Sliding Mode Extremum Seeking Control for Linear Quadratic Dynamic Game
|
|
- Oliver Arnold
- 5 years ago
- Views:
Transcription
1 Sliding Mode Exremum Seeking Conrol for Linear Quadraic Dynamic Game Yaodong Pan and Ümi Özgüner ITS Research Group, AIST Tsukuba Eas Namiki --, Tsukuba-shi,Ibaraki-ken 5-856, Japan Deparmen of Elecrical Engineering, The Ohio Sae Universiy 5 Neil Avenue, Columbus, OH umi@ee.eng.ohio-sae.edu Absrac The exremum seeking conrol has been proposed o find a se poin and/or rack a ime-varying se poin so ha a performance index of he sysem reaches is exremum poin. In his paper, he exremum seeking conrol wih sliding mode is exended o solve he Nash equilibrium soluion for an n-person linear quadraic dynamic game. For each player, a sliding mode exremum seeking conroller is designed o le he player s linear quadraic performance index rack a decreasing signal so ha he Nash equilibrium poin is reached. Keyword: Noncooperaive Dynamic Game, Linear Quadraic Performance Index, Nash Equilibrium Soluion, Exremum Seeking, Sliding Model. I. INTRODUCTION Exremum seeking conrol approaches have been sudied since 5 s and have been successfully implemened in he conrol of a axial-flow compressor, he opimizaion of he operaion of biological reacors, and he opimizaion of spark igniion auomoive engines. Wih he exremum seeking conrol, a sepoin and/or a ime-variable sepoin is racked o minimize or maximize a performance index of he sysem As one of he exremum seeking conrol approaches, he sliding mode exremum seeking conroller shown in Figure ensures (9) ha he sysem converges o a predesigned sliding mode in a finie ime, eners a viciniy of he exremum poin on he sliding mode, and says here wih oscillaion. Alhough i is a radeoff problem o deermine he conrol accuracy and convergence speed by choosing conroller parameers, i is possible o obain boh high conrol accuracy and fas convergence speed afer Fig.. Exremum Seeking Conrol Using Sliding Mode inroducing ime-variable parameers. Recenly, i is found ha he sliding mode exremum seeking conrol can also be implemened o solve he Nash Soluion. For an n-person noncooperaive dynamic game, each player defines a performance index and adjuss some of he conrol parameers o minimize his own performance index o find a Nash equilibrium soluion. In, i is assumed ha he performance index for each player is a funcion on he sae, he inpu and he oupu variables of he sysem, which may be in an unknown form bu is measurable or can be calculaed from he measurable variables. In his paper, we will consider he n-person noncooperaive linear quadraic dynamic game, where he conrol inpus o be adjused by each player are he feedback conrol gains K i (i =,,..., n) and he performance index (i =,,..., n) is he inegraion of a linear quadraic funcion on he sysem sae and inpu. In his case, he calculaion of he performance indices needs he fuure informaion of he sysem sae and inpu. The performance
2 indices can no be calculaed on-line and hus can no be direcly used in he exremum seeking conroller. As he firs sep o design an exremum seeking conroller for he n-person noncooperaive linear quadraic dynamic game, he linear quadraic index is ransferred o an equivalen performance index, which can be calculaed on-line based on he sysem parameers and he feedback gain. The arrangemen of he paper is as follows. Secion describes he problem formulaion and he ransformaion of he linear quadraic index; Secion proposes he sliding mode exremum seeking approach o find he Nash equilibrium soluion for a linear quadraic dynamic game; and Secion gives simulaion resuls. II. PROBLEM FORMULATION Consider an n-person noncooperaive linear quadraic dynamic game described by a linear dynamic sysem d n d x = Ax + B i u i () i= wih a linear quadraic performance index for i-h player = (x T Q i x + u T R i u)d, (i N) () where A and B i (i N) are known consan marices of appropriae dimensions, (A, B i ) (i N) are conrollable pairs, N is he index se of player defined as N = {,,, n}, x R m is he sysem sae variable, u i R (i N) is he conrol variable for each player, is he sysem iniial ime, Q i R m m and R i R (i N) are semi-posiive and posiive definie symmeric marices, respecively, and (Q i, A) (i N) are observable pairs. To simply he noaion and he discussion, he -player case is considered from now on. Exension o he n-player case is sraighforward. The opimal conrol of he above sysem is a game problem. The Nash Soluion wih he Nash feedback sraegy is given by u i = R i B T i P i x, (i =, ) which ensures for any sysem iniial sae x( ) (x( ) R m ) ha J u =u,u =u J u U,u =u J u =u,u =u u =u,u U where U and U are ses of possible conrol inpu for player and, respecively, P and P are he posiive definie soluions of he following coupled algebraic Riccai equaions: P A + A T P P B R BT P P B R BT P P B R BT P = Q P A + A T P P B R BT P P B R BT P P B R BT P = Q. Insead of solving he above Riccai equaions, in his paper he opimal feedback gains K i (K i = R BT P, i =, ) as he Nash soluion o minimize he performance index (i =, ) are calculaed by he sliding mode exremum seeking conrol approach. as Denoe he linear feedback conrol inpu for each player u i = K i x, (i =, ). () Then he closed-loop sysem of () wih he conrol inpu () is deermined by d x = Āx, () d and he linear quadraic performance index given in () can be rewrien as where = x T Q i xd, (i =, ), (5) Ā = A B K B K Q i = ĀT (Q i + Ki T R i K i )Ā. (i =, ) As (A, B i ) and (Q i, A) (i =, ) are conrollable and observable pairs, respecively, here exis wo parameer ses K and K so ha for any feedback gain K i (K i K i, i =, ), he Lyapunov funcions M i Ā + ĀT M i = Q i (i =, ) (6) have posiive definie symmeric soluions M i (i =, ). I is clear ha M i (i =, ) is a funcion on K and K and hus may be denoed as M i = M i (K, K ). (i =, ) (7) Then he linear quadraic performance index () can be rewrien as = x T M i x = x T ( )M i x( ) = r(x( )x T ( )M i ) K i K i, (i =, ) where r(.) is he race operaion.
3 According o he linear quadraic opimal conrol heory, he opimal soluion of he above performance index is independen o he iniial ime and he sysem iniial sae x( ), i.e. he opimal feedback gain Ki (i =, ) is unique no maer he sysem iniial sae x( ) is. Denoe he column vecor of he ideniy marix I m as e j (j =,,..., m), i.e. I m = diag{,,..., } = e e e m. III. EXTREMUM SEEKING WITH SLIDING MODE To design an exremum seeking conroller wih sliding mode for he i-h player (i =, ), a swiching funcion is defined as s i = g i () where he reference signal g i R is deermined by ġ i = ρ i, () Then he opimal feedback gain Ki (i =, ) can be where ρ i (i =, ) are posiive consans. described as Le he variable srucure conrol law be {K, K } = Arg min )x T ( )M i ) sgn(sin(πs i /α i )) K i K i,i=, = Arg min sgn(sin(πs i /α i )) je T j M i ), (j =,,..., m) v i = k i, (i =, ) K i K i,i=,... = Arg min m sgn(sin( m πs i /α i )) r(e j e T j M i ) () K i K i,i=, j= = Arg min r( m e j e T j M i ) K i K i,i=, j= = Arg min r(i mm i ) K i K i,i=, where α i and k i (i =, ) are posiive consans. = Arg min r(m i). (8) Assumpion : The parial derivaive of he performance K i K i,i=, index (i =, ) saisfies Thus he conrol objecive o solve he Nash equilibrium soluion is urned o minimize he performance index (K, K ) >> (K, K ), j i(i, j =, ) K i K j (K, K ) = r(m i ) = r(m i (K, K )) (i =, ) (9) by adjusing he feedback gain K i by each player (i =, ) independenly. I follows from he linear quadraic opimal conrol heory ha a unique Nash equilibrium soluion (K, K ) exiss such ha J (K, K ) (K, K ), K K J (K, K ) (K, K ), K K. During searching he Nash soluion, he feedback gain K i (i =, ) is adjused on-line by he exremum seeking conroller. Therefore K i (i =, ) is a funcion on ime. The performance index given in (9) hus can be described as a funcion on ime, oo, i.e. = (K, K ) = r(m i (K, K )) (i =, ) () To simplify he noaion, he same symbol is used o denoe he performance indices in (), (9), and (). and he feedback gain K i (i =, ) saisfy K i = v i, (i =, ) () which means ha each player can adjus his performance index mos effecively Assumpion : The Nash equilibrium poin (K, K ) is in he viciniy of he iniial -uple of K i () (i =, ). Thus he parial derivaive of he performance index on K i is bounded by a posiive consan γ i, i.e., (K, K ) γ i. (i =, ) (5) K i Theorem : Consider he dynamic noncooperaive game described by he sae equaion in () wih he linear quadraic performance index (), he exremum seeking conroller wih sliding mode for he i-h player (i =, ) designed by Equaions (), (), (), and () ensures ha he performance index (i =, ) are minimized o ge he Nash equilibrium soluion J (K, K ) and J (K, K ) if posiive consans ρ i, k i, and α i (i =, ) as he conroller parameers are chosen suiable. Proof: The compleed proof of his heorem needs much space. In his paper, only he seps of he proof are described as follows, which are similar o he resuls in and.
4 Based on he above assumpions, he derivaive of he swiching funcion s i is given by d d s i = j= From which, i can be shown ha K j (K, K ) K j ġ i K i (K, K ) K i ġ i. (6) For each player here exiss a viciniy of he minimum poin, which is deermined by ρi k i his viciniy, a sliding mode (i =, ). Ouside, s i, g i Performance Index, Swiching Funcion s i and Reference Signal g i (Player i) s i g i s i = lα i or s i = lα i will happen for some number l deermined by he iniial condiion of he sysem. On he sliding mode, he sysem converges o he viciniy. Afer enering he viciniy, i is possible ha eiher he sysem says inside he viciniy or go hrough he viciniy. In he laer case, anoher sliding mode will happen and he sysem will ener he viciniy again on he sliding mode. In boh cases, i.e. he case saying inside he viciniy and he case moving ou of he viciniy, he performance index J oscillaes and decreases in each oscillaion period as shown in Figures, and. 5 6 Fig.. Swiching Funcion wih Sliding Mode Exremum Seeking Conroller Performance Index (Player i) Convergence wih Sliding Mode Exremum Seeking Conrol (Player i) Ki Ki Fig.. Performance Index wih Sliding Mode Exremum Seeking Conroller, Ki, Ki 5 has been shown in ha fas convergen speed and high conrol accuracy may be obained if he conroller parameers ρ i, k i, and α i are chosen suiably and adjused online. IV. EXAMPLES 5 6 Fig.. Convergence wih Sliding Mode Exremum Seeking Conroller Finally he sysem oscillaes around he Nash equilibrium poin. In his way, he Nash soluion can be found by he proposed exremum seeking conroller wih sliding mode. And i Consider a wo-person noncooperaive linear quadraic dynamic game described by a second-order linear sysem..7. ẋ = x + u + u...9 The parameer marices of he performance index () are respecively given by Q =, R =.
5 Q =, R =. The proposed exremum seeking conrol algorihm is implemened o he above sysem wih sampling inerval as. T =. second and oher conroller parameers as k i =.5, ρ i =.5. (i =, ) The simulaion resuls wih α = α =.5 are given in Figures 5 and 6, which shows ha he sysem reaches a sliding mode in a finie ime, converges o he viciniy of he Nash equilibrium poin and hen oscillaes while he performance index keeps decreasing in each oscillaion period unil he Nash equilibrium poin is reached. s, s Swiching Funcions s s Fig. 5. Conrol Swiching Funcions wih Sliding Mode Exremum Seeking The ampliude of he oscillaion can be reduced by increasing he posiive consan ρ i (i =, ) as shown in Figure 7 wih ρ = ρ =. bu in his case, he convergen speed is slow. In his paper, a kind of on-line adjusing mehod is proposed. The parameer ρ is deermined by a ime-variable funcion as { ρ i =. >. (i =, ) The simulaion resuls in Figure 8 wih he above imevariable parameer ρ i (i =, ) show ha he Nash soluion is obained quickly wih higher conrol accuracy. To confirm he resuls obained by he proposed sliding mode exremum seeking conrol approach, he opimal feedback gains for he Nash soluion are obained as K =.6.65 K = (7) (8) by he ɛ-coupling approach, which are he same o hose resuls shown in Figures 6, 7, and 8. V. CONCLUSION The sliding mode exremum seeking conrol approach is successfully exended o he Nash equilibrium soluion for an n-person noncooperaive linear quadraic dynamic game. Wih he designed exremum seeking conroller for each player in he game, he sysem reaches a sliding mode, eners a viciniy of he Nash equilibrium poin, and says here wih oscillaing behavior. The simulaion resuls show he effeciveness. REFERENCES H. Tsien, Engineering Cyberneics. PA, USA: McGraw-HILL Book Company, Inc., 95. S. Y. Hsin-Hsiung Wang and M. Krsic, Experimenal applicaion of exremum seeking on an axial-flow compressor, in IEEE Transacions on Conrol Sysems Technology, Vol., No., pp. 8,. M. K. Hsin-Hsiung Wang and G. Basin, Opimizing bioreacors by exremum seeking, in Inernaional Journal of Adapive Conrol and Signal Processing,, pp , 999. P. G. Scoson and P. E. Wellsead, Self-uning opimizaion of spark igniion auomoive engines, IEEE Conrol Sysem Magazine, vol. -, pp. 9, B. Blackman, Exremum-seeking regulaors, in An Exposiion of Adapive Conrol, (New York), pp. 6 5, The Macmillan Company, K. Asrom and B. Wienmark, Adapive Conrol, nd ed. MA: Addison-Wesley, M. Krsic and H. Wang, Sabiliy of exremum seeking feedback for general nonlinear dyanmic sysems, Auomaica, vol. 6, pp ,. 8 M. Krsic, Performance improvemen and limiaions in exremum seeking conrol, Sysem & Conrol Leers, vol. 9, pp. 6,. 9 S. Drakunov and Ümi Özgüner, Opimizaion of nonlinear sysem oupu via sliding mode approach, in IEEE Inernaional Workshop on Variable Srucure and Lyapunov Conrol of Uncerain Dynamical Sysem, (UK), pp. 6 6, 99. S. Drakunov, Ümi Özgüner, P. Dix, and B. Ashrafi, ABS conrol using opimum search via sliding modes, IEEE Trans. on Conrol Sysems Technology, vol. -, pp , 995. Y. Pan, Ümi Özgüner, and T. Acarman, Sabiliy and performance improvemen of exremum seeking conrol wih sliding mode, o be published in In. J. Conrol,. Y. Pan, T. Acarman, and Ümi Özgüner, Nash soluion by exremum seeking conrol approach, in he h Conference on Decision and Conrol, (Las Vegas, Nevada), pp. 9,. T. Basar, Dynamic Noncooperaive Game Theory. Philadephia: SIAM, 999. Ümi Özgüner and W. Perkins, A series soluion o he nash sraegy for large scale inerconneced sysem, Auomaica, vol., pp. 5, 977.
6 .6. Exremum Seeking wih Sliding Mode (Player ) J K K.5 Exremum Seeking wih Sliding Mode (Player ) K K..5 J, K, K.8.6, K, K Fig. 6. Nash Soluion by Exremum Seeking Conrol(α = α =.5).6. Exremum Seeking wih Sliding Mode (Player ) J K K.5 Exremum Seeking wih Sliding Mode (Player ) K K. J, K, K.8.6, K, K Fig. 7. Nash Soluion by Exremum Seeking Conrol(α = α =.).6. Exremum Seeking wih Sliding Mode (Player ) J K K.5 Exremum Seeking wih Sliding Mode (Player ) K K. J, K, K.8.6, K, K Fig. 8. Nash Soluion by Exremum Seeking Conrol(α = α =.5.)
Lecture 20: Riccati Equations and Least Squares Feedback Control
34-5 LINEAR SYSTEMS Lecure : Riccai Equaions and Leas Squares Feedback Conrol 5.6.4 Sae Feedback via Riccai Equaions A recursive approach in generaing he marix-valued funcion W ( ) equaion for i for he
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 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 informationMean-square Stability Control for Networked Systems with Stochastic Time Delay
JOURNAL OF SIMULAION VOL. 5 NO. May 7 Mean-square Sabiliy Conrol for Newored Sysems wih Sochasic ime Delay YAO Hejun YUAN Fushun School of Mahemaics and Saisics Anyang Normal Universiy Anyang Henan. 455
More informationSUFFICIENT CONDITIONS FOR EXISTENCE SOLUTION OF LINEAR TWO-POINT BOUNDARY PROBLEM IN MINIMIZATION OF QUADRATIC FUNCTIONAL
HE PUBLISHING HOUSE PROCEEDINGS OF HE ROMANIAN ACADEMY, Series A, OF HE ROMANIAN ACADEMY Volume, Number 4/200, pp 287 293 SUFFICIEN CONDIIONS FOR EXISENCE SOLUION OF LINEAR WO-POIN BOUNDARY PROBLEM IN
More informationChapter 5 Digital PID control algorithm. Hesheng Wang Department of Automation,SJTU 2016,03
Chaper 5 Digial PID conrol algorihm Hesheng Wang Deparmen of Auomaion,SJTU 216,3 Ouline Absrac Quasi-coninuous PID conrol algorihm Improvemen of sandard PID algorihm Choosing parameer of PID regulaor Brief
More informationMATH 128A, SUMMER 2009, FINAL EXAM SOLUTION
MATH 28A, SUMME 2009, FINAL EXAM SOLUTION BENJAMIN JOHNSON () (8 poins) [Lagrange Inerpolaion] (a) (4 poins) Le f be a funcion defined a some real numbers x 0,..., x n. Give a defining equaion for he Lagrange
More informationA DELAY-DEPENDENT STABILITY CRITERIA FOR T-S FUZZY SYSTEM WITH TIME-DELAYS
A DELAY-DEPENDENT STABILITY CRITERIA FOR T-S FUZZY SYSTEM WITH TIME-DELAYS Xinping Guan ;1 Fenglei Li Cailian Chen Insiue of Elecrical Engineering, Yanshan Universiy, Qinhuangdao, 066004, China. Deparmen
More information10. State Space Methods
. Sae Space Mehods. Inroducion Sae space modelling was briefly inroduced in chaper. Here more coverage is provided of sae space mehods before some of heir uses in conrol sysem design are covered in he
More informationSliding Mode Controller for Unstable Systems
S. SIVARAMAKRISHNAN e al., Sliding Mode Conroller for Unsable Sysems, Chem. Biochem. Eng. Q. 22 (1) 41 47 (28) 41 Sliding Mode Conroller for Unsable Sysems S. Sivaramakrishnan, A. K. Tangirala, and M.
More informationRobust estimation based on the first- and third-moment restrictions of the power transformation model
h Inernaional Congress on Modelling and Simulaion, Adelaide, Ausralia, 6 December 3 www.mssanz.org.au/modsim3 Robus esimaion based on he firs- and hird-momen resricions of he power ransformaion Nawaa,
More informationGeorey E. Hinton. University oftoronto. Technical Report CRG-TR February 22, Abstract
Parameer Esimaion for Linear Dynamical Sysems Zoubin Ghahramani Georey E. Hinon Deparmen of Compuer Science Universiy oftorono 6 King's College Road Torono, Canada M5S A4 Email: zoubin@cs.orono.edu Technical
More informationEE363 homework 1 solutions
EE363 Prof. S. Boyd EE363 homework 1 soluions 1. LQR for a riple accumulaor. We consider he sysem x +1 = Ax + Bu, y = Cx, wih 1 1 A = 1 1, B =, C = [ 1 ]. 1 1 This sysem has ransfer funcion H(z) = (z 1)
More informationSTATE-SPACE MODELLING. A mass balance across the tank gives:
B. Lennox and N.F. Thornhill, 9, Sae Space Modelling, IChemE Process Managemen and Conrol Subjec Group Newsleer STE-SPACE MODELLING Inroducion: Over he pas decade or so here has been an ever increasing
More informationOptimal Path Planning for Flexible Redundant Robot Manipulators
25 WSEAS In. Conf. on DYNAMICAL SYSEMS and CONROL, Venice, Ialy, November 2-4, 25 (pp363-368) Opimal Pah Planning for Flexible Redundan Robo Manipulaors H. HOMAEI, M. KESHMIRI Deparmen of Mechanical Engineering
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 informationOrdinary Differential Equations
Ordinary Differenial Equaions 5. Examples of linear differenial equaions and heir applicaions We consider some examples of sysems of linear differenial equaions wih consan coefficiens y = a y +... + a
More informationOnline Partially Model-Free Solution of Two-Player Zero Sum Differential Games
Preprins of he 10h IFAC Inernaional Symposium on Dynamics and Conrol of Process Sysems The Inernaional Federaion of Auomaic Conrol Online Parially Model-Free Soluion of Two-Player Zero Sum Differenial
More informationSimulation-Solving Dynamic Models ABE 5646 Week 2, Spring 2010
Simulaion-Solving Dynamic Models ABE 5646 Week 2, Spring 2010 Week Descripion Reading Maerial 2 Compuer Simulaion of Dynamic Models Finie Difference, coninuous saes, discree ime Simple Mehods Euler Trapezoid
More informationChapter 7 Response of First-order RL and RC Circuits
Chaper 7 Response of Firs-order RL and RC Circuis 7.- The Naural Response of RL and RC Circuis 7.3 The Sep Response of RL and RC Circuis 7.4 A General Soluion for Sep and Naural Responses 7.5 Sequenial
More informationRC, RL and RLC circuits
Name Dae Time o Complee h m Parner Course/ Secion / Grade RC, RL and RLC circuis Inroducion In his experimen we will invesigae he behavior of circuis conaining combinaions of resisors, capaciors, and inducors.
More informationdi Bernardo, M. (1995). A purely adaptive controller to synchronize and control chaotic systems.
di ernardo, M. (995). A purely adapive conroller o synchronize and conrol chaoic sysems. hps://doi.org/.6/375-96(96)8-x Early version, also known as pre-prin Link o published version (if available):.6/375-96(96)8-x
More informationSTABILITY OF RESET SWITCHING SYSTEMS
STABILITY OF RESET SWITCHING SYSTEMS J.P. Paxman,G.Vinnicombe Cambridge Universiy Engineering Deparmen, UK, jpp7@cam.ac.uk Keywords: Sabiliy, swiching sysems, bumpless ransfer, conroller realizaion. Absrac
More informationOn-line Adaptive Optimal Timing Control of Switched Systems
On-line Adapive Opimal Timing Conrol of Swiched Sysems X.C. Ding, Y. Wardi and M. Egersed Absrac In his paper we consider he problem of opimizing over he swiching imes for a muli-modal dynamic sysem when
More informationOn Robust Stability of Uncertain Neutral Systems with Discrete and Distributed Delays
009 American Conrol Conference Hya Regency Riverfron S. Louis MO USA June 0-009 FrC09.5 On Robus Sabiliy of Uncerain Neural Sysems wih Discree and Disribued Delays Jian Sun Jie Chen G.P. Liu Senior Member
More informationdy dx = xey (a) y(0) = 2 (b) y(1) = 2.5 SOLUTION: See next page
Assignmen 1 MATH 2270 SOLUTION Please wrie ou complee soluions for each of he following 6 problems (one more will sill be added). You may, of course, consul wih your classmaes, he exbook or oher resources,
More informationPhysics 235 Chapter 2. Chapter 2 Newtonian Mechanics Single Particle
Chaper 2 Newonian Mechanics Single Paricle In his Chaper we will review wha Newon s laws of mechanics ell us abou he moion of a single paricle. Newon s laws are only valid in suiable reference frames,
More informationEXERCISES FOR SECTION 1.5
1.5 Exisence and Uniqueness of Soluions 43 20. 1 v c 21. 1 v c 1 2 4 6 8 10 1 2 2 4 6 8 10 Graph of approximae soluion obained using Euler s mehod wih = 0.1. Graph of approximae soluion obained using Euler
More information14 Autoregressive Moving Average Models
14 Auoregressive Moving Average Models In his chaper an imporan parameric family of saionary ime series is inroduced, he family of he auoregressive moving average, or ARMA, processes. For a large class
More informationAn introduction to the theory of SDDP algorithm
An inroducion o he heory of SDDP algorihm V. Leclère (ENPC) Augus 1, 2014 V. Leclère Inroducion o SDDP Augus 1, 2014 1 / 21 Inroducion Large scale sochasic problem are hard o solve. Two ways of aacking
More informationON THE BEAT PHENOMENON IN COUPLED SYSTEMS
8 h ASCE Specialy Conference on Probabilisic Mechanics and Srucural Reliabiliy PMC-38 ON THE BEAT PHENOMENON IN COUPLED SYSTEMS S. K. Yalla, Suden Member ASCE and A. Kareem, M. ASCE NaHaz Modeling Laboraory,
More informationCONTROL SYSTEMS, ROBOTICS AND AUTOMATION Vol. XI Control of Stochastic Systems - P.R. Kumar
CONROL OF SOCHASIC SYSEMS P.R. Kumar Deparmen of Elecrical and Compuer Engineering, and Coordinaed Science Laboraory, Universiy of Illinois, Urbana-Champaign, USA. Keywords: Markov chains, ransiion probabiliies,
More informationSingle-Pass-Based Heuristic Algorithms for Group Flexible Flow-shop Scheduling Problems
Single-Pass-Based Heurisic Algorihms for Group Flexible Flow-shop Scheduling Problems PEI-YING HUANG, TZUNG-PEI HONG 2 and CHENG-YAN KAO, 3 Deparmen of Compuer Science and Informaion Engineering Naional
More informationApplication of a Stochastic-Fuzzy Approach to Modeling Optimal Discrete Time Dynamical Systems by Using Large Scale Data Processing
Applicaion of a Sochasic-Fuzzy Approach o Modeling Opimal Discree Time Dynamical Sysems by Using Large Scale Daa Processing AA WALASZE-BABISZEWSA Deparmen of Compuer Engineering Opole Universiy of Technology
More informationLecture 2 October ε-approximation of 2-player zero-sum games
Opimizaion II Winer 009/10 Lecurer: Khaled Elbassioni Lecure Ocober 19 1 ε-approximaion of -player zero-sum games In his lecure we give a randomized ficiious play algorihm for obaining an approximae soluion
More informationMATH 5720: Gradient Methods Hung Phan, UMass Lowell October 4, 2018
MATH 5720: Gradien Mehods Hung Phan, UMass Lowell Ocober 4, 208 Descen Direcion Mehods Consider he problem min { f(x) x R n}. The general descen direcions mehod is x k+ = x k + k d k where x k is he curren
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 informationThe Asymptotic Behavior of Nonoscillatory Solutions of Some Nonlinear Dynamic Equations on Time Scales
Advances in Dynamical Sysems and Applicaions. ISSN 0973-5321 Volume 1 Number 1 (2006, pp. 103 112 c Research India Publicaions hp://www.ripublicaion.com/adsa.hm The Asympoic Behavior of Nonoscillaory Soluions
More informationKEY. Math 334 Midterm III Winter 2008 section 002 Instructor: Scott Glasgow
KEY Mah 334 Miderm III Winer 008 secion 00 Insrucor: Sco Glasgow Please do NOT wrie on his exam. No credi will be given for such work. Raher wrie in a blue book, or on your own paper, preferably engineering
More informationModal identification of structures from roving input data by means of maximum likelihood estimation of the state space model
Modal idenificaion of srucures from roving inpu daa by means of maximum likelihood esimaion of he sae space model J. Cara, J. Juan, E. Alarcón Absrac The usual way o perform a forced vibraion es is o fix
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 information4.6 One Dimensional Kinematics and Integration
4.6 One Dimensional Kinemaics and Inegraion When he acceleraion a( of an objec is a non-consan funcion of ime, we would like o deermine he ime dependence of he posiion funcion x( and he x -componen of
More informationChapter 2. First Order Scalar Equations
Chaper. Firs Order Scalar Equaions We sar our sudy of differenial equaions in he same way he pioneers in his field did. We show paricular echniques o solve paricular ypes of firs order differenial equaions.
More informationExercises: Similarity Transformation
Exercises: Similariy Transformaion Problem. Diagonalize he following marix: A [ 2 4 Soluion. Marix A has wo eigenvalues λ 3 and λ 2 2. Since (i) A is a 2 2 marix and (ii) i has 2 disinc eigenvalues, we
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 informationModule 3: The Damped Oscillator-II Lecture 3: The Damped Oscillator-II
Module 3: The Damped Oscillaor-II Lecure 3: The Damped Oscillaor-II 3. Over-damped Oscillaions. This refers o he siuaion where β > ω (3.) The wo roos are and α = β + α 2 = β β 2 ω 2 = (3.2) β 2 ω 2 = 2
More informationRecursive Least-Squares Fixed-Interval Smoother Using Covariance Information based on Innovation Approach in Linear Continuous Stochastic Systems
8 Froniers in Signal Processing, Vol. 1, No. 1, July 217 hps://dx.doi.org/1.2266/fsp.217.112 Recursive Leas-Squares Fixed-Inerval Smooher Using Covariance Informaion based on Innovaion Approach in Linear
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 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 informationIterative Learning Control for the Linear Model. with a Singular Feedthrough Term Via LQAT
Applied Mahemaical Sciences, Vol. 6,, no. 86, 483-494 Ieraive Learning Conrol for he Linear Model wih a Singular Feedhrough erm Via LQA Chia-Hsing Chen and Jason Sheng-Hong sai Conrol Sysem Laboraory,
More informationModel-Free based Optimal Iterative Learning Control for a Class of Discrete-Time Nonlinear Systems 1
Proceedings of he 7h World Congress he Inernaional Federaion of Auomaic Conrol Model-Free based Opimal Ieraive Learning Conrol for a Class of Discree-ime Nonlinear Sysems Shangai Jin Zhongsheng Hou Ming
More informationFractional Method of Characteristics for Fractional Partial Differential Equations
Fracional Mehod of Characerisics for Fracional Parial Differenial Equaions Guo-cheng Wu* Modern Teile Insiue, Donghua Universiy, 188 Yan-an ilu Road, Shanghai 51, PR China Absrac The mehod of characerisics
More informationProblemas das Aulas Práticas
Mesrado Inegrado em Engenharia Elecroécnica e de Compuadores Conrolo em Espaço de Esados Problemas das Aulas Práicas J. Miranda Lemos Fevereiro de 3 Translaed o English by José Gaspar, 6 J. M. Lemos, IST
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 informationAsymptotic instability of nonlinear differential equations
Elecronic Journal of Differenial Equaions, Vol. 1997(1997), No. 16, pp. 1 7. ISSN: 172-6691. URL: hp://ejde.mah.sw.edu or hp://ejde.mah.un.edu fp (login: fp) 147.26.13.11 or 129.12.3.113 Asympoic insabiliy
More informationSignaling equilibria for dynamic LQG games with. asymmetric information
Signaling equilibria for dynamic LQG games wih asymmeric informaion Deepanshu Vasal and Achilleas Anasasopoulos Absrac We consider a finie horizon dynamic game wih wo players who observe heir ypes privaely
More informationSome New Uniqueness Results of Solutions to Nonlinear Fractional Integro-Differential Equations
Annals of Pure and Applied Mahemaics Vol. 6, No. 2, 28, 345-352 ISSN: 2279-87X (P), 2279-888(online) Published on 22 February 28 www.researchmahsci.org DOI: hp://dx.doi.org/.22457/apam.v6n2a Annals of
More informationCourse Notes for EE227C (Spring 2018): Convex Optimization and Approximation
Course Noes for EE7C Spring 018: Convex Opimizaion and Approximaion Insrucor: Moriz Hard Email: hard+ee7c@berkeley.edu Graduae Insrucor: Max Simchowiz Email: msimchow+ee7c@berkeley.edu Ocober 15, 018 3
More information3.1.3 INTRODUCTION TO DYNAMIC OPTIMIZATION: DISCRETE TIME PROBLEMS. A. The Hamiltonian and First-Order Conditions in a Finite Time Horizon
3..3 INRODUCION O DYNAMIC OPIMIZAION: DISCREE IME PROBLEMS A. he Hamilonian and Firs-Order Condiions in a Finie ime Horizon Define a new funcion, he Hamilonian funcion, H. H he change in he oal value of
More informationSignal and System (Chapter 3. Continuous-Time Systems)
Signal and Sysem (Chaper 3. Coninuous-Time Sysems) Prof. Kwang-Chun Ho kwangho@hansung.ac.kr Tel: 0-760-453 Fax:0-760-4435 1 Dep. Elecronics and Informaion Eng. 1 Nodes, Branches, Loops A nework wih b
More informationarxiv: v1 [math.ca] 15 Nov 2016
arxiv:6.599v [mah.ca] 5 Nov 26 Counerexamples on Jumarie s hree basic fracional calculus formulae for non-differeniable coninuous funcions Cheng-shi Liu Deparmen of Mahemaics Norheas Peroleum Universiy
More informationGuest Lectures for Dr. MacFarlane s EE3350 Part Deux
Gues Lecures for Dr. MacFarlane s EE3350 Par Deux Michael Plane Mon., 08-30-2010 Wrie name in corner. Poin ou his is a review, so I will go faser. Remind hem o go lisen o online lecure abou geing an A
More informationAdaptation and Synchronization over a Network: stabilization without a reference model
Adapaion and Synchronizaion over a Nework: sabilizaion wihou a reference model Travis E. Gibson (gibson@mi.edu) Harvard Medical School Deparmen of Pahology, Brigham and Women s Hospial 55 h Conference
More information1 Review of Zero-Sum Games
COS 5: heoreical Machine Learning Lecurer: Rob Schapire Lecure #23 Scribe: Eugene Brevdo April 30, 2008 Review of Zero-Sum Games Las ime we inroduced a mahemaical model for wo player zero-sum games. Any
More informationAn Introduction to Malliavin calculus and its applications
An Inroducion o Malliavin calculus and is applicaions Lecure 5: Smoohness of he densiy and Hörmander s heorem David Nualar Deparmen of Mahemaics Kansas Universiy Universiy of Wyoming Summer School 214
More informationOnline Appendix to Solution Methods for Models with Rare Disasters
Online Appendix o Soluion Mehods for Models wih Rare Disasers Jesús Fernández-Villaverde and Oren Levinal In his Online Appendix, we presen he Euler condiions of he model, we develop he pricing Calvo block,
More informationNotes on Kalman Filtering
Noes on Kalman Filering Brian Borchers and Rick Aser November 7, Inroducion Daa Assimilaion is he problem of merging model predicions wih acual measuremens of a sysem o produce an opimal esimae of he curren
More informationTwo Coupled Oscillators / Normal Modes
Lecure 3 Phys 3750 Two Coupled Oscillaors / Normal Modes Overview and Moivaion: Today we ake a small, bu significan, sep owards wave moion. We will no ye observe waves, bu his sep is imporan in is own
More informationCONTRIBUTION TO IMPULSIVE EQUATIONS
European Scienific Journal Sepember 214 /SPECIAL/ ediion Vol.3 ISSN: 1857 7881 (Prin) e - ISSN 1857-7431 CONTRIBUTION TO IMPULSIVE EQUATIONS Berrabah Faima Zohra, MA Universiy of sidi bel abbes/ Algeria
More informationParticle Swarm Optimization
Paricle Swarm Opimizaion Speaker: Jeng-Shyang Pan Deparmen of Elecronic Engineering, Kaohsiung Universiy of Applied Science, Taiwan Email: jspan@cc.kuas.edu.w 7/26/2004 ppso 1 Wha is he Paricle Swarm Opimizaion
More informationF This leads to an unstable mode which is not observable at the output thus cannot be controlled by feeding back.
Lecure 8 Las ime: Semi-free configuraion design This is equivalen o: Noe ns, ener he sysem a he same place. is fixed. We design C (and perhaps B. We mus sabilize if i is given as unsable. Cs ( H( s = +
More informationAn Introduction to Backward Stochastic Differential Equations (BSDEs) PIMS Summer School 2016 in Mathematical Finance.
1 An Inroducion o Backward Sochasic Differenial Equaions (BSDEs) PIMS Summer School 2016 in Mahemaical Finance June 25, 2016 Chrisoph Frei cfrei@ualbera.ca This inroducion is based on Touzi [14], Bouchard
More informationThe Potential Effectiveness of the Detection of Pulsed Signals in the Non-Uniform Sampling
The Poenial Effeciveness of he Deecion of Pulsed Signals in he Non-Uniform Sampling Arhur Smirnov, Sanislav Vorobiev and Ajih Abraham 3, 4 Deparmen of Compuer Science, Universiy of Illinois a Chicago,
More informationLab 10: RC, RL, and RLC Circuits
Lab 10: RC, RL, and RLC Circuis In his experimen, we will invesigae he behavior of circuis conaining combinaions of resisors, capaciors, and inducors. We will sudy he way volages and currens change in
More informationFour Generations of Higher Order Sliding Mode Controllers. L. Fridman Universidad Nacional Autonoma de Mexico Aussois, June, 10th, 2015
Four Generaions of Higher Order Sliding Mode Conrollers L. Fridman Universidad Nacional Auonoma de Mexico Aussois, June, 1h, 215 Ouline 1 Generaion 1:Two Main Conceps of Sliding Mode Conrol 2 Generaion
More informationStability and Bifurcation in a Neural Network Model with Two Delays
Inernaional Mahemaical Forum, Vol. 6, 11, no. 35, 175-1731 Sabiliy and Bifurcaion in a Neural Nework Model wih Two Delays GuangPing Hu and XiaoLing Li School of Mahemaics and Physics, Nanjing Universiy
More informationTracking Adversarial Targets
A. Proofs Proof of Lemma 3. Consider he Bellman equaion λ + V π,l x, a lx, a + V π,l Ax + Ba, πax + Ba. We prove he lemma by showing ha he given quadraic form is he unique soluion of he Bellman equaion.
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 informationIMPLICIT AND INVERSE FUNCTION THEOREMS PAUL SCHRIMPF 1 OCTOBER 25, 2013
IMPLICI AND INVERSE FUNCION HEOREMS PAUL SCHRIMPF 1 OCOBER 25, 213 UNIVERSIY OF BRIISH COLUMBIA ECONOMICS 526 We have exensively sudied how o solve sysems of linear equaions. We know how o check wheher
More informationAppendix to Online l 1 -Dictionary Learning with Application to Novel Document Detection
Appendix o Online l -Dicionary Learning wih Applicaion o Novel Documen Deecion Shiva Prasad Kasiviswanahan Huahua Wang Arindam Banerjee Prem Melville A Background abou ADMM In his secion, we give a brief
More informationLinear Quadratic Regulator (LQR) - State Feedback Design
Linear Quadrai Regulaor (LQR) - Sae Feedbak Design A sysem is expressed in sae variable form as x = Ax + Bu n m wih x( ) R, u( ) R and he iniial ondiion x() = x A he sabilizaion problem using sae variable
More informationChapter 8 The Complete Response of RL and RC Circuits
Chaper 8 The Complee Response of RL and RC Circuis Seoul Naional Universiy Deparmen of Elecrical and Compuer Engineering Wha is Firs Order Circuis? Circuis ha conain only one inducor or only one capacior
More informationPredator - Prey Model Trajectories and the nonlinear conservation law
Predaor - Prey Model Trajecories and he nonlinear conservaion law James K. Peerson Deparmen of Biological Sciences and Deparmen of Mahemaical Sciences Clemson Universiy Ocober 28, 213 Ouline Drawing Trajecories
More informationStabilization of NCSs: Asynchronous Partial Transfer Approach
25 American Conrol Conference June 8-, 25 Porland, OR, USA WeC3 Sabilizaion of NCSs: Asynchronous Parial Transfer Approach Guangming Xie, Long Wang Absrac In his paper, a framework for sabilizaion of neworked
More informationMath 333 Problem Set #2 Solution 14 February 2003
Mah 333 Problem Se #2 Soluion 14 February 2003 A1. Solve he iniial value problem dy dx = x2 + e 3x ; 2y 4 y(0) = 1. Soluion: This is separable; we wrie 2y 4 dy = x 2 + e x dx and inegrae o ge The iniial
More informationGlobal Synchronization of Directed Networks with Fast Switching Topologies
Commun. Theor. Phys. (Beijing, China) 52 (2009) pp. 1019 1924 c Chinese Physical Sociey and IOP Publishing Ld Vol. 52, No. 6, December 15, 2009 Global Synchronizaion of Direced Neworks wih Fas Swiching
More informationChapter 6. Systems of First Order Linear Differential Equations
Chaper 6 Sysems of Firs Order Linear Differenial Equaions We will only discuss firs order sysems However higher order sysems may be made ino firs order sysems by a rick shown below We will have a sligh
More informationMatrix Versions of Some Refinements of the Arithmetic-Geometric Mean Inequality
Marix Versions of Some Refinemens of he Arihmeic-Geomeric Mean Inequaliy Bao Qi Feng and Andrew Tonge Absrac. We esablish marix versions of refinemens due o Alzer ], Carwrigh and Field 4], and Mercer 5]
More informationAnn. Funct. Anal. 2 (2011), no. 2, A nnals of F unctional A nalysis ISSN: (electronic) URL:
Ann. Func. Anal. 2 2011, no. 2, 34 41 A nnals of F uncional A nalysis ISSN: 2008-8752 elecronic URL: www.emis.de/journals/afa/ CLASSIFICAION OF POSIIVE SOLUIONS OF NONLINEAR SYSEMS OF VOLERRA INEGRAL EQUAIONS
More informationFinish reading Chapter 2 of Spivak, rereading earlier sections as necessary. handout and fill in some missing details!
MAT 257, Handou 6: Ocober 7-2, 20. I. Assignmen. Finish reading Chaper 2 of Spiva, rereading earlier secions as necessary. handou and fill in some missing deails! II. Higher derivaives. Also, read his
More informationEEEB113 CIRCUIT ANALYSIS I
9/14/29 1 EEEB113 CICUIT ANALYSIS I Chaper 7 Firs-Order Circuis Maerials from Fundamenals of Elecric Circuis 4e, Alexander Sadiku, McGraw-Hill Companies, Inc. 2 Firs-Order Circuis -Chaper 7 7.2 The Source-Free
More informationNovel robust stability criteria of neutral-type bidirectional associative memory neural networks
www.ijcsi.org 0 Novel robus sabiliy crieria of neural-ype bidirecional associaive memory neural neworks Shu-Lian Zhang and Yu-Li Zhang School of Science Dalian Jiaoong Universiy Dalian 608 P. R. China
More informationThe Optimal Stopping Time for Selling an Asset When It Is Uncertain Whether the Price Process Is Increasing or Decreasing When the Horizon Is Infinite
American Journal of Operaions Research, 08, 8, 8-9 hp://wwwscirporg/journal/ajor ISSN Online: 60-8849 ISSN Prin: 60-8830 The Opimal Sopping Time for Selling an Asse When I Is Uncerain Wheher he Price Process
More informationAnti-Disturbance Control for Multiple Disturbances
Workshop a 3 ACC Ani-Disurbance Conrol for Muliple Disurbances Lei Guo (lguo@buaa.edu.cn) Naional Key Laboraory on Science and Technology on Aircraf Conrol, Beihang Universiy, Beijing, 9, P.R. China. Presened
More informationChapter #1 EEE8013 EEE3001. Linear Controller Design and State Space Analysis
Chaper EEE83 EEE3 Chaper # EEE83 EEE3 Linear Conroller Design and Sae Space Analysis Ordinary Differenial Equaions.... Inroducion.... Firs Order ODEs... 3. Second Order ODEs... 7 3. General Maerial...
More informationDual Current-Mode Control for Single-Switch Two-Output Switching Power Converters
Dual Curren-Mode Conrol for Single-Swich Two-Oupu Swiching Power Converers S. C. Wong, C. K. Tse and K. C. Tang Deparmen of Elecronic and Informaion Engineering Hong Kong Polyechnic Universiy, Hunghom,
More informationMath 334 Fall 2011 Homework 11 Solutions
Dec. 2, 2 Mah 334 Fall 2 Homework Soluions Basic Problem. Transform he following iniial value problem ino an iniial value problem for a sysem: u + p()u + q() u g(), u() u, u () v. () Soluion. Le v u. Then
More informationThen. 1 The eigenvalues of A are inside R = n i=1 R i. 2 Union of any k circles not intersecting the other (n k)
Ger sgorin Circle Chaper 9 Approimaing Eigenvalues Per-Olof Persson persson@berkeley.edu Deparmen of Mahemaics Universiy of California, Berkeley Mah 128B Numerical Analysis (Ger sgorin Circle) Le A be
More informationEssential Microeconomics : OPTIMAL CONTROL 1. Consider the following class of optimization problems
Essenial Microeconomics -- 6.5: OPIMAL CONROL Consider he following class of opimizaion problems Max{ U( k, x) + U+ ( k+ ) k+ k F( k, x)}. { x, k+ } = In he language of conrol heory, he vecor k is he vecor
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 information