Discontinuity Preserving Noise Removal Method based on Anisotropic Diffusion for Band Pass Signals

Size: px
Start display at page:

Download "Discontinuity Preserving Noise Removal Method based on Anisotropic Diffusion for Band Pass Signals"

Transcription

1 isconini Preservin Noise emoval Mehod based on Anisoropic iffsion for Band Pass Sinals Sasan Mahmoodi School of lecronic and omper Science Universi of Sohampon Sohampon U sm3@ecs.soon.ac.k Absrac A nonlinear disconini-preservin mehod for noise removal for band pass sinals sch as sinals modlaed wih Binar Phase-Shif ein BPS modlaion is proposed in his paper. This mehod is inspired b he anisoropic diffsion alorihm o remove noise and preserve disconiniies in band pass sinals modlaed wih a sinle freqenc. I is demonsraed here ha nonlinear noise removal mehod for a real valed band pass sinal reqires a solion for a nonlinear parial differenial eqaion which is of forh order in space and second order in ime. The resls presened in his work show beer performance in nonlinear noise removal for real valed band pass sinals in comparison wih he previos work in he lierare ewords Anisoropic iffsion; Band Pass Sinals; Noise emoval; arrier Sinal; isconini Preservaion; I. INTOUTION Anisoropic diffsion for ede-preservin noise removal in imaes is iniiall p forward b Perona and Malik PM in heir seminal work [1]. Geri e al. eneralize he nonlinear noise removal mehod of PM o 3 volmeric MI imaes []. A color anisoropic diffsion is also developed b Sapiro e al. [3] o remove he noise and preserve edes in color imaes. A robs esimaion mehod o erac a piecewise smooh imae from an oriinal nois imae is sesed b Black e al. [4]. rvare-preservin parial differenial eqaions Ps are emploed b Tshmperie [5] o propose a fas anisoropic smoohin alorihm for he noise removal of mli-valed imaes. Lo e. al [6] propose a echniqe o smooh nois imaes b eploiin an ede-srenh srae o improve he preservaion of he deails of he smoohed imae. Finall a nonlinear filerin scheme based on a linear parial differenial eqaion of he pe of he Hea eqaion is proposed b Mahmoodi [7] o remove noise in band pass sinals b preservin disconiniies and modlain carrier sinal. The mehod proposed in [7] however can onl be sed for comple valed sinals. In order for his mehod o be sed for real valed sinals Hilber ransform is emploed in [7] o prodce comple valed sinals o of heir real valed ones. A new parial differenial eqaion is herefore reqired for noise removal in real valed sinals. This is no a rivial problem. Or conribion in his paper is ha a hiher order parial differenial eqaion based on he one invesiaed in [7] is proposed o perform he noise removal of real valed band pass sinals wih no reqiremen o se Hilber ransform o prodce he imainar par of a real valed sinal. This paper is srcred as follows. The heor is presened in secion II. Secion III deals wih implemenaion isses. Nmerical resls are hen presened in secion IV. onclsions are finall drawn in secion V. II. THOY The noise removal mehod proposed b Mahmoodi [7] for band pass sinals b preservin disconiniies is based on a linear parial differenial eqaion of he followin form: 1 wih iniial condiion where : : > and are he smoohed sinal oriinal nois sinal consan vales respecivel and 1. In eqaion 1 i is assmed ha he carrier sinal has freqenc and and are comple valed sinals. qaion 1 is associaed wih one carrier sinal wih freqenc. The nonlinear noise removal proposed in [7] can herefore be onl sed for comple valed sinals havin real and imainar pars. Sinals in real life however are real valed. Sch a sinal reqires a real valed carrier sinal. The specrm of a real valed carrier sinal herefore consiss of wo freqenc componens in freqenc domain in freqencies and. The anisoropic diffsion eqaion associaed wih freqenc is wrien as: 3 An iniial condiion similar o is also sed for his eqaion. qaions 1 and 3 can be rewrien as: MMSP 13 Sep. 3-Oc. 13 Pla Sardinia Ial /13/$ I MMSP13

2 5 To desin a noise removal echniqe for real valed sinals eqaions 4 and 5 need o be combined. In his paper we propose he followin eqaion combinin eqaions 4 and 5: Or 6 We assme he followin iniial condiions for eqaion 6: 7 8 I is noed ha in eqaion 6 : : are real valed sinals. B akin Laplace ransform wih respec o ime and Forier ransform wih respec o space from boh sides of eqaion 6 i becomes clear ha he reslin ransfer fncion conains wo cenral freqencies and. This is indeed similar o facorin mehod in he solion of wave parial differenial eqaion where wave eqaion is facored ino wo mliplin erms: one responsible for he wave ravelin in he lef direcion and he oher one in chare of he wave ravelin in he rih direcion [11]. I is also imporan o noice ha addiion and/or sbracion of eqaions 4 and 5 does no prodce he desired resls and herefore i does no lead o a ssem capable of dealin wih a real valed sinal conainin wo carrier freqencies a and. Before we se eqaion 6 o propose a nonlinear filerin alorihm o remove noise from real valed band pass sinals and preserve disconiniies and he carrier sinal le s invesiae linear eqaion 6. The propaaor of eqaion 6 is a real valed Gabor-like filer shown in fire 1 for consan vales of 1 5. and 15. Fire 1: The propaaor of eqaion 6 Zero mean Gassian noise is added o he noiseless sinal shown in fire -a o prodce a nois sinal depiced in fire -b wih SN.154. qaion 6 is applied o he nois sinal of fire -b wih 1 5. and 15 o prodce he smoohed sinal shown in fire -c. The hea eqaion wih 1 and 15 whose propaaor is a Gassian filer has also been applied o he nois sinal of fire -b o obain he smoohed sinal shown in fire - d. As shown in his fire he carrier sinal has been filered o and he smoohed sinal is compleel disored b he hea eqaion. In he ne secion eqaion 6 wih iniial condiions 7 and 8 are discreized and sed nonlinearl o remove he noise and preserve disconiniies and he real valed carrier sinal wih freqenc. III. IMPLMNTATION ISSUS We emplo an eplici finie difference scheme for he discreizaion of eqaion 6. A cenral finie difference approach is sed for spaial discreizaion and a forward finie difference scheme is emploed for emporal discreizaion. For he discreizaion prposes eqaion 6 can be wrien in he followin form: 9 B sin an eplici discreizaion scheme eqaion 9 can herefore be discreized as follows: L 1 where L Fncion can be chosen as one of he followin fncions: ep q 11 MMSP13 363

3 Or a d Fire : Linear filerin of eqaion 6 a a noiseless sinal wih a carrier freqenc of. 5 b Nois sinal prodced b conaminain he noiseless sinal of fire -a wih a zero mean Gassian noise wih SN.154 c he sinal smoohed b applin eqaion 6 wih 1. 5 and 15 o he nois sinal of fire -b d he sinal smoohed b applin he hea eqaion wih 1 and 15 o he nois sinal of fire -b b c q where q is a parameer deermined b sers. An disconini in sinal componens wih freqencies and wold prodce a local maima in erms sch as and in eqaion 9. The erms and L herefore approach o zero o preserve he disconini in case a local maimm is deeced in and. Throho his paper is se o ni. Time is reaed virall and corresponds o ieraions in he alorihm. The clidian disance beween wo consecive smoohed sinals is sed as a soppin crierion. If his disance is less han a hreshold he alorihm sops and he alorihm is said o have convered. Parameer is sed o ads he speed of he converence. Lare vales of ma increase he speed of he converence and ma also lead o he insabili of he alorihm as i is epeced in an eplici finie difference srae. Lower vales for on he oher hand aranees he alorihm s converence in he epense of lower speeds of he converence. Finall parameer q shold be seleced accordin o he amon of disconiniies in he oriinal noiseless sinals. Over-smoohin in he smoohed sinal ma occr if larer vales for q are chosen b he ser. This oversmoohin is demonsraed in he smoohed sinal wih some smoohed no preserved disconiniies. Smaller vales for q on he oher hand in a ver nois environmen ma lead o he failre of noise removal and preservin some disconiniies associaed wih noise raher han he oriinal noiseless sinal. Generall i is bes o choose lower vales for q in he presence of moderae noise o preserve disconiniies. We also noe ha o avoid he effecs associaed wih he ncerain principle [8] i is alwas assmed ha here is a leas one fll ccle of he carrier sinal beween wo consecive disconiniies. IV. NUMIAL SULTS In his secion we appl he nonlinear band pass filer derived in eqaion 1 on nois band pass sinals conainin disconiniies. Fire 3-a shows a noiseless band pass sinal wih freqenc. 5 conainin disconiniies. This is an eample of a diial sinal modlaed b sin Binar Phase- Shif ein BPS modlaion [9]. Zero mean Gassian noise is added o his noiseless sinal o resl in he nois sinal wih SN 1.49 shown in fire 3-b. Or nonlinear 364 MMSP13

4 a a b b c c Fire 3: Noise removal in a band pass sinal BPS modlaed sinal conainin disconiniies a Oriinal noiseless sinal wih freqenc. 5 wih disconiniies a locaions 1 and 3 b Nois sinal conaminaed wih zero mean Gassian noise wih SN1.49 c he sinal smoohed wih or mehod proposed here for q1 and.5 d he sinal smoohed wih a nonlinear low pass filer based on anisoropic eqaion [7] wih q1 and.5 d Fire 4: Noise removal of a band sinal conainin disconiniies a an oriinal noiseless band pass sinal wih.5 conainin a disconini a he locaion of b Nois sinal conaminaed wih a zero mean Gassian noise wih he sandard deviaion of. c The sinal smoohed b he mehod proposed in [7] wih q1 and. 1 d he sinal smoohed b or filerin mehod proposed here wih q1 and. 1. d 365 MMSP13

5 filer proposed here wih q 1 and. 5 is applied o he nois sinal of fire 3-b o obain he smoohed sinal shown in fire 3-c. As can be seen from his fire Noise is removed and carrier sinal as well as disconiniies are preserved. I akes or nonlinear filerin alorihm onl 1.6 seconds o convere o he solion shown in fire 3-c in a 64-bi Malab version 7.11 rnnin on a P worksaion wih a PU wih freqenc.67 GHz. A nonlinear low pass filer based on anisoropic diffsion eqaion [7] wih q 1 and.5 is also applied o he nois sinal of fire 3-b o obain he smoohed sinal shown in fire 3-d. As can be seen from fire 3-d he smoohed sinal has lower amplide owin o low pass filerin and also he disconiniies are considerabl smoohed. In he ne eperimen we demonsrae ha or alorihm proposed in his paper is compeiive in comparison wih a nonlinear band pass filer reqirin o compe he imainar par of a real sinal b eploiin he Hilber ransform [7]. In he nonlinear filerin scheme proposed here however here is no need o compe he Hilber ransform of he real valed sinal i.e. or parial differenial eqaion is applied o onl real valed sinals. Fire 4-a shows a noiseless band pass sinal wih a disconini a he locaion of and.5. Zero mean Gassian noise wih a sandard deviaion of. is hen added o he noiseless sinal o prodce he nois sinal of fire 4-b. The band pass nonlinear filerin process proposed in [7] wih q1 and. 1is applied o he nois sinal of fire 4-b o obain he smoohed sinal of fire 4-c. The nonlinear filerin echniqe proposed in his paper wih q1 and. 1 is also applied o he nois sinal of fire 4-b o compe he smoohed sinal shown in fire 4-d. As can be seen from fire 4 or noise removal alorihm based on a new parial differenial eqaion proposed here prodces compeiive resls in comparison wih he work presened in [7] wih no frher reqiremen and hassle of he Hilber ransform compaion needed o compe he imainar par of real valed sinals. FNS [1] P. Perona J. Malik Scale-Space and de eecion sin Anisoropic iffsion I Transacions on Paern econiion and Machine Inellience Vol. 1 No. 7 pp [] G. Geri O. bler. ikinis F. Jolesz Nonlinear Anisoropic Filerin of MI aa I Transacions on Medical Imain Vol. 7 No. 11 pp [3] G. Sapiro.L. inach Anisoropic iffsion of Mli-Valed Imaes wih Applicaions o olor Filerin I Transacions on Imae processin Vol. 5 No. 11 pp [4] M.J. Black G. Sapiro.H. Marimon. Heeer obs Anisoropic iffsion I Transacions on Imae Processin Vol. 7 No. 3 pp [5]. Tschmperie Fas Anisoropic Smoohin of Mli-Valed Imaes sin rvare-preservin Ps Inernaional Jornal of omper Vision Vol. 68 No. 1 pp [6] H. Lo L. Zh H. in opled Anisoropic iffsion for Imae Selecive Smoohin Sinal Processin Vol. 86 No. 1 pp [7] S. Mahmoodi Anisoropic iffsion for Noise emoval of Band Pass Sinals Sinal Processin Vol. 91 No.5 pp [8] V. Harvin B. Joricke The Uncerain Principle in Harmonic Analsis Spriner-Verla [9] H. Sern S. Mahmod ommnicaion Ssems Pearson Prenice Hall 4. [1] L. Hanzo S.X.Nq T. eller W.T. Webb Qadrare Amplide Modlaion: From Basics o Adapive Trellis-oded Trbo-qalised and Space-Time oded OFM MA and M-MA Ssems Wile- Blackwell 4. [11] G.B. Arfken H.J. Weber Mahemaical Mehods for Phsiciss Academic Press he 7 h diion 1. V. ONLUSION A nonlinear noise removal alorihm based on a new formlaion for band pass sinals o preserve disconiniies is presened in his paper. The filerin alorihm proposed here demonsraes sperior performance over he nonlinear low pass filer based on anisoropic diffsion. In conras wih he previos work of he noise removal for band pass sinals presened in [7] he alorihm presened here has he advanae ha he Hilber ransform is no reqired o prodce comple valed sinals needed for he mehod proposed in [7]. Or alorihm direcl is applied o he real valed sinals wih eqivalen resls obained from he alorihm presened in [7]. Frhermore he mahemaical framework presened in his paper paves he wa for noise removal alorihms siable for band pass sinals conainin carrier sinals wih more han one freqenc mli-freqenc carrier sinals sch as sinals modlaed b sin Orhoonal Freqenc-ivision Mliplein OFM modlaion scheme [1]. 366 MMSP13

PH2130 Mathematical Methods Lab 3. z x

PH2130 Mathematical Methods Lab 3. z x PH130 Mahemaical Mehods Lab 3 This scrip shold keep yo bsy for he ne wo weeks. Yo shold aim o creae a idy and well-srcred Mahemaica Noebook. Do inclde plenifl annoaions o show ha yo know wha yo are doing,

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

A Mathematical model to Solve Reaction Diffusion Equation using Differential Transformation Method

A Mathematical model to Solve Reaction Diffusion Equation using Differential Transformation Method Inernaional Jornal of Mahemaics Trends and Technology- Volme Isse- A Mahemaical model o Solve Reacion Diffsion Eqaion sing Differenial Transformaion Mehod Rahl Bhadaria # A.K. Singh * D.P Singh # #Deparmen

More information

Computers and Mathematics with Applications

Computers and Mathematics with Applications Compers and Mahemaics wih Applicaions 59 (00) 80 809 Conens liss available a ScienceDirec Compers and Mahemaics wih Applicaions jornal homepage: www.elsevier.com/locae/camwa Solving fracional bondary vale

More information

Scalar Conservation Laws

Scalar Conservation Laws MATH-459 Nmerical Mehods for Conservaion Laws by Prof. Jan S. Heshaven Solion se : Scalar Conservaion Laws Eercise. The inegral form of he scalar conservaion law + f ) = is given in Eq. below. ˆ 2, 2 )

More information

Ordinary Differential Equations

Ordinary 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 information

THE DARBOUX TRIHEDRONS OF REGULAR CURVES ON A REGULAR TIME-LIKE SURFACE. Emin Özyilmaz

THE DARBOUX TRIHEDRONS OF REGULAR CURVES ON A REGULAR TIME-LIKE SURFACE. Emin Özyilmaz Mahemaical and Compaional Applicaions, Vol. 9, o., pp. 7-8, 04 THE DARBOUX TRIHEDROS OF REULAR CURVES O A REULAR TIME-LIKE SURFACE Emin Özyilmaz Deparmen of Mahemaics, Facly of Science, Ee Uniersiy, TR-500

More information

The fundamental mass balance equation is ( 1 ) where: I = inputs P = production O = outputs L = losses A = accumulation

The 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 information

Numerical Dispersion

Numerical Dispersion eview of Linear Numerical Sabiliy Numerical Dispersion n he previous lecure, we considered he linear numerical sabiliy of boh advecion and diffusion erms when approimaed wih several spaial and emporal

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

Miscellanea Miscellanea

Miscellanea Miscellanea Miscellanea Miscellanea Miscellanea Miscellanea Miscellanea CENRAL EUROPEAN REVIEW OF ECONOMICS & FINANCE Vol., No. (4) pp. -6 bigniew Śleszński USING BORDERED MARICES FOR DURBIN WASON D SAISIC EVALUAION

More information

A Comparison Among Homotopy Perturbation Method And The Decomposition Method With The Variational Iteration Method For Dispersive Equation

A Comparison Among Homotopy Perturbation Method And The Decomposition Method With The Variational Iteration Method For Dispersive Equation Inernaional Jornal of Basic & Applied Sciences IJBAS-IJENS Vol:9 No: A Comparison Among Homoopy Perrbaion Mehod And The Decomposiion Mehod Wih The Variaional Ieraion Mehod For Dispersive Eqaion Hasan BULUT*

More information

Dynamic Response of Inclined Isotropic Elastic Damped Rectangular Mindlin Plate resting on Pasternak Foundation under a Moving Load

Dynamic Response of Inclined Isotropic Elastic Damped Rectangular Mindlin Plate resting on Pasternak Foundation under a Moving Load Proceedings of he Inernaional MliConference of Engineers and Comper Scieniss 016 Vol II, IMECS 016, March 16-18, 016, Hong Kong Dnamic Response of Inclined Isoropic Elasic Damped Recanglar Mindlin Plae

More information

Introduction to Bayesian Estimation. McGill COMP 765 Sept 12 th, 2017

Introduction to Bayesian Estimation. McGill COMP 765 Sept 12 th, 2017 Inrodcion o Baesian Esimaion McGill COM 765 Sep 2 h 207 Where am I? or firs core problem Las class: We can model a robo s moions and he world as spaial qaniies These are no perfec and herefore i is p o

More information

Modelling Traffic Flow with Constant Speed using the Galerkin Finite Element Method

Modelling Traffic Flow with Constant Speed using the Galerkin Finite Element Method Proceedings of he World Congress on Engineering 29 Vol II WCE 29, Jly - 3, 29, London, U.K. Modelling Traffic Flow wih Consan Speed sing he Galerin Finie Elemen Mehod Wesley Celemans, Magd A. Wahab, Kr

More information

ME 391 Mechanical Engineering Analysis

ME 391 Mechanical Engineering Analysis Fall 04 ME 39 Mechanical Engineering Analsis Eam # Soluions Direcions: Open noes (including course web posings). No books, compuers, or phones. An calculaor is fair game. Problem Deermine he posiion of

More information

CoE4TN3 Image Processing

CoE4TN3 Image Processing CoE4T3 Imae Processin Imae Reisraion Imae Reisraion Throuh Transform A B f Imae reisraion provides ransformaion of a source imae space o he are imae space. The are imae ma be of differen modaliies from

More information

, u denotes uxt (,) and u. mean first partial derivatives of u with respect to x and t, respectively. Equation (1.1) can be simply written as

, u denotes uxt (,) and u. mean first partial derivatives of u with respect to x and t, respectively. Equation (1.1) can be simply written as Proceedings of he rd IMT-GT Regional Conference on Mahemaics Saisics and Applicaions Universii Sains Malaysia ANALYSIS ON () + () () = G( ( ) ()) Jessada Tanhanch School of Mahemaics Insie of Science Sranaree

More information

Theory of! Partial Differential Equations!

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 information

An EM algorithm for maximum likelihood estimation given corrupted observations. E. E. Holmes, National Marine Fisheries Service

An EM algorithm for maximum likelihood estimation given corrupted observations. E. E. Holmes, National Marine Fisheries Service An M algorihm maimum likelihood esimaion given corruped observaions... Holmes Naional Marine Fisheries Service Inroducion M algorihms e likelihood esimaion o cases wih hidden saes such as when observaions

More information

Simulation-Solving Dynamic Models ABE 5646 Week 2, Spring 2010

Simulation-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 information

Kriging Models Predicting Atrazine Concentrations in Surface Water Draining Agricultural Watersheds

Kriging Models Predicting Atrazine Concentrations in Surface Water Draining Agricultural Watersheds 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 Kriging Models Predicing Arazine Concenraions in Surface Waer Draining Agriculural Waersheds Paul L. Mosquin, Jeremy Aldworh, Wenlin Chen Supplemenal Maerial Number

More information

A Direct Method for Solving Nonlinear PDEs and. New Exact Solutions for Some Examples

A Direct Method for Solving Nonlinear PDEs and. New Exact Solutions for Some Examples In. J. Conemp. Mah. Sciences, Vol. 6, 011, no. 46, 83-90 A Direc Mehod for Solving Nonlinear PDEs and New Eac Solions for Some Eamples Ameina S. Nseir Jordan Universiy of Science and Technology Deparmen

More information

Experiment 123 Determination of the sound wave velocity with the method of Lissajous figures

Experiment 123 Determination of the sound wave velocity with the method of Lissajous figures perimen 3 Deerminaion of he sound wave veloci wih he mehod of Lissajous figures The aim of he eercise To sud acousic wave propagaion in he air To deermine of he sound wave veloci in he air Mehodolog of

More information

Homotopy Perturbation Method for Solving Some Initial Boundary Value Problems with Non Local Conditions

Homotopy Perturbation Method for Solving Some Initial Boundary Value Problems with Non Local Conditions Proceedings of he World Congress on Engineering and Compuer Science 23 Vol I WCECS 23, 23-25 Ocober, 23, San Francisco, USA Homoopy Perurbaion Mehod for Solving Some Iniial Boundary Value Problems wih

More information

Exact solitary-wave Special Solutions for the Nonlinear Dispersive K(m,n) Equations by Means of the Homotopy Analysis Method

Exact solitary-wave Special Solutions for the Nonlinear Dispersive K(m,n) Equations by Means of the Homotopy Analysis Method Available a hp://pva.ed/aa Appl. Appl. Mah. ISSN: 93-9466 Special Isse No. (Ags ) pp. 8 93 Applicaions Applied Maheaics: An Inernaional Jornal (AAM) Eac soliary-wave Special Solions for he Nonlinear Dispersive

More information

Technical Report Doc ID: TR March-2013 (Last revision: 23-February-2016) On formulating quadratic functions in optimization models.

Technical Report Doc ID: TR March-2013 (Last revision: 23-February-2016) On formulating quadratic functions in optimization models. Technical Repor Doc ID: TR--203 06-March-203 (Las revision: 23-Februar-206) On formulaing quadraic funcions in opimizaion models. Auhor: Erling D. Andersen Convex quadraic consrains quie frequenl appear

More information

Dimitri Solomatine. D.P. Solomatine. Data-driven modelling (part 2). 2

Dimitri Solomatine. D.P. Solomatine. Data-driven modelling (part 2). 2 Daa-driven modelling. Par. Daa-driven Arificial di Neural modelling. Newors Par Dimiri Solomaine Arificial neural newors D.P. Solomaine. Daa-driven modelling par. 1 Arificial neural newors ANN: main pes

More information

On the numerical simulation of population dynamics with density-dependent migrations and the Allee effects

On the numerical simulation of population dynamics with density-dependent migrations and the Allee effects 7 Inernaional Symposim on Nonlinear Dynamics (7 ISND) IOP Pblishing Jornal of Physics: Conference Series 96 (8) 8 doi:88/74-6596/96//8 On he nmerical simlaion of poplaion dynamics wih densiy-dependen migraions

More information

Theory of! Partial Differential Equations-I!

Theory 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 information

Huazhong Tang 1 and Gerald Warnecke Introduction ANOTEON(2K + 1)-POINT CONSERVATIVE MONOTONE SCHEMES

Huazhong Tang 1 and Gerald Warnecke Introduction ANOTEON(2K + 1)-POINT CONSERVATIVE MONOTONE SCHEMES ESAIM: MAN Vol. 38, N o, 4, pp. 345 357 DOI:.5/man:46 ESAIM: Mahemaical Modelling and Nmerical Analysis ANOTEON(K + )-POINT CONSERVATIVE MONOTONE SCHEMES Hazhong Tang and Gerald Warnecke Absrac. Firs order

More information

Outline of Topics. Analysis of ODE models with MATLAB. What will we learn from this lecture. Aim of analysis: Why such analysis matters?

Outline of Topics. Analysis of ODE models with MATLAB. What will we learn from this lecture. Aim of analysis: Why such analysis matters? of Topics wih MATLAB Shan He School for Compuaional Science Universi of Birmingham Module 6-3836: Compuaional Modelling wih MATLAB Wha will we learn from his lecure Aim of analsis: Aim of analsis. Some

More information

MA 214 Calculus IV (Spring 2016) Section 2. Homework Assignment 1 Solutions

MA 214 Calculus IV (Spring 2016) Section 2. Homework Assignment 1 Solutions MA 14 Calculus IV (Spring 016) Secion Homework Assignmen 1 Soluions 1 Boyce and DiPrima, p 40, Problem 10 (c) Soluion: In sandard form he given firs-order linear ODE is: An inegraing facor is given by

More information

Chapters 6 & 7: Trigonometric Functions of Angles and Real Numbers. Divide both Sides by 180

Chapters 6 & 7: Trigonometric Functions of Angles and Real Numbers. Divide both Sides by 180 Algebra Chapers & : Trigonomeric Funcions of Angles and Real Numbers Chapers & : Trigonomeric Funcions of Angles and Real Numbers - Angle Measures Radians: - a uni (rad o measure he size of an angle. rad

More information

KEY. Math 334 Midterm I Fall 2008 sections 001 and 003 Instructor: Scott Glasgow

KEY. Math 334 Midterm I Fall 2008 sections 001 and 003 Instructor: Scott Glasgow 1 KEY Mah 4 Miderm I Fall 8 secions 1 and Insrucor: Sco Glasgow Please do NOT wrie on his eam. No credi will be given for such work. Raher wrie in a blue book, or on our own paper, preferabl engineering

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

first-order circuit Complete response can be regarded as the superposition of zero-input response and zero-state response.

first-order circuit Complete response can be regarded as the superposition of zero-input response and zero-state response. Experimen 4:he Sdies of ransiional processes of 1. Prpose firs-order circi a) Use he oscilloscope o observe he ransiional processes of firs-order circi. b) Use he oscilloscope o measre he ime consan of

More information

An Introduction to Malliavin calculus and its applications

An 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 information

Asymptotic Solution of the Anti-Plane Problem for a Two-Dimensional Lattice

Asymptotic Solution of the Anti-Plane Problem for a Two-Dimensional Lattice Asympoic Solion of he Ani-Plane Problem for a Two-Dimensional Laice N.I. Aleksandrova N.A. Chinakal Insie of Mining, Siberian Branch, Rssian Academy of Sciences, Krasnyi pr. 91, Novosibirsk, 6391 Rssia,

More information

Hf(x) := 1 π p.v. f(y)

Hf(x) := 1 π p.v. f(y) NOTES ON THE NUMERICAL SOLUTION OF THE BENJAMIN EQUATION arxiv:131.2749v3 [mah.na] 22 May 214 VASSILIOS A. DOUGALIS, ANGEL DURAN, AND DIMITRIOS MITSOTAKIS Absrac. In his paper we consider he Benjamin eqaion,

More information

Elementary Differential Equations and Boundary Value Problems

Elementary 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 information

APPLICATION OF CHEBYSHEV APPROXIMATION IN THE PROCESS OF VARIATIONAL ITERATION METHOD FOR SOLVING DIFFERENTIAL- ALGEBRAIC EQUATIONS

APPLICATION OF CHEBYSHEV APPROXIMATION IN THE PROCESS OF VARIATIONAL ITERATION METHOD FOR SOLVING DIFFERENTIAL- ALGEBRAIC EQUATIONS Mahemaical and Compuaional Applicaions, Vol., No. 4, pp. 99-978,. Associaion for Scienific Research APPLICATION OF CHEBYSHEV APPROXIMATION IN THE PROCESS OF VARIATIONAL ITERATION METHOD FOR SOLVING DIFFERENTIAL-

More information

LAPLACE TRANSFORM AND TRANSFER FUNCTION

LAPLACE 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 information

The Optimal Stopping Time for Selling an Asset When It Is Uncertain Whether the Price Process Is Increasing or Decreasing When the Horizon Is Infinite

The 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 information

CSE-4303/CSE-5365 Computer Graphics Fall 1996 Take home Test

CSE-4303/CSE-5365 Computer Graphics Fall 1996 Take home Test Comper Graphics roblem #1) A bi-cbic parameric srface is defined by Hermie geomery in he direcion of parameer. In he direcion, he geomery ecor is defined by a poin @0, a poin @0.5, a angen ecor @1 and

More information

Exact solution of the(2+1)-dimensional hyperbolic nonlinear Schrödinger equation by Adomian decomposition method

Exact solution of the(2+1)-dimensional hyperbolic nonlinear Schrödinger equation by Adomian decomposition method Malaa J Ma ((014 160 164 Exac soluion of he(+1-dimensional hperbolic nonlinear Schrödinger equaion b Adomian decomposiion mehod Ifikhar Ahmed, a, Chunlai Mu b and Pan Zheng c a,b,c College of Mahemaics

More information

ASTR415: Problem Set #5

ASTR415: Problem Set #5 ASTR45: Problem Se #5 Curran D. Muhlberger Universi of Marland (Daed: April 25, 27) Three ssems of coupled differenial equaions were sudied using inegraors based on Euler s mehod, a fourh-order Runge-Kua

More information

1 First Order Partial Differential Equations

1 First Order Partial Differential Equations Firs Order Parial Differenial Eqaions The profond sdy of nare is he mos ferile sorce of mahemaical discoveries. - Joseph Forier (768-830). Inrodcion We begin or sdy of parial differenial eqaions wih firs

More information

Lecture 8 Backlash and Quantization. Material. Linear and Angular Backlash. Example: Parallel Kinematic Robot. Backlash.

Lecture 8 Backlash and Quantization. Material. Linear and Angular Backlash. Example: Parallel Kinematic Robot. Backlash. Lecre 8 Backlash and Qanizaion Maerial Toda s Goal: To know models and compensaion mehods for backlash Lecre slides Be able o analze he effec of qanizaion errors Noe: We are sing analsis mehods from previos

More information

DISPLACEMENT ESTIMATION FOR IMAGE PREDICTIVE CODING AND FRAME MOTION-ADAPTIVE INTERPOLATION

DISPLACEMENT ESTIMATION FOR IMAGE PREDICTIVE CODING AND FRAME MOTION-ADAPTIVE INTERPOLATION DSPLACEMENT ESTMATON FOR MAGE PREDCTVE CODNG AND FRAME MOTON-ADAPTVE NTERPOLATON Georges TZRTAS Laboraoire des Signa e Ssèmes (C.N.R.S.), Ecole Spériere d'elecricié, Plaea d Molon 9119 GF-sr-YVETTE, FRANCE

More information

3.1.3 INTRODUCTION TO DYNAMIC OPTIMIZATION: DISCRETE TIME PROBLEMS. A. The Hamiltonian and First-Order Conditions in a Finite Time Horizon

3.1.3 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 information

CSE 5365 Computer Graphics. Take Home Test #1

CSE 5365 Computer Graphics. Take Home Test #1 CSE 5365 Comper Graphics Take Home Tes #1 Fall/1996 Tae-Hoon Kim roblem #1) A bi-cbic parameric srface is defined by Hermie geomery in he direcion of parameer. In he direcion, he geomery ecor is defined

More information

Vehicle Arrival Models : Headway

Vehicle Arrival Models : Headway Chaper 12 Vehicle Arrival Models : Headway 12.1 Inroducion Modelling arrival of vehicle a secion of road is an imporan sep in raffic flow modelling. I has imporan applicaion in raffic flow simulaion where

More information

Uncertainty & Localization I

Uncertainty & Localization I Advanced Roboics Uncerain & Localiaion I Moivaion Inrodcion basics represening ncerain Gassian Filers Kalman Filer eended Kalman Filer nscened Kalman Filer Agenda Localiaion Eample For Legged Leage Non-arameric

More information

Week 1 Lecture 2 Problems 2, 5. What if something oscillates with no obvious spring? What is ω? (problem set problem)

Week 1 Lecture 2 Problems 2, 5. What if something oscillates with no obvious spring? What is ω? (problem set problem) Week 1 Lecure Problems, 5 Wha if somehing oscillaes wih no obvious spring? Wha is ω? (problem se problem) Sar wih Try and ge o SHM form E. Full beer can in lake, oscillaing F = m & = ge rearrange: F =

More information

Improved Approximate Solutions for Nonlinear Evolutions Equations in Mathematical Physics Using the Reduced Differential Transform Method

Improved Approximate Solutions for Nonlinear Evolutions Equations in Mathematical Physics Using the Reduced Differential Transform Method Journal of Applied Mahemaics & Bioinformaics, vol., no., 01, 1-14 ISSN: 179-660 (prin), 179-699 (online) Scienpress Ld, 01 Improved Approimae Soluions for Nonlinear Evoluions Equaions in Mahemaical Physics

More information

Srednicki Chapter 20

Srednicki Chapter 20 Srednicki Chaper QFT Problems & Solions. George Ocober 4, Srednicki.. Verify eqaion.7. Using eqaion.7,., and he fac ha m = in his limi, or ask is o evalae his inegral:! x x x dx dx dx x sx + x + x + x

More information

Exam 1 Solutions. 1 Question 1. February 10, Part (A) 1.2 Part (B) To find equilibrium solutions, set P (t) = C = dp

Exam 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 information

The Research of Active Disturbance Rejection Control on Shunt Hybrid Active Power Filter

The Research of Active Disturbance Rejection Control on Shunt Hybrid Active Power Filter Available online a www.sciencedirec.com Procedia Engineering 29 (2) 456 46 2 Inernaional Workshop on Informaion and Elecronics Engineering (IWIEE) The Research of Acive Disrbance Rejecion Conrol on Shn

More information

I Let E(v! v 0 ) denote the event that v 0 is selected instead of v I The block error probability is the union of such events

I Let E(v! v 0 ) denote the event that v 0 is selected instead of v I The block error probability is the union of such events ED042 Error Conrol Coding Kodningseknik) Chaper 3: Opimal Decoding Mehods, Par ML Decoding Error Proailiy Sepemer 23, 203 ED042 Error Conrol Coding: Chaper 3 20 / 35 Pairwise Error Proailiy Assme ha v

More information

Riemann Function and Methods of Group Analysis

Riemann Function and Methods of Group Analysis American Research Jornal of Mahemaics Original Aricle ISSN 378-74X Volme Isse 3 5 Riemann Fncion and Mehods of Grop Analsis Akimov Andre Chernov Igor Abdllina Rfina 3 4533 Serliamak Rssia Lenina sree 47A

More information

6.2 Transforms of Derivatives and Integrals.

6.2 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

Space truss bridge optimization by dynamic programming and linear programming

Space truss bridge optimization by dynamic programming and linear programming 306 IABSE-JSCE Join Conference on Advances in Bridge Engineering-III, Ags 1-, 015, Dhaka, Bangladesh. ISBN: 978-984-33-9313-5 Amin, Oki, Bhiyan, Ueda (eds.) www.iabse-bd.org Space rss bridge opimizaion

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

Solution of Integro-Differential Equations by Using ELzaki Transform

Solution of Integro-Differential Equations by Using ELzaki Transform Global Journal of Mahemaical Sciences: Theory and Pracical. Volume, Number (), pp. - Inernaional Research Publicaion House hp://www.irphouse.com Soluion of Inegro-Differenial Equaions by Using ELzaki Transform

More information

Math 334 Test 1 KEY Spring 2010 Section: 001. Instructor: Scott Glasgow Dates: May 10 and 11.

Math 334 Test 1 KEY Spring 2010 Section: 001. Instructor: Scott Glasgow Dates: May 10 and 11. 1 Mah 334 Tes 1 KEY Spring 21 Secion: 1 Insrucor: Sco Glasgow Daes: Ma 1 and 11. Do NOT wrie on his problem saemen bookle, excep for our indicaion of following he honor code jus below. No credi will be

More information

and v y . The changes occur, respectively, because of the acceleration components a x and a y

and v y . The changes occur, respectively, because of the acceleration components a x and a y Week 3 Reciaion: Chaper3 : Problems: 1, 16, 9, 37, 41, 71. 1. A spacecraf is raveling wih a veloci of v0 = 5480 m/s along he + direcion. Two engines are urned on for a ime of 84 s. One engine gives he

More information

Chapter 2. First Order Scalar Equations

Chapter 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 information

Kalman filtering for maximum likelihood estimation given corrupted observations.

Kalman filtering for maximum likelihood estimation given corrupted observations. alman filering maimum likelihood esimaion given corruped observaions... Holmes Naional Marine isheries Service Inroducion he alman filer is used o eend likelihood esimaion o cases wih hidden saes such

More information

EE 435. Lecture 31. Absolute and Relative Accuracy DAC Design. The String DAC

EE 435. Lecture 31. Absolute and Relative Accuracy DAC Design. The String DAC EE 435 Lecure 3 Absolue and Relaive Accuracy DAC Design The Sring DAC . Review from las lecure. DFT Simulaion from Malab Quanizaion Noise DACs and ADCs generally quanize boh ampliude and ime If convering

More information

Multi-scale 2D acoustic full waveform inversion with high frequency impulsive source

Multi-scale 2D acoustic full waveform inversion with high frequency impulsive source Muli-scale D acousic full waveform inversion wih high frequency impulsive source Vladimir N Zubov*, Universiy of Calgary, Calgary AB vzubov@ucalgaryca and Michael P Lamoureux, Universiy of Calgary, Calgary

More information

Hyperchaos Synchronization Between two Different Hyperchaotic Systems

Hyperchaos Synchronization Between two Different Hyperchaotic Systems ISSN 76-769, England, UK Journal of Informaion and Compuing Science Vo3, No., 8, pp. 73-8 Hperchaos Snchroniaion Beween wo Differen Hperchaoic Ssems Qiang Jia + Facul of Science, Jiangsu Universi, Zhenjiang,

More information

23.2. Representing Periodic Functions by Fourier Series. Introduction. Prerequisites. Learning Outcomes

23.2. Representing Periodic Functions by Fourier Series. Introduction. Prerequisites. Learning Outcomes Represening Periodic Funcions by Fourier Series 3. Inroducion In his Secion we show how a periodic funcion can be expressed as a series of sines and cosines. We begin by obaining some sandard inegrals

More information

Symmetry and Numerical Solutions for Systems of Non-linear Reaction Diffusion Equations

Symmetry and Numerical Solutions for Systems of Non-linear Reaction Diffusion Equations Symmery and Numerical Soluions for Sysems of Non-linear Reacion Diffusion Equaions Sanjeev Kumar* and Ravendra Singh Deparmen of Mahemaics, (Dr. B. R. Ambedkar niversiy, Agra), I. B. S. Khandari, Agra-8

More information

Kinematics in two Dimensions

Kinematics in two Dimensions Lecure 5 Chaper 4 Phsics I Kinemaics in wo Dimensions Course websie: hp://facul.uml.edu/andri_danlo/teachin/phsicsi PHYS.141 Lecure 5 Danlo Deparmen of Phsics and Applied Phsics Toda we are oin o discuss:

More information

Second Order Linear Differential Equations

Second Order Linear Differential Equations Second Order Linear Differenial Equaions Second order linear equaions wih consan coefficiens; Fundamenal soluions; Wronskian; Exisence and Uniqueness of soluions; he characerisic equaion; soluions of homogeneous

More information

Probabilistic Robotics Sebastian Thrun-- Stanford

Probabilistic Robotics Sebastian Thrun-- Stanford robabilisic Roboics Sebasian Thrn-- Sanford Inrodcion robabiliies Baes rle Baes filers robabilisic Roboics Ke idea: Eplici represenaion of ncerain sing he calcls of probabili heor ercepion sae esimaion

More information

EXPLICIT TIME INTEGRATORS FOR NONLINEAR DYNAMICS DERIVED FROM THE MIDPOINT RULE

EXPLICIT TIME INTEGRATORS FOR NONLINEAR DYNAMICS DERIVED FROM THE MIDPOINT RULE Version April 30, 2004.Submied o CTU Repors. EXPLICIT TIME INTEGRATORS FOR NONLINEAR DYNAMICS DERIVED FROM THE MIDPOINT RULE Per Krysl Universiy of California, San Diego La Jolla, California 92093-0085,

More information

NMR Spectroscopy: Principles and Applications. Nagarajan Murali 1D - Methods Lecture 5

NMR Spectroscopy: Principles and Applications. Nagarajan Murali 1D - Methods Lecture 5 NMR pecroscop: Principles and Applicaions Nagarajan Murali D - Mehods Lecure 5 D-NMR To full appreciae he workings of D NMR eperimens we need o a leas consider wo coupled spins. omeimes we need o go up

More information

CH.7. PLANE LINEAR ELASTICITY. Continuum Mechanics Course (MMC) - ETSECCPB - UPC

CH.7. PLANE LINEAR ELASTICITY. Continuum Mechanics Course (MMC) - ETSECCPB - UPC CH.7. PLANE LINEAR ELASTICITY Coninuum Mechanics Course (MMC) - ETSECCPB - UPC Overview Plane Linear Elasici Theor Plane Sress Simplifing Hpohesis Srain Field Consiuive Equaion Displacemen Field The Linear

More information

The Application of Optimal Homotopy Asymptotic Method for One-Dimensional Heat and Advection- Diffusion Equations

The Application of Optimal Homotopy Asymptotic Method for One-Dimensional Heat and Advection- Diffusion Equations Inf. Sci. Le., No., 57-61 13) 57 Informaion Sciences Leers An Inernaional Journal hp://d.doi.org/1.1785/isl/ The Applicaion of Opimal Homoopy Asympoic Mehod for One-Dimensional Hea and Advecion- Diffusion

More information

Section 3.5 Nonhomogeneous Equations; Method of Undetermined Coefficients

Section 3.5 Nonhomogeneous Equations; Method of Undetermined Coefficients Secion 3.5 Nonhomogeneous Equaions; Mehod of Undeermined Coefficiens Key Terms/Ideas: Linear Differenial operaor Nonlinear operaor Second order homogeneous DE Second order nonhomogeneous DE Soluion o homogeneous

More information

Exponential Weighted Moving Average (EWMA) Chart Under The Assumption of Moderateness And Its 3 Control Limits

Exponential Weighted Moving Average (EWMA) Chart Under The Assumption of Moderateness And Its 3 Control Limits DOI: 0.545/mjis.07.5009 Exponenial Weighed Moving Average (EWMA) Char Under The Assumpion of Moderaeness And Is 3 Conrol Limis KALPESH S TAILOR Assisan Professor, Deparmen of Saisics, M. K. Bhavnagar Universiy,

More information

STATE-SPACE MODELLING. A mass balance across the tank gives:

STATE-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 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

Math 2214 Solution Test 1B Fall 2017

Math 2214 Solution Test 1B Fall 2017 Mah 14 Soluion Tes 1B Fall 017 Problem 1: A ank has a capaci for 500 gallons and conains 0 gallons of waer wih lbs of sal iniiall. A soluion conaining of 8 lbsgal of sal is pumped ino he ank a 10 galsmin.

More information

Variational Iteration Method for Solving System of Fractional Order Ordinary Differential Equations

Variational Iteration Method for Solving System of Fractional Order Ordinary Differential Equations IOSR Journal of Mahemaics (IOSR-JM) e-issn: 2278-5728, p-issn: 2319-765X. Volume 1, Issue 6 Ver. II (Nov - Dec. 214), PP 48-54 Variaional Ieraion Mehod for Solving Sysem of Fracional Order Ordinary Differenial

More information

20. Applications of the Genetic-Drift Model

20. Applications of the Genetic-Drift Model 0. Applicaions of he Geneic-Drif Model 1) Deermining he probabiliy of forming any paricular combinaion of genoypes in he nex generaion: Example: If he parenal allele frequencies are p 0 = 0.35 and q 0

More information

Earthquake, Volcano and Tsunami

Earthquake, Volcano and Tsunami A. Merapi Volcano Erpion Earhqake, Volcano and Tsnami Qesion Answer Marks A. Using Black s Principle he eqilibrim emperare can be obained Ths,.5 A. For ideal gas, pv e e RTe, hs.3 A.3 The relaive velociy

More information

1 1 + x 2 dx. tan 1 (2) = ] ] x 3. Solution: Recall that the given integral is improper because. x 3. 1 x 3. dx = lim dx.

1 1 + x 2 dx. tan 1 (2) = ] ] x 3. Solution: Recall that the given integral is improper because. x 3. 1 x 3. dx = lim dx. . Use Simpson s rule wih n 4 o esimae an () +. Soluion: Since we are using 4 seps, 4 Thus we have [ ( ) f() + 4f + f() + 4f 3 [ + 4 4 6 5 + + 4 4 3 + ] 5 [ + 6 6 5 + + 6 3 + ]. 5. Our funcion is f() +.

More information

THE EFFECT OF SUCTION AND INJECTION ON UNSTEADY COUETTE FLOW WITH VARIABLE PROPERTIES

THE EFFECT OF SUCTION AND INJECTION ON UNSTEADY COUETTE FLOW WITH VARIABLE PROPERTIES Kragujevac J. Sci. 3 () 7-4. UDC 53.5:536. 4 THE EFFECT OF SUCTION AND INJECTION ON UNSTEADY COUETTE FLOW WITH VARIABLE PROPERTIES Hazem A. Aia Dep. of Mahemaics, College of Science,King Saud Universiy

More information

Time Domain Transfer Function of the Induction Motor

Time Domain Transfer Function of the Induction Motor Sudies in Engineering and Technology Vol., No. ; Augus 0 ISSN 008 EISSN 006 Published by Redfame Publishing URL: hp://se.redfame.com Time Domain Transfer Funcion of he Inducion Moor N N arsoum Correspondence:

More information

Conservation Laws and Hamiltonian Symmetries of Whitham-Broer-Kaup Equations

Conservation Laws and Hamiltonian Symmetries of Whitham-Broer-Kaup Equations Indian Jornal of Science and Technology Vol 8( 78 84 Janary 05 ISSN (Prin : 0974-84 ISSN (Online : 0974-545 DOI : 0.7485/ijs/05/8i/47809 Conseraion Laws and Hamilonian Symmeries of Whiham-Broer-Kap Eqaions

More information

STRUCTURAL CHANGE IN TIME SERIES OF THE EXCHANGE RATES BETWEEN YEN-DOLLAR AND YEN-EURO IN

STRUCTURAL CHANGE IN TIME SERIES OF THE EXCHANGE RATES BETWEEN YEN-DOLLAR AND YEN-EURO IN Inernaional Journal of Applied Economerics and Quaniaive Sudies. Vol.1-3(004) STRUCTURAL CHANGE IN TIME SERIES OF THE EXCHANGE RATES BETWEEN YEN-DOLLAR AND YEN-EURO IN 001-004 OBARA, Takashi * Absrac The

More information

International Journal "Information Theories & Applications" Vol.10

International Journal Information Theories & Applications Vol.10 44 Inernaional Jornal "Informaion eories & Applicaions" Vol. [7] R.A.Jonson (994 iller & Frend s Probabili and Saisics for Engineers5 ediion Prenice Hall New Jerse 763. [8] J.Carroll ( Hman - Comper Ineracion

More information

Notes on Kalman Filtering

Notes 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 information

Traveling Waves. Chapter Introduction

Traveling Waves. Chapter Introduction Chaper 4 Traveling Waves 4.1 Inroducion To dae, we have considered oscillaions, i.e., periodic, ofen harmonic, variaions of a physical characerisic of a sysem. The sysem a one ime is indisinguishable from

More information

23.5. Half-Range Series. Introduction. Prerequisites. Learning Outcomes

23.5. Half-Range Series. Introduction. Prerequisites. Learning Outcomes Half-Range Series 2.5 Inroducion In his Secion we address he following problem: Can we find a Fourier series expansion of a funcion defined over a finie inerval? Of course we recognise ha such a funcion

More information

10. State Space Methods

10. 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 information

WEEK-3 Recitation PHYS 131. of the projectile s velocity remains constant throughout the motion, since the acceleration a x

WEEK-3 Recitation PHYS 131. of the projectile s velocity remains constant throughout the motion, since the acceleration a x WEEK-3 Reciaion PHYS 131 Ch. 3: FOC 1, 3, 4, 6, 14. Problems 9, 37, 41 & 71 and Ch. 4: FOC 1, 3, 5, 8. Problems 3, 5 & 16. Feb 8, 018 Ch. 3: FOC 1, 3, 4, 6, 14. 1. (a) The horizonal componen of he projecile

More information