Stability of the SDDRE based Estimator for Stochastic Nonlinear System

Size: px
Start display at page:

Download "Stability of the SDDRE based Estimator for Stochastic Nonlinear System"

Transcription

1 26 ISCEE Inernainal Cnference n he Science f Elecrical Engineering Sabiliy f he SDDRE based Esimar fr Schasic Nnlinear Sysem Ilan Rusnak Senir Research Fellw, RAFAEL (63, P.O.Bx 225, 322, Haifa, Israel.; als Adjunc Senir Lecurer, Faculy f Elecrical Engineering, echnin, Haifa 32, Israel. ( ilanru@rafael.c.il Absrac Bunded-Inpu-Bunded-Sae and Bunded- Inpu-Bunded-Oupu sabiliy f he Sae Dependen Differenial Riccai Equain (SDDRE based esimar f nnlinear schasic ime-varying sysems is prved by hree appraches. Each prf highlighs differen aspec f he SDDRE based esimar sabiliy. he Sae Dependen Cefficien (SDC frm represenain f nnlinear schasic sysem is used. In he firs apprach hery f linear ime-varying schasic sysems is used. In secnd apprach i is shwn ha he sae f he SDDRE based esimar is always bunded by defining a Lyapunv funcin and usage he Barkana's invariance principle. he expnenial sabiliy f he sae ransiin marix f he esimar and cmpuain f bunds n he sae, under specific cndiins, is prved by he hird apprach. I is shwn ha unifrm cmplee bservabiliy and cnrllabiliy, and respecive bundedness cndiins alng he esimar's rajecries is sufficien fr he resuls abve. Keywrds SDDRE, SDC, Esimars, Observers, Sabiliy, nn-linear sysems, Schasic sysems I. INRODUCION he research f esimars f nnlinear dynamic sysems is a vibran area f research. In curse f his wrk he auhr gahered mre han niney, and cuning, differen appraches esimain and smhing f nnlinear sysems. he issues deal wih in hese researches and are impran in implemenain are: perfrmance, sabiliy, rbusness, cmplexiy, numerical sabiliy, implemenain issues and mre. he Exended Kalman Filer (EKF [] is ne f he ms cmmn esimar f nnlinear sysem ha is widely used is. Hwever he sabiliy and unbiasness f he EKF is n guaraneed. he available herems f sabiliy can guaranee as fllws (lsely: If he iniial cndiins f he esimarbserver are sufficienly clse he iniial cndiins f he esimaed sysem and he measuremen and sysem driving nises (he mdelling errrs f he bserver are sufficienly small hen he EKF esimar-bserver will n diverge. ha is, neiher unifrm glbal sabiliy nr unbiasness can be guaraneed by he exising hery. In spie f is deficiency, he EKF is widely implemened. Recenly, he Sae Dependen Differenial Riccai Equain (SDDRE based apprach gained is place in research and applicain f esimars-bservers f nnlinear sysems [2, 3,4, 5,6]. he SDDRE apprach is based n exended linearizain [7] f he prcess dynamics and bservains. his mehd uses he marices A( and creaed when he dynamics f he nnlinear ime varying sysem are represened in he Sae Dependen Cefficien (SDC frm x. y = x Such represenain always exiss, albei i is n unique. Selecin f hese marices is knwn as he parameerizain prblem [8] and may affec he perfrmance f he esimar. An apprach fr slving he parameerizain prblem by crdinae basis selecin via sabiliy measure can be fund in [9]. he EKF and SDDRE filers are subpimal. he sabiliy f he SDDRE based esimar f nnlinear discree schasic sysems is cnsidered in [5] and f cninuus deerminisic sysems in [6] under he assumpin f he Lipschizian cndiins f he sysem's nnlinear funcins. he biasness is n reaed in hese references. hese resuls are based n []. he main issue deal wih in his paper is he design and implemenain f esimars f schasic nnlinear sysems, and heir perfrmance in erms f sabiliy and biasness wihu he requiremen f he Lipschizian cndiins f he sysem's nnlinear funcins. he Lipschizian cndiins are replaced by much milder cndiin f bundedness f he marices f he SDC frm represenain. In [4] he issue f implemenain f esimars f schasic nnlinear sysems is discussed wih respec he Sae Dependen Algebraic Riccai Equain (SDARE based bserver f nnlinear sysem. hey sae ha a sufficien cndiin fr sluin f he Riccai equain (and hus he sabiliy f he bserver-esimar, is ha he pair [A(ξ(,,ξ(,] mus be cninuusly bservable lcally fr all ime, i.e., he rank f he bservabiliy es marix O = [,..., (A( n ] mus be f full rank alng every bserver's rajecry ξ( ha he bserver aains. hey als cmmen ha: (i in sme cases, his sufficien cndiin can impse an "verly resricive requiremen n he bservabiliy f he nnlinear sysem in quesin"; and (ii his rank cndiin "may n hld in sme sysems ha are neverheless bservable in he mre general sense". he sabiliy f he SDDRE based bserver fr Deerminisic Nnlinear Sysems wihu he Lipschizian cndiins is deal wih []. his paper presens prfs f sabiliy f he SDDRE based esimar-bservers wihu he requiremen f he /6/$3. 26 IEEE

2 26 ISCEE Inernainal Cnference n he Science f Elecrical Engineering Lipschizian cndiins f he sysems nnlinear funcins by hree appraches. hus differen aspecs he sabiliy prpery are highlighed. hese are: Sabiliy f linear ime-varying sysems based prf; 2 Purely Lyapunv based analysis based prf by he use f Barkana's Invariance Principle [2]; 3 Parial Lyapunv based analysis and bunds cmpuain. he main nvely and imprance f he paper is presenain f cndiins fr unifrm glbal Bunded-Inpu- Bunded-Oupu (BIBO and Bunded-Inpu-Bunded-Sae (BIBS sabiliy (sufficien and necessary. I is shwn in he paper ha subjec unifrm glbal bservabiliy and cnrllabiliy, and cerain bundedness cndiins alng he esimar's rajecries he SDDRE based esimar-bserver is BIBS and BIBO sable and he iniial cndiins decay expnenially. Simulain f SDDRE based esimar f he Van der Pl equain is presened. II. HE SAE DEPENDEN COEFFICIEN FORM he fllwing nnlinear schasic sysem is cnsidered = f ( + B( u + G( w( y = g( + v( where, is he sae, u( is he inpu (measured, is he upu (measured, v( is he measuremen nise and w( represens he sysem driving nise and imbeds he difference beween he realiy and he mdel (. I is assumed ha w( and v( are bunded. Assuming f (, =, g(, = (2 he Sae Dependen Cefficien (SDC frm represenain f he nnlinear sysem is x + B( u + G( w( y = x + v( I is assumed here ha all marices A(,, B(, G( are knwn piecewise cninuus and unifrmly bunded wih respec all variables. Such represenain always exis albei is n unique (N all nnlinear sysem can be represened in he SDC frm wih unifrmly bunded marices. An impran prpery f he SDC represenain ha will be assumed in paper is i's he unifrm cmplee bservabiliy and cnrllabiliy, as a ime varying sysem (5, alng he rajecries f he SDDRE based esimar-bserver. All marices and vecrs are f he respecive dimensin. III. PROBLEM SAEMEN A nnlinear schasic sysem is cnsidered. In his case here are he sysem driving nise and he measuremen nise. he SDC represenain f he schasic nnlinear sysem is (3. In his case he sae,, f he sysem's mdel is unknwn. he prblem cnsidered here is he "esimain" f he sysem's sae by he SDDRE based esimar. ( (3 IV. HE SDDRE BASED ESIMAOR In his paper he SDDRE based [2,4,3], esimar f (,2 is ξ ( y ξ = C ( N ( Q ( + A ( + W ( C ( N (, = Q where: W is he specral densiy f he sysem driving nise, N> is he specral densiy f he measuremen nise; Nice ha wih sligh abuse f nain alng he aainable bserver's-esimar's rajecries we use he nain A ( ξ,, =, =, =. (5 his nain is used inerchangeably hrughu he paper. he esimar equains (4 can be slved as up he curren ime, ξ(, he esimaed sae, is perfecly knwn ime funcin, and he inpu and upu f he real sysem are measured. V. SABILIY PROOFS OVERVIEW hree prfs f BIBO and BIBS sabiliy f he SDDRE based esimar will be presened. Each f hem highlighs differen aspec he sabiliy prpery. hese are: Prf based n he sabiliy f linear ime-varying sysems; 2 Purely Lyapunv based analysis based prf by he use he Barkana's Invariance Principle [2]; 3 Lyapunv based analysis and bunds cmpuain. he prfs give cndiin n he BIBO and BIBS sabiliy f he SDDRE based esimar, hwever unbiasness, i.e. zer mean esimain errr, fr he schasic esimar, cann be guaraneed a his sage f he research, and is an issue f nging invesigain. VI. SABILIY PROOF BASED ON HE SABILIY OF LINEAR IME-VARYING SYSEMS he sabiliy herems fr linear ime-varying are based n [4]. he secin uses bservabiliy and cnrllabiliy as deal wih in [4,5]. he fac ha he esimar's rajecries, ξ(, are perfecly knwn up he curren ime, i.e. he esimar's rajecry is perfecly knwn funcin f ime is used. A. Sabiliy f he Esimar Alng he aainable rajecries f he esimar (4 he esimar can be wrien as (wihu he exernal inpu u(, ha is immaerial he sabiliy issue (4

3 26 ISCEE Inernainal Cnference n he Science f Elecrical Engineering ξ ξ + ( y ξ = C ( N ( Q ( + A ( + W ( C ( N (, = Q he fllwing herems f sabiliy frmalize he resuls. herem VI.: Cnsider he sysem in (6. Suppse ha A( is cninuus and bunded, ha, G(, W( and N( are piecewise cninuus and bunded, and furhermre ha W( αi, N(>βI, fr all and α,β> hen if he sysem in (6 is bh unifrmly cmpleely recnsrucible and unifrmly cmpleely cnrllable hen he sluin f he Riccai equain in (6 wih he iniial cndiin =Q cnverges Q ( as fr any Q. he prf is direc ucme f [4, herem 4.9]. herem VI.2: Cnsider he sysem (6. Suppse ha he sae exciain, w(, and bservain nises, v(, are uncrrelaed. Suppse ha he cninuiy, bundedness and psiive-definieness cndiins f herem VI. cncerning A(,, G(, W( and V( are saisfied. hen he seady-sae esimar ˆ( ξ ˆ( ξ + K ( [ ˆ( ξ ], (8 where K ( = Q ( C ( N ( is expnenially sable. Here Q ( is as defined in herem VI.. he prf is direc ucme f [4, herem 4.]. herems VI. and VI.2 give he cndiins ha he SDDRE esimar des n diverge (sable. Unfrunaely he biasness f he esimain errr cann be guaraneed. VII. SABILIY PROOF BASED ON BARKANA'S INVARIANCE PRINCIPLE his apprach defines Lyapunv funcin and uses he Barkana's Invariance Principle [2] shw ha he sae f he SDDRE based esimar is always bunded. Up dae ms prfs f sabiliy f nnlinear nnaunmus sysems f he frm ( (i.e. sysems where he ime variable explicily appears are based n s-called Barbala s Lemma [6, pp. 22]. his lemma seems require unifrm cninuiy f he Lyapunv derivaive and hus, f he sysem velciy. LaSalle s Invariance Principle [7] managed miigae his preliminary cndiin ha was apparenly needed fr he prf f sabiliy. Neverheless, because is frmulain uses he 'mdulus f cninuiy' μ(β α, i sill apparenly requires cninuiy f he rajecries. Hwever, because even his remaining cninuiy cndiin is n needed fr he prf f sabiliy [2], i is sufficien check saisfacin f ne f he fllwing w milder assumpins alng he rajecries f he sysem under invesigain: i. f (, is bunded fr any bunded x; r (2 (6 ii. β f τ, τ dτ α ( is bunded fr any finie ime inerval γ=β α. (3 his cndiin allws he presence f discninuiies and even impulse funcins and nly implies ha he rajecry cann pass an infinie disance in finie ime. herem VII.2 (he Barkana's Invariance Principle: Cnsider he nnlinear nnaunmus sysem (. Assume ha here exiss a psiive definie Lyapunv funcin V(x and ha is derivaive V (, alng he rajecries f Equain ( is negaive semi-definie, i.e., saisfies V (,. Fr any iniial cndiin x ( = = x define he dmain Ω = { x V ( x V ( x }. Because he Lyapunv derivaive is negaive semi-definie, i is clear ha all sysem rajecries are bunded and cnained wihin he dmain Ω. Nw, define he dmains Ω = { x e ( = } and Ω = { x i ( } (i.e, in Ω he Lyapunv derivaive is i idenically zer, namely, n jus equal zer. hen, if ne f he assumpins (24 r (25 hlds, all limi pins f he bunded rajecry belng he dmain Ω f = Ω Ω. e In paricular, limi pins ha are als equilibrium pins f belng Ω f = Ω Ω [2]. i he fllwing herem deals wih he BIBO sabiliy f he SDDRE based esimars. herem VII.3: Subjec he bundedness assumpins in secin II and herem VI. he SDDRE based esimar (4 is BIBO sable. Prf: he sabiliy f he aunmus par f he esimar (4, ξ = ( A( ξ. (4 is cnsidered alng he esimar's rajecries. A. he esimar's gain is bunded due he unifrm cmplee bservabiliy and cnrllabiliy assumpin f he sysem (2 alng he esimars rajecries. hen he requiremens f Barkana's invariance principle are saisfied. Furher, shw ha his unfrced sysem is asympically sable, we chse he Lyapunv funcin V = ξ Q ( ξ (5 hen i can be shwn ha ( C ( N ( + W( Q ( ξ V = ξ Q ( (6 and i is negaive definie, which implies ha he unfrced sysem is BIBS asympically sable. As A(, are bunded and N( βi, W( αi, α,β> are bunded and psiive definie he sysem is BIBO sable. B. he bundedness f he sysem sae wih he exernal signal cmmands alng he sysem's rajecries is cnsidered, i.e. he sabiliy f ξ ( ξ (7 ξ = ( A( ξ (8

4 26 ISCEE Inernainal Cnference n he Science f Elecrical Engineering hen fr he Lyapunv funcin (5 ( ξ, C ( ξ, N ( ξ, ξ, ξ, + W( = ξ Q ( ξ, + ξ Q ( ξ, B( u + u B( Q ( ξ, ξ + ξ Q ( ξ, ξ, y + y K ( ξ, Q ( ξ, ξ Q ( ξ, ξ (9 Assuming ha u( and are bunded and as all marices are bunded fr bunded han if ξ ends increase, he firs negaive erm ha is quadraic in ξ becmes dminan and s he Lyapunv derivaive becmes negaive and i guaranees bundedness f ξ. VIII. SABILIY BASED ON HE EXPONENIAL SABILIY OF HE SAE RANSIION MARIX he expnenial sabiliy f he sae ransiin marix f he esimar is prved and bunds n he sae are cmpued. herem VIII.: he sae ransiin marix f he SDDRE based bserver-esimar (6, subjec assumpin f herem VI., is asympically/expnenially sable and BIBO sable. Prf: A. he sabiliy f he aunmus sysem alng he sysem's rajecries he unfrced sysem (26 alng he sysem's rajecries wih he nain (7 is ξ = [ A( K ( ]ξ. (2 shw ha he aunmus sysem is asympically sable, we chse he Lyapunv funcin V = ξ Q ( ξ = ξ Q ( ξ (2 hen = e Q [ W ( + QC ( N ( Q] Q ( e <, fr all e (22 his immediaely guaranees asympic sabiliy. If he respecive cndiins are guaraneed his give expnenial sabiliy. his is furher elabraed. Fr he ime varying sysem his means ha he sae ransiin marix [ A( K ( ],, I Φ ( = (23 = is asympically/expnenially sable, ha is (24 shw expnenial sabiliy he cndiins f herem VI. are required. Dene, fllwing [8, herem ], = ξ Mξ Μ = Q [ W ( + QC ( N ( Q] Q ( > (25 and we require ha fr all < here exis α and β such ha α I Μ β I <, < α < β < (26 < i.e. M is unifrmly psiive definie and unifrmly bunded. hen β x M = α (27 ( Furher we assume ha here exis sme < a < b such ha i.e. V is bunded (guaraneed frm herem VI. a V b, < a < b, (28 hen ( a V ( V ( < α = α (29 Frm Grnwall-Bellman Lemma ( a V ( V (exp α (3 ha is, expnenial sabiliy alng he rajecries ξ(. he + expnenial sabiliy means ha here exis c, c2 R such ha Φ (3 c2 ( ( < c e B. Quaniaive esimae-bund n he BIBO sabiliy - Cmpuain f he H 2 gains he nn-aunmus esimar is [ y ξ ] ξ (32 and alng he aainable rajecries i may be wrien as [ y ξ ] ξ u + K ( hen we have τ τ ] ξ ( = ξ + τ + dτ (49 where Φ (, = I hen ξ ( = ξ + ξ + τ τ τ + dτ τ + dτ (33 (34 (35 Given ha he cndiins fr expnenial sabiliy f he sae ransiin marix presened in he previus secin are saisfied hen ξ ( c τ c2 ( c2 ( τ e ξ + c e + dτ (36 If [ ( τ B + is unifrmly glbally bunded, hen if here exiss finie M R, M < such ha [ B ( u( τ + < M τ. (37

5 26 ISCEE Inernainal Cnference n he Science f Elecrical Engineering Ne: u( and are he measured inpu and upu f he real plan and hus inherenly bunded. hus he requiremen is ha B( is unifrmly bunded by design and = is unifrmly bunded as i is he sluin f he ime-varying Riccai equain (4 under he respecive unifrm cmplee bservabiliy and cnrllabiliy cndiins. IX. ESIMAOR OF HE VAN DER POL EQUAION - SIMULAION he Van der Pl equain [6, pp. 8] is simulaed. he deails will be presened in he full paper. Figures presen he phase plane pl f he Van der Pl scillar sae, he esimaed sae and is esimaed errrs, respecively. esimaed velciy esimaed velciy errrs esimaed psiin real sae esimaed sae real and esimaed sae esimain errrs esimaed psiin errrs Figure : Phase plane pls f he Van der Pl scillar rajecries and is sae esimain errr. I. Biasness f he esimaed sae We shwed ha he esimaed sae, ξ(, is bunded (nn diverging. Hwever he mre ineresing issue if his esimae is unbiased. ha is if E[ ξ ( ] = E[ e( ] =. (37 where e( is he esimain errr. I is difficul analyze his issue fr nnlinear sysems. I is hined in [5,6] ha addiinal requiremens n he nnlineariies like Lipschizian cndiins (and may be sme addiinal cndiins can lead unbiased esimar. his is an addiin he requiremen ha all marices A(,, B(, G( are knwn piecewise cninuus and unifrmly bunded wih respec all variables. REFERENCES [] Gelb, A. Ed.: Applied Opimal Esimain, he MI press, 974. [2] Mracek,C.P., Cluier, J.R., and D'Suza, C.A.: A New echnique fr Nnlinear Esimain, Prceedings f he 996 IEEE Inernainal Cnference n Cnrl Applicains, Dearbrn, MI, Sepember 5-8, 996. [3] Xin, M. and Balakrishnan, S.N.: A New Filering echnique fr a Class f Nnlinear Sysems, Prceedings f he 4s IEEE Cnference n Decisin and Cnrl, Las- Vegas, Nevada USA, December 22. [4] Haessig, D.A. and Friedland, B.: Sae Dependen Differenial Riccai Equain fr Nnlinear Esimain and Cnrl, 22 IFAC, 5h riennial Wrld Cngress, Barcelna, Spain. [5] Beikzadeh, H. and aghirad, H.D.(29: Sabiliy Analysis f he Discree-ime Difference SDRE Sae Esimar in a Nisy Envirnmen 29 IEEE Inernainal Cnference n Cnrl and Aumain Chrischurch, New Zealand, December 9-, 29. [6] Beikzadeh, H. and aghirad, H.D.(22: Expnenial Nnlinear Observer Based n he Differenial Sae-Dependen Riccai Equain, Inernainal Jurnal f Aumain and Cmpuing, 9(4, Augus 22, DOI:.7/s y [7] Williams, D., B. Friedland and A. N. Madiwale (987: Mdern Cnrl hery fr Design f Aupils fr Bank-- urn Missiles, AIAA Jurnal f Guidance, Cnrl, and Dynamics, Vl., N. 4, pp [8] Cluier, J. R., C. N. D Suza and C. P. Mracek, (996 Nnlinear Regulain and Nnlinear H Cnrl via he Sae- Dependen Riccai Equain echnique: Par 2, Examples, Firs In. Cnf n Nnlinear Prblems in Aviain and Aerspace, Dayna,Beach, FL. [9] Weiss, H. and Mre, J.B.: Imprved Exended Kalman Filer Design fr Passive racking, IEEE ransacins n Aumaic Cnrl, Vl. AC-25, N. 4, Augus 98, pp [] arn,. J. and Rasis, Y. Observers fr Nnlinear Schasic Sysems, IEEE rans. n Aumaic Cnrl, Vl. 2, N. 4, pp , 976. [] Rusnak, I. and Barkana, I.: Sabiliy f he SDDRE based Observer fr Deerminisic Nnlinear Sysems, ECC 26, Eurpean Cnrl Cnference, June 29 July, 26, Aalbrg, Denmark. [2] Barkana, I.: Defending he beauy f he Invariance Principle, Inernainal Jurnal f Cnrl, 24, Vl. 87, N., 86-26, hp://dx. DOI:.8/ [3] Çimen,. and Merpçu lu, A. O.: Asympically Opimal Nnlinear Filering: hery and Examples wih Applicain arge Sae Esimain, Prceedings f he 7h Wrld Cngress, he Inernainal Federain f Aumaic Cnrl, Seul, Krea, July 6-, 28. [4] Kwakernaak, H. and Sivan, R.: Linear Opimal Cnrl Sysems, Wiley-Inerscience, 972. [5] Chen, C..: Linear Sysem hery and Design, Hl Rinehar and Winsn, Inc, 984. [6] Sline, J.J., & Li, M.: Applied nnlinear cnrl. Englewd Cliffs, NJ: Prenice Hall. 99. [7] LaSalle, J.P. he sabiliy f dynamical sysems. New Yrk: SIAM [8] Vidyasagar, M.: Nnlinear Sysems Analysis, Prenice Hall,2nd Ediin, 993.

MASSACHUSETTS INSTITUTE OF TECHNOLOGY 6.265/15.070J Fall 2013 Lecture 15 10/30/2013. Ito integral for simple processes

MASSACHUSETTS INSTITUTE OF TECHNOLOGY 6.265/15.070J Fall 2013 Lecture 15 10/30/2013. Ito integral for simple processes MASSACHUSETTS INSTITUTE OF TECHNOLOGY 6.65/15.7J Fall 13 Lecure 15 1/3/13 I inegral fr simple prcesses Cnen. 1. Simple prcesses. I ismery. Firs 3 seps in cnsrucing I inegral fr general prcesses 1 I inegral

More information

Brace-Gatarek-Musiela model

Brace-Gatarek-Musiela model Chaper 34 Brace-Gaarek-Musiela mdel 34. Review f HJM under risk-neural IP where f ( T Frward rae a ime fr brrwing a ime T df ( T ( T ( T d + ( T dw ( ( T The ineres rae is r( f (. The bnd prices saisfy

More information

Fractional Order Disturbance Observer based Robust Control

Fractional Order Disturbance Observer based Robust Control 201 Inernainal Cnference n Indusrial Insrumenain and Cnrl (ICIC) Cllege f Engineering Pune, India. May 28-30, 201 Fracinal Order Disurbance Observer based Rbus Cnrl Bhagyashri Tamhane 1, Amrua Mujumdar

More information

AP Physics 1 MC Practice Kinematics 1D

AP Physics 1 MC Practice Kinematics 1D AP Physics 1 MC Pracice Kinemaics 1D Quesins 1 3 relae w bjecs ha sar a x = 0 a = 0 and mve in ne dimensin independenly f ne anher. Graphs, f he velciy f each bjec versus ime are shwn belw Objec A Objec

More information

Productivity changes of units: A directional measure of cost Malmquist index

Productivity changes of units: A directional measure of cost Malmquist index Available nline a hp://jnrm.srbiau.ac.ir Vl.1, N.2, Summer 2015 Jurnal f New Researches in Mahemaics Science and Research Branch (IAU Prduciviy changes f unis: A direcinal measure f cs Malmquis index G.

More information

Convex Stochastic Duality and the Biting Lemma

Convex Stochastic Duality and the Biting Lemma Jurnal f Cnvex Analysis Vlume 9 (2002), N. 1, 237 244 Cnvex Schasic Dualiy and he Biing Lemma Igr V. Evsigneev Schl f Ecnmic Sudies, Universiy f Mancheser, Oxfrd Rad, Mancheser, M13 9PL, UK igr.evsigneev@man.ac.uk

More information

Lyapunov Stability Stability of Equilibrium Points

Lyapunov Stability Stability of Equilibrium Points Lyapunv Stability Stability f Equilibrium Pints 1. Stability f Equilibrium Pints - Definitins In this sectin we cnsider n-th rder nnlinear time varying cntinuus time (C) systems f the frm x = f ( t, x),

More information

Successive ApproxiInations and Osgood's Theorenl

Successive ApproxiInations and Osgood's Theorenl Revisa de la Unin Maemaica Argenina Vlumen 40, Niimers 3 y 4,1997. 73 Successive ApprxiInains and Osgd's Therenl Calix P. Caldern Virginia N. Vera de Seri.July 29, 1996 Absrac The Picard's mehd fr slving

More information

An application of nonlinear optimization method to. sensitivity analysis of numerical model *

An application of nonlinear optimization method to. sensitivity analysis of numerical model * An applicain f nnlinear pimizain mehd sensiiviy analysis f numerical mdel XU Hui 1, MU Mu 1 and LUO Dehai 2 (1. LASG, Insiue f Amspheric Physics, Chinese Academy f Sciences, Beijing 129, China; 2. Deparmen

More information

10.7 Temperature-dependent Viscoelastic Materials

10.7 Temperature-dependent Viscoelastic Materials Secin.7.7 Temperaure-dependen Viscelasic Maerials Many maerials, fr example plymeric maerials, have a respnse which is srngly emperaure-dependen. Temperaure effecs can be incrpraed in he hery discussed

More information

5.1 Angles and Their Measure

5.1 Angles and Their Measure 5. Angles and Their Measure Secin 5. Nes Page This secin will cver hw angles are drawn and als arc lengh and rains. We will use (hea) represen an angle s measuremen. In he figure belw i describes hw yu

More information

( ) ( ) if t = t. It must satisfy the identity. So, bulkiness of the unit impulse (hyper)function is equal to 1. The defining characteristic is

( ) ( ) if t = t. It must satisfy the identity. So, bulkiness of the unit impulse (hyper)function is equal to 1. The defining characteristic is UNIT IMPULSE RESPONSE, UNIT STEP RESPONSE, STABILITY. Uni impulse funcion (Dirac dela funcion, dela funcion) rigorously defined is no sricly a funcion, bu disribuion (or measure), precise reamen requires

More information

The Components of Vector B. The Components of Vector B. Vector Components. Component Method of Vector Addition. Vector Components

The Components of Vector B. The Components of Vector B. Vector Components. Component Method of Vector Addition. Vector Components Upcming eens in PY05 Due ASAP: PY05 prees n WebCT. Submiing i ges yu pin ward yur 5-pin Lecure grade. Please ake i seriusly, bu wha cuns is wheher r n yu submi i, n wheher yu ge hings righ r wrng. Due

More information

and Sun (14) and Due and Singlen (19) apply he maximum likelihd mehd while Singh (15), and Lngsa and Schwarz (12) respecively emply he hreesage leas s

and Sun (14) and Due and Singlen (19) apply he maximum likelihd mehd while Singh (15), and Lngsa and Schwarz (12) respecively emply he hreesage leas s A MONTE CARLO FILTERING APPROACH FOR ESTIMATING THE TERM STRUCTURE OF INTEREST RATES Akihik Takahashi 1 and Seish Sa 2 1 The Universiy f Tky, 3-8-1 Kmaba, Megur-ku, Tky 153-8914 Japan 2 The Insiue f Saisical

More information

Impact Switch Study Modeling & Implications

Impact Switch Study Modeling & Implications L-3 Fuzing & Ordnance Sysems Impac Swich Sudy Mdeling & Implicains Dr. Dave Frankman May 13, 010 NDIA 54 h Annual Fuze Cnference This presenain cnsiss f L-3 Crprain general capabiliies infrmain ha des

More information

Motion Along a Straight Line

Motion Along a Straight Line PH 1-3A Fall 010 Min Alng a Sraigh Line Lecure Chaper (Halliday/Resnick/Walker, Fundamenals f Physics 8 h ediin) Min alng a sraigh line Sudies he min f bdies Deals wih frce as he cause f changes in min

More information

Linear Response Theory: The connection between QFT and experiments

Linear Response Theory: The connection between QFT and experiments Phys540.nb 39 3 Linear Response Theory: The connecion beween QFT and experimens 3.1. Basic conceps and ideas Q: How do we measure he conduciviy of a meal? A: we firs inroduce a weak elecric field E, and

More information

Tracking Adversarial Targets

Tracking Adversarial Targets A. Proofs Proof of Lemma 3. Consider he Bellman equaion λ + V π,l x, a lx, a + V π,l Ax + Ba, πax + Ba. We prove he lemma by showing ha he given quadraic form is he unique soluion of he Bellman equaion.

More information

Unit-I (Feedback amplifiers) Features of feedback amplifiers. Presentation by: S.Karthie, Lecturer/ECE SSN College of Engineering

Unit-I (Feedback amplifiers) Features of feedback amplifiers. Presentation by: S.Karthie, Lecturer/ECE SSN College of Engineering Uni-I Feedback ampliiers Feaures eedback ampliiers Presenain by: S.Karhie, Lecurer/ECE SSN Cllege Engineering OBJECTIVES T make he sudens undersand he eec negaive eedback n he llwing ampliier characerisics:

More information

GMM Estimation of the Number of Latent Factors

GMM Estimation of the Number of Latent Factors GMM Esimain f he Number f aen Facrs Seung C. Ahn a, Marcs F. Perez b March 18, 2007 Absrac We prpse a generalized mehd f mmen (GMM) esimar f he number f laen facrs in linear facr mdels. he mehd is apprpriae

More information

A Note on the Approximation of the Wave Integral. in a Slightly Viscous Ocean of Finite Depth. due to Initial Surface Disturbances

A Note on the Approximation of the Wave Integral. in a Slightly Viscous Ocean of Finite Depth. due to Initial Surface Disturbances Applied Mahemaical Sciences, Vl. 7, 3, n. 36, 777-783 HIKARI Ld, www.m-hikari.cm A Ne n he Apprximain f he Wave Inegral in a Slighly Viscus Ocean f Finie Deph due Iniial Surface Disurbances Arghya Bandypadhyay

More information

Numerical solution of some types of fractional optimal control problems

Numerical solution of some types of fractional optimal control problems Numerical Analysis and Scienific mpuing Preprin Seria Numerical sluin f sme ypes f fracinal pimal cnrl prblems N.H. Sweilam T.M. Al-Ajmi R.H.W. Hppe Preprin #23 Deparmen f Mahemaics Universiy f Husn Nvember

More information

Efficient and Fast Simulation of RF Circuits and Systems via Spectral Method

Efficient and Fast Simulation of RF Circuits and Systems via Spectral Method Efficien and Fas Simulain f RF Circuis and Sysems via Specral Mehd 1. Prjec Summary The prpsed research will resul in a new specral algrihm, preliminary simular based n he new algrihm will be subsanially

More information

Microwave Engineering

Microwave Engineering Micrwave Engineering Cheng-Hsing Hsu Deparmen f Elecrical Engineering Nainal Unied Universiy Ouline. Transmissin ine Thery. Transmissin ines and Waveguides eneral Sluins fr TEM, TE, and TM waves ; Parallel

More information

THE DETERMINATION OF CRITICAL FLOW FACTORS FOR NATURAL GAS MIXTURES. Part 3: The Calculation of C* for Natural Gas Mixtures

THE DETERMINATION OF CRITICAL FLOW FACTORS FOR NATURAL GAS MIXTURES. Part 3: The Calculation of C* for Natural Gas Mixtures A REPORT ON THE DETERMINATION OF CRITICAL FLOW FACTORS FOR NATURAL GAS MIXTURES Par 3: The Calculain f C* fr Naural Gas Mixures FOR NMSPU Deparmen f Trade and Indusry 151 Buckingham Palace Rad Lndn SW1W

More information

independenly fllwing square-r prcesses, he inuiive inerpreain f he sae variables is n clear, and smeimes i seems dicul nd admissible parameers fr whic

independenly fllwing square-r prcesses, he inuiive inerpreain f he sae variables is n clear, and smeimes i seems dicul nd admissible parameers fr whic A MONTE CARLO FILTERING APPROACH FOR ESTIMATING THE TERM STRUCTURE OF INTEREST RATES Akihik Takahashi 1 and Seish Sa 2 1 The Universiy f Tky, 3-8-1 Kmaba, Megur-ku, Tky 153-8914 Japan 2 The Insiue f Saisical

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

Kinematics Review Outline

Kinematics Review Outline Kinemaics Review Ouline 1.1.0 Vecrs and Scalars 1.1 One Dimensinal Kinemaics Vecrs have magniude and direcin lacemen; velciy; accelerain sign indicaes direcin + is nrh; eas; up; he righ - is suh; wes;

More information

A NOTE ON THE EXISTENCE OF AN OPTIMAL SOLUTION FOR CONCAVE INFINITE HORIZON ECONOMIC MODELS

A NOTE ON THE EXISTENCE OF AN OPTIMAL SOLUTION FOR CONCAVE INFINITE HORIZON ECONOMIC MODELS A NOTE ON THE EXISTENCE OF AN OPTIMAL SOLUTION FOR CONCAVE INFINITE HORIZON ECONOMIC MODELS by Smdeb Lahiri Discussin Paper N. 221, Sepember 1985 Cener fr Ecnmic Research Deparmen f Ecnmics Universiy f

More information

PRINCE SULTAN UNIVERSITY Department of Mathematical Sciences Final Examination Second Semester (072) STAT 271.

PRINCE SULTAN UNIVERSITY Department of Mathematical Sciences Final Examination Second Semester (072) STAT 271. PRINCE SULTAN UNIVERSITY Deparmen f Mahemaical Sciences Final Examinain Secnd Semeser 007 008 (07) STAT 7 Suden Name Suden Number Secin Number Teacher Name Aendance Number Time allwed is ½ hurs. Wrie dwn

More information

- polynomial with real coefficients.

- polynomial with real coefficients. THE ASYMPTOTIC BEHAVIOUR OF SOLUTIONS OF BOUNDARY VALUE PROBLEMS FOR LINEARIZED KdV EQUATION Barabash Tayana O., Eidel'man Samuil D. (Ukraine,Kiev) I.Saemen fhe prblem.we invesigaehe asympicbehaviur (when

More information

Recursive Least-Squares Fixed-Interval Smoother Using Covariance Information based on Innovation Approach in Linear Continuous Stochastic Systems

Recursive Least-Squares Fixed-Interval Smoother Using Covariance Information based on Innovation Approach in Linear Continuous Stochastic Systems 8 Froniers in Signal Processing, Vol. 1, No. 1, July 217 hps://dx.doi.org/1.2266/fsp.217.112 Recursive Leas-Squares Fixed-Inerval Smooher Using Covariance Informaion based on Innovaion Approach in Linear

More information

CHAPTER 7 CHRONOPOTENTIOMETRY. In this technique the current flowing in the cell is instantaneously stepped from

CHAPTER 7 CHRONOPOTENTIOMETRY. In this technique the current flowing in the cell is instantaneously stepped from CHAPTE 7 CHONOPOTENTIOMETY In his echnique he curren flwing in he cell is insananeusly sepped frm zer sme finie value. The sluin is n sirred and a large ecess f suppring elecrlye is presen in he sluin;

More information

MATH 5720: Gradient Methods Hung Phan, UMass Lowell October 4, 2018

MATH 5720: Gradient Methods Hung Phan, UMass Lowell October 4, 2018 MATH 5720: Gradien Mehods Hung Phan, UMass Lowell Ocober 4, 208 Descen Direcion Mehods Consider he problem min { f(x) x R n}. The general descen direcions mehod is x k+ = x k + k d k where x k is he curren

More information

CONTROL SYSTEMS, ROBOTICS AND AUTOMATION Vol. XI Control of Stochastic Systems - P.R. Kumar

CONTROL SYSTEMS, ROBOTICS AND AUTOMATION Vol. XI Control of Stochastic Systems - P.R. Kumar CONROL OF SOCHASIC SYSEMS P.R. Kumar Deparmen of Elecrical and Compuer Engineering, and Coordinaed Science Laboraory, Universiy of Illinois, Urbana-Champaign, USA. Keywords: Markov chains, ransiion probabiliies,

More information

Answers: ( HKMO Heat Events) Created by: Mr. Francis Hung Last updated: 21 September 2018

Answers: ( HKMO Heat Events) Created by: Mr. Francis Hung Last updated: 21 September 2018 nswers: (009-0 HKMO Hea Evens) reaed by: Mr. Francis Hung Las updaed: Sepember 08 09-0 Individual 6 7 7 0 Spare 8 9 0 08 09-0 8 0 0.8 Spare Grup 6 0000 7 09 8 00 9 0 0 Individual Evens I In hw many pssible

More information

Lecture 3: Resistive forces, and Energy

Lecture 3: Resistive forces, and Energy Lecure 3: Resisive frces, and Energy Las ie we fund he velciy f a prjecile ving wih air resisance: g g vx ( ) = vx, e vy ( ) = + v + e One re inegrain gives us he psiin as a funcin f ie: dx dy g g = vx,

More information

Module 4. Analysis of Statically Indeterminate Structures by the Direct Stiffness Method. Version 2 CE IIT, Kharagpur

Module 4. Analysis of Statically Indeterminate Structures by the Direct Stiffness Method. Version 2 CE IIT, Kharagpur Mdle Analysis f Saically Indeerminae Srcres by he Direc Siffness Mehd Versin CE IIT, Kharagr Lessn The Direc Siffness Mehd: Temerare Changes and Fabricain Errrs in Trss Analysis Versin CE IIT, Kharagr

More information

The lower limit of interval efficiency in Data Envelopment Analysis

The lower limit of interval efficiency in Data Envelopment Analysis Jurnal f aa nelpmen nalysis and ecisin Science 05 N. (05) 58-66 ailable nline a www.ispacs.cm/dea lume 05, Issue, ear 05 ricle I: dea-00095, 9 Pages di:0.5899/05/dea-00095 Research ricle aa nelpmen nalysis

More information

Finite time L 1 Approach for Missile Overload Requirement Analysis in Terminal Guidance

Finite time L 1 Approach for Missile Overload Requirement Analysis in Terminal Guidance Chinese Jurnal Aernauics 22(29) 413-418 Chinese Jurnal Aernauics www.elsevier.cm/lcae/cja Finie ime L 1 Apprach r Missile Overlad Requiremen Analysis in Terminal Guidance Ji Dengga*, He Fenghua, Ya Yu

More information

Physics 235 Chapter 2. Chapter 2 Newtonian Mechanics Single Particle

Physics 235 Chapter 2. Chapter 2 Newtonian Mechanics Single Particle Chaper 2 Newonian Mechanics Single Paricle In his Chaper we will review wha Newon s laws of mechanics ell us abou he moion of a single paricle. Newon s laws are only valid in suiable reference frames,

More information

Lecture II Simple One-Dimensional Vibrating Systems

Lecture II Simple One-Dimensional Vibrating Systems UIUC Physics 406 Acusical Physics f Music Lecure II Simple One-Dimensinal Vibraing Sysems One mehd f prducing a sund relies n a physical bjec (e.g. varius ypes f musical insrumens sringed and wind insrumens

More information

EXERCISES FOR SECTION 1.5

EXERCISES FOR SECTION 1.5 1.5 Exisence and Uniqueness of Soluions 43 20. 1 v c 21. 1 v c 1 2 4 6 8 10 1 2 2 4 6 8 10 Graph of approximae soluion obained using Euler s mehod wih = 0.1. Graph of approximae soluion obained using Euler

More information

ON THE COMPONENT DISTRIBUTION COEFFICIENTS AND SOME REGULARITIES OF THE CRYSTALLIZATION OF SOLID SOLUTION ALLOYS IN MULTICOMPONENT SYSTEMS*

ON THE COMPONENT DISTRIBUTION COEFFICIENTS AND SOME REGULARITIES OF THE CRYSTALLIZATION OF SOLID SOLUTION ALLOYS IN MULTICOMPONENT SYSTEMS* METL 006.-5.5.006, Hradec nad Mravicí ON THE OMPONENT DISTRIUTION OEFFIIENTS ND SOME REGULRITIES OF THE RYSTLLIZTION OF SOLID SOLUTION LLOYS IN MULTIOMPONENT SYSTEMS* Eugenij V.Sidrv a, M.V.Pikunv b, Jarmír.Drápala

More information

Lecture 4 ( ) Some points of vertical motion: Here we assumed t 0 =0 and the y axis to be vertical.

Lecture 4 ( ) Some points of vertical motion: Here we assumed t 0 =0 and the y axis to be vertical. Sme pins f erical min: Here we assumed and he y axis be erical. ( ) y g g y y y y g dwnwards 9.8 m/s g Lecure 4 Accelerain The aerage accelerain is defined by he change f elciy wih ime: a ; In analgy,

More information

An Introduction to Wavelet Analysis. with Applications to Vegetation Monitoring

An Introduction to Wavelet Analysis. with Applications to Vegetation Monitoring An Inrducin Wavele Analysis wih Applicains Vegeain Mniring Dn Percival Applied Physics Labrary, Universiy f Washingn Seale, Washingn, USA verheads fr alk available a hp://saff.washingn.edu/dbp/alks.hml

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

GAMS Handout 2. Utah State University. Ethan Yang

GAMS Handout 2. Utah State University. Ethan Yang Uah ae Universiy DigialCmmns@UU All ECAIC Maerials ECAIC Repsiry 2017 GAM Handu 2 Ehan Yang yey217@lehigh.edu Fllw his and addiinal wrs a: hps://digialcmmns.usu.edu/ecsaic_all Par f he Civil Engineering

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

Stability and Bifurcation in a Neural Network Model with Two Delays

Stability and Bifurcation in a Neural Network Model with Two Delays Inernaional Mahemaical Forum, Vol. 6, 11, no. 35, 175-1731 Sabiliy and Bifurcaion in a Neural Nework Model wih Two Delays GuangPing Hu and XiaoLing Li School of Mahemaics and Physics, Nanjing Universiy

More information

An recursive analytical technique to estimate time dependent physical parameters in the presence of noise processes

An recursive analytical technique to estimate time dependent physical parameters in the presence of noise processes WHAT IS A KALMAN FILTER An recursive analyical echnique o esimae ime dependen physical parameers in he presence of noise processes Example of a ime and frequency applicaion: Offse beween wo clocks PREDICTORS,

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

POSITIVE AND MONOTONE SYSTEMS IN A PARTIALLY ORDERED SPACE

POSITIVE AND MONOTONE SYSTEMS IN A PARTIALLY ORDERED SPACE Urainian Mahemaical Journal, Vol. 55, No. 2, 2003 POSITIVE AND MONOTONE SYSTEMS IN A PARTIALLY ORDERED SPACE A. G. Mazo UDC 517.983.27 We invesigae properies of posiive and monoone differenial sysems wih

More information

Lecture Notes 3: Quantitative Analysis in DSGE Models: New Keynesian Model

Lecture Notes 3: Quantitative Analysis in DSGE Models: New Keynesian Model Lecure Noes 3: Quaniaive Analysis in DSGE Models: New Keynesian Model Zhiwei Xu, Email: xuzhiwei@sju.edu.cn The moneary policy plays lile role in he basic moneary model wihou price sickiness. We now urn

More information

2.160 System Identification, Estimation, and Learning. Lecture Notes No. 8. March 6, 2006

2.160 System Identification, Estimation, and Learning. Lecture Notes No. 8. March 6, 2006 2.160 Sysem Idenificaion, Esimaion, and Learning Lecure Noes No. 8 March 6, 2006 4.9 Eended Kalman Filer In many pracical problems, he process dynamics are nonlinear. w Process Dynamics v y u Model (Linearized)

More information

99 Union Matematica Argen tina Volumen 4 1, 1, PROBLEMS FOR A SE M I - I N F I N ITE STR I P WITH A N O N - U N I F O R M H EAT S O U RCE

99 Union Matematica Argen tina Volumen 4 1, 1, PROBLEMS FOR A SE M I - I N F I N ITE STR I P WITH A N O N - U N I F O R M H EAT S O U RCE Revisa de la 99 Unin Maemaica Argen ina Vlumen 4 1 1 1 998 S O M E N O N L I N EA R H EAT C O N D U CTI O N PROBLEMS FOR A SE M I - I N F I N ITE STR I P WITH A N O N - U N I F O R M H EAT S O U RCE Dming

More information

Matrix Versions of Some Refinements of the Arithmetic-Geometric Mean Inequality

Matrix Versions of Some Refinements of the Arithmetic-Geometric Mean Inequality Marix Versions of Some Refinemens of he Arihmeic-Geomeric Mean Inequaliy Bao Qi Feng and Andrew Tonge Absrac. We esablish marix versions of refinemens due o Alzer ], Carwrigh and Field 4], and Mercer 5]

More information

Guest Lectures for Dr. MacFarlane s EE3350 Part Deux

Guest Lectures for Dr. MacFarlane s EE3350 Part Deux Gues Lecures for Dr. MacFarlane s EE3350 Par Deux Michael Plane Mon., 08-30-2010 Wrie name in corner. Poin ou his is a review, so I will go faser. Remind hem o go lisen o online lecure abou geing an A

More 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

Testing for a Single Factor Model in the Multivariate State Space Framework

Testing for a Single Factor Model in the Multivariate State Space Framework esing for a Single Facor Model in he Mulivariae Sae Space Framework Chen C.-Y. M. Chiba and M. Kobayashi Inernaional Graduae School of Social Sciences Yokohama Naional Universiy Japan Faculy of Economics

More information

Chapter 3 Boundary Value Problem

Chapter 3 Boundary Value Problem Chaper 3 Boundary Value Problem A boundary value problem (BVP) is a problem, ypically an ODE or a PDE, which has values assigned on he physical boundary of he domain in which he problem is specified. Le

More information

RAPIDLY ADAPTIVE CFAR DETECTION BY MERGING INDIVIDUAL DECISIONS FROM TWO-STAGE ADAPTIVE DETECTORS

RAPIDLY ADAPTIVE CFAR DETECTION BY MERGING INDIVIDUAL DECISIONS FROM TWO-STAGE ADAPTIVE DETECTORS RAPIDLY ADAPIVE CFAR DEECION BY MERGING INDIVIDUAL DECISIONS FROM WO-SAGE ADAPIVE DEECORS Analii A. Knnv, Sung-yun Chi and Jin-a Kim Research Cener, SX Engine Yngin-si, 694 Krea kaa@ieee.rg; dkrein@nesx.cm;

More information

if N =2 J, obtain analysis (decomposition) of sample variance:

if N =2 J, obtain analysis (decomposition) of sample variance: Wavele Mehds fr Time Series Analysis Eamples: Time Series X Versus Time Inde Par VII: Wavele Variance and Cvariance X (a) (b) eamples f ime series mivae discussin decmpsiin f sample variance using waveles

More information

Machine Learning for Signal Processing Prediction and Estimation, Part II

Machine Learning for Signal Processing Prediction and Estimation, Part II Machine Learning fr Signal Prceing Predicin and Eimain, Par II Bhikha Raj Cla 24. 2 Nv 203 2 Nv 203-755/8797 Adminirivia HW cre u Sme uden wh g really pr mark given chance upgrade Make i all he way he

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

Coherent PSK. The functional model of passband data transmission system is. Signal transmission encoder. x Signal. decoder.

Coherent PSK. The functional model of passband data transmission system is. Signal transmission encoder. x Signal. decoder. Cheren PSK he funcinal mdel f passand daa ransmissin sysem is m i Signal ransmissin encder si s i Signal Mdular Channel Deecr ransmissin decder mˆ Carrier signal m i is a sequence f syml emied frm a message

More information

Course Notes for EE227C (Spring 2018): Convex Optimization and Approximation

Course Notes for EE227C (Spring 2018): Convex Optimization and Approximation Course Noes for EE7C Spring 018: Convex Opimizaion and Approximaion Insrucor: Moriz Hard Email: hard+ee7c@berkeley.edu Graduae Insrucor: Max Simchowiz Email: msimchow+ee7c@berkeley.edu Ocober 15, 018 3

More information

Augmented Reality II - Kalman Filters - Gudrun Klinker May 25, 2004

Augmented Reality II - Kalman Filters - Gudrun Klinker May 25, 2004 Augmened Realiy II Kalman Filers Gudrun Klinker May 25, 2004 Ouline Moivaion Discree Kalman Filer Modeled Process Compuing Model Parameers Algorihm Exended Kalman Filer Kalman Filer for Sensor Fusion Lieraure

More information

A game theory approach to the robot tracking problem.

A game theory approach to the robot tracking problem. A game hery apprach he rb racing prblem. CARLOS RODRÍGEZ LCATERO, ALVARO DE ALBORNOZ BENO, & RAFAEL LOZANO ESPINOSA Deparamen de Cmpuación ITESM Campus Ciudad de Méxic Tlalpan Ciudad de Méxic, Méxic, C.P.

More information

(1) (2) Differentiation of (1) and then substitution of (3) leads to. Therefore, we will simply consider the second-order linear system given by (4)

(1) (2) Differentiation of (1) and then substitution of (3) leads to. Therefore, we will simply consider the second-order linear system given by (4) Phase Plane Analysis of Linear Sysems Adaped from Applied Nonlinear Conrol by Sloine and Li The general form of a linear second-order sysem is a c b d From and b bc d a Differeniaion of and hen subsiuion

More 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

Ramsey model. Rationale. Basic setup. A g A exogenous as in Solow. n L each period.

Ramsey model. Rationale. Basic setup. A g A exogenous as in Solow. n L each period. Ramsey mdel Rainale Prblem wih he Slw mdel: ad-hc assumpin f cnsan saving rae Will cnclusins f Slw mdel be alered if saving is endgenusly deermined by uiliy maximizain? Yes, bu we will learn a l abu cnsumpin/saving

More information

Section 12 Time Series Regression with Non- Stationary Variables

Section 12 Time Series Regression with Non- Stationary Variables Secin Time Series Regressin wih Nn- Sainary Variables The TSMR assumpins include, criically, he assumpin ha he variables in a regressin are sainary. Bu many (ms?) ime-series variables are nnsainary. We

More information

The Asymptotic Behavior of Nonoscillatory Solutions of Some Nonlinear Dynamic Equations on Time Scales

The Asymptotic Behavior of Nonoscillatory Solutions of Some Nonlinear Dynamic Equations on Time Scales Advances in Dynamical Sysems and Applicaions. ISSN 0973-5321 Volume 1 Number 1 (2006, pp. 103 112 c Research India Publicaions hp://www.ripublicaion.com/adsa.hm The Asympoic Behavior of Nonoscillaory Soluions

More information

Research & Reviews: Journal of Statistics and Mathematical Sciences

Research & Reviews: Journal of Statistics and Mathematical Sciences Research & Reviews: Jural f Saisics ad Mahemaical Scieces iuus Depedece f he Slui f A Schasic Differeial Equai Wih Nlcal diis El-Sayed AMA, Abd-El-Rahma RO, El-Gedy M Faculy f Sciece, Alexadria Uiversiy,

More information

4. Advanced Stability Theory

4. Advanced Stability Theory Applied Nonlinear Conrol Nguyen an ien - 4 4 Advanced Sabiliy heory he objecive of his chaper is o presen sabiliy analysis for non-auonomous sysems 41 Conceps of Sabiliy for Non-Auonomous Sysems Equilibrium

More information

Visco-elastic Layers

Visco-elastic Layers Visc-elasic Layers Visc-elasic Sluins Sluins are bained by elasic viscelasic crrespndence principle by applying laplace ransfrm remve he ime variable Tw mehds f characerising viscelasic maerials: Mechanical

More information

i-clicker Question lim Physics 123 Lecture 2 1 Dimensional Motion x 1 x 2 v is not constant in time v = v(t) acceleration lim Review:

i-clicker Question lim Physics 123 Lecture 2 1 Dimensional Motion x 1 x 2 v is not constant in time v = v(t) acceleration lim Review: Reiew: Physics 13 Lecure 1 Dimensinal Min Displacemen: Dx = x - x 1 (If Dx < 0, he displacemen ecr pins he lef.) Aerage elciy: (N he same as aerage speed) a slpe = a x x 1 1 Dx D x 1 x Crrecin: Calculus

More information

Zürich. ETH Master Course: L Autonomous Mobile Robots Localization II

Zürich. ETH Master Course: L Autonomous Mobile Robots Localization II Roland Siegwar Margaria Chli Paul Furgale Marco Huer Marin Rufli Davide Scaramuzza ETH Maser Course: 151-0854-00L Auonomous Mobile Robos Localizaion II ACT and SEE For all do, (predicion updae / ACT),

More information

Comments on Window-Constrained Scheduling

Comments on Window-Constrained Scheduling Commens on Window-Consrained Scheduling Richard Wes Member, IEEE and Yuing Zhang Absrac This shor repor clarifies he behavior of DWCS wih respec o Theorem 3 in our previously published paper [1], and describes

More information

Book Corrections for Optimal Estimation of Dynamic Systems, 2 nd Edition

Book Corrections for Optimal Estimation of Dynamic Systems, 2 nd Edition Boo Correcions for Opimal Esimaion of Dynamic Sysems, nd Ediion John L. Crassidis and John L. Junins November 17, 017 Chaper 1 This documen provides correcions for he boo: Crassidis, J.L., and Junins,

More information

A DELAY-DEPENDENT STABILITY CRITERIA FOR T-S FUZZY SYSTEM WITH TIME-DELAYS

A DELAY-DEPENDENT STABILITY CRITERIA FOR T-S FUZZY SYSTEM WITH TIME-DELAYS A DELAY-DEPENDENT STABILITY CRITERIA FOR T-S FUZZY SYSTEM WITH TIME-DELAYS Xinping Guan ;1 Fenglei Li Cailian Chen Insiue of Elecrical Engineering, Yanshan Universiy, Qinhuangdao, 066004, China. Deparmen

More information

From Particles to Rigid Bodies

From Particles to Rigid Bodies Rigid Body Dynamics From Paricles o Rigid Bodies Paricles No roaions Linear velociy v only Rigid bodies Body roaions Linear velociy v Angular velociy ω Rigid Bodies Rigid bodies have boh a posiion and

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

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

On Gronwall s Type Integral Inequalities with Singular Kernels

On Gronwall s Type Integral Inequalities with Singular Kernels Filoma 31:4 (217), 141 149 DOI 1.2298/FIL17441A Published by Faculy of Sciences and Mahemaics, Universiy of Niš, Serbia Available a: hp://www.pmf.ni.ac.rs/filoma On Gronwall s Type Inegral Inequaliies

More information

ψ(t) = V x (0)V x (t)

ψ(t) = V x (0)V x (t) .93 Home Work Se No. (Professor Sow-Hsin Chen Spring Term 5. Due March 7, 5. This problem concerns calculaions of analyical expressions for he self-inermediae scaering funcion (ISF of he es paricle in

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

Class Meeting # 10: Introduction to the Wave Equation

Class Meeting # 10: Introduction to the Wave Equation MATH 8.5 COURSE NOTES - CLASS MEETING # 0 8.5 Inroducion o PDEs, Fall 0 Professor: Jared Speck Class Meeing # 0: Inroducion o he Wave Equaion. Wha is he wave equaion? The sandard wave equaion for a funcion

More information

Properties Of Solutions To A Generalized Liénard Equation With Forcing Term

Properties Of Solutions To A Generalized Liénard Equation With Forcing Term Applied Mahemaics E-Noes, 8(28), 4-44 c ISSN 67-25 Available free a mirror sies of hp://www.mah.nhu.edu.w/ amen/ Properies Of Soluions To A Generalized Liénard Equaion Wih Forcing Term Allan Kroopnick

More information

( ) = b n ( t) n " (2.111) or a system with many states to be considered, solving these equations isn t. = k U I ( t,t 0 )! ( t 0 ) (2.

( ) = b n ( t) n  (2.111) or a system with many states to be considered, solving these equations isn t. = k U I ( t,t 0 )! ( t 0 ) (2. Andrei Tokmakoff, MIT Deparmen of Chemisry, 3/14/007-6.4 PERTURBATION THEORY Given a Hamilonian H = H 0 + V where we know he eigenkes for H 0 : H 0 n = E n n, we can calculae he evoluion of he wavefuncion

More information

The Buck Resonant Converter

The Buck Resonant Converter EE646 Pwer Elecrnics Chaper 6 ecure Dr. Sam Abdel-Rahman The Buck Resnan Cnverer Replacg he swich by he resnan-ype swich, ba a quasi-resnan PWM buck cnverer can be shwn ha here are fur mdes f pera under

More information

Lecture 1 Overview. course mechanics. outline & topics. what is a linear dynamical system? why study linear systems? some examples

Lecture 1 Overview. course mechanics. outline & topics. what is a linear dynamical system? why study linear systems? some examples EE263 Auumn 27-8 Sephen Boyd Lecure 1 Overview course mechanics ouline & opics wha is a linear dynamical sysem? why sudy linear sysems? some examples 1 1 Course mechanics all class info, lecures, homeworks,

More information

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

Physics Courseware Physics I Constant Acceleration

Physics Courseware Physics I Constant Acceleration Physics Curseware Physics I Cnsan Accelerain Equains fr cnsan accelerain in dimensin x + a + a + ax + x Prblem.- In he 00-m race an ahlee acceleraes unifrmly frm res his p speed f 0m/s in he firs x5m as

More information

Revelation of Soft-Switching Operation for Isolated DC to Single-phase AC Converter with Power Decoupling

Revelation of Soft-Switching Operation for Isolated DC to Single-phase AC Converter with Power Decoupling Revelain f Sf-Swiching Operain fr Islaed DC Single-phase AC Cnverer wih wer Decupling Nagisa Takaka, Jun-ichi Ih Dep. f Elecrical Engineering Nagaka Universiy f Technlgy Nagaka, Niigaa, Japan nakaka@sn.nagakau.ac.jp,

More information

AN OPTIMAL CONTROL PROBLEM FOR SPLINES ASSOCIATED TO LINEAR DIFFERENTIAL OPERATORS

AN OPTIMAL CONTROL PROBLEM FOR SPLINES ASSOCIATED TO LINEAR DIFFERENTIAL OPERATORS CONTROLO 6 7h Poruguese Conference on Auomaic Conrol Insiuo Superior Técnico, Lisboa, Porugal Sepember -3, 6 AN OPTIMAL CONTROL PROBLEM FOR SPLINES ASSOCIATED TO LINEAR DIFFERENTIAL OPERATORS Rui C. Rodrigues,

More information

Chapter #1 EEE8013 EEE3001. Linear Controller Design and State Space Analysis

Chapter #1 EEE8013 EEE3001. Linear Controller Design and State Space Analysis Chaper EEE83 EEE3 Chaper # EEE83 EEE3 Linear Conroller Design and Sae Space Analysis Ordinary Differenial Equaions.... Inroducion.... Firs Order ODEs... 3. Second Order ODEs... 7 3. General Maerial...

More information

h[n] is the impulse response of the discrete-time system:

h[n] is the impulse response of the discrete-time system: Definiion Examples Properies Memory Inveribiliy Causaliy Sabiliy Time Invariance Lineariy Sysems Fundamenals Overview Definiion of a Sysem x() h() y() x[n] h[n] Sysem: a process in which inpu signals are

More information

ADDITIONAL PROBLEMS (a) Find the Fourier transform of the half-cosine pulse shown in Fig. 2.40(a). Additional Problems 91

ADDITIONAL PROBLEMS (a) Find the Fourier transform of the half-cosine pulse shown in Fig. 2.40(a). Additional Problems 91 ddiional Problems 9 n inverse relaionship exiss beween he ime-domain and freuency-domain descripions of a signal. Whenever an operaion is performed on he waveform of a signal in he ime domain, a corresponding

More information