Fractional Order Disturbance Observer based Robust Control
|
|
- Mark Joseph
- 5 years ago
- Views:
Transcription
1 201 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 2 and Dr. Shailaja Kurde 3 1 Deparmen f Elecrical Engineering, Cllege f Engineering Pune, India, 2 PEIM, CME, Pune and PhD Suden a Cllege f Engineering Pune, India, 3 Deparmen f Elecrical Engineering, Cllege f Engg, Pune, India 1 aamujumdar@yah.cm, 2 Cbhagyashri@yah.c.in, 3 srk.elec@cep.ac.in Absrac: Cnrl under heavy uncerain cndiins is ne f he ms impran cnrl prblems in ineger as well as fracinal rder sysems. This paper invesigaes a fracinal rder disurbance bserver based n full sae infrmain. This wrk is he exensin f ineger rder disurbance bserver in 111 fracinal dmain. An exra cmpensar based n esimaed disurbance is added he classical sae feedback cnrl. Effeciveness f he prpsed scheme is illusraed by simulain resuls. I. INTRODUCTION Advanced cnrl echniques are researched and being applied fr varius plans encmpassing indusrial cnrl space echnlgy. These advanced cnrl mechanisms are being sudied by researchers wih an bjecive prvide rbus and precise perfrmance wih pimum cnrl effrs. T achieve his aim, rbus cnrl echniques like H CXJ cnrl, feedback linearizain, sliding mde cnrl ec. are being researched since las few decades. Anher apprach which has evlved fr rbus cnrl is esimain f disurbances in he sysem and heir cmpensain. Tha is a signal represening he disurbance and uncerainy is apprximaed and cmprmised by deducing in he cnrl inpu. Varius appraches like unknwn inpu bserver (UIO), perurbain bserver (PO), disurbance bserver ( O), exended sae bserver (ESO), ime delay cnrl (TDC), uncerainy and disurbance esimar (UDE) ec. have been invesigaed ver he years fr disurbance and uncerainy esimain. Ample research is being carried u by varius researchers in mdifying and implemening hese mehdlgies. The disurbance esimain apprach is used nly fr disurbance rejecin, and he verall perfrmance f he clsed lp sysem depends n he nminal cnrl. Therefre, he implemenain f cnrl requires w lps in which he inner lp is jus esimae f he disurbance and he uer lp f cnrl cnains he nminal cnrl which is required achieve he desired perfrmance f he sysem. Fracinal calculus is a name fr he hery f inegrals and derivaives f nn-ineger rders. I suggess a paradigm shif frm ineger rder varians fracinal nes [2], [3], [4]. Fracinal calculus finds is majr applicain in cnrl dmain []. I has been prved ha fracinal calculus describes mdel mre accuraely han he ineger cunerpar. Wih he develpmen f fracinal calculus, i is bserved ha fracinal differenial equains can describe memry and geneic characerisics mre accuraely. In fac he dynamics f ms f he physical plans are msly fracinal, alhugh fr many f hem he fracinaliy is very lw. Ineger perars f cnveninal cnrl sraegies like PID, fuzzy, neural ec have als been replaced using fracinal varians enhancing he scpe f cnrl hery. Nw sliding mde cnrl (SMC) is als exended using fracinal calculus uilizing advanages f bh he heries. Fracinal mdeling f sysems has necessiaed he implemenain f esimain appraches using fracinal heries. Mahemaical mdels in fracinal dmain have differenial equains f fracinal rder. Hence, ineger rder disurbance esimain appraches cann be used fr fracinal mdels direcly. They require sme mdificains. The basic disurbance bserver which invlves mahemaical inversin f he plan mdel alng wih a filer has been mdified in [6] sui fracinal dmain apprach. The fracinal disurbance bserver design became n lnger cnservaive, i.e., given he cuff frequency and he desired phase margin, he fracinal rder f he lw pass filer culd be deermined. This fracinal rder disurbance bserver is based n he fracinal rder Q filer. This design has been applied fr cerain applicain like vibrain suppressin in w ineria sysem [7], rbus grinding mill cnrl [8] ec. This DO esimaes mached perurbains and uncerainies. A fracinal disurbance bserver has been prpsed in discree dmain in [9]. Sabiliy analysis f fracinal sysems is similar ineger rder sysems. The exensins f cnveninal sabiliy mehds like Lyapunv analysis have been exended in fracinal dmain [] [11] [12] ec. A nnlinear exensin f DO has been prpsed by W.H. Chen e. al which esimaes sysem uncerainies and disurbances [1] [13]. The scheme f nnlinear DO (NLDO) has been sudied fr varius applicains by many researchers fr linear, nnlinear sysems. In his paper, a fracinal disurbance bserver (FDO) n he lines f [1] is prpsed esimae mached disurbances in sysems. This esimaed disurbance is used deliver a rbus sae feedback cnrl. Sabiliy f he prpsed bserver is esablished using fracinal exensin /1/$ IEEE 1412
2 f Lyapunv mehd. A. Srucure f Paper Sme preliminaries and definiins f fracinal calculus are given in he nex secin. Secin 3 describes he fracinal disurbance bserver alng wih is sabiliy prf. Simulain resuls are given in Secin 4 and Secin cncludes he sudy. II. PRELIMINARIES AND DEFINITIONS OF FRACTIONAL CALCULUS Fracinal calculus uses nn-ineger rders f derivaives and inegrains. Many definiins f hese fracinal rder (FO) derivaives are fund in he lieraure, bu he cmmnly used definiins which are used in engineering applicains are given belw. A. Definiins f FO inegrain and derivaive 1) Riemann Liuville fracinal rder inegrain(rlfi): RLFI f a funcin f () can be deermined using Cauchy's clsed frm fr successive inegrain as Ja f() r a) J ( - T) (,,- l ) f(t)dt (1) where J represens inegrain perar, a E lr+ and rc) is he Eulers gamma funcin defined as 00 r(a) J e- a-1d 2) Definiin f Capu fracinal derivaives (CFD): Capu Derivaive Df wih rder a f a funcin f () is deermined as D"f() e Jm _ dm f() a dm (rn - 1) -s: a < rn, where m is an ineger and a is a real number. D represens differeniain perar. In rder find he ah derivaive using CFD, firs funcin is differeniaed by rnh rder and hen i is (rn - a) fld inegraed. Frm (I) and (2), CFD can be expressed as ed f() (2) 1 j' ( ) m-,,- l dm - T f () T dt r.( Tn - a ) -d m 3) Definiin f Riemann Liuville fracinal derivaive (RLFD): RLFD Df wih rder a f a funcin f() is deermined as dm (Jm-a f()) RL Daj'() (3) dm In rder find he ah derivaive using RLFD, iniially he funcin is (rn - a) fld inegraed and hen i is differeniaed by rnh rder. Frm (1) and (3), RLFD can be expressed as B. The Laplace ransfrm The Laplace ransfrm f he abve menined definiins are given as 1) L[Ja f()] s-a F(s) m- l 2) L[RLDf f()] sa F(s) - L: sk [RD -k- l f()] k l m- l 3) L[eDf f()] sa F(s) - L: s,,-k- l f(k )(O) k l The iniial cndiin arising in case f RLFD is n physical (value f RLFI a O) s RLFD definiin has limiains in erms f is applicains in mdeling. In case f Capu FD, he iniial cndiins have physical meanings eg f(o), j(o) ec. Hence his definiin is mre ppular amng physiciss and engineers. C. Fracinal exensin f Lyapunv Mehd The fracinal rder exensin f Lyapunv direc mehd [] is given as; Le x 0 be an equilibrium pin fr he nn-aunmus fracinal rder sysem. Assume here exiss a Lyapunv funcin V(, x) and class-k funcins Ii, i 1,2,3 saisfying Il(llxll) -s: V(, x) -s: 12 (llxll), DaV(, x) -s: 13 (llxll) (4) where a E (0,1). Then he sysem is asympically sable. III. FRACTIONAL ORDER DISTURBANCE OBSERVER Cnsider dynamics fr a secnd rder fracinal sysem; D"x y() f(x) + gl(x)u + g2(x)d() h(x) Here x is he sae vecr, U is cnrl inpu, d( ) is inpu channel disurbance and y is he upu. f(x),gl(x),g2(x) are he sae funcins. Assumpin: The disurbance d() is cninuus and bunded hence saisfies fr a E (0,1). Here fl is a psiive number. The fracinal disurbance bserver (FDO) fr () is prpsed as; d() Lx() - z() Daz() L(f(x) + gl(x)u + g2(x)d()) Here z is he inernal sae f FDO, L is he bserver gain. Le he errr in disurbance esimain be cnsidered as, e() d- } } () (6) 1413
3 d. The errr dynamics can be derived by aking ah derivaive A. Esimain f Disurbances and subsiuing he FDO dynamics, Dae() A. Sabiliy Analysis Dad- Dad Dad - Da(Lx() - z()) Dad - L(f(x) + gl(x)u + g2(x)d()) +L(f(x) + gl(x)u + g2(x)d()) Dae() Dad - Lg2(X)(d - d) The bserver gain is be chsen such ha he errr dynamics (7) are sable. T analyze he sabiliy, fracinal rder exensin f Lyapunv direc mehd (4) is be used. Cnsider a psiive definie Lyapunv funcin V ( e) e 2. Is ah derivaive is given as per Leibniz rule f fracinal differeniain [II] as fllws, (7) (8) This sysem was simulaed fllw a delayed uni sep cmmand a ime O.1 sec. The sysem is cnrlled using an sae feedback cnrller wih desired ple lcains a -4. and -.3. The prpsed fracinal disurbance bserver can handle a large class f disurbances such as cnsan, sinusidal r sae dependen disurbances. The simulain sudy fr hese disurbances is as shwn belw; Cnsan Disurbance A cnsan signal d 0. 6 was given as disurbance he sysem. Figure 1 shws he pls f acual and esimaed disurbance alng wih is esimain errr. where r(l + a) P f DkeDa-ke. e k r(l+k)r(l -k+a) l I is assumed ha he fllwing inequaliy hlds where N is a psiive number []. Therefre, subsiuing (7) in he Lyapunv funcin, DaV Taking inequaliy, e(dad - Lg2(X)(d - d)) + Nlel e(mlldll - Lg2(x)e) + Nlel w 0.6f.,.: i i c Therefre, as , he esimain errr is bunded by, (9) Thus, wih a prper chice f gain L, he asympic cnvergence f he errr he bunds f he ah derivaive f disurbance can be ensured. IV. SIMULATION RESULTS Cnsider a linear secnd rder fracinal sysem as fllws, Dax Ax + bu + ed () Fig. I: Disurbance Esimain using FDO where, A [ ] b [ ] e [ ] y [ [ ] (I I) d is he added mached disurbance in he sysem (). Sinusidal Disurbance A disurbance signal d 0. sin(w), frequency1.hz was given he sysem. Figure 2 shws he w pls. 1414
4 b is he scaling facr; here b Using his cnrl he sysem was simulaed wih a grwing disurbance d 0. sin(w) + /6, frequency1.hz. The perfrmance f he sysem using cmpensain wih disurbance esimain is shwn belw. Figure 4 shws he evluin f he saes wih and wihu cmpensain and Figure shws he crrespnding cnrl inpus. Fig. 2: Disurbance Esimain using FDO Sae dependen Disurbance A disurbance signal d 0. sin(w)x, frequencyi.hz was given he sysem and he esimain f his signal is shwn in Figure 3. Fig. 4: Evluin f saes W Fig. 3: Disurbance Esimain using FDO B. Rbus sae fe edback cnrl I was bserved ha he saes f he sysem were perurbed n addiin f disurbance in he inpu channel. Hence he cnrl was augmened include he knwledge f disurbance in i. The mdified cnrl is Fig. : Cnrl inpu U ue q + Un where ue q is he equivalen cnrl designed fr nminal sysem (i.e. he sae feedback cnrller) and Un - -b1 d. The esimaed and acual disurbance is shwn in Figure
5 [12] H. Ahn, Y. Chen, and 1. Pdlubny, "Rbus sabiliy es f a class f linear ime-invarian inerval fracinal-rder sysem using lyapunv inequaliy," Science Direc, [13] W.-H.Chen, "Disurbance bserver based cnrl fr nnlinear sysems," IEEEIASME Transacins n Mecharnics, vl. 9, December Fig. 6: Disurbance Esimain using FDO I is clearly seen frm he figures ha cmpensain f he mached disurbance is achieved using he mdified cnrl law based n FDO. V. CONCLUSION A fracinal disurbance bserver is prpsed in his paper alng wih is sabiliy analysis. This FDO has been used esimae he uncerainies and perurbains f a fracinal rder sysem which is laer used augmen he cnrl law. This mdified sae feedback cnrl shws rbusness mached disurbances when cmpared wih is simple cunerpar. Simulain resuls are included suppr he sudy. I is fund ha he FDO can handle a large class f mached disurbances. Thus i can be bserved ha a FDO alng wih cnveninal cnrl sraegies can render rbusness a large class f fracinal rder sysems. REFERENCES [1] W.-H.Chen, D. Balance, P.J.Gawhrp, J. Gribble, and J.O'Reilly, "Nnlinear pid predicive cnrller," lee Prc.-Cnrl TheOlY Appl., vl. 146, Nvember [2] D. C. A. Mnje, D. Y. Chen, and D. B. M. Vinagre, Fracinal-rder Sysems and Cnrls. Springer, 20. [3] S. Das, Funcinal Fracinal Calculus fr Sysem Idenificain and Cnrls. Springer, [4] 1. Pdlubny, Fracinal Di ferenial Equains. Academic Press, 1999, vl [] B. Bandypadhyay and S. Kamal, Sabilizain and Cnrl f Fracinal Order Sysems : ASliding Mde Apprach. Springer Inernainal Publishing, 201. [6] Y. Chen, B. M. Vinagre, and 1. Pdlubny, "Fracinal rder disurbance bserver fr rbus vibrain suppressin," Nnlinear Dynamics, vl. 38, p. 3367, [7] w. Li and Y. Hri, "Vibrain suppressin using single neurn-based pi fuzzy cnrller and fracinal-rder disurbance bserver," Indusrial Elecrnics, IEEE 7)'ansacins n, vl. 4, n. I, pp , Feb [8] L. E. Olivier, 1. K. Craig, and Y. Chen, "Fracinal rder disurbance bserver fr a run-f-mine re milling circui," in IEEE A}i"icn, Sepember [9] S. Kamal and B. Bandypadhyay, "Rbus cnrller design fr discree racinal rder sysem: A disurbance bserver based apprach," in ACODS, Sepember [] Y. Li, Y. Chen, and 1. Pdlubny, "Sabiliy f fracinal-rder nnlinear dynamic sysems: Lyapunv direc mehd and generalized miag-ieffier sabiliy," Elsevier: Cmpuers and Mahemaics wih Applicains, 20. [11] M. O. Efe, "Fracinal fuzzy adapive sliding-mde cnrl f a 2- df direc-drive rb ann," IEEE 7)'ansacins n sysems, man, and cyberneics, Decemeber
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 informationBrace-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 information10.7 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 informationUnit-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 informationStability of the SDDRE based Estimator for Stochastic Nonlinear System
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.;
More informationNumerical 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 informationProductivity 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 information5.1 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 informationAn 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 informationSliding Mode Control: An Approach To Regulate Nonlinear Chemical Processes
Sliding Mde Cnrl: An Apprach T Regulae Nnlinear Chemical rcesses Oscar Camach Deparamen de Circuis y Medidas Universidad de Ls Andes Mérida 5. Venezuela Carls A. Smih Chemical Engineering Deparmen Universiy
More informationAP 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 informationRevelation 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 informationThe 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 informationEfficient 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 informationTHE 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 informationVisco-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 informationConvex 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 informationPRINCE 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 informationThe 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 informationGMM 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 informationLecture 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 informationDelay-Dependent Robust Stability and Control of Uncertain Discrete Singular Systems with State-Delay
Jurnal Mahemaical Cnrl Science an Applicains (JMCSA) Vl. 1 N. 1 (January-June, Vl. 1 N. 1 (January-June, 215), ISSN 215) : 974-57 ISSN Jurnal : 974-57 Mahemaical Cnrl Science an Applicains (JMCSA) Vl.
More informationThe 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 informationMotion 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 informationKinematics 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 informationCoherent 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 informationA 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 information20th Iranian Conference on Electrical Engineering, (ICEE2012), May 15-17, Tehran, Iran. T-S Fuzzy Model
20h Iranian Cnference n Elecrical Engineering, (ICEE2012), May 15-17, ehran, Iran Speed and rque Cnrl f Inducin Mr by Using Rbus R Mixed-Sensiiviy Prblem Via Vahid Azimi 1 Elecrical Engineering Deparmen
More informationOptimization of Four-Button BPM Configuration for Small-Gap Beam Chambers
Opimizain f Fur-Bun BPM Cnfigurain fr Small-Gap Beam Chamers S. H. Kim Advanced Phn Surce Argnne Nainal Larary 9700 Suh Cass Avenue Argnne, Illinis 60439 USA Asrac. The cnfigurain f fur-un eam psiin mnirs
More informationMicrowave 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 informationSTATE-SPACE MODELLING. A mass balance across the tank gives:
B. Lennox and N.F. Thornhill, 9, Sae Space Modelling, IChemE Process Managemen and Conrol Subjec Group Newsleer STE-SPACE MODELLING Inroducion: Over he pas decade or so here has been an ever increasing
More informationAn 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 informationAnti-Disturbance Control for Multiple Disturbances
Workshop a 3 ACC Ani-Disurbance Conrol for Muliple Disurbances Lei Guo (lguo@buaa.edu.cn) Naional Key Laboraory on Science and Technology on Aircraf Conrol, Beihang Universiy, Beijing, 9, P.R. China. Presened
More informationLecture 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 informationON 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 informationFinite 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 informationSection 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 informationPHY305F Electronics Laboratory I. Section 2. AC Circuit Basics: Passive and Linear Components and Circuits. Basic Concepts
PHY305F Elecrnics abrary I Secin ircui Basics: Passie and inear mpnens and ircuis Basic nceps lernaing curren () circui analysis deals wih (sinusidally) ime-arying curren and lage signals whse ime aerage
More informationA DELAY-DEPENDENT STABILITY CRITERIA FOR T-S FUZZY SYSTEM WITH TIME-DELAYS
A DELAY-DEPENDENT STABILITY CRITERIA FOR T-S FUZZY SYSTEM WITH TIME-DELAYS Xinping Guan ;1 Fenglei Li Cailian Chen Insiue of Elecrical Engineering, Yanshan Universiy, Qinhuangdao, 066004, China. Deparmen
More informationGAMS 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 informationSuccessive 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 informationDISTANCE PROTECTION OF HVDC TRANSMISSION LINE WITH NOVEL FAULT LOCATION TECHNIQUE
IJRET: Inernainal Jurnal f Research in Engineering and Technlgy eissn: 9-6 pissn: -78 DISTANCE PROTECTION OF HVDC TRANSMISSION LINE WITH NOVEL FAULT LOCATION TECHNIQUE Ruchia Nale, P. Suresh Babu Suden,
More informationPhysics 111. Exam #1. September 28, 2018
Physics xam # Sepember 8, 08 ame Please read and fllw hese insrucins carefully: Read all prblems carefully befre aemping slve hem. Yur wrk mus be legible, and he rganizain clear. Yu mus shw all wrk, including
More informationLecture 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( ) ( ) 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 informationImpact 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 informationCHAPTER 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 informationShandong Qingdao , China. Shandong Qingdao, , China
2016 Inernainal Cnference n Maerials, Manufacuring and Mechanical Engineering (MMME 2016) ISB: 978-1-60595-413-4 Min Cnrl Sysem f C Turre Punch Feeding Mechanism Based n Min Cnrl Card Ai-xia CAO 1, Pei-si
More informationRamsey 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 informationEECE 301 Signals & Systems Prof. Mark Fowler
EECE 31 Signals & Sysems Prof. Mark Fowler Noe Se #1 C-T Sysems: Convoluion Represenaion Reading Assignmen: Secion 2.6 of Kamen and Heck 1/11 Course Flow Diagram The arrows here show concepual flow beween
More informationPASSIVE PFC FOR FLYBACK CONVERTORS
PASSIE PFC FOR FLYBACK COERORS Parviz Par and Keyue M Sedley Dep f Elecrical and Cpuer Engineering Universiy f Califrnia, Irvine Irvine, Califrnia 9697 Absrac A new passive Pwer Facr Crrecr (PFC) based
More informationPhysics 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 informationChapter 8 The Complete Response of RL and RC Circuits
Chaper 8 The Complee Response of RL and RC Circuis Seoul Naional Universiy Deparmen of Elecrical and Compuer Engineering Wha is Firs Order Circuis? Circuis ha conain only one inducor or only one capacior
More informationRAPIDLY 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 informationChapter 5 Digital PID control algorithm. Hesheng Wang Department of Automation,SJTU 2016,03
Chaper 5 Digial PID conrol algorihm Hesheng Wang Deparmen of Auomaion,SJTU 216,3 Ouline Absrac Quasi-coninuous PID conrol algorihm Improvemen of sandard PID algorihm Choosing parameer of PID regulaor Brief
More informationChapter 2. First Order Scalar Equations
Chaper. Firs Order Scalar Equaions We sar our sudy of differenial equaions in he same way he pioneers in his field did. We show paricular echniques o solve paricular ypes of firs order differenial equaions.
More informationLyapunov 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 informationMATH 128A, SUMMER 2009, FINAL EXAM SOLUTION
MATH 28A, SUMME 2009, FINAL EXAM SOLUTION BENJAMIN JOHNSON () (8 poins) [Lagrange Inerpolaion] (a) (4 poins) Le f be a funcion defined a some real numbers x 0,..., x n. Give a defining equaion for he Lagrange
More informationON STABILITY OF CONTROLLED SYSTEMS IN BANACH SPACES. M. Megan, Timi~oara, Romania. 1. Introduction
GLASNIK MATEMATICKI Vl. 18 (38) (1983), 187-201. ON STABILITY OF CONTROLLED SYSTEMS IN BANACH SPACES M. Megan, Timi~ara, Rmania Absrac. In his paper we sudy sabiliy prperies fr linear sysems, he evluin
More informationSliding Mode Controller for Unstable Systems
S. SIVARAMAKRISHNAN e al., Sliding Mode Conroller for Unsable Sysems, Chem. Biochem. Eng. Q. 22 (1) 41 47 (28) 41 Sliding Mode Conroller for Unsable Sysems S. Sivaramakrishnan, A. K. Tangirala, and M.
More informationEECE 301 Signals & Systems Prof. Mark Fowler
EECE 3 Signals & Sysems Prof. Mark Fowler Noe Se #2 Wha are Coninuous-Time Signals??? Reading Assignmen: Secion. of Kamen and Heck /22 Course Flow Diagram The arrows here show concepual flow beween ideas.
More informationand 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 informationFractional Method of Characteristics for Fractional Partial Differential Equations
Fracional Mehod of Characerisics for Fracional Parial Differenial Equaions Guo-cheng Wu* Modern Teile Insiue, Donghua Universiy, 188 Yan-an ilu Road, Shanghai 51, PR China Absrac The mehod of characerisics
More informationRC, RL and RLC circuits
Name Dae Time o Complee h m Parner Course/ Secion / Grade RC, RL and RLC circuis Inroducion In his experimen we will invesigae he behavior of circuis conaining combinaions of resisors, capaciors, and inducors.
More informationNotes 04 largely plagiarized by %khc
Noes 04 largely plagiarized by %khc Convoluion Recap Some ricks: x() () =x() x() (, 0 )=x(, 0 ) R ț x() u() = x( )d x() () =ẋ() This hen ells us ha an inegraor has impulse response h() =u(), and ha a differeniaor
More informationd 1 = c 1 b 2 - b 1 c 2 d 2 = c 1 b 3 - b 1 c 3
and d = c b - b c c d = c b - b c c This process is coninued unil he nh row has been compleed. The complee array of coefficiens is riangular. Noe ha in developing he array an enire row may be divided or
More informationEmbedded Systems and Software. A Simple Introduction to Embedded Control Systems (PID Control)
Embedded Sysems and Sofware A Simple Inroducion o Embedded Conrol Sysems (PID Conrol) Embedded Sysems and Sofware, ECE:3360. The Universiy of Iowa, 2016 Slide 1 Acknowledgemens The maerial in his lecure
More informationClass 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 informationthe results to larger systems due to prop'erties of the projection algorithm. First, the number of hidden nodes must
M.E. Aggune, M.J. Dambrg, M.A. El-Sharkawi, R.J. Marks II and L.E. Atlas, "Dynamic and static security assessment f pwer systems using artificial neural netwrks", Prceedings f the NSF Wrkshp n Applicatins
More informationDynamic Effects of Feedback Control!
Dynamic Effecs of Feedback Conrol! Rober Sengel! Roboics and Inelligen Sysems MAE 345, Princeon Universiy, 2017 Inner, Middle, and Ouer Feedback Conrol Loops Sep Response of Linear, Time- Invarian (LTI)
More informationindependenly 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 informationDriver Phase Correlated Fluctuations in the Rotation of a Strongly Driven Quantum Bit
[acceped fr PRA Rapid Cmm; quan-ph/] Driver Phase Crrelaed Flucuains in he Rain f a Srngly Driven Quanum Bi M.S. Shahriar,, P. Pradhan,, and J. Mrzinski Dep. f Elecrical and Cmpuer Engineering, Nrhwesern
More informationContinuous Time. Time-Domain System Analysis. Impulse Response. Impulse Response. Impulse Response. Impulse Response. ( t) + b 0.
Time-Domain Sysem Analysis Coninuous Time. J. Robers - All Righs Reserved. Edied by Dr. Rober Akl 1. J. Robers - All Righs Reserved. Edied by Dr. Rober Akl 2 Le a sysem be described by a 2 y ( ) + a 1
More informationSimulation-Solving Dynamic Models ABE 5646 Week 2, Spring 2010
Simulaion-Solving Dynamic Models ABE 5646 Week 2, Spring 2010 Week Descripion Reading Maerial 2 Compuer Simulaion of Dynamic Models Finie Difference, coninuous saes, discree ime Simple Mehods Euler Trapezoid
More informationStability and Bifurcation in a Neural Network Model with Two Delays
Inernaional Mahemaical Forum, Vol. 6, 11, no. 35, 175-1731 Sabiliy and Bifurcaion in a Neural Nework Model wih Two Delays GuangPing Hu and XiaoLing Li School of Mahemaics and Physics, Nanjing Universiy
More informationLAPLACE TRANSFORM AND TRANSFER FUNCTION
CHBE320 LECTURE V LAPLACE TRANSFORM AND TRANSFER FUNCTION Professor Dae Ryook Yang Spring 2018 Dep. of Chemical and Biological Engineering 5-1 Road Map of he Lecure V Laplace Transform and Transfer funcions
More informationDifferential Equations
Mah 21 (Fall 29) Differenial Equaions Soluion #3 1. Find he paricular soluion of he following differenial equaion by variaion of parameer (a) y + y = csc (b) 2 y + y y = ln, > Soluion: (a) The corresponding
More informationINFLUENCE OF WIND VELOCITY TO SUPPLY WATER TEMPERATURE IN HOUSE HEATING INSTALLATION AND HOT-WATER DISTRICT HEATING SYSTEM
Dr. Branislav Zivkvic, B. Eng. Faculy f Mechanical Engineering, Belgrade Universiy Predrag Zeknja, B. Eng. Belgrade Municipal DH Cmpany Angelina Kacar, B. Eng. Faculy f Agriculure, Belgrade Universiy INFLUENCE
More informationTHE WAVE EQUATION. part hand-in for week 9 b. Any dilation v(x, t) = u(λx, λt) of u(x, t) is also a solution (where λ is constant).
THE WAVE EQUATION 43. (S) Le u(x, ) be a soluion of he wave equaion u u xx = 0. Show ha Q43(a) (c) is a. Any ranslaion v(x, ) = u(x + x 0, + 0 ) of u(x, ) is also a soluion (where x 0, 0 are consans).
More informationAnswers: ( 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 information6.302 Feedback Systems Recitation 4: Complex Variables and the s-plane Prof. Joel L. Dawson
Number 1 quesion: Why deal wih imaginary and complex numbers a all? One answer is ha, as an analyical echnique, hey make our lives easier. Consider passing a cosine hrough an LTI filer wih impulse response
More informationSOLUTIONS TO ECE 3084
SOLUTIONS TO ECE 384 PROBLEM 2.. For each sysem below, specify wheher or no i is: (i) memoryless; (ii) causal; (iii) inverible; (iv) linear; (v) ime invarian; Explain your reasoning. If he propery is no
More informationTesting 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 informationResearch & 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 informationMath 334 Fall 2011 Homework 11 Solutions
Dec. 2, 2 Mah 334 Fall 2 Homework Soluions Basic Problem. Transform he following iniial value problem ino an iniial value problem for a sysem: u + p()u + q() u g(), u() u, u () v. () Soluion. Le v u. Then
More informationa. (1) Assume T = 20 ºC = 293 K. Apply Equation 2.22 to find the resistivity of the brass in the disk with
Aignmen #5 EE7 / Fall 0 / Aignmen Sluin.7 hermal cnducin Cnider bra ally wih an X amic fracin f Zn. Since Zn addiin increae he number f cnducin elecrn, we have cale he final ally reiiviy calculaed frm
More informationULTRAFAST TIME DOMAIN OPTICS OF SINGLE-CYCLE LASER PULSE INTERACTION WITH MATERIALS
Universiy f Nebraska - Lincln DigialCmmns@Universiy f Nebraska - Lincln Theses, Disserains, and Suden Research frm Elecrical & Cmpuer Engineering Elecrical & Cmpuer Engineering, Deparmen f 1-010 ULTRAFAST
More informationCIRCUITS AND ELECTRONICS. Op Amps Positive Feedback
6.00 CIRCUITS AND ELECTRONICS Op Amps Psiie Feedback Cie as: Anan Agarwal and Jeffrey Lang, curse maerials fr 6.00 Circuis and Elecrnics, Spring 007. MIT OpenCurseWare (hp://cw.mi.edu/), Massachuses Insiue
More informationMath 23 Spring Differential Equations. Final Exam Due Date: Tuesday, June 6, 5pm
Mah Spring 6 Differenial Equaions Final Exam Due Dae: Tuesday, June 6, 5pm Your name (please prin): Insrucions: This is an open book, open noes exam. You are free o use a calculaor or compuer o check your
More informationSystem Processes input signal (excitation) and produces output signal (response)
Signal A funcion of ime Sysem Processes inpu signal (exciaion) and produces oupu signal (response) Exciaion Inpu Sysem Oupu Response 1. Types of signals 2. Going from analog o digial world 3. An example
More informationdi Bernardo, M. (1995). A purely adaptive controller to synchronize and control chaotic systems.
di ernardo, M. (995). A purely adapive conroller o synchronize and conrol chaoic sysems. hps://doi.org/.6/375-96(96)8-x Early version, also known as pre-prin Link o published version (if available):.6/375-96(96)8-x
More informationIndex-based Most Similar Trajectory Search
Index-based Ms Similar rajecry Search Elias Frenzs Ksas Grasias Yannis hedridis ep. f Infrmaics, Universiy f Piraeus, Greece ep. f Infrmaics, Universiy f Piraeus, Greece ep. f Infrmaics, Universiy f Piraeus,
More informationSliding Mode Extremum Seeking Control for Linear Quadratic Dynamic Game
Sliding Mode Exremum Seeking Conrol for Linear Quadraic Dynamic Game Yaodong Pan and Ümi Özgüner ITS Research Group, AIST Tsukuba Eas Namiki --, Tsukuba-shi,Ibaraki-ken 5-856, Japan e-mail: pan.yaodong@ais.go.jp
More information6.2 Transforms of Derivatives and Integrals.
SEC. 6.2 Transforms of Derivaives and Inegrals. ODEs 2 3 33 39 23. Change of scale. If l( f ()) F(s) and c is any 33 45 APPLICATION OF s-shifting posiive consan, show ha l( f (c)) F(s>c)>c (Hin: In Probs.
More informationOrdinary Differential Equations
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 informationt 2 B F x,t n dsdt t u x,t dxdt
Evoluion Equaions For 0, fixed, le U U0, where U denoes a bounded open se in R n.suppose ha U is filled wih a maerial in which a conaminan is being ranspored by various means including diffusion and convecion.
More informationAn 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 informationNotes on Kalman Filtering
Noes on Kalman Filering Brian Borchers and Rick Aser November 7, Inroducion Daa Assimilaion is he problem of merging model predicions wih acual measuremens of a sysem o produce an opimal esimae of he curren
More informationSome Basic Information about M-S-D Systems
Some Basic Informaion abou M-S-D Sysems 1 Inroducion We wan o give some summary of he facs concerning unforced (homogeneous) and forced (non-homogeneous) models for linear oscillaors governed by second-order,
More informationLinear Time-invariant systems, Convolution, and Cross-correlation
Linear Time-invarian sysems, Convoluion, and Cross-correlaion (1) Linear Time-invarian (LTI) sysem A sysem akes in an inpu funcion and reurns an oupu funcion. x() T y() Inpu Sysem Oupu y() = T[x()] An
More information