Notes on Optimal Control

Size: px
Start display at page:

Download "Notes on Optimal Control"

Transcription

1 F.L. Lewis Moncief-O Donnell Endowed Chai Head Conols & Sensos Gop Aomaion & Roboics Reseach Insie ARRI he Univesiy of eas a Alingon Noes on Opimal Conol Sppoed by : NSF - PAUL WERBOS ARO RANDY ZACHERY Dagna abie al available online a hp://arri.a.ed/acs

2 Michael K. Sain Blocing zeos Zeo synhesis modle heoy of mlivaiable zeos of dynamical sysems Eacness of maps SP nonlinea feedbac synhesis James L. Massey Michael K. Sain: Invese Poblems in Coding Aomaa and Coninos Sysems FOCS 967: Michael K. Sain: Minimal osion Spaces and he Paial Inp/Op Poblem Infomaion and Conol 292: M.K. Sain B.F. Wyman J.L. Peczowsi Eended zeos and model maching SIAM Jonal on Conol and Opimizaion May 99 Cheyl B. Schade and Michael K. Sain Zeo Pinciples fo Implici Feedbac Sysems Cicis Sysems and Signal Pocessing: Special Isse on Implici and Robs Sysems ol. 3 No. 2-3 pp Michael K. Sain and Cheyl B. Schade Feedbac Zeos and Blocing Dynamics in Recen Advances in Mahemaical heoy of Sysems Conol Newos and Signal Pocessing I. H. Kima and S. Kodama eds. oyo: Mia Pess pp Michael K. Sain and Cheyl B. Schade Bilinea Opeaos and Maices in Mahemaics fo Cicis and Files. Wai-Kai Chen ed. CRC Pess pp Ronald W. Diesing Michael K. Sain and Chang-Hee Won Bi-Cmlan Games: A genealizaion of H-inf and H2/H-inf Conol" IEEE ansacions on Aomaic Conol Sbmied 2007.

3 Modle heoeic zeo sces fo sysem maices Ahos: Wyman Boswic F.; Sain Michael K. Absac: he coodinae-fee modle-heoeic eamen of ansmission zeos fo MIMO ansfe fncions developed by Wyman and Sain 98 is genealized o inclde nonconollable and nonobsevable linea dynamical sysems.... NASA Cene: NASA non Cene Specific Pblicaion Yea: 987 Added o NRS: Accession Nmbe: 87A3090; Docmen ID:

4 Did I say ha? Well ha was hen. his is now. -M.K. Sain EIC edioial IEEE Cicis & Sysems magazine v.3 no. 2003

5 Opimaliy in Biological Sysems Cell Homeosasis he individal cell is a comple feedbac conol sysem. I pmps ions acoss he cell membane o mainain homeosais and has only limied enegy o do so. Pemeabiliy conol of he cell membane Cellla Meabolism hp://

6 Opimaliy in Conol Sysems Design R. Kalman 960 Roce Obi Injecion Dynamics w 2 v μ F w sinφ 2 m wv F v cosφ m m Fm Objecives Ge o obi in minimm ime Use minimm fel hp://micosa.sm.bms./e-libay/lanch/dnep_geo.pdf

7 Adapive Conol is No Opimal Opimal Conol is off-line and needs o now he sysem dynamics o solve design eqs. We wan ONLINE ADAPIE OPIMAL Conol

8 f d R Q d 0 H f 0 0 min min 0 * * f g R h * 2 * d d g gr d d Q f d d * * 4 * Sysem Cos Hamilonian Opimal cos Opimal conol HJB eqaion Coninos-ime Opimal Conol Bellman min min 0 f Fo a given conol he cos saisfies his eq. In LQR his is a Lyapnov eq In LQR his is a Riccai eq

9 Linea sysem qadaic cos Sysem: Uiliy: A B Q R; R > 0 Q 0 he cos is qadaic Opimal conol sae feedbac: R BP L dτ P HJB eqaion is he algebaic Riccai eqaion ARE: 0 PA A P Q PBR B P Fll sysem dynamics ms be nown

10 C Policy Ieaion o avoid solving HJB eqaion Uiliy Q R Cos fo any given 0 f H Lyapnov eqaion Ieaive solion Pic sabilizing iniial conol Find cos 0 f h h 0 0 Updae conol h 2 R g Convegence poved by Saidis 979 if Lyapnov eq. solved eacly Bead & Saidis sed complicaed Galein Inegals o solve Lyapnov eq. Ab Khalaf & Lewis sed NN o appo. fo nonlinea sysems and poved convegence Fll sysem dynamics ms be nown

11 LQR Policy ieaion Kleinman algoihm. Fo a given conol policy L solve fo he cos: 0 A A P P A C C 2. Impove policy: L A BL R B P L RL If saed wih a sabilizing conol policy L0 he mai P monoonically conveges o he niqe posiive definie solion of he Riccai eqaion. Evey ieaion sep will en a sabilizing conolle. he sysem has o be nown. Lyapnov eq. Kleinman 968

12 Policy Ieaion Solion Policy ieaion A BB P P P A BB P PBB P Q 0 i i i i i i his is in fac a Newon s Mehod Ric P A P PA Q PBB P hen Policy Ieaion is Pi Pi Ric P Ric Pi i 0 i Feche Deivaive Ric' P i P A BB P i P P A BB P i

13 Dagna abie Policy Ieaions wiho Lyapnov Eqaions Dynamic pogamming bil on Bellman s opimaliy pinciple alenaive fom fo C Sysems [Lewis & Symos 995] min d Δ Δ * * τ τ τ τ τ < Δ τ τ τ Q τ τ R τ f and g do no appea

14 Dagna abie Solving fo he cos O appoach Fo a given conol he cos saisfies L Q R d f and g do no appea LQR case P Q R d P Opimal gain is L R B P

15 Dagna abie Solving fo he cos O appoach. Policy ieaion Cos pdae Fo LQR case Q R d L τ τ τ A and B do no appea P Q L RL d P Conol gain pdae L R B P B needed fo conol pdae Iniial sabilizing conol is needed

16 A B B P i P i P i A B B P i P i B B P i Q 0 P P R ic R ic P i 0 i i Pi i Lemma is eqivalen o τ τ τ P Q L RL d P L R B P Solves Lyapnov eqaion wiho nowing A o B A BR B P P P A BR B P P BR B P Q 0 Poof: d d P i A i P i P A i i K i RK i Q Q K RK dτ d P P P heoem i i i i i his algoihm conveges and is eqivalen o Kleinman s Algoihm Only B is needed

17 Algoihm Implemenaion Ciic pdae τ τ τ P Q L RL d P Use Konece podc vec ABC C A vec B o se his p as is he qadaic basis se p τ Q Ki RKi τ dτ p p ϕ p [ ] τ Q Ki RKi τ dτ ρ Reinfocemen on ime ineval [ ] Qadaic egession veco Now se RLS along he ajecoy o ge new weighs p Unpac weighs ino he mai P hen find pdaed FB gain L R B P

18 . Selec iniial conol policy 2. Find associaed cos Solves Lyapnov eq. wiho nowing dynamics [ ] p τ Q L RL τ dτ ρ 3. Impove conol obseve apply L obseve cos inegal L obseve R B P pdae P Mease cos incemen einfocemen by adding as a sae. hen Q R A is no needed anywhee do RLS nil convegence o P pdae conol gain o L

19 Algoihm Implemenaion he Ciic pdae τ τ τ P Q L RL d P can be sep as O se bach Leas-Sqaes solion along he ajecoy i ϕ i [ ] τ τ τ p p Q L RL d d L is he qadaic basis se Evalaing d L fo nn/2 ajecoy poins one can sep a leas sqaes poblem o solve i 2 N X [ ϕ ϕ... ϕ ] 2 N Y d Ki d Ki d Ki p XX XY [... ]

20 Dagna abie Diec Opimal Adapive Conolle his is a vey weid Conol Sce whose lies I have no seen in conol sysem heoy Aco Sysem A B; 0 - sspicios qoe by F.L. Lewis 2007 mliplie L ZOH Q R FB Gain L Ciic Dynamic Conol Sysem A hybid coninos/discee dynamic conolle whose inenal sae is he obseved cos ove he ineval

21 Gain pdae Policy L Conol L Sample peiods need no be he same hey can be seleced on-line in eal ime Coninos-ime conol wih discee gain pdaes

22 Dagna abie 2. C ADP Geedy ieaion Cos pdae Q R d Conol policy L LQR τ τ τ P Q L RL d P Conol gain pdae L R B P A and B do no appea B needed fo conol pdae No iniial sabilizing conol needed Diec Opimal Adapive Conol fo Paially Unnown C Sysems

23 Algoihm Implemenaion he ciic pdae τ τ τ P Q L RL d P Use Konece podc o se his p as vec ABC C A vec B is he qadaic basis se p τ Q L RL τ dτ p Regession veco Pevios weighs Now se RLS along he ajecoy o ge new weighs p Unpac weighs ino he mai P hen find pdaed FB gain L R B P

24 . Selec conol policy Solves fo cos pdae wiho nowing dynamics 2. Find associaed cos p τ Q L RL τ dτ p 3. Impove conol obseve apply obseve cos inegal obseve L R B P pdae P Mease cos incemen by adding as a sae. hen Q R i i No iniial sabilizing conol needed do RLS nil convegence o P pdae conol gain o L A is no needed anywhee

25 Dagna abie Diec Opimal Adapive Conolle A hybid coninos/discee dynamic conolle whose inenal sae is he obseved vale ove he ineval Aco Sysem A B; 0 L ZOH Q R FB Gain L Ciic Dynamic Conol Sysem Has a diffeen ciic cos pdae No iniial sabilizing gain needed

26 Dagna abie Analysis of he algoihm Fo a given conol policy L wih L R B P A A BR B P Geedy pdae { } Q R dτ 0 0 is eqivalen o A A A A P e Q L RL e d e Pe a sange psedo-disceized RE c.f. D RE P A P A Q A P B P A P A Q L P B PK B B P A P B P K B L

27 Dagna abie Analysis of he algoihm Lemma 2. C HDP is eqivalen o P A P e P A AP Q L RL e 0 A his ea em means he iniial Conol acion need no be sabilizing d A A BR B P When ADP conveges he esling P saisfies he Coninos-ime ARE!! ADP solves he C ARE wiho nowledge of he sysem dynamics A

28 Solve he Riccai Eqaion WIHOU nowing he plan dynamics Model-fee ADP Diec OPIMAL ADAPIE CONROL Wos fo Nonlinea Sysems a neal newo is sed o appoimae he cos Robsness? Compaison wih adapive conol mehods?

29 Policy Evalaion Ciic pdae Le K be any sae feedbac gain fo he sysem. One can mease he associaed cos ove he infinie ime hoizon τ Q K RK τ dτ W whee W is an iniial infinie hoizon cos o go. Wha o do abo he ail isses in Receding Hoizon Conol

30 Gain pdae Policy L Conol L Sample peiods need no be he same Coninos-ime conol wih discee gain pdaes

31 Simlaions on: F-6 aopilo Load feqency conol fo powe sysem A mai no needed 0 Conol signal Sysem saes ime s Conolle paamees ime s ime s Ciic paamees P P2 P22 P - opimal P2 - opimal P22 - opimal Convege o SS Riccai eqaion soln ime s

32

33 f d R Q d 0 H f 0 0 min min 0 * * f g R h * 2 * d d g gr d d Q f d d * * 4 * Sysem Cos Hamilonian Opimal cos Opimal conol HJB eqaion Coninos-ime Opimal Conol Bellman min min 0 f h h h γ c.f. D vale ecsion whee f g do no appea

Adaptive Optimal Control F.L. Lewis Automation & Robotics Research Institute (ARRI) The University of Texas at Arlington

Adaptive Optimal Control F.L. Lewis Automation & Robotics Research Institute (ARRI) The University of Texas at Arlington Adapive Opimal Conol F.L. Lewis Aomaion & Roboics Reseach Insie ARRI he Univesiy of eas a Alingon F.L. Lewis Moncief-O Donnell Endowed Chai Head Conols & Sensos Gop Aomaion & Roboics Reseach Insie ARRI

More information

Reinforcement learning

Reinforcement learning Lecue 3 Reinfocemen leaning Milos Hauskech milos@cs.pi.edu 539 Senno Squae Reinfocemen leaning We wan o lean he conol policy: : X A We see examples of x (bu oupus a ae no given) Insead of a we ge a feedback

More information

Notes on Optimal Control

Notes on Optimal Control F.L. Lews Moncef-O Donnell Endowed Cha Head Conols & Sensos Gop Aomaon & Robocs Reseach Inse ARRI he Unvesy of eas a Alngon Noes on Opmal Conol Sppoed by : NSF - PAUL WERBOS ARO RANDY ZACHERY Dagna abe

More information

On Control Problem Described by Infinite System of First-Order Differential Equations

On Control Problem Described by Infinite System of First-Order Differential Equations Ausalian Jounal of Basic and Applied Sciences 5(): 736-74 ISS 99-878 On Conol Poblem Descibed by Infinie Sysem of Fis-Ode Diffeenial Equaions Gafujan Ibagimov and Abbas Badaaya J'afau Insiue fo Mahemaical

More information

Nonlinear Network Structures for Optimal Control

Nonlinear Network Structures for Optimal Control Nonlinear Neork Srcres or Opimal Conrol Cheng ao & Frank. eis Advanced Conrols & Sensors Grop Aomaion & Roboics Research Insie (ARRI) he Universiy o eas a Arlingon Slide Neral Neork Solion or Fied-Final

More information

Chapter Finite Difference Method for Ordinary Differential Equations

Chapter Finite Difference Method for Ordinary Differential Equations Chape 8.7 Finie Diffeence Mehod fo Odinay Diffeenial Eqaions Afe eading his chape, yo shold be able o. Undesand wha he finie diffeence mehod is and how o se i o solve poblems. Wha is he finie diffeence

More information

Optimal Control and Online Game Solutions Using Ui ADP.

Optimal Control and Online Game Solutions Using Ui ADP. F.L. Lewis, K. Vamvodais Aomaion & Roboics Research Insie (ARRI) he Universiy of exas a Arlingon and Opimal Conrol and Online Game Solions Using Ui ADP ADP Using Op Feedbac Dragna Vrabie Senior Research

More information

Combinatorial Approach to M/M/1 Queues. Using Hypergeometric Functions

Combinatorial Approach to M/M/1 Queues. Using Hypergeometric Functions Inenaional Mahemaical Foum, Vol 8, 03, no 0, 463-47 HIKARI Ld, wwwm-hikaicom Combinaoial Appoach o M/M/ Queues Using Hypegeomeic Funcions Jagdish Saan and Kamal Nain Depamen of Saisics, Univesiy of Delhi,

More information

Integration of the constitutive equation

Integration of the constitutive equation Inegaion of he consiive eqaion REMAINDER ON NUMERICAL INTEGRATION Analyical inegaion f ( x( ), x ( )) x x x f () Exac/close-fom solion (no always possible) Nmeical inegaion. i. N T i N [, T ] [ i, i ]

More information

Risk tolerance and optimal portfolio choice

Risk tolerance and optimal portfolio choice Risk oleance and opimal pofolio choice Maek Musiela BNP Paibas London Copoae and Invesmen Join wok wih T. Zaiphopoulou (UT usin) Invesmens and fowad uiliies Pepin 6 Backwad and fowad dynamic uiliies and

More information

Low-complexity Algorithms for MIMO Multiplexing Systems

Low-complexity Algorithms for MIMO Multiplexing Systems Low-complexiy Algoihms fo MIMO Muliplexing Sysems Ouline Inoducion QRD-M M algoihm Algoihm I: : o educe he numbe of suviving pahs. Algoihm II: : o educe he numbe of candidaes fo each ansmied signal. :

More information

and Zero Sum Game Solutions

and Zero Sum Game Solutions F.L. Lewis, K. Vamvoudakis, and D. Vrabie Moncrief-O Donnell Endowed Chair Head, Conrols & Sensors Group Auomaion & Roboics Research Insiue (ARRI) he Universiy of exas a Arlingon Suppored by : NSF PAUL

More information

MEEN 617 Handout #11 MODAL ANALYSIS OF MDOF Systems with VISCOUS DAMPING

MEEN 617 Handout #11 MODAL ANALYSIS OF MDOF Systems with VISCOUS DAMPING MEEN 67 Handou # MODAL ANALYSIS OF MDOF Sysems wih VISCOS DAMPING ^ Symmeic Moion of a n-dof linea sysem is descibed by he second ode diffeenial equaions M+C+K=F whee () and F () ae n ows vecos of displacemens

More information

Servomechanism Design

Servomechanism Design Sevomechanism Design Sevomechanism (sevo-sysem) is a conol sysem in which he efeence () (age, Se poin) changes as ime passes. Design mehods PID Conol u () Ke P () + K I ed () + KDe () Sae Feedback u()

More information

Lecture 18: Kinetics of Phase Growth in a Two-component System: general kinetics analysis based on the dilute-solution approximation

Lecture 18: Kinetics of Phase Growth in a Two-component System: general kinetics analysis based on the dilute-solution approximation Lecue 8: Kineics of Phase Gowh in a Two-componen Sysem: geneal kineics analysis based on he dilue-soluion appoximaion Today s opics: In he las Lecues, we leaned hee diffeen ways o descibe he diffusion

More information

MATHEMATICAL FOUNDATIONS FOR APPROXIMATING PARTICLE BEHAVIOUR AT RADIUS OF THE PLANCK LENGTH

MATHEMATICAL FOUNDATIONS FOR APPROXIMATING PARTICLE BEHAVIOUR AT RADIUS OF THE PLANCK LENGTH Fundamenal Jounal of Mahemaical Phsics Vol 3 Issue 013 Pages 55-6 Published online a hp://wwwfdincom/ MATHEMATICAL FOUNDATIONS FOR APPROXIMATING PARTICLE BEHAVIOUR AT RADIUS OF THE PLANCK LENGTH Univesias

More information

Interaction of Lamb Waves with Geometric Discontinuities: An Analytical Approach Compared with FEM

Interaction of Lamb Waves with Geometric Discontinuities: An Analytical Approach Compared with FEM Ineacion of Lamb Waves ih Geomeic Disconiniies: An Analyical Appoach Compaed ih FEM Banibaa Podda a) and Vico Gigii a) a) Depamen of Mechanical Engineeing, Univesiy of Soh Caolina, USA Absac. The non-descive

More information

Reinforcement learning

Reinforcement learning CS 75 Mchine Lening Lecue b einfocemen lening Milos Huskech milos@cs.pi.edu 539 Senno Sque einfocemen lening We wn o len conol policy: : X A We see emples of bu oupus e no given Insed of we ge feedbck

More information

ROTOR SUPPORTED. J. Tůma, J. Škuta, R. Klečka VSB Technical University of Ostrava J. Šimek TECHLAB Praha

ROTOR SUPPORTED. J. Tůma, J. Škuta, R. Klečka VSB Technical University of Ostrava J. Šimek TECHLAB Praha 9h CONFERENCE on Acive noise and vibaion conol mehods KRAKOW-ZAKOPANE, POLAND Ma 4-7, 9 A 3D MODEL OF THE RIGID ROTOR SUPPORTED BY JOURNAL BEARINGS J. Tůma, J. Ška, R. Klečka VSB Technical Univesi of Osava

More information

Lecture 17: Kinetics of Phase Growth in a Two-component System:

Lecture 17: Kinetics of Phase Growth in a Two-component System: Lecue 17: Kineics of Phase Gowh in a Two-componen Sysem: descipion of diffusion flux acoss he α/ ineface Today s opics Majo asks of oday s Lecue: how o deive he diffusion flux of aoms. Once an incipien

More information

Lecture 22 Electromagnetic Waves

Lecture 22 Electromagnetic Waves Lecue Elecomagneic Waves Pogam: 1. Enegy caied by he wave (Poyning veco).. Maxwell s equaions and Bounday condiions a inefaces. 3. Maeials boundaies: eflecion and efacion. Snell s Law. Quesions you should

More information

[ ] 0. = (2) = a q dimensional vector of observable instrumental variables that are in the information set m constituents of u

[ ] 0. = (2) = a q dimensional vector of observable instrumental variables that are in the information set m constituents of u Genealized Mehods of Momens he genealized mehod momens (GMM) appoach of Hansen (98) can be hough of a geneal pocedue fo esing economics and financial models. he GMM is especially appopiae fo models ha

More information

4.2 Continuous-Time Systems and Processes Problem Definition Let the state variable representation of a linear system be

4.2 Continuous-Time Systems and Processes Problem Definition Let the state variable representation of a linear system be 4 COVARIANCE ROAGAION 41 Inrodcion Now ha we have compleed or review of linear sysems and random processes, we wan o eamine he performance of linear sysems ecied by random processes he sandard approach

More information

Propagation of Torsional Surface Waves. in Heterogeneous Half-Space. with Irregular Free Surface

Propagation of Torsional Surface Waves. in Heterogeneous Half-Space. with Irregular Free Surface Applied Mahemaical Sciences Vol. 7 no. 9 49 437 Popagaion of Tosional Sface Waves in Heeogeneos Half-Space wih Iegla Fee Sface M. M. Selim Depamen of Mahemaics Facly of Еdcaion Se Canal Univesiy Se Egyp

More information

Online Partially Model-Free Solution of Two-Player Zero Sum Differential Games

Online 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 information

A STOCHASTIC MODELING FOR THE UNSTABLE FINANCIAL MARKETS

A STOCHASTIC MODELING FOR THE UNSTABLE FINANCIAL MARKETS A STOCHASTIC MODELING FOR THE UNSTABLE FINANCIAL MARKETS Assoc. Pof. Romeo Negea Ph. D Poliehnica Univesiy of Timisoaa Depamen of Mahemaics Timisoaa, Romania Assoc. Pof. Cipian Peda Ph. D Wes Univesiy

More information

Lecture 20: Riccati Equations and Least Squares Feedback Control

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 information

Variance and Covariance Processes

Variance and Covariance Processes Vaiance and Covaiance Pocesses Pakash Balachandan Depamen of Mahemaics Duke Univesiy May 26, 2008 These noes ae based on Due s Sochasic Calculus, Revuz and Yo s Coninuous Maingales and Bownian Moion, Kaazas

More information

Today - Lecture 13. Today s lecture continue with rotations, torque, Note that chapters 11, 12, 13 all involve rotations

Today - Lecture 13. Today s lecture continue with rotations, torque, Note that chapters 11, 12, 13 all involve rotations Today - Lecue 13 Today s lecue coninue wih oaions, oque, Noe ha chapes 11, 1, 13 all inole oaions slide 1 eiew Roaions Chapes 11 & 1 Viewed fom aboe (+z) Roaional, o angula elociy, gies angenial elociy

More information

Kalman Filter: an instance of Bayes Filter. Kalman Filter: an instance of Bayes Filter. Kalman Filter. Linear dynamics with Gaussian noise

Kalman Filter: an instance of Bayes Filter. Kalman Filter: an instance of Bayes Filter. Kalman Filter. Linear dynamics with Gaussian noise COM47 Inoducion o Roboics and Inelligen ysems he alman File alman File: an insance of Bayes File alman File: an insance of Bayes File Linea dynamics wih Gaussian noise alman File Linea dynamics wih Gaussian

More information

Q-LEARNING is a method of reinforcement learning

Q-LEARNING is a method of reinforcement learning IEEE TRANSACTIONS ON CYBERNETICS, VOL. 45, NO. 2, FEBRUARY 2015 165 Coninos-Time Q-Learning for Infinie-Horizon Disconed Cos Linear Qadraic Reglaor Problems Mhkmar Palanisamy, Hamidreza Modares, Frank

More information

Dual Hierarchies of a Multi-Component Camassa Holm System

Dual Hierarchies of a Multi-Component Camassa Holm System Commun. heo. Phys. 64 05 37 378 Vol. 64, No. 4, Ocobe, 05 Dual Hieachies of a Muli-Componen Camassa Holm Sysem LI Hong-Min, LI Yu-Qi, and CHEN Yong Shanghai Key Laboaoy of uswohy Compuing, Eas China Nomal

More information

International Journal of Mathematical Archive-5(6), 2014, Available online through ISSN

International Journal of Mathematical Archive-5(6), 2014, Available online through   ISSN Inenaional Jonal o Mahemaical Achive-6, 0, 09-8 Availale online hogh www.ijma.ino ISSN 9 06 EXISENCE OF NONOSCILLAORY SOLUIONS OF A CLASS OF NONLINEAR NEURAL DELAY DIFFERENIAL EQUAIONS OF HIRD ORDER K

More information

7 Wave Equation in Higher Dimensions

7 Wave Equation in Higher Dimensions 7 Wave Equaion in Highe Dimensions We now conside he iniial-value poblem fo he wave equaion in n dimensions, u c u x R n u(x, φ(x u (x, ψ(x whee u n i u x i x i. (7. 7. Mehod of Spheical Means Ref: Evans,

More information

ENGI 4430 Advanced Calculus for Engineering Faculty of Engineering and Applied Science Problem Set 9 Solutions [Theorems of Gauss and Stokes]

ENGI 4430 Advanced Calculus for Engineering Faculty of Engineering and Applied Science Problem Set 9 Solutions [Theorems of Gauss and Stokes] ENGI 44 Avance alculus fo Engineeing Faculy of Engineeing an Applie cience Poblem e 9 oluions [Theoems of Gauss an okes]. A fla aea A is boune by he iangle whose veices ae he poins P(,, ), Q(,, ) an R(,,

More information

Regional Controllability of Semi-Linear Distributed Parabolic Systems: Theory and Simulation

Regional Controllability of Semi-Linear Distributed Parabolic Systems: Theory and Simulation Inelligen Conol an omaion,,, 46-58 hp://xoiog/46/ica7 Pblishe Online May (hp://wwwscirpog/jonal/ica) Regional Conollabiliy of Semi-Linea Disibe Paabolic Sysems: heoy an Simlaion smae Kamal, li Boolo, Sii

More information

Lecture-V Stochastic Processes and the Basic Term-Structure Equation 1 Stochastic Processes Any variable whose value changes over time in an uncertain

Lecture-V Stochastic Processes and the Basic Term-Structure Equation 1 Stochastic Processes Any variable whose value changes over time in an uncertain Lecue-V Sochasic Pocesses and he Basic Tem-Sucue Equaion 1 Sochasic Pocesses Any vaiable whose value changes ove ime in an unceain way is called a Sochasic Pocess. Sochasic Pocesses can be classied as

More information

KINEMATICS OF RIGID BODIES

KINEMATICS OF RIGID BODIES KINEMTICS OF RIGID ODIES In igid body kinemaics, we use he elaionships govening he displacemen, velociy and acceleaion, bu mus also accoun fo he oaional moion of he body. Descipion of he moion of igid

More information

The Nehari Manifold for a Class of Elliptic Equations of P-laplacian Type. S. Khademloo and H. Mohammadnia. afrouzi

The Nehari Manifold for a Class of Elliptic Equations of P-laplacian Type. S. Khademloo and H. Mohammadnia. afrouzi Wold Alied cieces Joal (8): 898-95 IN 88-495 IDOI Pblicaios = h x g x x = x N i W whee is a eal aamee is a boded domai wih smooh boday i R N 3 ad< < INTRODUCTION Whee s ha is s = I his ae we ove he exisece

More information

On The Estimation of Two Missing Values in Randomized Complete Block Designs

On The Estimation of Two Missing Values in Randomized Complete Block Designs Mahemaical Theoy and Modeling ISSN 45804 (Pape ISSN 505 (Online Vol.6, No.7, 06 www.iise.og On The Esimaion of Two Missing Values in Randomized Complee Bloc Designs EFFANGA, EFFANGA OKON AND BASSE, E.

More information

Optimal Control. Lecture 5. Prof. Daniela Iacoviello

Optimal Control. Lecture 5. Prof. Daniela Iacoviello Opimal Conrol ecre 5 Pro. Daniela Iacoviello THESE SIDES ARE NOT SUFFICIENT FOR THE EXAM: YOU MUST STUDY ON THE BOOKS Par o he slides has been aken rom he Reerences indicaed below Pro. D.Iacoviello - Opimal

More information

arxiv: v1 [math.co] 4 Apr 2019

arxiv: v1 [math.co] 4 Apr 2019 Dieced dominaion in oiened hypegaphs axiv:1904.02351v1 [mah.co] 4 Ap 2019 Yai Cao Dep. of Mahemaics Univesiy of Haifa-Oanim Tivon 36006, Isael yacao@kvgeva.og.il This pape is dedicaed o Luz Volkmann on

More information

General Non-Arbitrage Model. I. Partial Differential Equation for Pricing A. Traded Underlying Security

General Non-Arbitrage Model. I. Partial Differential Equation for Pricing A. Traded Underlying Security 1 Geneal Non-Abiage Model I. Paial Diffeenial Equaion fo Picing A. aded Undelying Secuiy 1. Dynamics of he Asse Given by: a. ds = µ (S, )d + σ (S, )dz b. he asse can be eihe a sock, o a cuency, an index,

More information

Online Completion of Ill-conditioned Low-Rank Matrices

Online Completion of Ill-conditioned Low-Rank Matrices Online Compleion of Ill-condiioned Low-Rank Maices Ryan Kennedy and Camillo J. Taylo Compue and Infomaion Science Univesiy of Pennsylvania Philadelphia, PA, USA keny, cjaylo}@cis.upenn.edu Laua Balzano

More information

Millennium Theory Equations Original Copyright 2002 Joseph A. Rybczyk Updated Copyright 2003 Joseph A. Rybczyk Updated March 16, 2006

Millennium Theory Equations Original Copyright 2002 Joseph A. Rybczyk Updated Copyright 2003 Joseph A. Rybczyk Updated March 16, 2006 Millennim heoy Eqaions Oiginal Copyigh 00 Joseph A. Rybzyk Updaed Copyigh 003 Joseph A. Rybzyk Updaed Mah 6, 006 Following is a omplee lis o he Millennim heoy o Relaiviy eqaions: Fo easy eeene, all eqaions

More information

AN EFFICIENT INTEGRAL METHOD FOR THE COMPUTATION OF THE BODIES MOTION IN ELECTROMAGNETIC FIELD

AN EFFICIENT INTEGRAL METHOD FOR THE COMPUTATION OF THE BODIES MOTION IN ELECTROMAGNETIC FIELD AN EFFICIENT INTEGRAL METHOD FOR THE COMPUTATION OF THE BODIES MOTION IN ELECTROMAGNETIC FIELD GEORGE-MARIAN VASILESCU, MIHAI MARICARU, BOGDAN DUMITRU VĂRĂTICEANU, MARIUS AUREL COSTEA Key wods: Eddy cuen

More information

The shortest path between two truths in the real domain passes through the complex domain. J. Hadamard

The shortest path between two truths in the real domain passes through the complex domain. J. Hadamard Complex Analysis R.G. Halbud R.Halbud@ucl.ac.uk Depamen of Mahemaics Univesiy College London 202 The shoes pah beween wo uhs in he eal domain passes hough he complex domain. J. Hadamad Chape The fis fundamenal

More information

r P + '% 2 r v(r) End pressures P 1 (high) and P 2 (low) P 1 , which must be independent of z, so # dz dz = P 2 " P 1 = " #P L L,

r P + '% 2 r v(r) End pressures P 1 (high) and P 2 (low) P 1 , which must be independent of z, so # dz dz = P 2  P 1 =  #P L L, Lecue 36 Pipe Flow and Low-eynolds numbe hydodynamics 36.1 eading fo Lecues 34-35: PKT Chape 12. Will y fo Monday?: new daa shee and daf fomula shee fo final exam. Ou saing poin fo hydodynamics ae wo equaions:

More information

Localization and Map Making

Localization and Map Making Localiaion and Map Making My old office DILab a UTK ar of he following noes are from he book robabilisic Roboics by S. Thrn W. Brgard and D. Fo Two Remaining Qesions Where am I? Localiaion Where have I

More information

Critical statics and dynamics of QCD CEP

Critical statics and dynamics of QCD CEP Ciical saics and dynamics of QCD CEP Eiji Nakano Dep. Physics, Kochi Univesiy, and ExeMe Mae Insie @ GSI,Gemany w/ B. Fiman, V. Skokov, K. Redlich, and B-J. Schaefe Conen: 1. Moivaion. Basics on ciical

More information

On the Semi-Discrete Davey-Stewartson System with Self-Consistent Sources

On the Semi-Discrete Davey-Stewartson System with Self-Consistent Sources Jounal of Applied Mahemaics and Physics 25 3 478-487 Published Online May 25 in SciRes. hp://www.scip.og/jounal/jamp hp://dx.doi.og/.4236/jamp.25.356 On he Semi-Discee Davey-Sewason Sysem wih Self-Consisen

More information

@FMI c Kyung Moon Sa Co.

@FMI c Kyung Moon Sa Co. Annals of Fuzzy Mahemaics Infomaics Volume, No. 2, (Apil 20), pp. 9-3 ISSN 2093 930 hp://www.afmi.o.k @FMI c Kyung Moon Sa Co. hp://www.kyungmoon.com On lacunay saisical convegence in inuiionisic fuzzy

More information

POSITIVE SOLUTIONS WITH SPECIFIC ASYMPTOTIC BEHAVIOR FOR A POLYHARMONIC PROBLEM ON R n. Abdelwaheb Dhifli

POSITIVE SOLUTIONS WITH SPECIFIC ASYMPTOTIC BEHAVIOR FOR A POLYHARMONIC PROBLEM ON R n. Abdelwaheb Dhifli Opuscula Mah. 35, no. (205), 5 9 hp://dx.doi.og/0.7494/opmah.205.35..5 Opuscula Mahemaica POSITIVE SOLUTIONS WITH SPECIFIC ASYMPTOTIC BEHAVIOR FOR A POLYHARMONIC PROBLEM ON R n Abdelwaheb Dhifli Communicaed

More information

Synchronization of Fractional Chaotic Systems via Fractional-Order Adaptive Controller

Synchronization of Fractional Chaotic Systems via Fractional-Order Adaptive Controller Synchonizaion of Facional Chaoic Sysems via Facional-Ode Adapive Conolle S.H. Hosseinnia*, R. Ghadei*, A. Ranjba N.*, J. Sadai*, S. Momani** * Noshivani Univesiy of Technology, Faculy of Elecical Compue

More information

Sections 3.1 and 3.4 Exponential Functions (Growth and Decay)

Sections 3.1 and 3.4 Exponential Functions (Growth and Decay) Secions 3.1 and 3.4 Eponenial Funcions (Gowh and Decay) Chape 3. Secions 1 and 4 Page 1 of 5 Wha Would You Rahe Have... $1million, o double you money evey day fo 31 days saing wih 1cen? Day Cens Day Cens

More information

Extremal problems for t-partite and t-colorable hypergraphs

Extremal problems for t-partite and t-colorable hypergraphs Exemal poblems fo -paie and -coloable hypegaphs Dhuv Mubayi John Talbo June, 007 Absac Fix ineges and an -unifom hypegaph F. We pove ha he maximum numbe of edges in a -paie -unifom hypegaph on n veices

More information

Discretization of Fractional Order Differentiator and Integrator with Different Fractional Orders

Discretization of Fractional Order Differentiator and Integrator with Different Fractional Orders Inelligen Conol and Auomaion, 207, 8, 75-85 hp://www.scip.og/jounal/ica ISSN Online: 253-066 ISSN Pin: 253-0653 Disceizaion of Facional Ode Diffeeniao and Inegao wih Diffeen Facional Odes Qi Zhang, Baoye

More information

Advanced Control Systems Problem Sheet for Part B: Multivariable Systems

Advanced Control Systems Problem Sheet for Part B: Multivariable Systems 436-45 Advanced Conrol Ssems Problem Shee for Par B: Mlivariable Ssems Qesion B 998 Given a lan o be conrolled, which is described b a sae-sace model A B C Oline he rocess b which o wold design a discree

More information

STUDY OF THE STRESS-STRENGTH RELIABILITY AMONG THE PARAMETERS OF GENERALIZED INVERSE WEIBULL DISTRIBUTION

STUDY OF THE STRESS-STRENGTH RELIABILITY AMONG THE PARAMETERS OF GENERALIZED INVERSE WEIBULL DISTRIBUTION Inenaional Jounal of Science, Technology & Managemen Volume No 04, Special Issue No. 0, Mach 205 ISSN (online): 2394-537 STUDY OF THE STRESS-STRENGTH RELIABILITY AMONG THE PARAMETERS OF GENERALIZED INVERSE

More information

BU Macro BU Macro Fall 2008, Lecture 4

BU Macro BU Macro Fall 2008, Lecture 4 Dynamic Programming BU Macro 2008 Lecure 4 1 Ouline 1. Cerainy opimizaion problem used o illusrae: a. Resricions on exogenous variables b. Value funcion c. Policy funcion d. The Bellman equaion and an

More information

DESIGN OF TENSION MEMBERS

DESIGN OF TENSION MEMBERS CHAPTER Srcral Seel Design LRFD Mehod DESIGN OF TENSION MEMBERS Third Ediion A. J. Clark School of Engineering Deparmen of Civil and Environmenal Engineering Par II Srcral Seel Design and Analysis 4 FALL

More information

( ) exp i ω b ( ) [ III-1 ] exp( i ω ab. exp( i ω ba

( ) exp i ω b ( ) [ III-1 ] exp( i ω ab. exp( i ω ba THE INTEACTION OF ADIATION AND MATTE: SEMICLASSICAL THEOY PAGE 26 III. EVIEW OF BASIC QUANTUM MECHANICS : TWO -LEVEL QUANTUM SYSTEMS : The lieaue of quanum opics and lase specoscop abounds wih discussions

More information

NUMERICAL SIMULATION FOR NONLINEAR STATIC & DYNAMIC STRUCTURAL ANALYSIS

NUMERICAL SIMULATION FOR NONLINEAR STATIC & DYNAMIC STRUCTURAL ANALYSIS Join Inenaional Confeence on Compuing and Decision Making in Civil and Building Engineeing June 14-16, 26 - Monéal, Canada NUMERICAL SIMULATION FOR NONLINEAR STATIC & DYNAMIC STRUCTURAL ANALYSIS ABSTRACT

More information

A FINITE-MEMORY DISCRETE-TIME CONVOLUTION APPROACH FOR THE NON-LINEAR DYNAMIC MODELLING OF S/H-ADC DEVICES

A FINITE-MEMORY DISCRETE-TIME CONVOLUTION APPROACH FOR THE NON-LINEAR DYNAMIC MODELLING OF S/H-ADC DEVICES FINITE-MEMORY DISCRETE-TIME CONVOLUTION PPROCH FOR THE NON-LINER DYNMIC MODELLING OF S/H-DC DEVICES D. Mii, G. Pasini, P.. Taveso 2, F. Filicoi 2, G. Iclano 3 Depaen of Elecical Engineeing, Univesiy of

More information

Gradient-based Neural Network for Online Solution of Lyapunov Matrix Equation with Li Activation Function

Gradient-based Neural Network for Online Solution of Lyapunov Matrix Equation with Li Activation Function Intenational Confeence on Infomation echnology and Management Innovation (ICIMI 05) Gadient-based Neual Netwok fo Online Solution of Lyapunov Matix Equation with Li Activation unction Shiheng Wang, Shidong

More information

EE363 homework 1 solutions

EE363 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 information

AN EVOLUTIONARY APPROACH FOR SOLVING DIFFERENTIAL EQUATIONS

AN EVOLUTIONARY APPROACH FOR SOLVING DIFFERENTIAL EQUATIONS AN EVOLUTIONARY APPROACH FOR SOLVING DIFFERENTIAL EQUATIONS M. KAMESWAR RAO AND K.P. RAVINDRAN Depamen of Mechanical Engineeing, Calicu Regional Engineeing College, Keala-67 6, INDIA. Absac:- We eploe

More information

ON 3-DIMENSIONAL CONTACT METRIC MANIFOLDS

ON 3-DIMENSIONAL CONTACT METRIC MANIFOLDS Mem. Fac. Inegaed As and Sci., Hioshima Univ., Se. IV, Vol. 8 9-33, Dec. 00 ON 3-DIMENSIONAL CONTACT METRIC MANIFOLDS YOSHIO AGAOKA *, BYUNG HAK KIM ** AND JIN HYUK CHOI ** *Depamen of Mahemaics, Faculy

More information

Linear Quadratic Regulator (LQR) - State Feedback Design

Linear 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 information

PHYS PRACTICE EXAM 2

PHYS PRACTICE EXAM 2 PHYS 1800 PRACTICE EXAM Pa I Muliple Choice Quesions [ ps each] Diecions: Cicle he one alenaive ha bes complees he saemen o answes he quesion. Unless ohewise saed, assume ideal condiions (no ai esisance,

More information

Orthotropic Materials

Orthotropic Materials Kapiel 2 Ohoopic Maeials 2. Elasic Sain maix Elasic sains ae elaed o sesses by Hooke's law, as saed below. The sesssain elaionship is in each maeial poin fomulaed in he local caesian coodinae sysem. ε

More information

ÖRNEK 1: THE LINEAR IMPULSE-MOMENTUM RELATION Calculate the linear momentum of a particle of mass m=10 kg which has a. kg m s

ÖRNEK 1: THE LINEAR IMPULSE-MOMENTUM RELATION Calculate the linear momentum of a particle of mass m=10 kg which has a. kg m s MÜHENDİSLİK MEKANİĞİ. HAFTA İMPULS- MMENTUM-ÇARPIŞMA Linea oenu of a paicle: The sybol L denoes he linea oenu and is defined as he ass ies he elociy of a paicle. L ÖRNEK : THE LINEAR IMPULSE-MMENTUM RELATIN

More information

An Automatic Door Sensor Using Image Processing

An Automatic Door Sensor Using Image Processing An Auomaic Doo Senso Using Image Pocessing Depamen o Elecical and Eleconic Engineeing Faculy o Engineeing Tooi Univesiy MENDEL 2004 -Insiue o Auomaion and Compue Science- in BRNO CZECH REPUBLIC 1. Inoducion

More information

Sharif University of Technology - CEDRA By: Professor Ali Meghdari

Sharif University of Technology - CEDRA By: Professor Ali Meghdari Shaif Univesiy of echnology - CEDRA By: Pofesso Ali Meghai Pupose: o exen he Enegy appoach in eiving euaions of oion i.e. Lagange s Meho fo Mechanical Syses. opics: Genealize Cooinaes Lagangian Euaion

More information

Suppose we have observed values t 1, t 2, t n of a random variable T.

Suppose we have observed values t 1, t 2, t n of a random variable T. Sppose we have obseved vales, 2, of a adom vaable T. The dsbo of T s ow o belog o a cea ype (e.g., expoeal, omal, ec.) b he veco θ ( θ, θ2, θp ) of ow paamees assocaed wh s ow (whee p s he mbe of ow paamees).

More information

Essential Microeconomics : OPTIMAL CONTROL 1. Consider the following class of optimization problems

Essential 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 information

SUFFICIENT CONDITIONS FOR EXISTENCE SOLUTION OF LINEAR TWO-POINT BOUNDARY PROBLEM IN MINIMIZATION OF QUADRATIC FUNCTIONAL

SUFFICIENT 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 information

Control Volume Derivation

Control Volume Derivation School of eospace Engineeing Conol Volume -1 Copyigh 1 by Jey M. Seizman. ll ighs esee. Conol Volume Deiaion How o cone ou elaionships fo a close sysem (conol mass) o an open sysem (conol olume) Fo mass

More information

Unitary Matrices in Fiber Optical Communications: Applications

Unitary Matrices in Fiber Optical Communications: Applications Uniay Maices in Fibe Opical Communicaions: Applicaions Ais Mousaas A. Kaadimiais Ahens P. Vivo KCL R. Couille Pais-Cenal L. Sanguinei Pisa A. Mulle Huawei H. Hafemann Huawei Ais Mousaas, Univesiy of Ahens

More information

The Production of Polarization

The Production of Polarization Physics 36: Waves Lecue 13 3/31/211 The Poducion of Polaizaion Today we will alk abou he poducion of polaized ligh. We aleady inoduced he concep of he polaizaion of ligh, a ansvese EM wave. To biefly eview

More information

, on the power of the transmitter P t fed to it, and on the distance R between the antenna and the observation point as. r r t

, on the power of the transmitter P t fed to it, and on the distance R between the antenna and the observation point as. r r t Lecue 6: Fiis Tansmission Equaion and Rada Range Equaion (Fiis equaion. Maximum ange of a wieless link. Rada coss secion. Rada equaion. Maximum ange of a ada. 1. Fiis ansmission equaion Fiis ansmission

More information

EFFECT OF PERMISSIBLE DELAY ON TWO-WAREHOUSE INVENTORY MODEL FOR DETERIORATING ITEMS WITH SHORTAGES

EFFECT OF PERMISSIBLE DELAY ON TWO-WAREHOUSE INVENTORY MODEL FOR DETERIORATING ITEMS WITH SHORTAGES Volume, ssue 3, Mach 03 SSN 39-4847 EFFEC OF PERMSSBLE DELAY ON WO-WAREHOUSE NVENORY MODEL FOR DEERORANG EMS WH SHORAGES D. Ajay Singh Yadav, Ms. Anupam Swami Assisan Pofesso, Depamen of Mahemaics, SRM

More information

Relations on the Apostol Type (p, q)-frobenius-euler Polynomials and Generalizations of the Srivastava-Pintér Addition Theorems

Relations on the Apostol Type (p, q)-frobenius-euler Polynomials and Generalizations of the Srivastava-Pintér Addition Theorems Tish Joal of Aalysis ad Nmbe Theoy 27 Vol 5 No 4 26-3 Available olie a hp://pbssciepbcom/ja/5/4/2 Sciece ad Edcaio Pblishig DOI:269/ja-5-4-2 Relaios o he Aposol Type (p -Fobeis-Ele Polyomials ad Geealizaios

More information

Application of Bernoulli wavelet method for numerical solution of fuzzy linear Volterra-Fredholm integral equations Abstract Keywords

Application of Bernoulli wavelet method for numerical solution of fuzzy linear Volterra-Fredholm integral equations Abstract Keywords Applicaion o enoulli wavele mehod o numeical soluion o uzz linea Volea-edholm inegal equaions Mohamed A. Ramadan a and Mohamed R. Ali b a Depamen o Mahemaics acul o Science Menouia Univesi Egp mamadan@eun.eg;

More information

An Analytical Study of Strong Non Planer Shock. Waves in Magnetogasdynamics

An Analytical Study of Strong Non Planer Shock. Waves in Magnetogasdynamics Adv Theo Appl Mech Vol no 6 9-97 An Analyical Sdy of Song Non Plane Shock Waves in Magneogasdynaics L P Singh Depaen of Applied Maheaics Insie of Technology Banaas Hind Univesiy Vaanasi-5 India Akal Hsain

More information

The k-filtering Applied to Wave Electric and Magnetic Field Measurements from Cluster

The k-filtering Applied to Wave Electric and Magnetic Field Measurements from Cluster The -fileing pplied o Wave lecic and Magneic Field Measuemens fom Cluse Jean-Louis PINÇON and ndes TJULIN LPC-CNRS 3 av. de la Recheche Scienifique 4507 Oléans Fance jlpincon@cns-oleans.f OUTLINS The -fileing

More information

Dispersive Systems. 1) Schrödinger equation 2) Cubic Schrödinger 3) KdV 4) Discreterised hyperbolic equation 5) Discrete systems.

Dispersive Systems. 1) Schrödinger equation 2) Cubic Schrödinger 3) KdV 4) Discreterised hyperbolic equation 5) Discrete systems. Dispersive Sysems 1) Schrödinger eqaion ) Cbic Schrödinger 3) KdV 4) Discreerised hyperbolic eqaion 5) Discree sysems KdV + + ε =, = ( ) ( ) d d + = d d =, =. ( ) = ( ) DISCONTINUITY, prescribed cri Collision

More information

Tracking Control for Hybrid Systems via Embedding of Known Reference Trajectories

Tracking Control for Hybrid Systems via Embedding of Known Reference Trajectories Tacking Conol fo Hybid Sysems via Embedding of Known Refeence Tajecoies Ricado G. Sanfelice, J. J. Benjamin Biemond, Nahan van de Wouw, and W. P. Mauice H. Heemels Absac We sudy he poblem of designing

More information

PHYS GENERAL RELATIVITY AND COSMOLOGY PROBLEM SET 7 - SOLUTIONS

PHYS GENERAL RELATIVITY AND COSMOLOGY PROBLEM SET 7 - SOLUTIONS PHYS 54 - GENERAL RELATIVITY AND COSMOLOGY - 07 - PROBLEM SET 7 - SOLUTIONS TA: Jeome Quinin Mach, 07 Noe ha houghou hee oluion, we wok in uni whee c, and we chooe he meic ignaue (,,, ) a ou convenion..

More information

Computer Propagation Analysis Tools

Computer Propagation Analysis Tools Compue Popagaion Analysis Tools. Compue Popagaion Analysis Tools Inoducion By now you ae pobably geing he idea ha pedicing eceived signal sengh is a eally impoan as in he design of a wieless communicaion

More information

Reserves measures have an economic component eg. what could be extracted at current prices?

Reserves measures have an economic component eg. what could be extracted at current prices? 3.2 Non-renewable esources A. Are socks of non-renewable resources fixed? eserves measures have an economic componen eg. wha could be exraced a curren prices? - Locaion and quaniies of reserves of resources

More information

ON THE OSCILLATION OF THIRD ORDER FUNCTIONAL DIFFERENTIAL EQUATIONS. Cairo University, Orman, Giza 12221, Egypt

ON THE OSCILLATION OF THIRD ORDER FUNCTIONAL DIFFERENTIAL EQUATIONS. Cairo University, Orman, Giza 12221, Egypt a 1/α s)ds < Indian J. pre appl. Mah., 396): 491-507, December 2008 c Prined in India. ON THE OSCILLATION OF THIRD ORDER FUNCTIONAL DIFFERENTIAL EQUATIONS SAID R. GRACE 1, RAVI P. AGARWAL 2 AND MUSTAFA

More information

Molecular Evolution and Phylogeny. Based on: Durbin et al Chapter 8

Molecular Evolution and Phylogeny. Based on: Durbin et al Chapter 8 Molecula Evoluion and hylogeny Baed on: Dubin e al Chape 8. hylogeneic Tee umpion banch inenal node leaf Topology T : bifucaing Leave - N Inenal node N+ N- Lengh { i } fo each banch hylogeneic ee Topology

More information

The sudden release of a large amount of energy E into a background fluid of density

The sudden release of a large amount of energy E into a background fluid of density 10 Poin explosion The sudden elease of a lage amoun of enegy E ino a backgound fluid of densiy ceaes a song explosion, chaaceized by a song shock wave (a blas wave ) emanaing fom he poin whee he enegy

More information

WORK POWER AND ENERGY Consevaive foce a) A foce is said o be consevaive if he wok done by i is independen of pah followed by he body b) Wok done by a consevaive foce fo a closed pah is zeo c) Wok done

More information

SZG Macro 2011 Lecture 3: Dynamic Programming. SZG macro 2011 lecture 3 1

SZG Macro 2011 Lecture 3: Dynamic Programming. SZG macro 2011 lecture 3 1 SZG Macro 2011 Lecure 3: Dynamic Programming SZG macro 2011 lecure 3 1 Background Our previous discussion of opimal consumpion over ime and of opimal capial accumulaion sugges sudying he general decision

More information

336 ERIDANI kfk Lp = sup jf(y) ; f () jj j p p whee he supemum is aken ove all open balls = (a ) inr n, jj is he Lebesgue measue of in R n, () =(), f

336 ERIDANI kfk Lp = sup jf(y) ; f () jj j p p whee he supemum is aken ove all open balls = (a ) inr n, jj is he Lebesgue measue of in R n, () =(), f TAMKANG JOURNAL OF MATHEMATIS Volume 33, Numbe 4, Wine 2002 ON THE OUNDEDNESS OF A GENERALIED FRATIONAL INTEGRAL ON GENERALIED MORREY SPAES ERIDANI Absac. In his pape we exend Nakai's esul on he boundedness

More information

Circular Motion. Radians. One revolution is equivalent to which is also equivalent to 2π radians. Therefore we can.

Circular Motion. Radians. One revolution is equivalent to which is also equivalent to 2π radians. Therefore we can. 1 Cicula Moion Radians One evoluion is equivalen o 360 0 which is also equivalen o 2π adians. Theefoe we can say ha 360 = 2π adians, 180 = π adians, 90 = π 2 adians. Hence 1 adian = 360 2π Convesions Rule

More information

Predictive Control of Parabolic PDEs with State and Control Constraints*

Predictive Control of Parabolic PDEs with State and Control Constraints* Predicive Conrol of Parabolic PDEs wih Sae and Conrol Consrains* Sevan Dbljevic, Nael H. El-Farra, Prashan Mhaskar, and Panagiois D. Chrisofides Deparmen of Chemical Engineering Universiy of California,

More information

MATH 128A, SUMMER 2009, FINAL EXAM SOLUTION

MATH 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 information