nonlinear system Signals & systems Output signals Input signals Dynamic system
|
|
- Hubert Hawkins
- 5 years ago
- Views:
Transcription
1 nonlinear ssem Signals & ssems Inpu signals Dnamic ssem Oupu signals nonlinear ssems b meiling chen 009
2 nonlinear ssem Signal Classiicaion Coninuous signal Discree signal nonlinear ssems b meiling chen 009
3 Ssem classiicaion nonlinear ssem Finie-dimensional ssem lumped-parameers ssem described b dierenial equaions Linear ssems and nonlinear ssems Coninuous ime and discree ime ssems Time-invarian and ime varing ssems Ininie-dimensional ssem disribued parameers ssem described b parial dierenial equaions Power ransmission line Anennas Hea conducion Opical iber ec. nonlinear ssems b meiling chen 009
4 Coninuous-ime ssem ---characerized b dierenial equaions Deiniion: inpu and oupu o he ssem are coninuous uncions o he coninuous variable ime. nonlinear ssem Discree-ime ssem ---characerized b dieren equaions Deiniion: inpu and oupu o he ssem change a onl discree insans o ime. nonlinear ssems b meiling chen 009 4
5 nonlinear ssem Linear ime invarian LTI--coninuous Described b a linear dierenial equaion in ime domain can be ranserred o linear algebra orm b using Laplace ransorm. nonlinear ssems b meiling chen 009 5
6 nonlinear ssems b meiling chen LTI ssem Ordinar Linear dierenial equaion Z k k a k a m k a k b k b n k b m n 0 0 L L Ordinar Linear dierence equaion Coninuous ssem discree ssem nonlinear ssem
7 nonlinear ssems b meiling chen Linear ime-varing Nonlinear ime-invarian Linear ime-invarian Nonlinear ime-varing eamples nonlinear ssem
8 Linear ssem nonlinear ssem Deiniion: A ssem is linear i superposiion principle is saisied Lineari : a homogeneous principle muliplicaion b addiion principle c superposiion principle > a b nonlinear ssems b meiling chen 009 8
9 nonlinear ssems b meiling chen ] ] ] ] ] 5 ] ] ] ] ] ] ] 5 ] ] 5 5 ] 5 ] ] ] ] k k k k k k k k k Muliplicaion law saisied Addiion law saisied
10 Nonlinear ssem nonlinear ssems b meiling chen 009 0
11 Common nonlinear phenomena Ideal rela sgn u, 0,, u > 0 u 0 u < 0 Sauraion Eample: ampliier Ideal sauraion: sa u u sgn u u u > nonlinear ssems b meiling chen 009
12 Dead zone Eample: ampliier wih low inpu signals nonlinear ssems b meiling chen 009
13 Common nonlinear phenomena Back lash Eample:. Gear gap. hseresis loop 4 Dead zone Eample: ampliier wih low inpu signals nonlinear ssems b meiling chen 009
14 Common nonlinear phenomena 5 hseresis Eample: window comparaor/schmi rigger 6 parabola nonlinear ssems b meiling chen 009 4
15 Nonlinear ssem eamples nonlinear ssem Pendulum equaion ml && θ kl & θ mg sin θ 0 l θ m ml & θ kl & θ mgθ 0 For small θ nonlinear ssems b meiling chen 009 5
16 Nonlinear spring equaion m && B& k k 0 k m Nonlinear spring linear nonlinear B a hard spring k > 0 b so spring k < 0 nonlinear ssems b meiling chen 009 6
17 c linear spring k 0 k 0 ied k < 0 k > 0 Jump resonance : nonlinear ssem wih orce k > 0 m&& B& k k p cos nonlinear ssems b meiling chen 009 7
18 k < 0 m&& B& k k p cos 4 Harmonic oscillaion u A0 sin Linear ssem Ao G j sin G j] u A0 sin Nonlinear ssem A A sin θ ] sin θ ] L A sin θ ] nonlinear ssems b meiling chen 009 8
19 nonlinear ssems b meiling chen Eample: A u sin 0 u A A A u sin 4 sin 4 sin Subharmonic oscillaion Nonlinear ssem A u sin 0 L ] sin ] sin ] sin θ θ θ A A A
20 6 Limi ccle Eample: Van der pol s equaion & ε & & 0 ε > 0 << ε < 0 >> ε > 0 Sable limi ccle nonlinear ssems b meiling chen 009 0
21 & ε & 0 & << ε > 0 ε > 0 >> ε < 0 Unsable limi ccle nonlinear ssems b meiling chen 009
Theory of! Partial Differential Equations!
hp://www.nd.edu/~gryggva/cfd-course/! Ouline! Theory o! Parial Dierenial Equaions! Gréar Tryggvason! Spring 011! Basic Properies o PDE!! Quasi-linear Firs Order Equaions! - Characerisics! - Linear and
More informationTheory of! Partial Differential Equations-I!
hp://users.wpi.edu/~grear/me61.hml! Ouline! Theory o! Parial Dierenial Equaions-I! Gréar Tryggvason! Spring 010! Basic Properies o PDE!! Quasi-linear Firs Order Equaions! - Characerisics! - Linear and
More informationEA Properties of NCGPC applied to nonlinear SISO systems with a relative degree one or two M. DABO, N. LANGLOIS & H. CHAFOUK
EA 4353 Properies o NCGPC applied o nonlinear SISO ssems wi a relaive degree one or wo. DABO, N. ANGOIS H. CHAFOU G Commande Prédicive Non inéaire ENSA, Paris 3 janvier Ouline Relaive degree o nonlinear
More informationQ1) [20 points] answer for the following questions (ON THIS SHEET):
Dr. Anas Al Tarabsheh The Hashemie Universiy Elecrical and Compuer Engineering Deparmen (Makeup Exam) Signals and Sysems Firs Semeser 011/01 Final Exam Dae: 1/06/01 Exam Duraion: hours Noe: means convoluion
More informationConvolution. Lecture #6 2CT.3 8. BME 333 Biomedical Signals and Systems - J.Schesser
Convoluion Lecure #6 C.3 8 Deiniion When we compue he ollowing inegral or τ and τ we say ha he we are convoluing wih g d his says: ae τ, lip i convolve in ime -τ, hen displace i in ime by seconds -τ, and
More informationEELE Lecture 8 Example of Fourier Series for a Triangle from the Fourier Transform. Homework password is: 14445
EELE445-4 Lecure 8 Eample o Fourier Series or a riangle rom he Fourier ransorm Homework password is: 4445 3 4 EELE445-4 Lecure 8 LI Sysems and Filers 5 LI Sysem 6 3 Linear ime-invarian Sysem Deiniion o
More informationChapter 1 Fundamental Concepts
Chaper 1 Fundamenal Conceps 1 Signals A signal is a paern of variaion of a physical quaniy, ofen as a funcion of ime (bu also space, disance, posiion, ec). These quaniies are usually he independen variables
More informationCharacteristics of Linear System
Characerisics o Linear Sysem h g h : Impulse response F G : Frequency ranser uncion Represenaion o Sysem in ime an requency. Low-pass iler g h G F he requency ranser uncion is he Fourier ransorm o he impulse
More informationh[n] is the impulse response of the discrete-time system:
Definiion Examples Properies Memory Inveribiliy Causaliy Sabiliy Time Invariance Lineariy Sysems Fundamenals Overview Definiion of a Sysem x() h() y() x[n] h[n] Sysem: a process in which inpu signals are
More informationContinuous Time Linear Time Invariant (LTI) Systems. Dr. Ali Hussein Muqaibel. Introduction
/9/ Coninuous Time Linear Time Invarian (LTI) Sysems Why LTI? Inroducion Many physical sysems. Easy o solve mahemaically Available informaion abou analysis and design. We can apply superposiion LTI Sysem
More information(1) (2) Differentiation of (1) and then substitution of (3) leads to. Therefore, we will simply consider the second-order linear system given by (4)
Phase Plane Analysis of Linear Sysems Adaped from Applied Nonlinear Conrol by Sloine and Li The general form of a linear second-order sysem is a c b d From and b bc d a Differeniaion of and hen subsiuion
More informationCOSC 3361 Numerical Analysis I Ordinary Differential Equations (I) - Introduction
COSC 336 Numerial Analsis I Ordinar Dierenial Equaions I - Inroduion Edgar Gabriel Fall 5 COSC 336 Numerial Analsis I Edgar Gabriel Terminolog Dierenial equaions: equaions onaining e derivaive o a union
More informationMA 366 Review - Test # 1
MA 366 Review - Tes # 1 Fall 5 () Resuls from Calculus: differeniaion formulas, implici differeniaion, Chain Rule; inegraion formulas, inegraion b pars, parial fracions, oher inegraion echniques. (1) Order
More informationSignals and Systems Linear Time-Invariant (LTI) Systems
Signals and Sysems Linear Time-Invarian (LTI) Sysems Chang-Su Kim Discree-Time LTI Sysems Represening Signals in Terms of Impulses Sifing propery 0 x[ n] x[ k] [ n k] k x[ 2] [ n 2] x[ 1] [ n1] x[0] [
More informationDynamic Effects of Feedback Control!
Dynamic Effecs of Feedback Conrol! Rober Sengel! Roboics and Inelligen Sysems MAE 345, Princeon Universiy, 2017 Inner, Middle, and Ouer Feedback Conrol Loops Sep Response of Linear, Time- Invarian (LTI)
More informationNonlinear spring-mass system
Basic phenomenology of simple nonlinear vibraion (free and forced) Manoj Srinivasan (6) Nonlinear spring-mass sysem Damper Spring Mass Hardening Sofening O No damping graviy g lengh l A mass m Do.8.6..
More informationSignals and Systems Profs. Byron Yu and Pulkit Grover Fall Midterm 1 Solutions
8-90 Signals and Sysems Profs. Byron Yu and Pulki Grover Fall 07 Miderm Soluions Name: Andrew ID: Problem Score Max 0 8 4 6 5 0 6 0 7 8 9 0 6 Toal 00 Miderm Soluions. (0 poins) Deermine wheher he following
More informationChapter 1 Random Process
Chaper Random Process.0 Probabiliies is considered an imporan background or analysis and design o communicaions sysems. Inroducion Physical phenomenon Deerminisic model : No uncerainy abou is imedependen
More informationCS537. Numerical Analysis
CS57 Numerical Analsis Lecure Numerical Soluion o Ordinar Dierenial Equaions Proessor Jun Zang Deparmen o Compuer Science Universi o enuck Leingon, Y 4006 0046 April 5, 00 Wa is ODE An Ordinar Dierenial
More informatione 2t u(t) e 2t u(t) =?
EE : Signals, Sysems, and Transforms Fall 7. Skech he convoluion of he following wo signals. Tes No noes, closed book. f() Show your work. Simplify your answers. g(). Using he convoluion inegral, find
More informationInstitute for Mathematical Methods in Economics. University of Technology Vienna. Singapore, May Manfred Deistler
MULTIVARIATE TIME SERIES ANALYSIS AND FORECASTING Manfred Deisler E O S Economerics and Sysems Theory Insiue for Mahemaical Mehods in Economics Universiy of Technology Vienna Singapore, May 2004 Inroducion
More informationUniversity of Cyprus Biomedical Imaging and Applied Optics. Appendix. DC Circuits Capacitors and Inductors AC Circuits Operational Amplifiers
Universiy of Cyprus Biomedical Imaging and Applied Opics Appendix DC Circuis Capaciors and Inducors AC Circuis Operaional Amplifiers Circui Elemens An elecrical circui consiss of circui elemens such as
More informationF (u) du. or f(t) = t
8.3 Topic 9: Impulses and dela funcions. Auor: Jeremy Orloff Reading: EP 4.6 SN CG.3-4 pp.2-5. Warmup discussion abou inpu Consider e rae equaion d + k = f(). To be specific, assume is in unis of d kilograms.
More information4/9/2012. Signals and Systems KX5BQY EE235. Today s menu. System properties
Signals and Sysems hp://www.youube.com/v/iv6fo KX5BQY EE35 oday s menu Good weeend? Sysem properies iy Superposiion! Sysem properies iy: A Sysem is if i mees he following wo crieria: If { x( )} y( ) and
More informationSolutions - Midterm Exam
DEPARTMENT OF ELECTRICAL AND COMPUTER ENGINEERING, THE UNIVERITY OF NEW MEXICO ECE-34: ignals and ysems ummer 203 PROBLEM (5 PT) Given he following LTI sysem: oluions - Miderm Exam a) kech he impulse response
More informationLaplace Transforms. Examples. Is this equation differential? y 2 2y + 1 = 0, y 2 2y + 1 = 0, (y ) 2 2y + 1 = cos x,
Laplace Transforms Definiion. An ordinary differenial equaion is an equaion ha conains one or several derivaives of an unknown funcion which we call y and which we wan o deermine from he equaion. The equaion
More informationSOLUTIONS TO ECE 3084
SOLUTIONS TO ECE 384 PROBLEM 2.. For each sysem below, specify wheher or no i is: (i) memoryless; (ii) causal; (iii) inverible; (iv) linear; (v) ime invarian; Explain your reasoning. If he propery is no
More informationElectrical Circuits. 1. Circuit Laws. Tools Used in Lab 13 Series Circuits Damped Vibrations: Energy Van der Pol Circuit
V() R L C 513 Elecrical Circuis Tools Used in Lab 13 Series Circuis Damped Vibraions: Energy Van der Pol Circui A series circui wih an inducor, resisor, and capacior can be represened by Lq + Rq + 1, a
More informationLaplace Transform and its Relation to Fourier Transform
Chaper 6 Laplace Transform and is Relaion o Fourier Transform (A Brief Summary) Gis of he Maer 2 Domains of Represenaion Represenaion of signals and sysems Time Domain Coninuous Discree Time Time () [n]
More informationData Fusion using Kalman Filter. Ioannis Rekleitis
Daa Fusion using Kalman Filer Ioannis Rekleiis Eample of a arameerized Baesian Filer: Kalman Filer Kalman filers (KF represen poserior belief b a Gaussian (normal disribuion A -d Gaussian disribuion is
More informationProblem set 6: Solutions Math 207A, Fall x 0 2 x
Problem se 6: Soluions Mah 7A, Fall 14 1 Skech phase planes of he following linear ssems: 4 a = ; 9 4 b = ; 9 1 c = ; 1 d = ; 4 e = ; f = 1 3 In each case, classif he equilibrium, =, as a saddle poin,
More informationMA Study Guide #1
MA 66 Su Guide #1 (1) Special Tpes of Firs Order Equaions I. Firs Order Linear Equaion (FOL): + p() = g() Soluion : = 1 µ() [ ] µ()g() + C, where µ() = e p() II. Separable Equaion (SEP): dx = h(x) g()
More informationLAPLACE TRANSFORM AND TRANSFER FUNCTION
CHBE320 LECTURE V LAPLACE TRANSFORM AND TRANSFER FUNCTION Professor Dae Ryook Yang Spring 2018 Dep. of Chemical and Biological Engineering 5-1 Road Map of he Lecure V Laplace Transform and Transfer funcions
More informationFinite element method for structural dynamic and stability analyses
Finie elemen mehod for srucural dynamic and sabiliy analyses Module-3 Analysis of equaions of moion Lecure-8: FRF-s and Damping models Prof C S Manohar Deparmen of Civil Engineering IISc, Bangalore 56
More informationModule 4: Time Response of discrete time systems Lecture Note 2
Module 4: Time Response of discree ime sysems Lecure Noe 2 1 Prooype second order sysem The sudy of a second order sysem is imporan because many higher order sysem can be approimaed by a second order model
More informationOpen loop vs Closed Loop. Example: Open Loop. Example: Feedforward Control. Advanced Control I
Open loop vs Closed Loop Advanced I Moor Command Movemen Overview Open Loop vs Closed Loop Some examples Useful Open Loop lers Dynamical sysems CPG (biologically inspired ), Force Fields Feedback conrol
More informationLecture #6: Continuous-Time Signals
EEL5: Discree-Time Signals and Sysems Lecure #6: Coninuous-Time Signals Lecure #6: Coninuous-Time Signals. Inroducion In his lecure, we discussed he ollowing opics:. Mahemaical represenaion and ransormaions
More informationMath Wednesday March 3, , 4.3: First order systems of Differential Equations Why you should expect existence and uniqueness for the IVP
Mah 2280 Wednesda March 3, 200 4., 4.3: Firs order ssems of Differenial Equaions Wh ou should epec eisence and uniqueness for he IVP Eample: Consider he iniial value problem relaed o page 4 of his eserda
More informationCHE302 LECTURE VI DYNAMIC BEHAVIORS OF REPRESENTATIVE PROCESSES. Professor Dae Ryook Yang
CHE30 LECTURE VI DYNAMIC BEHAVIORS OF REPRESENTATIVE PROCESSES Professor Dae Ryook Yang Fall 00 Dep. of Chemical and Biological Engineering orea Universiy CHE30 Process Dynamics and Conrol orea Universiy
More informationDEPARTMENT OF ELECTRICAL AND ELECTRONIC ENGINEERING EXAMINATIONS 2008
[E5] IMPERIAL COLLEGE LONDON DEPARTMENT OF ELECTRICAL AND ELECTRONIC ENGINEERING EXAMINATIONS 008 EEE/ISE PART II MEng BEng and ACGI SIGNALS AND LINEAR SYSTEMS Time allowed: :00 hours There are FOUR quesions
More informationIII-A. Fourier Series Expansion
Summer 28 Signals & Sysems S.F. Hsieh III-A. Fourier Series Expansion Inroducion. Divide and conquer Signals can be decomposed as linear combinaions of: (a) shifed impulses: (sifing propery) Why? x() x()δ(
More informationTopic Astable Circuits. Recall that an astable circuit has two unstable states;
Topic 2.2. Asable Circuis. Learning Objecives: A he end o his opic you will be able o; Recall ha an asable circui has wo unsable saes; Explain he operaion o a circui based on a Schmi inverer, and esimae
More information5. Stochastic processes (1)
Lec05.pp S-38.45 - Inroducion o Teleraffic Theory Spring 2005 Conens Basic conceps Poisson process 2 Sochasic processes () Consider some quaniy in a eleraffic (or any) sysem I ypically evolves in ime randomly
More information( ) = Q 0. ( ) R = R dq. ( t) = I t
ircuis onceps The addiion of a simple capacior o a circui of resisors allows wo relaed phenomena o occur The observaion ha he ime-dependence of a complex waveform is alered by he circui is referred o as
More informationOn Likelihood Ratio and Stochastic Order. for Skew-symmetric Distributions. with a Common Kernel
In. J. Conemp. Mah. Sciences Vol. 8 3 no. 957-967 HIKARI Ld www.m-hikari.com hp://d.doi.org/.988/icms.3.38 On Likelihood Raio and Sochasic Order or Skew-symmeric Disribuions wih a Common Kernel Werner
More information5. Response of Linear Time-Invariant Systems to Random Inputs
Sysem: 5. Response of inear ime-invarian Sysems o Random Inpus 5.. Discree-ime linear ime-invarian (IV) sysems 5... Discree-ime IV sysem IV sysem xn ( ) yn ( ) [ xn ( )] Inpu Signal Sysem S Oupu Signal
More informationCHBE320 LECTURE IV MATHEMATICAL MODELING OF CHEMICAL PROCESS. Professor Dae Ryook Yang
CHBE320 LECTURE IV MATHEMATICAL MODELING OF CHEMICAL PROCESS Professor Dae Ryook Yang Spring 208 Dep. of Chemical and Biological Engineering CHBE320 Process Dynamics and Conrol 4- Road Map of he Lecure
More informationI. OBJECTIVE OF THE EXPERIMENT.
I. OBJECTIVE OF THE EXPERIMENT. Swissmero raels a high speeds hrough a unnel a low pressure. I will hereore undergo ricion ha can be due o: ) Viscosiy o gas (c. "Viscosiy o gas" eperimen) ) The air in
More informationElementary Differential Equations and Boundary Value Problems
Elemenar Differenial Equaions and Boundar Value Problems Boce. & DiPrima 9 h Ediion Chaper 1: Inroducion 1006003 คณ ตศาสตร ว ศวกรรม 3 สาขาว ชาว ศวกรรมคอมพ วเตอร ป การศ กษา 1/2555 ผศ.ดร.อร ญญา ผศ.ดร.สมศ
More informationBasic definitions and relations
Basic definiions and relaions Lecurer: Dmiri A. Molchanov E-mail: molchan@cs.u.fi hp://www.cs.u.fi/kurssi/tlt-2716/ Kendall s noaion for queuing sysems: Arrival processes; Service ime disribuions; Examples.
More informationChapter 4. Truncation Errors
Chaper 4. Truncaion Errors and he Taylor Series Truncaion Errors and he Taylor Series Non-elemenary funcions such as rigonomeric, eponenial, and ohers are epressed in an approimae fashion using Taylor
More informationRepresenting a Signal. Continuous-Time Fourier Methods. Linearity and Superposition. Real and Complex Sinusoids. Jean Baptiste Joseph Fourier
Represening a Signal Coninuous-ime ourier Mehods he convoluion mehod for finding he response of a sysem o an exciaion aes advanage of he lineariy and imeinvariance of he sysem and represens he exciaion
More informationIntroduction to Differential Equations
Math0 Lecture # Introduction to Differential Equations Basic definitions Definition : (What is a DE?) A differential equation (DE) is an equation that involves some of the derivatives (or differentials)
More informationTutorial Sheet #2 discrete vs. continuous functions, periodicity, sampling
2.39 Tuorial Shee #2 discree vs. coninuous uncions, periodiciy, sampling We will encouner wo classes o signals in his class, coninuous-signals and discree-signals. The disinc mahemaical properies o each,
More informationContinuous Time. Time-Domain System Analysis. Impulse Response. Impulse Response. Impulse Response. Impulse Response. ( t) + b 0.
Time-Domain Sysem Analysis Coninuous Time. J. Robers - All Righs Reserved. Edied by Dr. Rober Akl 1. J. Robers - All Righs Reserved. Edied by Dr. Rober Akl 2 Le a sysem be described by a 2 y ( ) + a 1
More informationREPETITION before the exam PART 2, Transform Methods. Laplace transforms: τ dτ. L1. Derive the formulas : L2. Find the Laplace transform F(s) if.
Tranform Mhod and Calculu of Svral Variabl H7, p Lcurr: Armin Halilovic KTH, Campu Haning E-mail: armin@dkh, wwwdkh/armin REPETITION bfor h am PART, Tranform Mhod Laplac ranform: L Driv h formula : a L[
More informationChapter 3 Boundary Value Problem
Chaper 3 Boundary Value Problem A boundary value problem (BVP) is a problem, ypically an ODE or a PDE, which has values assigned on he physical boundary of he domain in which he problem is specified. Le
More informationHybrid Control and Switched Systems. Lecture #3 What can go wrong? Trajectories of hybrid systems
Hybrid Conrol and Swiched Sysems Lecure #3 Wha can go wrong? Trajecories of hybrid sysems João P. Hespanha Universiy of California a Sana Barbara Summary 1. Trajecories of hybrid sysems: Soluion o a hybrid
More informationOutline Chapter 2: Signals and Systems
Ouline Chaper 2: Signals and Sysems Signals Basics abou Signal Descripion Fourier Transform Harmonic Decomposiion of Periodic Waveforms (Fourier Analysis) Definiion and Properies of Fourier Transform Imporan
More informationEECE 301 Signals & Systems Prof. Mark Fowler
EECE 31 Signals & Sysems Prof. Mar Fowler Noe Se #1 C-T Signals: Circuis wih Periodic Sources 1/1 Solving Circuis wih Periodic Sources FS maes i easy o find he response of an RLC circui o a periodic source!
More informationReview of EM and Introduction to FDTD
1/13/016 5303 lecromagneic Analsis Using Finie Difference Time Domain Lecure #4 Review of M and Inroducion o FDTD Lecure 4These noes ma conain coprighed maerial obained under fair use rules. Disribuion
More informationMath Week 14 April 16-20: sections first order systems of linear differential equations; 7.4 mass-spring systems.
Mah 2250-004 Week 4 April 6-20 secions 7.-7.3 firs order sysems of linear differenial equaions; 7.4 mass-spring sysems. Mon Apr 6 7.-7.2 Sysems of differenial equaions (7.), and he vecor Calculus we need
More informationUNIVERSITY OF TRENTO MEASUREMENTS OF TRANSIENT PHENOMENA WITH DIGITAL OSCILLOSCOPES. Antonio Moschitta, Fabrizio Stefani, Dario Petri.
UNIVERSIY OF RENO DEPARMEN OF INFORMAION AND COMMUNICAION ECHNOLOGY 385 Povo reno Ialy Via Sommarive 4 hp://www.di.unin.i MEASUREMENS OF RANSIEN PHENOMENA WIH DIGIAL OSCILLOSCOPES Anonio Moschia Fabrizio
More informationStability analysis of nonsmooth limit cycles with applications from power electronics
Inernaional Workshop on Resonance Oscillaions & Sabiliy of Nonsmooh Sysems Imperial College June 29 Sabiliy analysis of nonsmooh limi cycles wih applicaions from power elecronics Dr D. Giaouris damian.giaouris@ncl.ac.uk
More informationIntroduction to Physical Oceanography Homework 5 - Solutions
Laure Zanna //5 Inroducion o Phsical Oceanograph Homework 5 - Soluions. Inerial oscillaions wih boom fricion non-selecive scale: The governing equaions for his problem are This ssem can be wrien as where
More informationMath 23 Spring Differential Equations. Final Exam Due Date: Tuesday, June 6, 5pm
Mah Spring 6 Differenial Equaions Final Exam Due Dae: Tuesday, June 6, 5pm Your name (please prin): Insrucions: This is an open book, open noes exam. You are free o use a calculaor or compuer o check your
More informationOrdinary Differential Equations
Lecure 22 Ordinary Differenial Equaions Course Coordinaor: Dr. Suresh A. Karha, Associae Professor, Deparmen of Civil Engineering, IIT Guwahai. In naure, mos of he phenomena ha can be mahemaically described
More informationReview - Quiz # 1. 1 g(y) dy = f(x) dx. y x. = u, so that y = xu and dy. dx (Sometimes you may want to use the substitution x y
Review - Quiz # 1 (1) Solving Special Tpes of Firs Order Equaions I. Separable Equaions (SE). d = f() g() Mehod of Soluion : 1 g() d = f() (The soluions ma be given implicil b he above formula. Remember,
More information4. Advanced Stability Theory
Applied Nonlinear Conrol Nguyen an ien - 4 4 Advanced Sabiliy heory he objecive of his chaper is o presen sabiliy analysis for non-auonomous sysems 41 Conceps of Sabiliy for Non-Auonomous Sysems Equilibrium
More informationCHAPTER 3 PSM BUCK DC-DC CONVERTER UNDER DISCONTINUOUS CONDUCTION MODE
7 HAPER PSM BUK D-D ONVERER UNDER DISONINUOUS ONDUION MODE Disconinuous conducion mode is he operaing mode in which he inducor curren reaches zero periodicall. In pulse widh modulaed converers under disconinuous
More informationEstimation of Diffusion Coefficient in Gas Exchange Process with in Human Respiration Via an Inverse Problem
Ausralian Journal o Basic and Applied Sciences 5(): 333-3330 0 ISS 99-878 Esimaion o Diusion Coeicien in Gas Exchange Process wih in Human Respiraion Via an Inverse Problem M Ebrahimi Deparmen o Mahemaics
More informationLecture 4. Goals: Be able to determine bandwidth of digital signals. Be able to convert a signal from baseband to passband and back IV-1
Lecure 4 Goals: Be able o deermine bandwidh o digial signals Be able o conver a signal rom baseband o passband and back IV-1 Bandwidh o Digial Daa Signals A digial daa signal is modeled as a random process
More informationOrdinary dierential equations
Chaper 5 Ordinary dierenial equaions Conens 5.1 Iniial value problem........................... 31 5. Forward Euler's mehod......................... 3 5.3 Runge-Kua mehods.......................... 36
More informationChapter 10. Optimization: More than One Choice Variable
Chaper Opimiaion: More han One Choice Variable William Sanle Jevons 85-88 Carl Menger 8 9. Opimiaion Problems Chaper 9: ma u one choice variable: consumpion Chaper : ma u o choice variables: leisure Chaper
More informationThe fundamental mass balance equation is ( 1 ) where: I = inputs P = production O = outputs L = losses A = accumulation
Hea (iffusion) Equaion erivaion of iffusion Equaion The fundamenal mass balance equaion is I P O L A ( 1 ) where: I inpus P producion O oupus L losses A accumulaion Assume ha no chemical is produced or
More informationExam I. Name. Answer: a. W B > W A if the volume of the ice cubes is greater than the volume of the water.
Name Exam I 1) A hole is punched in a full milk caron, 10 cm below he op. Wha is he iniial veloci of ouflow? a. 1.4 m/s b. 2.0 m/s c. 2.8 m/s d. 3.9 m/s e. 2.8 m/s Answer: a 2) In a wind unnel he pressure
More information6.2 Transforms of Derivatives and Integrals.
SEC. 6.2 Transforms of Derivaives and Inegrals. ODEs 2 3 33 39 23. Change of scale. If l( f ()) F(s) and c is any 33 45 APPLICATION OF s-shifting posiive consan, show ha l( f (c)) F(s>c)>c (Hin: In Probs.
More information( ) ( ) Incident light, p-polarization Z. We ll work through the Fresnel factor for the X-polarized incident field first. ω in.
1 3 d Objecives: 1. Define he individual Fresnel correcion facors for inerfacial SFG and SHG.. Define Lorenz local field correcion facors for SHG and SFG microscopy. 3. Inroduce he problem of refracive
More informationCommunication Systems, 5e
Communicaion Sysems, 5e Chaper : Signals and Specra A. Bruce Carlson Paul B. Crilly The McGraw-Hill Companies Chaper : Signals and Specra Line specra and ourier series Fourier ransorms Time and requency
More informationProblem Set 11(Practice Problems) Spring 2014
Issued: Wednesday April, ECE Signals and Sysems I Problem Se (Pracice Problems) Spring Due: For pracice only. No due. Reading in Oppenheim/Willsky/Nawab /9/ Secions 6.-6. // Secions 6.-6. See revised schedule
More information1 st order ODE Initial Condition
Mah-33 Chapers 1-1 s Order ODE Sepember 1, 17 1 1 s order ODE Iniial Condiion f, sandard form LINEAR NON-LINEAR,, p g differenial form M x dx N x d differenial form is equivalen o a pair of differenial
More informationd 1 = c 1 b 2 - b 1 c 2 d 2 = c 1 b 3 - b 1 c 3
and d = c b - b c c d = c b - b c c This process is coninued unil he nh row has been compleed. The complee array of coefficiens is riangular. Noe ha in developing he array an enire row may be divided or
More informationCHE302 LECTURE IV MATHEMATICAL MODELING OF CHEMICAL PROCESS. Professor Dae Ryook Yang
CHE302 LECTURE IV MATHEMATICAL MODELING OF CHEMICAL PROCESS Professor Dae Ryook Yang Fall 200 Dep. of Chemical and Biological Engineering Korea Universiy CHE302 Process Dynamics and Conrol Korea Universiy
More informationPhysics 4A FINAL EXAM Chapters 1-16 Fall 1998
Name: Posing Code Solve he following problems in he space provided Use he back of he page if needed Each problem is worh 10 poins You mus show our work in a logical fashion saring wih he correcl applied
More informationChapter 2. Sampling. 2.1 Sampling. Impulse Sampling 2-1
2- Chaper 2 Sampling 2. Sampling In his chaper, we sudy he represenaion o a coninuous-ime signal by is samples. his is provided in erms o he sampling heorem. Consider hree coninuous-ime signals x (), x
More information( ) ( ) if t = t. It must satisfy the identity. So, bulkiness of the unit impulse (hyper)function is equal to 1. The defining characteristic is
UNIT IMPULSE RESPONSE, UNIT STEP RESPONSE, STABILITY. Uni impulse funcion (Dirac dela funcion, dela funcion) rigorously defined is no sricly a funcion, bu disribuion (or measure), precise reamen requires
More informationLecture 1: Contents of the course. Advanced Digital Control. IT tools CCSDEMO
Goals of he course Lecure : Advanced Digial Conrol To beer undersand discree-ime sysems To beer undersand compuer-conrolled sysems u k u( ) u( ) Hold u k D-A Process Compuer y( ) A-D y ( ) Sampler y k
More informationy h h y
Porland Communiy College MTH 51 Lab Manual Limis and Coninuiy Aciviy 4 While working problem 3.6 you compleed Table 4.1 (ormerly Table 3.1). In he cone o ha problem he dierence quoien being evaluaed reurned
More informationLecture Outline. Introduction Transmission Line Equations Transmission Line Wave Equations 8/10/2018. EE 4347 Applied Electromagnetics.
8/10/018 Course Insrucor Dr. Raymond C. Rumpf Office: A 337 Phone: (915) 747 6958 E Mail: rcrumpf@uep.edu EE 4347 Applied Elecromagneics Topic 4a Transmission Line Equaions Transmission These Line noes
More informationCalculus Tricks #1. So if you understand derivatives, you ll understand the course material much better. a few preliminaries exponents
Calculus Tricks # Eric Doviak Calculus is no a pre-requisie or his course. However, he oundaions o economics are based on calculus, so wha we ll be discussing over he course o he semeser is he inuiion
More informationEE 313 Linear Signals & Systems (Fall 2018) Solution Set for Homework #8 on Continuous-Time Signals & Systems
EE 33 Linear Signals & Sysems (Fall 08) Soluion Se for Homework #8 on Coninuous-Time Signals & Sysems By: Mr. Houshang Salimian & Prof. Brian L. Evans Here are several useful properies of he Dirac dela
More informationSymmetry Reduction for a System of Nonlinear Evolution Equations
Nonlinear Mahemaical Physics 1996, V.3, N 3 4, 447 452. Symmery Reducion for a Sysem of Nonlinear Evoluion Equaions Lyudmila BARANNYK Insiue of Mahemaics of he Naional Ukrainian Academy of Sciences, 3
More informationChapter One Fourier Series and Fourier Transform
Chaper One I. Fourier Series Represenaion of Periodic Signals -Trigonomeric Fourier Series: The rigonomeric Fourier series represenaion of a periodic signal x() x( + T0 ) wih fundamenal period T0 is given
More informationSOME PROPERTIES OF GENERALIZED STRONGLY HARMONIC CONVEX FUNCTIONS MUHAMMAD ASLAM NOOR, KHALIDA INAYAT NOOR, SABAH IFTIKHAR AND FARHAT SAFDAR
Inernaional Journal o Analysis and Applicaions Volume 16, Number 3 2018, 427-436 URL: hps://doi.org/10.28924/2291-8639 DOI: 10.28924/2291-8639-16-2018-427 SOME PROPERTIES OF GENERALIZED STRONGLY HARMONIC
More informationEE 224 Signals and Systems I Complex numbers sinusodal signals Complex exponentials e jωt phasor addition
EE 224 Signals and Sysems I Complex numbers sinusodal signals Complex exponenials e jω phasor addiion 1/28 Complex Numbers Recangular Polar y z r z θ x Good for addiion/subracion Good for muliplicaion/division
More informationLecture 1 Overview. course mechanics. outline & topics. what is a linear dynamical system? why study linear systems? some examples
EE263 Auumn 27-8 Sephen Boyd Lecure 1 Overview course mechanics ouline & opics wha is a linear dynamical sysem? why sudy linear sysems? some examples 1 1 Course mechanics all class info, lecures, homeworks,
More informationLinear Time-invariant systems, Convolution, and Cross-correlation
Linear Time-invarian sysems, Convoluion, and Cross-correlaion (1) Linear Time-invarian (LTI) sysem A sysem akes in an inpu funcion and reurns an oupu funcion. x() T y() Inpu Sysem Oupu y() = T[x()] An
More informationf t te e = possesses a Laplace transform. Exercises for Module-III (Transform Calculus)
Exercises for Module-III (Transform Calculus) ) Discuss he piecewise coninuiy of he following funcions: =,, +, > c) e,, = d) sin,, = ) Show ha he funcion ( ) sin ( ) f e e = possesses a Laplace ransform.
More informationExam 1 Solutions. 1 Question 1. February 10, Part (A) 1.2 Part (B) To find equilibrium solutions, set P (t) = C = dp
Exam Soluions Februar 0, 05 Quesion. Par (A) To find equilibrium soluions, se P () = C = = 0. This implies: = P ( P ) P = P P P = P P = P ( + P ) = 0 The equilibrium soluion are hus P () = 0 and P () =..
More informationChapter 7: Inverse-Response Systems
Chaper 7: Invere-Repone Syem Normal Syem Invere-Repone Syem Baic Sar ou in he wrong direcion End up in he original eady-ae gain value Two or more yem wih differen magniude and cale in parallel Main yem
More information