SlideShare una empresa de Scribd logo
1 de 13
EEEC4340318 INSTRUMENTATION AND CONTROL SYSTEMS
Stability And Routh-Hurwitz Condition
FACULTY OF ENGINEERING AND COMPUTER TECHNOLOGY
DIPLOMA IN ELECTRICALAND ELECTRONIC ENGINEERING
Ravandran Muttiah BEng (Hons) MSc MIET
1
Stability
A systems is said to be stable if all bounded inputs 𝑟 𝑡 give rise to
bounded outputs 𝑦 𝑡 .
Figure 1
𝑌 𝑠
𝑅 𝑠 𝐺 𝑠
2
Conditions For Stability
𝑦 𝑡 =
−∞
∞
𝑔 𝜏 𝑟 𝑡 − 𝜏 d𝜏
Let 𝑟 𝑡 be such that 𝑟 𝑡 ≤ 𝑟
𝑦 𝑡 =
−∞
∞
𝑔 𝜏 𝑟 𝑡 − 𝜏 d𝜏
≤
−∞
∞
𝑔 𝜏 𝑟 𝑡 − 𝜏 d𝜏
≤ 𝑟
−∞
∞
𝑔 𝜏 d𝜏
Using this: system 𝐺 𝑠 is stable if −∞
∞
𝑔 𝜏 d𝜏 is finite
Figure 2
𝑌 𝑠
𝑅 𝑠 𝐺 𝑠
3
Condition In Terms Of Poles ?
We want −∞
∞
𝑔 𝜏 d𝜏 to be finite
Can we determine this from 𝐺 𝑠
We can write a general rational transfer function in the form
𝐺 𝑠 =
𝐾 𝑖 𝑠 + 𝑧𝑖
𝑠𝑁
𝑘 𝑠 + 𝜎𝑘 𝑚 𝑠2 + 2𝛼𝑚𝑠 + 𝛼𝑚
2
+ 𝜔𝑚
2
Poles: 0, −𝜎𝑘, −𝛼𝑚 ± j𝜔𝑚
Assuming 𝑁 = 0 and no repeated roots, the impulse response is,
𝑔 𝑡 =
𝑘
𝐴𝑘𝑒−𝜎𝑘𝑡
+
𝑚
𝐵𝑚𝑒−𝛼𝑚𝑡
sin 𝜔𝑚𝑡 + 𝜃𝑚
Stability requires 𝑔 𝑡 d𝑡 to be bounded;
that requires 𝜎𝑘 > 0, 𝜎𝑚 > 0
In fact, system is stable if poles have negative real parts.
4
Marginal Stability
Consider integrator: 𝐺 𝑠 =
1
s
; simple pole at origin,
𝑦 𝑡 =
−∞
∞
𝑟 𝑡 d𝑡
If 𝑟 𝑡 = cos 𝑡 , which is bounded,
then 𝑦 𝑡 = sin 𝑡 . Bounded.
If 𝑟 𝑡 = 𝑢 𝑡 , which is bounded,
then 𝑦 𝑡 = 𝑡. Not bounded.
Consider 𝐺 𝑠 =
1
𝑠2+1
, simple poles at 𝑠 = ±j1
Unit step response: 𝑢 𝑡 − cos 𝑡 . Bounded
What if 𝑟 𝑡 is a sinusoid of frequency
1
2π
Hz ?
Not bounded.
If 𝐺 𝑠 has a pole with positive real part, or a repeated pole on j𝜔-axis,
output is always unbounded.
5
Routh-Hurwitz Condition
We have seen how to determine stability from the poles.
Much easier than having to find impulse response and then determining
if 𝑔 𝜏 d𝜏 < ∞
Can we determine stability without having to determine the poles ?
Yes! Routh-Hurwitz condition.
6
Let 𝐺 𝑠 =
𝑝 𝑠
𝑞 𝑠
, where
𝑞 𝑠 = 𝑎𝑛𝑠𝑛
+ 𝑎𝑛−1𝑠𝑛−1
+ ⋯ 𝑎1𝑠 + 𝑎0
= 𝑎𝑛 𝑠 − 𝑟1 𝑠 − 𝑟2 ⋯ 𝑠 − 𝑟𝑛
where 𝑟𝑖 are the roots of 𝑞 𝑠 = 0.
By multiplying out, 𝑞 𝑠 = 0 can be written as,
𝑞 𝑠
= 𝑎𝑛𝑠𝑛
− 𝑎𝑛 𝑟1 + 𝑟2 + ⋯ + 𝑟𝑛 𝑠𝑛−1
+ 𝑎𝑛 𝑟1𝑟2 + 𝑟2𝑟3 + ⋯ 𝑠𝑛−2
− 𝑎𝑛 𝑟1𝑟2𝑟3 + 𝑟1𝑟2𝑟4 + ⋯ 𝑠𝑛−3
+ ⋯ + −1 𝑛
𝑎𝑛 𝑟1𝑟2𝑟3 ⋯ 𝑟𝑛 = 0
If all 𝑟𝑖 are real and in left half plane, what is sign of coefficients of 𝑠𝑘
the
same!
7
That observation leads to a necessary condition.
Hence, not that useful for design.
A more sophisticated analysis leads to the Routh-Hurwitz condition,
which is necessary and sufficient.
Hence, can be quite useful for design.
8
Routh-Hurwitz Condition: A First Look
Consider 𝐺 𝑠 =
𝑝 𝑠
𝑞 𝑠
. Poles are solutions to 𝑞 𝑠 = 0; i.e.,
𝑎𝑛𝑠𝑛
+ 𝑎𝑛−1𝑠𝑛−1
+ 𝑎𝑛−2𝑠𝑛−2
+ ⋯ + 𝑎1𝑠 + 𝑎0 = 0
Construct a table of the form,
𝑠𝑛
𝑠𝑛−1
𝑠𝑛−2
𝑠𝑛−3
⋮
𝑠0
𝑎𝑛
𝑎𝑛−1
𝑏𝑛−1
𝑐𝑛−1
⋮
ℎ𝑛−1
𝑎𝑛−2
𝑎𝑛−3
𝑏𝑛−3
𝑐𝑛−3
⋮
𝑎𝑛−4 ⋯
𝑎𝑛−5 ⋯
𝑏𝑛−5 ⋯
𝑐𝑛−5 ⋯
⋮ ⋯
where,
𝑏𝑛−1 =
𝑎𝑛−1𝑎𝑛−2 − 𝑎𝑛𝑎𝑛−3
𝑎𝑛−1
=
−1
𝑎𝑛−1
𝑎𝑛 𝑎𝑛−2
𝑎𝑛−1 𝑎𝑛−3
𝑏𝑛−3 =
−1
𝑎𝑛−1
𝑎𝑛 𝑎𝑛−4
𝑎𝑛−1 𝑎𝑛−5
𝑐𝑛−1 =
−1
𝑏𝑛−1
𝑎𝑛−1 𝑎𝑛−3
𝑏𝑛−1 𝑏𝑛−3
9
Now consider the table we have just constructed.
𝑠𝑛
𝑠𝑛−1
𝑠𝑛−2
𝑠𝑛−3
⋮
𝑠0
𝑎𝑛
𝑎𝑛−1
𝑏𝑛−1
𝑐𝑛−1
⋮
ℎ𝑛−1
𝑎𝑛−2
𝑎𝑛−3
𝑏𝑛−3
𝑐𝑛−3
⋮
𝑎𝑛−4 ⋯
𝑎𝑛−5 ⋯
𝑏𝑛−5 ⋯
𝑐𝑛−5 ⋯
⋮ ⋯
Loosely speaking:
Number of roots in the right half plane is equal to the number of sign
changes in the first column of the table.
Stability if no sign changes in the first column.
Now let’s move towards a more sophisticated statement.
10
Let 𝐺 𝑠 =
𝑝 𝑠
𝑞 𝑠
where 𝑞 𝑠 = 𝑎𝑛𝑠𝑛
+ 𝑎𝑛−1𝑠𝑛−1
+ ⋯ 𝑎1𝑠 + 𝑎0
System is stable if all poles of 𝐺 𝑠 have negative real parts.
Recall, poles are solutions to 𝑞 𝑠 = 0.
Can we find a necessary and sufficient condition that depends only on
𝑎𝑘 so that we don’t have to solve 𝑞 𝑠 = 0 ?
Stability (Revision)
Figure 3
𝑌 𝑠
𝑅 𝑠 𝐺 𝑠
11
(1) Consider 𝑞 𝑠 with 𝑎𝑛 > 0
𝑎𝑛𝑠𝑛
+ 𝑎𝑛−1𝑠𝑛−1
+ 𝑎𝑛−2𝑠𝑛−2
+ ⋯ 𝑎1𝑠 + 𝑎0 = 0
(2) Construct a table of the form,
Row 𝑛
Row 𝑛 − 1
Row 𝑛 − 2
Row 𝑛 − 3
⋮
Row 0
𝑎𝑛
𝑎𝑛−1
𝑏𝑛−1
𝑐𝑛−1
⋮
ℎ𝑛−1
𝑎𝑛−2
𝑎𝑛−3
𝑏𝑛−3
𝑐𝑛−3
⋮
𝑎𝑛−4 ⋯
𝑎𝑛−5 ⋯
𝑏𝑛−5 ⋯
𝑐𝑛−5 ⋯
⋮ ⋯
Procedure provided on the following slides.
(3) Count the sign changes in the first column.
(4) That is the number of roots in the right half plane.
Stability (poles in Left Half Plane if 𝑎𝑘 > 0 and all terms in first column > 0
Routh-Hurwitz Condition
12
References
(1) Tim Davidson, Introduction to Linear Control Systems, McMaster
University, 2018.

Más contenido relacionado

La actualidad más candente

Power series convergence ,taylor & laurent's theorem
Power series  convergence ,taylor & laurent's theoremPower series  convergence ,taylor & laurent's theorem
Power series convergence ,taylor & laurent's theoremPARIKH HARSHIL
 
Inverse laplacetransform
Inverse laplacetransformInverse laplacetransform
Inverse laplacetransformTarun Gehlot
 
The Laplace Transform of Modeling of a Spring-Mass-Damper System
The Laplace Transform of Modeling of a Spring-Mass-Damper System The Laplace Transform of Modeling of a Spring-Mass-Damper System
The Laplace Transform of Modeling of a Spring-Mass-Damper System Mahmoud Farg
 
Meeting w6 chapter 2 part 3
Meeting w6   chapter 2 part 3Meeting w6   chapter 2 part 3
Meeting w6 chapter 2 part 3mkazree
 
Partial fraction decomposition for inverse laplace transform
Partial fraction decomposition for inverse laplace transformPartial fraction decomposition for inverse laplace transform
Partial fraction decomposition for inverse laplace transformVishalsagar657
 
Frequency Response Analysis and Bode Diagrams for First Order Systems
Frequency Response Analysis and Bode Diagrams for First Order SystemsFrequency Response Analysis and Bode Diagrams for First Order Systems
Frequency Response Analysis and Bode Diagrams for First Order SystemsVishvaraj Chauhan
 
Infinite Series Presentation by Jatin Dhola
Infinite Series Presentation by Jatin DholaInfinite Series Presentation by Jatin Dhola
Infinite Series Presentation by Jatin DholaJatin Dhola
 
Jif 315 lesson 1 Laplace and fourier transform
Jif 315 lesson 1 Laplace and fourier transformJif 315 lesson 1 Laplace and fourier transform
Jif 315 lesson 1 Laplace and fourier transformKurenai Ryu
 

La actualidad más candente (20)

Routh
RouthRouth
Routh
 
Group 4 reporting c.s.
Group 4 reporting c.s.Group 4 reporting c.s.
Group 4 reporting c.s.
 
Power series convergence ,taylor & laurent's theorem
Power series  convergence ,taylor & laurent's theoremPower series  convergence ,taylor & laurent's theorem
Power series convergence ,taylor & laurent's theorem
 
Ch05 1
Ch05 1Ch05 1
Ch05 1
 
Power series
Power seriesPower series
Power series
 
Inverse laplacetransform
Inverse laplacetransformInverse laplacetransform
Inverse laplacetransform
 
1605 power series
1605 power series1605 power series
1605 power series
 
Laplace transformation
Laplace transformationLaplace transformation
Laplace transformation
 
The Laplace Transform of Modeling of a Spring-Mass-Damper System
The Laplace Transform of Modeling of a Spring-Mass-Damper System The Laplace Transform of Modeling of a Spring-Mass-Damper System
The Laplace Transform of Modeling of a Spring-Mass-Damper System
 
Meeting w6 chapter 2 part 3
Meeting w6   chapter 2 part 3Meeting w6   chapter 2 part 3
Meeting w6 chapter 2 part 3
 
Laplace
LaplaceLaplace
Laplace
 
Partial fraction decomposition for inverse laplace transform
Partial fraction decomposition for inverse laplace transformPartial fraction decomposition for inverse laplace transform
Partial fraction decomposition for inverse laplace transform
 
Power series
Power seriesPower series
Power series
 
Frequency Response Analysis and Bode Diagrams for First Order Systems
Frequency Response Analysis and Bode Diagrams for First Order SystemsFrequency Response Analysis and Bode Diagrams for First Order Systems
Frequency Response Analysis and Bode Diagrams for First Order Systems
 
Routh Hurwitz contd
Routh Hurwitz contd Routh Hurwitz contd
Routh Hurwitz contd
 
Inverse laplace transforms
Inverse laplace transformsInverse laplace transforms
Inverse laplace transforms
 
Infinite Series Presentation by Jatin Dhola
Infinite Series Presentation by Jatin DholaInfinite Series Presentation by Jatin Dhola
Infinite Series Presentation by Jatin Dhola
 
Laplace transforms
Laplace transformsLaplace transforms
Laplace transforms
 
Inverse laplace
Inverse laplaceInverse laplace
Inverse laplace
 
Jif 315 lesson 1 Laplace and fourier transform
Jif 315 lesson 1 Laplace and fourier transformJif 315 lesson 1 Laplace and fourier transform
Jif 315 lesson 1 Laplace and fourier transform
 

Similar a Lecture Notes: EEEC4340318 Instrumentation and Control Systems - Stability and Routh-Hurwitz Condition

Integral method of the Analytic solutions to the heat equation With Experimen...
Integral method of the Analytic solutions to the heat equation With Experimen...Integral method of the Analytic solutions to the heat equation With Experimen...
Integral method of the Analytic solutions to the heat equation With Experimen...Wasswaderrick3
 
HEAT CONDUCTION DEMYSTIFIED.pdf
HEAT CONDUCTION DEMYSTIFIED.pdfHEAT CONDUCTION DEMYSTIFIED.pdf
HEAT CONDUCTION DEMYSTIFIED.pdfWasswaderrick3
 
FUNDAMENTALS OF HEAT TRANSFER .pdf
FUNDAMENTALS OF HEAT TRANSFER .pdfFUNDAMENTALS OF HEAT TRANSFER .pdf
FUNDAMENTALS OF HEAT TRANSFER .pdfWasswaderrick3
 
3). work & energy (finished)
3). work & energy (finished)3). work & energy (finished)
3). work & energy (finished)PhysicsLover
 
Uniform Boundedness of Shift Operators
Uniform Boundedness of Shift OperatorsUniform Boundedness of Shift Operators
Uniform Boundedness of Shift Operatorsiosrjce
 
PhyChem3_vector_matrix_mechanics.pptx
PhyChem3_vector_matrix_mechanics.pptxPhyChem3_vector_matrix_mechanics.pptx
PhyChem3_vector_matrix_mechanics.pptxErickson Fajiculay
 
Rational function 11
Rational function 11Rational function 11
Rational function 11AjayQuines
 
International Refereed Journal of Engineering and Science (IRJES)
International Refereed Journal of Engineering and Science (IRJES)International Refereed Journal of Engineering and Science (IRJES)
International Refereed Journal of Engineering and Science (IRJES)irjes
 
BSC_COMPUTER _SCIENCE_UNIT-2_DISCRETE MATHEMATICS
BSC_COMPUTER _SCIENCE_UNIT-2_DISCRETE MATHEMATICSBSC_COMPUTER _SCIENCE_UNIT-2_DISCRETE MATHEMATICS
BSC_COMPUTER _SCIENCE_UNIT-2_DISCRETE MATHEMATICSRai University
 
Contour integration and Mittag Leffler theorem
Contour integration and Mittag Leffler theoremContour integration and Mittag Leffler theorem
Contour integration and Mittag Leffler theoremAmenahGondal1
 
ANALTICAL SOLUTIONS TO THE HEAT EQUATION USING THE INTEGRAL METHODS.pdf
ANALTICAL SOLUTIONS TO THE HEAT EQUATION USING THE INTEGRAL METHODS.pdfANALTICAL SOLUTIONS TO THE HEAT EQUATION USING THE INTEGRAL METHODS.pdf
ANALTICAL SOLUTIONS TO THE HEAT EQUATION USING THE INTEGRAL METHODS.pdfWasswaderrick3
 
Integral methods for the analytic solutions to the heat equation.pdf
Integral methods for the analytic solutions to the heat equation.pdfIntegral methods for the analytic solutions to the heat equation.pdf
Integral methods for the analytic solutions to the heat equation.pdfWasswaderrick3
 
Integral dalam Bahasa Inggris
Integral dalam Bahasa InggrisIntegral dalam Bahasa Inggris
Integral dalam Bahasa Inggrisimmochacha
 
Engineering Analysis -Third Class.ppsx
Engineering Analysis -Third Class.ppsxEngineering Analysis -Third Class.ppsx
Engineering Analysis -Third Class.ppsxHebaEng
 

Similar a Lecture Notes: EEEC4340318 Instrumentation and Control Systems - Stability and Routh-Hurwitz Condition (20)

Integral method of the Analytic solutions to the heat equation With Experimen...
Integral method of the Analytic solutions to the heat equation With Experimen...Integral method of the Analytic solutions to the heat equation With Experimen...
Integral method of the Analytic solutions to the heat equation With Experimen...
 
HEAT CONDUCTION DEMYSTIFIED.pdf
HEAT CONDUCTION DEMYSTIFIED.pdfHEAT CONDUCTION DEMYSTIFIED.pdf
HEAT CONDUCTION DEMYSTIFIED.pdf
 
FUNDAMENTALS OF HEAT TRANSFER .pdf
FUNDAMENTALS OF HEAT TRANSFER .pdfFUNDAMENTALS OF HEAT TRANSFER .pdf
FUNDAMENTALS OF HEAT TRANSFER .pdf
 
Lecture5_Laplace_ODE.pdf
Lecture5_Laplace_ODE.pdfLecture5_Laplace_ODE.pdf
Lecture5_Laplace_ODE.pdf
 
3). work & energy (finished)
3). work & energy (finished)3). work & energy (finished)
3). work & energy (finished)
 
Uniform Boundedness of Shift Operators
Uniform Boundedness of Shift OperatorsUniform Boundedness of Shift Operators
Uniform Boundedness of Shift Operators
 
PhyChem3_vector_matrix_mechanics.pptx
PhyChem3_vector_matrix_mechanics.pptxPhyChem3_vector_matrix_mechanics.pptx
PhyChem3_vector_matrix_mechanics.pptx
 
C0560913
C0560913C0560913
C0560913
 
Rational function 11
Rational function 11Rational function 11
Rational function 11
 
Fourier series
Fourier series Fourier series
Fourier series
 
Waveguides
WaveguidesWaveguides
Waveguides
 
International Refereed Journal of Engineering and Science (IRJES)
International Refereed Journal of Engineering and Science (IRJES)International Refereed Journal of Engineering and Science (IRJES)
International Refereed Journal of Engineering and Science (IRJES)
 
BSC_COMPUTER _SCIENCE_UNIT-2_DISCRETE MATHEMATICS
BSC_COMPUTER _SCIENCE_UNIT-2_DISCRETE MATHEMATICSBSC_COMPUTER _SCIENCE_UNIT-2_DISCRETE MATHEMATICS
BSC_COMPUTER _SCIENCE_UNIT-2_DISCRETE MATHEMATICS
 
Contour integration and Mittag Leffler theorem
Contour integration and Mittag Leffler theoremContour integration and Mittag Leffler theorem
Contour integration and Mittag Leffler theorem
 
ANALTICAL SOLUTIONS TO THE HEAT EQUATION USING THE INTEGRAL METHODS.pdf
ANALTICAL SOLUTIONS TO THE HEAT EQUATION USING THE INTEGRAL METHODS.pdfANALTICAL SOLUTIONS TO THE HEAT EQUATION USING THE INTEGRAL METHODS.pdf
ANALTICAL SOLUTIONS TO THE HEAT EQUATION USING THE INTEGRAL METHODS.pdf
 
Integral methods for the analytic solutions to the heat equation.pdf
Integral methods for the analytic solutions to the heat equation.pdfIntegral methods for the analytic solutions to the heat equation.pdf
Integral methods for the analytic solutions to the heat equation.pdf
 
Inequalities list-2
Inequalities list-2Inequalities list-2
Inequalities list-2
 
Mod 3.pptx
Mod 3.pptxMod 3.pptx
Mod 3.pptx
 
Integral dalam Bahasa Inggris
Integral dalam Bahasa InggrisIntegral dalam Bahasa Inggris
Integral dalam Bahasa Inggris
 
Engineering Analysis -Third Class.ppsx
Engineering Analysis -Third Class.ppsxEngineering Analysis -Third Class.ppsx
Engineering Analysis -Third Class.ppsx
 

Más de AIMST University

Future Generation of Mobile and Satellite Communication Technology
Future Generation of Mobile and Satellite Communication TechnologyFuture Generation of Mobile and Satellite Communication Technology
Future Generation of Mobile and Satellite Communication TechnologyAIMST University
 
Research Cluster - Wireless Communications for 5G/6G
Research Cluster - Wireless Communications for 5G/6GResearch Cluster - Wireless Communications for 5G/6G
Research Cluster - Wireless Communications for 5G/6GAIMST University
 
1G, 2G, 3G, 4G, and 5G Technology
1G, 2G, 3G, 4G, and 5G Technology1G, 2G, 3G, 4G, and 5G Technology
1G, 2G, 3G, 4G, and 5G TechnologyAIMST University
 
Lecture Notes - EEEC6430310 Electromagnetic Fields and Waves - Smith Chart
Lecture Notes - EEEC6430310 Electromagnetic Fields and Waves - Smith ChartLecture Notes - EEEC6430310 Electromagnetic Fields and Waves - Smith Chart
Lecture Notes - EEEC6430310 Electromagnetic Fields and Waves - Smith ChartAIMST University
 
Mini Project 2 - Wien Bridge Oscillator
Mini Project 2 - Wien Bridge OscillatorMini Project 2 - Wien Bridge Oscillator
Mini Project 2 - Wien Bridge OscillatorAIMST University
 
Experiment 1 - Frequency Determination Using The Lissajous Polar
Experiment 1 - Frequency Determination Using The Lissajous PolarExperiment 1 - Frequency Determination Using The Lissajous Polar
Experiment 1 - Frequency Determination Using The Lissajous PolarAIMST University
 
Experiment 2 - Phase Determination Using The Lissajous Polar
Experiment 2 - Phase Determination Using The Lissajous PolarExperiment 2 - Phase Determination Using The Lissajous Polar
Experiment 2 - Phase Determination Using The Lissajous PolarAIMST University
 
Experiment 3 - Dynamic Characteristic of Thermistor
Experiment 3 - Dynamic Characteristic of ThermistorExperiment 3 - Dynamic Characteristic of Thermistor
Experiment 3 - Dynamic Characteristic of ThermistorAIMST University
 
Mini Project 1 - Wheatstone Bridge Light Detector
Mini Project 1 - Wheatstone Bridge Light DetectorMini Project 1 - Wheatstone Bridge Light Detector
Mini Project 1 - Wheatstone Bridge Light DetectorAIMST University
 
Lecture Notes: EEEC6430310 Electromagnetic Fields And Waves - Dipole Arrays
Lecture Notes:  EEEC6430310 Electromagnetic Fields And Waves - Dipole ArraysLecture Notes:  EEEC6430310 Electromagnetic Fields And Waves - Dipole Arrays
Lecture Notes: EEEC6430310 Electromagnetic Fields And Waves - Dipole ArraysAIMST University
 
Lecture Notes: EEEE6490345 RF And Microwave Electronics - Radio Communicatio...
Lecture Notes:  EEEE6490345 RF And Microwave Electronics - Radio Communicatio...Lecture Notes:  EEEE6490345 RF And Microwave Electronics - Radio Communicatio...
Lecture Notes: EEEE6490345 RF And Microwave Electronics - Radio Communicatio...AIMST University
 
Lecture Notes: EEEC6430312 Measurements And Instrumentation - Instrumentation
Lecture Notes:  EEEC6430312 Measurements And Instrumentation - InstrumentationLecture Notes:  EEEC6430312 Measurements And Instrumentation - Instrumentation
Lecture Notes: EEEC6430312 Measurements And Instrumentation - InstrumentationAIMST University
 
Lecture Notes: EEEC6430312 Measurements And Instrumentation - Fundamentals O...
Lecture Notes:  EEEC6430312 Measurements And Instrumentation - Fundamentals O...Lecture Notes:  EEEC6430312 Measurements And Instrumentation - Fundamentals O...
Lecture Notes: EEEC6430312 Measurements And Instrumentation - Fundamentals O...AIMST University
 
Lecture Notes: EEEC6430312 Measurements And Instrumentation - Instrument Typ...
Lecture Notes:  EEEC6430312 Measurements And Instrumentation - Instrument Typ...Lecture Notes:  EEEC6430312 Measurements And Instrumentation - Instrument Typ...
Lecture Notes: EEEC6430312 Measurements And Instrumentation - Instrument Typ...AIMST University
 
Lecture Notes: EEEC6430312 Measurements And Instrumentation - Errors During ...
Lecture Notes:  EEEC6430312 Measurements And Instrumentation - Errors During ...Lecture Notes:  EEEC6430312 Measurements And Instrumentation - Errors During ...
Lecture Notes: EEEC6430312 Measurements And Instrumentation - Errors During ...AIMST University
 
Lecture Notes: EEEC6430310 Electromagnetic Fields And Waves - Maxwell's Equa...
Lecture Notes:  EEEC6430310 Electromagnetic Fields And Waves - Maxwell's Equa...Lecture Notes:  EEEC6430310 Electromagnetic Fields And Waves - Maxwell's Equa...
Lecture Notes: EEEC6430310 Electromagnetic Fields And Waves - Maxwell's Equa...AIMST University
 
Lecture Notes: EEEC6430310 Electromagnetic Fields And Waves - Transmission Line
Lecture Notes:  EEEC6430310 Electromagnetic Fields And Waves - Transmission LineLecture Notes:  EEEC6430310 Electromagnetic Fields And Waves - Transmission Line
Lecture Notes: EEEC6430310 Electromagnetic Fields And Waves - Transmission LineAIMST University
 
Lecture Notes: EEEC6430310 Electromagnetic Fields And Waves - Cylindrical Ca...
Lecture Notes:  EEEC6430310 Electromagnetic Fields And Waves - Cylindrical Ca...Lecture Notes:  EEEC6430310 Electromagnetic Fields And Waves - Cylindrical Ca...
Lecture Notes: EEEC6430310 Electromagnetic Fields And Waves - Cylindrical Ca...AIMST University
 
Lecture Notes: EEEC6440315 Communication Systems - Time Frequency Analysis -...
Lecture Notes:  EEEC6440315 Communication Systems - Time Frequency Analysis -...Lecture Notes:  EEEC6440315 Communication Systems - Time Frequency Analysis -...
Lecture Notes: EEEC6440315 Communication Systems - Time Frequency Analysis -...AIMST University
 
Mini Project 1: Impedance Matching With A Single Stub Tuner
Mini Project 1:  Impedance Matching With A Single Stub TunerMini Project 1:  Impedance Matching With A Single Stub Tuner
Mini Project 1: Impedance Matching With A Single Stub TunerAIMST University
 

Más de AIMST University (20)

Future Generation of Mobile and Satellite Communication Technology
Future Generation of Mobile and Satellite Communication TechnologyFuture Generation of Mobile and Satellite Communication Technology
Future Generation of Mobile and Satellite Communication Technology
 
Research Cluster - Wireless Communications for 5G/6G
Research Cluster - Wireless Communications for 5G/6GResearch Cluster - Wireless Communications for 5G/6G
Research Cluster - Wireless Communications for 5G/6G
 
1G, 2G, 3G, 4G, and 5G Technology
1G, 2G, 3G, 4G, and 5G Technology1G, 2G, 3G, 4G, and 5G Technology
1G, 2G, 3G, 4G, and 5G Technology
 
Lecture Notes - EEEC6430310 Electromagnetic Fields and Waves - Smith Chart
Lecture Notes - EEEC6430310 Electromagnetic Fields and Waves - Smith ChartLecture Notes - EEEC6430310 Electromagnetic Fields and Waves - Smith Chart
Lecture Notes - EEEC6430310 Electromagnetic Fields and Waves - Smith Chart
 
Mini Project 2 - Wien Bridge Oscillator
Mini Project 2 - Wien Bridge OscillatorMini Project 2 - Wien Bridge Oscillator
Mini Project 2 - Wien Bridge Oscillator
 
Experiment 1 - Frequency Determination Using The Lissajous Polar
Experiment 1 - Frequency Determination Using The Lissajous PolarExperiment 1 - Frequency Determination Using The Lissajous Polar
Experiment 1 - Frequency Determination Using The Lissajous Polar
 
Experiment 2 - Phase Determination Using The Lissajous Polar
Experiment 2 - Phase Determination Using The Lissajous PolarExperiment 2 - Phase Determination Using The Lissajous Polar
Experiment 2 - Phase Determination Using The Lissajous Polar
 
Experiment 3 - Dynamic Characteristic of Thermistor
Experiment 3 - Dynamic Characteristic of ThermistorExperiment 3 - Dynamic Characteristic of Thermistor
Experiment 3 - Dynamic Characteristic of Thermistor
 
Mini Project 1 - Wheatstone Bridge Light Detector
Mini Project 1 - Wheatstone Bridge Light DetectorMini Project 1 - Wheatstone Bridge Light Detector
Mini Project 1 - Wheatstone Bridge Light Detector
 
Lecture Notes: EEEC6430310 Electromagnetic Fields And Waves - Dipole Arrays
Lecture Notes:  EEEC6430310 Electromagnetic Fields And Waves - Dipole ArraysLecture Notes:  EEEC6430310 Electromagnetic Fields And Waves - Dipole Arrays
Lecture Notes: EEEC6430310 Electromagnetic Fields And Waves - Dipole Arrays
 
Lecture Notes: EEEE6490345 RF And Microwave Electronics - Radio Communicatio...
Lecture Notes:  EEEE6490345 RF And Microwave Electronics - Radio Communicatio...Lecture Notes:  EEEE6490345 RF And Microwave Electronics - Radio Communicatio...
Lecture Notes: EEEE6490345 RF And Microwave Electronics - Radio Communicatio...
 
Lecture Notes: EEEC6430312 Measurements And Instrumentation - Instrumentation
Lecture Notes:  EEEC6430312 Measurements And Instrumentation - InstrumentationLecture Notes:  EEEC6430312 Measurements And Instrumentation - Instrumentation
Lecture Notes: EEEC6430312 Measurements And Instrumentation - Instrumentation
 
Lecture Notes: EEEC6430312 Measurements And Instrumentation - Fundamentals O...
Lecture Notes:  EEEC6430312 Measurements And Instrumentation - Fundamentals O...Lecture Notes:  EEEC6430312 Measurements And Instrumentation - Fundamentals O...
Lecture Notes: EEEC6430312 Measurements And Instrumentation - Fundamentals O...
 
Lecture Notes: EEEC6430312 Measurements And Instrumentation - Instrument Typ...
Lecture Notes:  EEEC6430312 Measurements And Instrumentation - Instrument Typ...Lecture Notes:  EEEC6430312 Measurements And Instrumentation - Instrument Typ...
Lecture Notes: EEEC6430312 Measurements And Instrumentation - Instrument Typ...
 
Lecture Notes: EEEC6430312 Measurements And Instrumentation - Errors During ...
Lecture Notes:  EEEC6430312 Measurements And Instrumentation - Errors During ...Lecture Notes:  EEEC6430312 Measurements And Instrumentation - Errors During ...
Lecture Notes: EEEC6430312 Measurements And Instrumentation - Errors During ...
 
Lecture Notes: EEEC6430310 Electromagnetic Fields And Waves - Maxwell's Equa...
Lecture Notes:  EEEC6430310 Electromagnetic Fields And Waves - Maxwell's Equa...Lecture Notes:  EEEC6430310 Electromagnetic Fields And Waves - Maxwell's Equa...
Lecture Notes: EEEC6430310 Electromagnetic Fields And Waves - Maxwell's Equa...
 
Lecture Notes: EEEC6430310 Electromagnetic Fields And Waves - Transmission Line
Lecture Notes:  EEEC6430310 Electromagnetic Fields And Waves - Transmission LineLecture Notes:  EEEC6430310 Electromagnetic Fields And Waves - Transmission Line
Lecture Notes: EEEC6430310 Electromagnetic Fields And Waves - Transmission Line
 
Lecture Notes: EEEC6430310 Electromagnetic Fields And Waves - Cylindrical Ca...
Lecture Notes:  EEEC6430310 Electromagnetic Fields And Waves - Cylindrical Ca...Lecture Notes:  EEEC6430310 Electromagnetic Fields And Waves - Cylindrical Ca...
Lecture Notes: EEEC6430310 Electromagnetic Fields And Waves - Cylindrical Ca...
 
Lecture Notes: EEEC6440315 Communication Systems - Time Frequency Analysis -...
Lecture Notes:  EEEC6440315 Communication Systems - Time Frequency Analysis -...Lecture Notes:  EEEC6440315 Communication Systems - Time Frequency Analysis -...
Lecture Notes: EEEC6440315 Communication Systems - Time Frequency Analysis -...
 
Mini Project 1: Impedance Matching With A Single Stub Tuner
Mini Project 1:  Impedance Matching With A Single Stub TunerMini Project 1:  Impedance Matching With A Single Stub Tuner
Mini Project 1: Impedance Matching With A Single Stub Tuner
 

Último

ANG SEKTOR NG agrikultura.pptx QUARTER 4
ANG SEKTOR NG agrikultura.pptx QUARTER 4ANG SEKTOR NG agrikultura.pptx QUARTER 4
ANG SEKTOR NG agrikultura.pptx QUARTER 4MiaBumagat1
 
Virtual-Orientation-on-the-Administration-of-NATG12-NATG6-and-ELLNA.pdf
Virtual-Orientation-on-the-Administration-of-NATG12-NATG6-and-ELLNA.pdfVirtual-Orientation-on-the-Administration-of-NATG12-NATG6-and-ELLNA.pdf
Virtual-Orientation-on-the-Administration-of-NATG12-NATG6-and-ELLNA.pdfErwinPantujan2
 
Science 7 Quarter 4 Module 2: Natural Resources.pptx
Science 7 Quarter 4 Module 2: Natural Resources.pptxScience 7 Quarter 4 Module 2: Natural Resources.pptx
Science 7 Quarter 4 Module 2: Natural Resources.pptxMaryGraceBautista27
 
Culture Uniformity or Diversity IN SOCIOLOGY.pptx
Culture Uniformity or Diversity IN SOCIOLOGY.pptxCulture Uniformity or Diversity IN SOCIOLOGY.pptx
Culture Uniformity or Diversity IN SOCIOLOGY.pptxPoojaSen20
 
call girls in Kamla Market (DELHI) 🔝 >༒9953330565🔝 genuine Escort Service 🔝✔️✔️
call girls in Kamla Market (DELHI) 🔝 >༒9953330565🔝 genuine Escort Service 🔝✔️✔️call girls in Kamla Market (DELHI) 🔝 >༒9953330565🔝 genuine Escort Service 🔝✔️✔️
call girls in Kamla Market (DELHI) 🔝 >༒9953330565🔝 genuine Escort Service 🔝✔️✔️9953056974 Low Rate Call Girls In Saket, Delhi NCR
 
Inclusivity Essentials_ Creating Accessible Websites for Nonprofits .pdf
Inclusivity Essentials_ Creating Accessible Websites for Nonprofits .pdfInclusivity Essentials_ Creating Accessible Websites for Nonprofits .pdf
Inclusivity Essentials_ Creating Accessible Websites for Nonprofits .pdfTechSoup
 
ACC 2024 Chronicles. Cardiology. Exam.pdf
ACC 2024 Chronicles. Cardiology. Exam.pdfACC 2024 Chronicles. Cardiology. Exam.pdf
ACC 2024 Chronicles. Cardiology. Exam.pdfSpandanaRallapalli
 
Student Profile Sample - We help schools to connect the data they have, with ...
Student Profile Sample - We help schools to connect the data they have, with ...Student Profile Sample - We help schools to connect the data they have, with ...
Student Profile Sample - We help schools to connect the data they have, with ...Seán Kennedy
 
AUDIENCE THEORY -CULTIVATION THEORY - GERBNER.pptx
AUDIENCE THEORY -CULTIVATION THEORY -  GERBNER.pptxAUDIENCE THEORY -CULTIVATION THEORY -  GERBNER.pptx
AUDIENCE THEORY -CULTIVATION THEORY - GERBNER.pptxiammrhaywood
 
USPS® Forced Meter Migration - How to Know if Your Postage Meter Will Soon be...
USPS® Forced Meter Migration - How to Know if Your Postage Meter Will Soon be...USPS® Forced Meter Migration - How to Know if Your Postage Meter Will Soon be...
USPS® Forced Meter Migration - How to Know if Your Postage Meter Will Soon be...Postal Advocate Inc.
 
ENGLISH 7_Q4_LESSON 2_ Employing a Variety of Strategies for Effective Interp...
ENGLISH 7_Q4_LESSON 2_ Employing a Variety of Strategies for Effective Interp...ENGLISH 7_Q4_LESSON 2_ Employing a Variety of Strategies for Effective Interp...
ENGLISH 7_Q4_LESSON 2_ Employing a Variety of Strategies for Effective Interp...JhezDiaz1
 
Barangay Council for the Protection of Children (BCPC) Orientation.pptx
Barangay Council for the Protection of Children (BCPC) Orientation.pptxBarangay Council for the Protection of Children (BCPC) Orientation.pptx
Barangay Council for the Protection of Children (BCPC) Orientation.pptxCarlos105
 
What is Model Inheritance in Odoo 17 ERP
What is Model Inheritance in Odoo 17 ERPWhat is Model Inheritance in Odoo 17 ERP
What is Model Inheritance in Odoo 17 ERPCeline George
 
THEORIES OF ORGANIZATION-PUBLIC ADMINISTRATION
THEORIES OF ORGANIZATION-PUBLIC ADMINISTRATIONTHEORIES OF ORGANIZATION-PUBLIC ADMINISTRATION
THEORIES OF ORGANIZATION-PUBLIC ADMINISTRATIONHumphrey A Beña
 
How to Add Barcode on PDF Report in Odoo 17
How to Add Barcode on PDF Report in Odoo 17How to Add Barcode on PDF Report in Odoo 17
How to Add Barcode on PDF Report in Odoo 17Celine George
 
Choosing the Right CBSE School A Comprehensive Guide for Parents
Choosing the Right CBSE School A Comprehensive Guide for ParentsChoosing the Right CBSE School A Comprehensive Guide for Parents
Choosing the Right CBSE School A Comprehensive Guide for Parentsnavabharathschool99
 
Procuring digital preservation CAN be quick and painless with our new dynamic...
Procuring digital preservation CAN be quick and painless with our new dynamic...Procuring digital preservation CAN be quick and painless with our new dynamic...
Procuring digital preservation CAN be quick and painless with our new dynamic...Jisc
 
Visit to a blind student's school🧑‍🦯🧑‍🦯(community medicine)
Visit to a blind student's school🧑‍🦯🧑‍🦯(community medicine)Visit to a blind student's school🧑‍🦯🧑‍🦯(community medicine)
Visit to a blind student's school🧑‍🦯🧑‍🦯(community medicine)lakshayb543
 
INTRODUCTION TO CATHOLIC CHRISTOLOGY.pptx
INTRODUCTION TO CATHOLIC CHRISTOLOGY.pptxINTRODUCTION TO CATHOLIC CHRISTOLOGY.pptx
INTRODUCTION TO CATHOLIC CHRISTOLOGY.pptxHumphrey A Beña
 

Último (20)

ANG SEKTOR NG agrikultura.pptx QUARTER 4
ANG SEKTOR NG agrikultura.pptx QUARTER 4ANG SEKTOR NG agrikultura.pptx QUARTER 4
ANG SEKTOR NG agrikultura.pptx QUARTER 4
 
Virtual-Orientation-on-the-Administration-of-NATG12-NATG6-and-ELLNA.pdf
Virtual-Orientation-on-the-Administration-of-NATG12-NATG6-and-ELLNA.pdfVirtual-Orientation-on-the-Administration-of-NATG12-NATG6-and-ELLNA.pdf
Virtual-Orientation-on-the-Administration-of-NATG12-NATG6-and-ELLNA.pdf
 
Science 7 Quarter 4 Module 2: Natural Resources.pptx
Science 7 Quarter 4 Module 2: Natural Resources.pptxScience 7 Quarter 4 Module 2: Natural Resources.pptx
Science 7 Quarter 4 Module 2: Natural Resources.pptx
 
Culture Uniformity or Diversity IN SOCIOLOGY.pptx
Culture Uniformity or Diversity IN SOCIOLOGY.pptxCulture Uniformity or Diversity IN SOCIOLOGY.pptx
Culture Uniformity or Diversity IN SOCIOLOGY.pptx
 
call girls in Kamla Market (DELHI) 🔝 >༒9953330565🔝 genuine Escort Service 🔝✔️✔️
call girls in Kamla Market (DELHI) 🔝 >༒9953330565🔝 genuine Escort Service 🔝✔️✔️call girls in Kamla Market (DELHI) 🔝 >༒9953330565🔝 genuine Escort Service 🔝✔️✔️
call girls in Kamla Market (DELHI) 🔝 >༒9953330565🔝 genuine Escort Service 🔝✔️✔️
 
Inclusivity Essentials_ Creating Accessible Websites for Nonprofits .pdf
Inclusivity Essentials_ Creating Accessible Websites for Nonprofits .pdfInclusivity Essentials_ Creating Accessible Websites for Nonprofits .pdf
Inclusivity Essentials_ Creating Accessible Websites for Nonprofits .pdf
 
ACC 2024 Chronicles. Cardiology. Exam.pdf
ACC 2024 Chronicles. Cardiology. Exam.pdfACC 2024 Chronicles. Cardiology. Exam.pdf
ACC 2024 Chronicles. Cardiology. Exam.pdf
 
Student Profile Sample - We help schools to connect the data they have, with ...
Student Profile Sample - We help schools to connect the data they have, with ...Student Profile Sample - We help schools to connect the data they have, with ...
Student Profile Sample - We help schools to connect the data they have, with ...
 
FINALS_OF_LEFT_ON_C'N_EL_DORADO_2024.pptx
FINALS_OF_LEFT_ON_C'N_EL_DORADO_2024.pptxFINALS_OF_LEFT_ON_C'N_EL_DORADO_2024.pptx
FINALS_OF_LEFT_ON_C'N_EL_DORADO_2024.pptx
 
AUDIENCE THEORY -CULTIVATION THEORY - GERBNER.pptx
AUDIENCE THEORY -CULTIVATION THEORY -  GERBNER.pptxAUDIENCE THEORY -CULTIVATION THEORY -  GERBNER.pptx
AUDIENCE THEORY -CULTIVATION THEORY - GERBNER.pptx
 
USPS® Forced Meter Migration - How to Know if Your Postage Meter Will Soon be...
USPS® Forced Meter Migration - How to Know if Your Postage Meter Will Soon be...USPS® Forced Meter Migration - How to Know if Your Postage Meter Will Soon be...
USPS® Forced Meter Migration - How to Know if Your Postage Meter Will Soon be...
 
ENGLISH 7_Q4_LESSON 2_ Employing a Variety of Strategies for Effective Interp...
ENGLISH 7_Q4_LESSON 2_ Employing a Variety of Strategies for Effective Interp...ENGLISH 7_Q4_LESSON 2_ Employing a Variety of Strategies for Effective Interp...
ENGLISH 7_Q4_LESSON 2_ Employing a Variety of Strategies for Effective Interp...
 
Barangay Council for the Protection of Children (BCPC) Orientation.pptx
Barangay Council for the Protection of Children (BCPC) Orientation.pptxBarangay Council for the Protection of Children (BCPC) Orientation.pptx
Barangay Council for the Protection of Children (BCPC) Orientation.pptx
 
What is Model Inheritance in Odoo 17 ERP
What is Model Inheritance in Odoo 17 ERPWhat is Model Inheritance in Odoo 17 ERP
What is Model Inheritance in Odoo 17 ERP
 
THEORIES OF ORGANIZATION-PUBLIC ADMINISTRATION
THEORIES OF ORGANIZATION-PUBLIC ADMINISTRATIONTHEORIES OF ORGANIZATION-PUBLIC ADMINISTRATION
THEORIES OF ORGANIZATION-PUBLIC ADMINISTRATION
 
How to Add Barcode on PDF Report in Odoo 17
How to Add Barcode on PDF Report in Odoo 17How to Add Barcode on PDF Report in Odoo 17
How to Add Barcode on PDF Report in Odoo 17
 
Choosing the Right CBSE School A Comprehensive Guide for Parents
Choosing the Right CBSE School A Comprehensive Guide for ParentsChoosing the Right CBSE School A Comprehensive Guide for Parents
Choosing the Right CBSE School A Comprehensive Guide for Parents
 
Procuring digital preservation CAN be quick and painless with our new dynamic...
Procuring digital preservation CAN be quick and painless with our new dynamic...Procuring digital preservation CAN be quick and painless with our new dynamic...
Procuring digital preservation CAN be quick and painless with our new dynamic...
 
Visit to a blind student's school🧑‍🦯🧑‍🦯(community medicine)
Visit to a blind student's school🧑‍🦯🧑‍🦯(community medicine)Visit to a blind student's school🧑‍🦯🧑‍🦯(community medicine)
Visit to a blind student's school🧑‍🦯🧑‍🦯(community medicine)
 
INTRODUCTION TO CATHOLIC CHRISTOLOGY.pptx
INTRODUCTION TO CATHOLIC CHRISTOLOGY.pptxINTRODUCTION TO CATHOLIC CHRISTOLOGY.pptx
INTRODUCTION TO CATHOLIC CHRISTOLOGY.pptx
 

Lecture Notes: EEEC4340318 Instrumentation and Control Systems - Stability and Routh-Hurwitz Condition

  • 1. EEEC4340318 INSTRUMENTATION AND CONTROL SYSTEMS Stability And Routh-Hurwitz Condition FACULTY OF ENGINEERING AND COMPUTER TECHNOLOGY DIPLOMA IN ELECTRICALAND ELECTRONIC ENGINEERING Ravandran Muttiah BEng (Hons) MSc MIET
  • 2. 1 Stability A systems is said to be stable if all bounded inputs 𝑟 𝑡 give rise to bounded outputs 𝑦 𝑡 . Figure 1 𝑌 𝑠 𝑅 𝑠 𝐺 𝑠
  • 3. 2 Conditions For Stability 𝑦 𝑡 = −∞ ∞ 𝑔 𝜏 𝑟 𝑡 − 𝜏 d𝜏 Let 𝑟 𝑡 be such that 𝑟 𝑡 ≤ 𝑟 𝑦 𝑡 = −∞ ∞ 𝑔 𝜏 𝑟 𝑡 − 𝜏 d𝜏 ≤ −∞ ∞ 𝑔 𝜏 𝑟 𝑡 − 𝜏 d𝜏 ≤ 𝑟 −∞ ∞ 𝑔 𝜏 d𝜏 Using this: system 𝐺 𝑠 is stable if −∞ ∞ 𝑔 𝜏 d𝜏 is finite Figure 2 𝑌 𝑠 𝑅 𝑠 𝐺 𝑠
  • 4. 3 Condition In Terms Of Poles ? We want −∞ ∞ 𝑔 𝜏 d𝜏 to be finite Can we determine this from 𝐺 𝑠 We can write a general rational transfer function in the form 𝐺 𝑠 = 𝐾 𝑖 𝑠 + 𝑧𝑖 𝑠𝑁 𝑘 𝑠 + 𝜎𝑘 𝑚 𝑠2 + 2𝛼𝑚𝑠 + 𝛼𝑚 2 + 𝜔𝑚 2 Poles: 0, −𝜎𝑘, −𝛼𝑚 ± j𝜔𝑚 Assuming 𝑁 = 0 and no repeated roots, the impulse response is, 𝑔 𝑡 = 𝑘 𝐴𝑘𝑒−𝜎𝑘𝑡 + 𝑚 𝐵𝑚𝑒−𝛼𝑚𝑡 sin 𝜔𝑚𝑡 + 𝜃𝑚 Stability requires 𝑔 𝑡 d𝑡 to be bounded; that requires 𝜎𝑘 > 0, 𝜎𝑚 > 0 In fact, system is stable if poles have negative real parts.
  • 5. 4 Marginal Stability Consider integrator: 𝐺 𝑠 = 1 s ; simple pole at origin, 𝑦 𝑡 = −∞ ∞ 𝑟 𝑡 d𝑡 If 𝑟 𝑡 = cos 𝑡 , which is bounded, then 𝑦 𝑡 = sin 𝑡 . Bounded. If 𝑟 𝑡 = 𝑢 𝑡 , which is bounded, then 𝑦 𝑡 = 𝑡. Not bounded. Consider 𝐺 𝑠 = 1 𝑠2+1 , simple poles at 𝑠 = ±j1 Unit step response: 𝑢 𝑡 − cos 𝑡 . Bounded What if 𝑟 𝑡 is a sinusoid of frequency 1 2π Hz ? Not bounded. If 𝐺 𝑠 has a pole with positive real part, or a repeated pole on j𝜔-axis, output is always unbounded.
  • 6. 5 Routh-Hurwitz Condition We have seen how to determine stability from the poles. Much easier than having to find impulse response and then determining if 𝑔 𝜏 d𝜏 < ∞ Can we determine stability without having to determine the poles ? Yes! Routh-Hurwitz condition.
  • 7. 6 Let 𝐺 𝑠 = 𝑝 𝑠 𝑞 𝑠 , where 𝑞 𝑠 = 𝑎𝑛𝑠𝑛 + 𝑎𝑛−1𝑠𝑛−1 + ⋯ 𝑎1𝑠 + 𝑎0 = 𝑎𝑛 𝑠 − 𝑟1 𝑠 − 𝑟2 ⋯ 𝑠 − 𝑟𝑛 where 𝑟𝑖 are the roots of 𝑞 𝑠 = 0. By multiplying out, 𝑞 𝑠 = 0 can be written as, 𝑞 𝑠 = 𝑎𝑛𝑠𝑛 − 𝑎𝑛 𝑟1 + 𝑟2 + ⋯ + 𝑟𝑛 𝑠𝑛−1 + 𝑎𝑛 𝑟1𝑟2 + 𝑟2𝑟3 + ⋯ 𝑠𝑛−2 − 𝑎𝑛 𝑟1𝑟2𝑟3 + 𝑟1𝑟2𝑟4 + ⋯ 𝑠𝑛−3 + ⋯ + −1 𝑛 𝑎𝑛 𝑟1𝑟2𝑟3 ⋯ 𝑟𝑛 = 0 If all 𝑟𝑖 are real and in left half plane, what is sign of coefficients of 𝑠𝑘 the same!
  • 8. 7 That observation leads to a necessary condition. Hence, not that useful for design. A more sophisticated analysis leads to the Routh-Hurwitz condition, which is necessary and sufficient. Hence, can be quite useful for design.
  • 9. 8 Routh-Hurwitz Condition: A First Look Consider 𝐺 𝑠 = 𝑝 𝑠 𝑞 𝑠 . Poles are solutions to 𝑞 𝑠 = 0; i.e., 𝑎𝑛𝑠𝑛 + 𝑎𝑛−1𝑠𝑛−1 + 𝑎𝑛−2𝑠𝑛−2 + ⋯ + 𝑎1𝑠 + 𝑎0 = 0 Construct a table of the form, 𝑠𝑛 𝑠𝑛−1 𝑠𝑛−2 𝑠𝑛−3 ⋮ 𝑠0 𝑎𝑛 𝑎𝑛−1 𝑏𝑛−1 𝑐𝑛−1 ⋮ ℎ𝑛−1 𝑎𝑛−2 𝑎𝑛−3 𝑏𝑛−3 𝑐𝑛−3 ⋮ 𝑎𝑛−4 ⋯ 𝑎𝑛−5 ⋯ 𝑏𝑛−5 ⋯ 𝑐𝑛−5 ⋯ ⋮ ⋯ where, 𝑏𝑛−1 = 𝑎𝑛−1𝑎𝑛−2 − 𝑎𝑛𝑎𝑛−3 𝑎𝑛−1 = −1 𝑎𝑛−1 𝑎𝑛 𝑎𝑛−2 𝑎𝑛−1 𝑎𝑛−3 𝑏𝑛−3 = −1 𝑎𝑛−1 𝑎𝑛 𝑎𝑛−4 𝑎𝑛−1 𝑎𝑛−5 𝑐𝑛−1 = −1 𝑏𝑛−1 𝑎𝑛−1 𝑎𝑛−3 𝑏𝑛−1 𝑏𝑛−3
  • 10. 9 Now consider the table we have just constructed. 𝑠𝑛 𝑠𝑛−1 𝑠𝑛−2 𝑠𝑛−3 ⋮ 𝑠0 𝑎𝑛 𝑎𝑛−1 𝑏𝑛−1 𝑐𝑛−1 ⋮ ℎ𝑛−1 𝑎𝑛−2 𝑎𝑛−3 𝑏𝑛−3 𝑐𝑛−3 ⋮ 𝑎𝑛−4 ⋯ 𝑎𝑛−5 ⋯ 𝑏𝑛−5 ⋯ 𝑐𝑛−5 ⋯ ⋮ ⋯ Loosely speaking: Number of roots in the right half plane is equal to the number of sign changes in the first column of the table. Stability if no sign changes in the first column. Now let’s move towards a more sophisticated statement.
  • 11. 10 Let 𝐺 𝑠 = 𝑝 𝑠 𝑞 𝑠 where 𝑞 𝑠 = 𝑎𝑛𝑠𝑛 + 𝑎𝑛−1𝑠𝑛−1 + ⋯ 𝑎1𝑠 + 𝑎0 System is stable if all poles of 𝐺 𝑠 have negative real parts. Recall, poles are solutions to 𝑞 𝑠 = 0. Can we find a necessary and sufficient condition that depends only on 𝑎𝑘 so that we don’t have to solve 𝑞 𝑠 = 0 ? Stability (Revision) Figure 3 𝑌 𝑠 𝑅 𝑠 𝐺 𝑠
  • 12. 11 (1) Consider 𝑞 𝑠 with 𝑎𝑛 > 0 𝑎𝑛𝑠𝑛 + 𝑎𝑛−1𝑠𝑛−1 + 𝑎𝑛−2𝑠𝑛−2 + ⋯ 𝑎1𝑠 + 𝑎0 = 0 (2) Construct a table of the form, Row 𝑛 Row 𝑛 − 1 Row 𝑛 − 2 Row 𝑛 − 3 ⋮ Row 0 𝑎𝑛 𝑎𝑛−1 𝑏𝑛−1 𝑐𝑛−1 ⋮ ℎ𝑛−1 𝑎𝑛−2 𝑎𝑛−3 𝑏𝑛−3 𝑐𝑛−3 ⋮ 𝑎𝑛−4 ⋯ 𝑎𝑛−5 ⋯ 𝑏𝑛−5 ⋯ 𝑐𝑛−5 ⋯ ⋮ ⋯ Procedure provided on the following slides. (3) Count the sign changes in the first column. (4) That is the number of roots in the right half plane. Stability (poles in Left Half Plane if 𝑎𝑘 > 0 and all terms in first column > 0 Routh-Hurwitz Condition
  • 13. 12 References (1) Tim Davidson, Introduction to Linear Control Systems, McMaster University, 2018.