijaya Laxmi, Dept. of EEE, BIT, Mesra
Complex exponential signal
• The complex exponential signal is defined as
• An important property of a complex signal x(t) is that it is a
periodic signal for any value of w0.
• The fundamental period T0 of x(t) is given by
  tjSintCosetx tj
00
0


• The fundamental period T0 of x(t) is given by
0
0
2


T
   
 tjSintCoseeetx ttjst
00 
 
General Complex exponential signal
  t
etx 
 Real exponential signal
28Vijaya Laxmi, Dept. of EEE, BIT, Mesra
Exponentially increasing
sinusoidal signal
Exponentially decreasing
sinusoidal signal
Real Exponential signal for σ>0 and σ<0
29Vijaya Laxmi, Dept. of EEE, BIT, Mesra
Sinusoidal Signals
• A continuous-time sinusoidal signal can be expressed
as
     tACostx 0
30Vijaya Laxmi, Dept. of EEE, BIT, Mesra
Basic discrete-time signals
• Unit step sequence
• Unit impulse sequence
• Complex exponential sequence
• Real exponential sequence• Real exponential sequence
• Sinusoidal sequence
31Vijaya Laxmi, Dept. of EEE, BIT, Mesra
Unit step sequence
• The unit step sequence u[n] is defined as
• It is discontinuous at n=0.
 






00
01
n
n
nu
• It is discontinuous at n=0.
• The shifted unit step sequence u[n-k] is defined as
 






kn
kn
knu
0
1
32Vijaya Laxmi, Dept. of EEE, BIT, Mesra
Unit impulse sequence
• The unit impulse sequence δ[n], is defined as
 






01
00
n
n
n
• The shifted unit impulse sequence δ[n-k], is defined as
 






kn
kn
kn
1
0

33Vijaya Laxmi, Dept. of EEE, BIT, Mesra
Complex exponential sequence
• The complex exponential sequence is defined as
• In order for x[n] to be periodic with period N(>0), Ω0 must
satisfy the following condition:
  njSinnCosenx nj
00
0
 
egerpositivem
m
int,0


• Thus, the sequence in not periodic for any value of Ω0 . It is
periodic only if the above ratio is a rational number.
• In case of continuous-time complex exponentials, the signals
are all distinct for distinct values of w0, but this is not the case
for discrete-time complex exponentials
General Complex exponential signal
Real exponential signal
egerpositivem
N
m
int,
2
0



  n
Cnx 
101,10,1   and
34Vijaya Laxmi, Dept. of EEE, BIT, Mesra
Real exponential sequences
α>1 1>α>0
0>α>-1 α<-1
35Vijaya Laxmi, Dept. of EEE, BIT, Mesra
Sinusoidal Sequence
• A continuous-time sinusoidal sequence can be
expresses as
    nACosnx 0
Sinusoidal periodic Sequence Sinusoidal non-periodic Sequence
36Vijaya Laxmi, Dept. of EEE, BIT, Mesra
Energy and Power signals
• Consider v(t) as the voltage across a resistor R producing a
current i(t). The instantaneous power p(t) per ohm is defined
as
• Total energy E and average power P on a per ohm basis are
 ti
R
titv
tp 2)()(
)( 
• Total energy E and average power P on a per ohm basis are
 
  attswdtti
T
P
joulesdttiE
T
T
T 







2/
2/
2
2
1
lim
37Vijaya Laxmi, Dept. of EEE, BIT, Mesra
• For arbitrary cont-time signal x(t), the normalized energy
content E of x(t) is defined as
• The power of a periodic signal with period T0 is the average
 


 dttxE
2
• The power of a periodic signal with period T0 is the average
energy
• The normalized average power P of any signal x(t) is defined
as
 


2/
2/
21
lim
T
T
T
dttx
T
P
 
0
2
0 0
1
T
P x t dt
T
 
The limit may be zero also like exponential function etc.
38Vijaya Laxmi, Dept. of EEE, BIT, Mesra
• Similarly, for discrete-time signal x[n], the normalized energy
content E of x[n] is defined as
• The normalized average power P of x[n] is defined as




n
nxE
2
][
• The normalized average power P of x[n] is defined as

 

N
Nn
N
nx
N
P
2
][
12
1
lim
39Vijaya Laxmi, Dept. of EEE, BIT, Mesra
• X(t) or x[n] is said to be an energy signal (or sequence) if and
only if 0<E<∞ and so P=0.
• X(t) or x[n] is said to be an power signal (or sequence) if and
only if 0<P<∞ and thus E= ∞.
• Signals that satisfy neither property are referred to as neither• Signals that satisfy neither property are referred to as neither
energy signals nor power signals.
• A periodic signal is a power signal if its energy content per
period is finite and then the average power of this signal need
only be calculated over a period.
40Vijaya Laxmi, Dept. of EEE, BIT, Mesra
Problem
• Determine whether the following signals are energy
signals, power signals or neither.
 
at
tAtxb
atuetxa
cos)(.
0),()(.

 
 
 
nj
n
enxf
nunxe
nunxd
ttutxc
tAtxb
3
0
2][.
][][.
][5.0][.
)()(.
cos)(.




 
41Vijaya Laxmi, Dept. of EEE, BIT, Mesra
• A.
• B.
   




a
dtedttxE at
2
1
0
22
Energy signal
• B. The sinusoidal signal is periodic with T0=2π/w0.
 
   
















00
0
2
00
2
0
0
2/
2/
2
11
lim
,lim
1
lim,
TT
k
T
T
T
dttx
T
dttxk
kT
P
kTTastakenbetoittheallowing
dttx
T
PpowerAverage
42Vijaya Laxmi, Dept. of EEE, BIT, Mesra
Systems
• A system is a mathematical model of a physical
process that relates the input (or excitation) signal to
the output (or response) signal.
• A system is a collection of components which workA system is a collection of components which work
together to provide an output for a given input.
43Vijaya Laxmi, Dept. of EEE, BIT, Mesra
Classification of systems
• SISO and MIMO
• Continuous-time and Discrete-time systems
• Systems with memory and without memory
• Causal and Noncausal systems
• Linear and Nonlinear systems• Linear and Nonlinear systems
• Time-invariant and Time-varying systems
• Linear time-invariant systems
• Stable systems
• Feedback systems
44Vijaya Laxmi, Dept. of EEE, BIT, Mesra
SISO and MIMO system
45Vijaya Laxmi, Dept. of EEE, BIT, Mesra
Continuous-time and Discrete-time
systems
• If the input and output signals are Continuous-time
signals, then the system is called Continuous-time
systems.
• If the input and output signals are Discrete-time
sequences, then the system is called Discrete-time
systems.
46Vijaya Laxmi, Dept. of EEE, BIT, Mesra
Systems with memory and without
memory
• A system is said to be memoryless, if the output at any time
depends on only the input at that same time.
• Otherwise the system is said to have memory.
• Example: Resistor R with the input x(t) taken as the current
and voltage taken as the output y(t). The relation betweenand voltage taken as the output y(t). The relation between
them is
• The capacitor C with current as input x(t) and the voltage as
the output y(t)
• In discrete-time system, the system with memory is
)()( tRxty 


t
dx
C
ty )(
1
)(
   

n
k
kxny
47Vijaya Laxmi, Dept. of EEE, BIT, Mesra
Causal and Noncausal systems
• A system is called causal, if its output y(t) at an arbitrary
time t=t0 depends on only the input x(t) for t≤0, i.e., the
output of a causal system at the present time depends on
only the present and/or past values of the input, not on
its future values.its future values.
• Thus, in case of causal system, it is not possible to obtain
an output before an input is applied to the system.
• A system is said to be noncausal, if it is not causal.
• All memoryless systems are causal, but not vice versa.
48Vijaya Laxmi, Dept. of EEE, BIT, Mesra
Linear and Nonlinear systems
• The systems with follows the principles of
superposition and homogeneity are called linear
systems and the systems, which does not follow
them are called nonlinear systems.
• Principle of superposition (additivity): If for any• Principle of superposition (additivity): If for any
signals x1 and x2
• Principle of homogeneity (scaling): For any signals x
and y
• Hence, a system is called linear if
  2121
2211
yyxxTThen
yTxandyTx


  yxT  
  22112211 yyxxT  
49Vijaya Laxmi, Dept. of EEE, BIT, Mesra
Time-invariant and Time-varying
systems
• A system is called time-invariant, if a time shift (delay
or advance) in the input signal causes the same time
shift in the output signal. Thus, for a continuous-time
system, the system is time-invariant if
     . ofvaluerealanyfortytxT 
50Vijaya Laxmi, Dept. of EEE, BIT, Mesra
Linear time-invariant systems
• If a system is linear and also time-invariant, then it is
called linear time-invariant (LTI) system.
51Vijaya Laxmi, Dept. of EEE, BIT, Mesra
Stable systems
• A system is bounded-input/bounded-output
(BIBO) stable, if for any bounded input x
defined by , the corresponding
output y is also bounded defined by
1kx 
2ky output y is also bounded defined by
where k1 and k2 are finite real constants.
2ky 
52Vijaya Laxmi, Dept. of EEE, BIT, Mesra
Feedback systems
• In the feedback system, the output signal is fed back
and added to/subtracted from the input to the
system.
53Vijaya Laxmi, Dept. of EEE, BIT, Mesra

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IST module 1

  • 1. Introduction to System Theory Vijaya Laxmi Dept. of EEE BIT, Mesra 1Vijaya Laxmi, Dept. of EEE, BIT, Mesra
  • 2. Course Objectives The course enables the students : • To outline the fundamentals of common signals, systems, and recall the list of electrical and non-electrical components. • To summarize different transform methods, state-space techniques and different stability conditions of linear time-invariant systemand different stability conditions of linear time-invariant system using Routh-Hurwitz criteria. • To analyze the transient and steady-state performance of first order and second order systems when subjected to different signals and also the absolute stability using above criterion. • Actualize the electrical, mechanical, hydraulic and thermal systems using differential equations, transfer functions and state variables. 2Vijaya Laxmi, Dept. of EEE, BIT, Mesra
  • 3. Syllabus:EE 3201 INTRODUCTION TO SYSTEM THEORY • MODULE – I: Introduction to Signals and Systems: Definition, Basis of classification, Representation of common signals and their properties, System modeling. (4) • MODULE – II: Analogous System: Introduction, D Alembert's Principle, Force-voltage and force-current analogies, Electrical analogue of mechanical, Hydraulic and thermal systems. (5) • MODULE – III: Fourier Transform Method: Introduction, Fourier transform pair, Amplitude spectrum and phase spectrum of signals, Sinusoidal transfer function. (3) • MODULE – IV: Laplace Transform Method: Introduction, Laplace transform pair, Laplace transformation of common functions, Gate function, Step function and impulse function, Laplace theorems shifting, initial value, final value and convolution theorems, Inverse Laplace transform by partial fraction expansion and convolution integralInverse Laplace transform by partial fraction expansion and convolution integral method. (12) • MODULE – V: System Analysis: System Analysis by Laplace Transform method, System response. Natural, forced, transient and steady state responses. Transfer function and characteristic equation, Superposition integral, Concept of poles and zeros, Nature of system response from poles and zeros. (6) • MODULE – VI: System Stability: Concept of stability, Types, Necessary and sufficient conditions, Routh-Hurwitz stability criterion, Limitations and its applications to closed loop systems. (4) • MODULE – VII: State-Space Concept: Introduction, Definition: State, State variable, State vector and state space, State space representation, Derivation of State model from transfer function, Bush form and diagonal canonical form of state model, Non- uniqueness of state model, Derivation of transfer function from state model, Transition matrix and its properties, Solution of time invariant state equation. (6)3Vijaya Laxmi, Dept. of EEE, BIT, Mesra
  • 4. Books • Text Books: 1. Analysis of Linear Systems – D.K.Cheng. Narosa Publishing House, Indian Student Edition, 8th Reprint, 1994 2. Control System Engineering – Nagrath & Gopal, New Age International Pvt. Ltd. New Delhi, 2nd Edition 3. Control System – A. Anand Kumar3. Control System – A. Anand Kumar • Reference Books: 1. Networks and Systems – D. Roy Choudhury, New Age International Pvt. Ltd. New Delhi 2. Signal and Systems- Haykin 3. Signal and Systems- B.P. Lathi 4. Signals and Systems - Basu & Natarajan 4Vijaya Laxmi, Dept. of EEE, BIT, Mesra
  • 5. Course Outcomes After the completion of this course, students will be able to: • Describe characteristics of different signals and systems • Interpret the transform domains like Laplace equations, concept of poles and zeros, Fourier equations and time- domain state-space techniques • Solve mathematical model of electrical and non-electrical components with the knowledge of system science, related mathematics of simple engineering problems and concept ofmathematics of simple engineering problems and concept of analogous quantities • Relate Laplace equations, Fourier equations and time-domain state-space techniques to solve any given linear ordinary differential equations and analyze transient and steady-state performance of a first order and second order linear time- invariant system using standard test signals • Evaluate and formulate electrical or non-electrical linear time invariant systems for desired transient behaviour, steady state error and stability. 5Vijaya Laxmi, Dept. of EEE, BIT, Mesra
  • 6. Module I Introduction to Signals and SystemsIntroduction to Signals and Systems 6Vijaya Laxmi, Dept. of EEE, BIT, Mesra
  • 7. Objectives: Module I • To introduce introduce common signals and systems needed in almost all electrical and other engineering fields and scientific disciplines as well. • The mathematical description and representation of signals and systems and their classification.and systems and their classification. • Define several basic properties of signals and systems. 7Vijaya Laxmi, Dept. of EEE, BIT, Mesra
  • 8. Signal • It is a function representing a physical quantity or variable, and typically it contains information about the behavior or nature of the phenomenon. • Example: In RLC circuit the signal may be the voltageExample: In RLC circuit the signal may be the voltage across the capacitor or current flowing through the inductor or resistor. • Mathematically, a signal may be represented as a function of an independent variable ‘t’ and denoted by x(t). 8Vijaya Laxmi, Dept. of EEE, BIT, Mesra
  • 9. Classification of Signals • Continuous-time and Discrete-time Signals • Analog and Digital Signals • Real and Complex Signals • Deterministic and Random Signals• Deterministic and Random Signals • Even and odd signals • Periodic and Nonperiodic Signals 9Vijaya Laxmi, Dept. of EEE, BIT, Mesra
  • 10. Continuous-time and Discrete-time Signals • A signal x(t) is called continuous-time signal, if t is a continuous variable. • A signal x(t) is called discrete-time signal, if t is a discrete variable, i.e., x(t) is defined at discrete times, often called sequence of numbers and denoted by x[n], where n=integer.sequence of numbers and denoted by x[n], where n=integer. • Discrete-time signal may be also obtained by sampling a continuous-time signal x(t) such as         ,...,...,,, ],...[],...1[],0[ ,....,...,,, 210 210 n n xxxx or nxxx or txtxtxtx )(][.,. nn txnxxei  For uniform sampling,  sn nTxnxx  ][ Where Ts is the sampling interval 10Vijaya Laxmi, Dept. of EEE, BIT, Mesra
  • 11. Continuous-time signal Discrete-time signal 11Vijaya Laxmi, Dept. of EEE, BIT, Mesra
  • 12. Analog and Digital Signal • If a continuous-time signal x(t) can take on any value in the continuous interval (a,b), where a may be -∞ and b may be +∞, then the continuous-time signal is called analog signal. • If the discrete-time signal x[n] can take on only a finite number of distinct values, then it is called a digital signal. 12Vijaya Laxmi, Dept. of EEE, BIT, Mesra
  • 13. Real and Complex Signal • A signal x(t) is a real signal, if its value is a real number, and signal x(t) is a complex signal if its value is a complex number. 13Vijaya Laxmi, Dept. of EEE, BIT, Mesra
  • 14. Deterministic and Random Signal • Deterministic signals are those signals, whose values are completely specified for any given time. Thus, a deterministic signal can be modeled by a known function of time t. • Random signals are those signals that take random values at any given time and must be characterized statistically. 14Vijaya Laxmi, Dept. of EEE, BIT, Mesra
  • 15. Even and Odd signals • A signal x(t) or x[n] is referred to as an even signal if        nxnx txtx   • A signal x(t) or x[n] is referred to as an odd signal if        nxnx txtx   15Vijaya Laxmi, Dept. of EEE, BIT, Mesra
  • 16. Even signalsEven signals Odd Signals 16Vijaya Laxmi, Dept. of EEE, BIT, Mesra
  • 17. Periodic and Nonperiodic signals • A continuous-time signal x(t) is said to be periodic with period T, if there is a positive nonzero value of T for which • Any continuous-time signal which is not periodic is called a nonperiodic (aperiodic) signal.     tallfortxTtx  a nonperiodic (aperiodic) signal. • A discrete-time signal x[n] is said to be periodic with period N, if there is a positive nonzero value of N for which • Any discrete-time signal which is not periodic is called a nonperiodic (aperiodic) signal.     nallfornxNnx  17Vijaya Laxmi, Dept. of EEE, BIT, Mesra
  • 18. Periodic Signals 18Vijaya Laxmi, Dept. of EEE, BIT, Mesra
  • 19. Basic continuous-time signals • Unit step function • Ramp function • Unit impulse function • Complex exponential signals• Complex exponential signals • Real exponential signals • Sinusoidal signals 19Vijaya Laxmi, Dept. of EEE, BIT, Mesra
  • 20. Unit step function • The unit step function u(t) is defined as • It is discontinuous at t=0.       00 01 )( t t tu • It is discontinuous at t=0. • The shifted unit step function u(t-t0) is defined as       0 0 0 0 1 )( tt tt ttu 20Vijaya Laxmi, Dept. of EEE, BIT, Mesra
  • 21. Gate function • It can be written as sum of two step functions.      tftftf                     btUatUKtfhence btKUtfand atKUtfwhere tftftf     , , 2 1 21      tbUatKUtf  . It can also be represented as the product of two step functions as 21Vijaya Laxmi, Dept. of EEE, BIT, Mesra
  • 22. Ramp function • A ramp function is described as     0; 0;0   ttKr ttf     atatKr attfand   ; ;0 22Vijaya Laxmi, Dept. of EEE, BIT, Mesra
  • 23. Impulse function • Consider a pulse function as • The area of pulse =TX1/T=1. • It can be represented mathematically as       TtUtU T Ltt T   1 0  23Vijaya Laxmi, Dept. of EEE, BIT, Mesra
  • 24. Problem • Express the half sine wave function using step functions. 24Vijaya Laxmi, Dept. of EEE, BIT, Mesra
  • 25. Solution • The sine wave can be represented as           2/,0 2/,2/ 0,0 0, 2 1 Tt TtTtUtSinVtvand t tttUSinVtv m m       2/,0 Tt                   2/ 2/ 21 TtUtUtSinV TtUtSinttUSinV tvtvtv m m      25Vijaya Laxmi, Dept. of EEE, BIT, Mesra
  • 26. Problem • Express the triangular wave using ramp functions. 26Vijaya Laxmi, Dept. of EEE, BIT, Mesra
  • 27. Solution • We have,           TtTTtrT TttrTtv   2/;22//2 2/0;/2     TtfortvwhileTtforTtrBut  0,02/,              TtrTTtrTtrTtv Hence  /22//4/2 , 27Vijaya Laxmi, Dept. of EEE, BIT, Mesra
  • 28. Complex exponential signal • The complex exponential signal is defined as • An important property of a complex signal x(t) is that it is a periodic signal for any value of w0. • The fundamental period T0 of x(t) is given by   tjSintCosetx tj 00 0   • The fundamental period T0 of x(t) is given by 0 0 2   T      tjSintCoseeetx ttjst 00    General Complex exponential signal   t etx   Real exponential signal 28Vijaya Laxmi, Dept. of EEE, BIT, Mesra
  • 29. Exponentially increasing sinusoidal signal Exponentially decreasing sinusoidal signal Real Exponential signal for σ>0 and σ<0 29Vijaya Laxmi, Dept. of EEE, BIT, Mesra
  • 30. Sinusoidal Signals • A continuous-time sinusoidal signal can be expressed as      tACostx 0 30Vijaya Laxmi, Dept. of EEE, BIT, Mesra
  • 31. Basic discrete-time signals • Unit step sequence • Unit impulse sequence • Complex exponential sequence • Real exponential sequence• Real exponential sequence • Sinusoidal sequence 31Vijaya Laxmi, Dept. of EEE, BIT, Mesra
  • 32. Unit step sequence • The unit step sequence u[n] is defined as • It is discontinuous at n=0.         00 01 n n nu • It is discontinuous at n=0. • The shifted unit step sequence u[n-k] is defined as         kn kn knu 0 1 32Vijaya Laxmi, Dept. of EEE, BIT, Mesra
  • 33. Unit impulse sequence • The unit impulse sequence δ[n], is defined as         01 00 n n n • The shifted unit impulse sequence δ[n-k], is defined as         kn kn kn 1 0  33Vijaya Laxmi, Dept. of EEE, BIT, Mesra
  • 34. Complex exponential sequence • The complex exponential sequence is defined as • In order for x[n] to be periodic with period N(>0), Ω0 must satisfy the following condition:   njSinnCosenx nj 00 0   egerpositivem m int,0   • Thus, the sequence in not periodic for any value of Ω0 . It is periodic only if the above ratio is a rational number. • In case of continuous-time complex exponentials, the signals are all distinct for distinct values of w0, but this is not the case for discrete-time complex exponentials General Complex exponential signal Real exponential signal egerpositivem N m int, 2 0      n Cnx  101,10,1   and 34Vijaya Laxmi, Dept. of EEE, BIT, Mesra
  • 35. Real exponential sequences α>1 1>α>0 0>α>-1 α<-1 35Vijaya Laxmi, Dept. of EEE, BIT, Mesra
  • 36. Sinusoidal Sequence • A continuous-time sinusoidal sequence can be expresses as     nACosnx 0 Sinusoidal periodic Sequence Sinusoidal non-periodic Sequence 36Vijaya Laxmi, Dept. of EEE, BIT, Mesra
  • 37. Energy and Power signals • Consider v(t) as the voltage across a resistor R producing a current i(t). The instantaneous power p(t) per ohm is defined as • Total energy E and average power P on a per ohm basis are  ti R titv tp 2)()( )(  • Total energy E and average power P on a per ohm basis are     attswdtti T P joulesdttiE T T T         2/ 2/ 2 2 1 lim 37Vijaya Laxmi, Dept. of EEE, BIT, Mesra
  • 38. • For arbitrary cont-time signal x(t), the normalized energy content E of x(t) is defined as • The power of a periodic signal with period T0 is the average      dttxE 2 • The power of a periodic signal with period T0 is the average energy • The normalized average power P of any signal x(t) is defined as     2/ 2/ 21 lim T T T dttx T P   0 2 0 0 1 T P x t dt T   The limit may be zero also like exponential function etc. 38Vijaya Laxmi, Dept. of EEE, BIT, Mesra
  • 39. • Similarly, for discrete-time signal x[n], the normalized energy content E of x[n] is defined as • The normalized average power P of x[n] is defined as     n nxE 2 ][ • The normalized average power P of x[n] is defined as     N Nn N nx N P 2 ][ 12 1 lim 39Vijaya Laxmi, Dept. of EEE, BIT, Mesra
  • 40. • X(t) or x[n] is said to be an energy signal (or sequence) if and only if 0<E<∞ and so P=0. • X(t) or x[n] is said to be an power signal (or sequence) if and only if 0<P<∞ and thus E= ∞. • Signals that satisfy neither property are referred to as neither• Signals that satisfy neither property are referred to as neither energy signals nor power signals. • A periodic signal is a power signal if its energy content per period is finite and then the average power of this signal need only be calculated over a period. 40Vijaya Laxmi, Dept. of EEE, BIT, Mesra
  • 41. Problem • Determine whether the following signals are energy signals, power signals or neither.   at tAtxb atuetxa cos)(. 0),()(.        nj n enxf nunxe nunxd ttutxc tAtxb 3 0 2][. ][][. ][5.0][. )()(. cos)(.       41Vijaya Laxmi, Dept. of EEE, BIT, Mesra
  • 42. • A. • B.         a dtedttxE at 2 1 0 22 Energy signal • B. The sinusoidal signal is periodic with T0=2π/w0.                       00 0 2 00 2 0 0 2/ 2/ 2 11 lim ,lim 1 lim, TT k T T T dttx T dttxk kT P kTTastakenbetoittheallowing dttx T PpowerAverage 42Vijaya Laxmi, Dept. of EEE, BIT, Mesra
  • 43. Systems • A system is a mathematical model of a physical process that relates the input (or excitation) signal to the output (or response) signal. • A system is a collection of components which workA system is a collection of components which work together to provide an output for a given input. 43Vijaya Laxmi, Dept. of EEE, BIT, Mesra
  • 44. Classification of systems • SISO and MIMO • Continuous-time and Discrete-time systems • Systems with memory and without memory • Causal and Noncausal systems • Linear and Nonlinear systems• Linear and Nonlinear systems • Time-invariant and Time-varying systems • Linear time-invariant systems • Stable systems • Feedback systems 44Vijaya Laxmi, Dept. of EEE, BIT, Mesra
  • 45. SISO and MIMO system 45Vijaya Laxmi, Dept. of EEE, BIT, Mesra
  • 46. Continuous-time and Discrete-time systems • If the input and output signals are Continuous-time signals, then the system is called Continuous-time systems. • If the input and output signals are Discrete-time sequences, then the system is called Discrete-time systems. 46Vijaya Laxmi, Dept. of EEE, BIT, Mesra
  • 47. Systems with memory and without memory • A system is said to be memoryless, if the output at any time depends on only the input at that same time. • Otherwise the system is said to have memory. • Example: Resistor R with the input x(t) taken as the current and voltage taken as the output y(t). The relation betweenand voltage taken as the output y(t). The relation between them is • The capacitor C with current as input x(t) and the voltage as the output y(t) • In discrete-time system, the system with memory is )()( tRxty    t dx C ty )( 1 )(      n k kxny 47Vijaya Laxmi, Dept. of EEE, BIT, Mesra
  • 48. Causal and Noncausal systems • A system is called causal, if its output y(t) at an arbitrary time t=t0 depends on only the input x(t) for t≤0, i.e., the output of a causal system at the present time depends on only the present and/or past values of the input, not on its future values.its future values. • Thus, in case of causal system, it is not possible to obtain an output before an input is applied to the system. • A system is said to be noncausal, if it is not causal. • All memoryless systems are causal, but not vice versa. 48Vijaya Laxmi, Dept. of EEE, BIT, Mesra
  • 49. Linear and Nonlinear systems • The systems with follows the principles of superposition and homogeneity are called linear systems and the systems, which does not follow them are called nonlinear systems. • Principle of superposition (additivity): If for any• Principle of superposition (additivity): If for any signals x1 and x2 • Principle of homogeneity (scaling): For any signals x and y • Hence, a system is called linear if   2121 2211 yyxxTThen yTxandyTx     yxT     22112211 yyxxT   49Vijaya Laxmi, Dept. of EEE, BIT, Mesra
  • 50. Time-invariant and Time-varying systems • A system is called time-invariant, if a time shift (delay or advance) in the input signal causes the same time shift in the output signal. Thus, for a continuous-time system, the system is time-invariant if      . ofvaluerealanyfortytxT  50Vijaya Laxmi, Dept. of EEE, BIT, Mesra
  • 51. Linear time-invariant systems • If a system is linear and also time-invariant, then it is called linear time-invariant (LTI) system. 51Vijaya Laxmi, Dept. of EEE, BIT, Mesra
  • 52. Stable systems • A system is bounded-input/bounded-output (BIBO) stable, if for any bounded input x defined by , the corresponding output y is also bounded defined by 1kx  2ky output y is also bounded defined by where k1 and k2 are finite real constants. 2ky  52Vijaya Laxmi, Dept. of EEE, BIT, Mesra
  • 53. Feedback systems • In the feedback system, the output signal is fed back and added to/subtracted from the input to the system. 53Vijaya Laxmi, Dept. of EEE, BIT, Mesra