Discrete Time Linear Quadratic Optimal Control for an Electrical Servo Drive System

Size: px
Start display at page:

Download "Discrete Time Linear Quadratic Optimal Control for an Electrical Servo Drive System"

Transcription

1 Discrete ime Linear Quaratic Optimal Control or an Electrical Servo Drive System CORNELIU BOAN, FLORIN OSAFI an ALEXANDRU ONEA Dept. o Automatic Control an Inustrial Inormatics Gh. Asachi echnical University o Iasi B. D. Mangeron 53A ROMANIA Abstract: - he iscrete-time linear quaratic optimal problem with inite inal time or a servo-rive system with a brushless or a c motor is presente. he propose algorithm allows simpliying the optimal control law implementation. he optimal control ensures a goo behavior o the system an the ecrease o the energy consumption. Key-Wors:- Optimal control, Brushless, DC machines, Eiciency, Servo rives. Introuction he optimal control o the electrical rive systems allows to obtain several avantages: the reuction o the energy consumption an, in some cases, the reuction o the rate power o the rive motor an thus the ecrease o the imensions an the weight o the system; in the same time, a goo behavior in the transient perio can be achieve. hese avantages are very important nowaays, when the aspects connecte with the prouction quality, the cost o the plants an the energy losses are consiere with priority. he paper reers to a linear servo-rive system controlle on the basis o the linear quaratic optimal (LQ) problem []. In orer to obtain a ast response, a inite inal time is impose. A servo-rive system with a c or brushless motor is consiere. A linear moel or the system is aopte: x(t) = A x(t) + B u(t) + W m(t) () c c c 3 where x(t) =θ [ ω i] is the state vector ( enotes the transposition), u(t) is the control variable, m(t) is the isturbance (loa torque), θ an ω are the angular position an spee, respectively, an a A = a a, B =, W = w () c 3 c c c a3 a 33 b 3 he elements o the matrices in () epen on the parameters o the servo-rive system (incluing motor, converter, gear an transucers) an these are: ρ Cm Ce R a = r, a =, a 3 =, a3 =, a33 =, J J L L where r is the gear constant, ρ is the viscous riction coeicient, J is the inertia, an R, L are the resistance an inuctance o the controlle circuit o the motor. For a.c. motor, i an u are the rotor current an voltage, respectively. In the case o a brushless motor (a surace mounte permanent rotor is consiere), in the q reerence rame, i=i q an u=u q represent the q-axis current an voltage, respectively. It is suppose that u is chosen so that i is very small []. Since the optimal controller must be implemente in a iscrete manner, it is useul to treat the problem in iscrete case. With the notations A c A c t A c t c c (3) A= e, B= e tb, W= e tw ( is the sampling perio), the iscrete moel o the servo-rive system is x(k + ) = Ax(k) + Bu(k) + Wm(k) (4) where x(k) = x(k), k, an similar notations are use or all other variables. he aim o the optimal control is to obtain a convenient transient response, a small error or the inal position an a reuce energy consumption.

2 he ollowing iscrete criterion is introuce or this purpose: s s J = ( θ(k ) θ ) + ( ω(k ) ω) (5) + [q ( θ(k) θ ) + q ( ω(k) ω ) + q3i(k) + pu(k) ] k = where k correspons to the inal time, s, s, q, q, q 3, p> are the weight coeicients an x [ ] = θ ω i is the esire state vector. Usually, ω = an i is ree. he irst an the secon terms in (5) penalize the inal errors o the position an o the spee, respectively. he terms containe in the sum penalize the transient errors an the great values o the current an o the control voltage; note that the presence o the term q3i(k) in the criterion ensures a small value or the issipate energy in the wening on the optimization interval [, k ]. he criterion (5) can be expresse in the general orm J= [ x(k ) x] S[ x(k ) x] x (k)qx(k) u (k)pu(k) k= (6) where S=iag(s,s, ), Q=iag(q, q, q 3 ) an P=p. he problem is to in the optimal control u(x(t)) which minimizes the criterion (6) having in view the equation (4) o the servo rive system. A similar problem but or the continuous case was stuie in [3]. here are two type o optimal control problems in connection with the inal state: the ixe enpoint problem an the ree en-point problem, respectively. In the irst one, the inal value o the state vector is impose, or instance x(k ) = x. For the other type o problems, the inal vector x(k ) is ree, but the minimization o the criterion (6) ensures that x(k ) is in the proximity o the esire value x. he ixe en-point problem ensures that the esire vector is achieve at the inal moment k an this act is very important. We have to remark that usually the optimal control law o not ensures that the system stops in x or k>k. In many applications it is suicient to arrive at a ixe moment k in a neighborhoo o x. I x must be achieve, we can change the control law (not obligatory optimal) in the last part o the traectory, ater k. he main avantage o the ree en-point problem is the act that the control variable u(k) is smaller than in the ixe en-point problem. he present paper reers to a ree en-point optimal control problem.. Main Results Using the Hamilton conitions [], the optimal control is u(k) P B (k ) = λ +, (7) n where λ(k) is the state vector that in the classical proceures is aopte as λ (k) = R(k)x(k) + v(k), (8) where the component v(k) epens on the exogenous variables x an m(t). In orer to avoi the on-line computation in inverse time the time-variant matrix R(k) as solution to a Riccati ierence matrix equation, instea o (8) one proposes to choose λ(k) as λ (k) = Rx(k) + v(k) (9) where R is a constant matrix an v(k) = v(k) + v(k) ; the corrective component v(k) ensures that the solution is the same as one obtaine i the orm (8) is aopte. Using the Hamilton equations an transversallity conitions, one obtains that R satisies the Riccati matrix algebraic equation or the iscrete case [4]: + = = () R A R(I NR) A Q, N BP B (I-the ientity matrix). In orer to establish the vector v(k), some supplementary issues must be solve, since the transversallity conitions oer only the inal value ( ) ( ) v k = (S R)x k Sx () his inal value can not be use in the real time computing an have to be replace with x(), that is beorehan known. For this purpose, the vector z(k) = x (k) v (k) is introuce. One can veriy that z(k) satisies the equation z(k + ) = Gz(k) + r(k), ()

3 where r(k) r(k) = r(k) = ENZ E Q x A REWm(k) = Z Wm(k) with Z = A (I REN) an E = (I + NR) an G G G EA ENZ = G = Z his matrix an its inverse G G A E A N G = = G Z (3) (4) (5) () = h(k) = Z r (k + ). Remark. he computation o the vector g impose to beorehan know the vector r(k), epening on exogenous variables. his act implies to know at least the shape o the loa torque m(k) an to estimate its amplitue [5] in the beginning o the optimization perio. he simplest an most requently met case or the servo-rive systems is m(k)=const. In this case, r an r have constant values in (9) an (), an the vector g in (9) is constant. Finally, rom (7), (9) an (), the optimal control can be written as * u (k) u (k) u c(k) = + () he eeback component u(k) = P BREAx(k) (3) have some useul eatures, as G G G =, with G A similar eature is obtaine or G -. From () yiels k = i i i= G = G G G (6) z(k) = G z(k ) (G ) r(k + ) (7) One obtains rom () an (7) or k= = +, (8) x(k ) M [x() g] where M= G + G (S R) an i= g= G r(i ) + G r (i ) + G Sx From () an (7) we also obtain k k v(k) Z (S R)M (x() g) Sx h(k) with (9) = +,() is ientical with one obtaine in the similar problem, but with ininite inal time. he corrective component u (k) = P B (A ) v(k) + Qx (4) c [ ] (with v(k) given by ()) epens on the initial state x() an on the exogenous variables x an m. Remark. he above relations are rather complicate, but the most part o the computation is perorme o-line, in the stage o the controller esign, when are establishe all the constant matrices. In the real time computing, only two variable elements must be compute: the vector h(k) given by () an the matrix k k Γ k = Z. he both elements can be recurrently compute: Γ =Γ Γ = h(k) h(k ) Z Z r k k Z, Z, + = = = = h() Z r, k,,...,k (5) he terms epening on x an m rom u c (k) must be compute inepenently o the use metho. he speciic term or the propose algorithm is the term epening on x() o the corrective component u c (k). his term ensures the ientity o the optimal control () with one

4 obtaine via classical proceures, base on relations (7) an (8). In this last case the time variant matrix R(k) have to be compute on-line in inverse time as a solution to a Riccati ierence matrix equation. his signiicant iiculty is avoie in the propose metho. Remark 3. Generally, the optimal control reers to a speciie time interval. Usually, the control law u * (k) must be change ater the inal time t = k so that to ensure the esire state x. In the stuie problem with ree en-point, usually x(k ) x. In orer to achieve the esire inal state, the control law is change, or instance in the orm u(k) =α( θ θ(k)) βω (k), k >, α >, β> (6) I it is necessary, a iscrete low pass ilter can be introuce in orer to avoi an abrupt change o u(k) at the moment k. 3. Simulation Results he above results were veriie by simulation. he applications are or R=3.Ω, L=.6H, Ce=.58Vs/ra, Cm=.58Nm/A, J=.8Nms /ra, r=/5, =.3s, t =.9s, θ =ra. Some simulations were perorme or ierent weight matrices in (6). Figure shows the system behavior in the case S=iag(6, 5, ), Q=iag(,, 3.), P=.6. he behavior o the system or the same parameters o the optimal controller in the case o the change o the optimal control law at the moment t (see Remark 3) is presente in the igure. One can remark that the motor runs as a brake in the last part o the optimization interval. Remark 4: It is well-know the result obtaine or the ixe en-point problem or a simple irst orer servo-rive system, where the current i(k) is consiere as control variable: the open loop optimal control i(k) has a linear variation an the spee ω(k) has a parabolic variation. he igures presente above inicate that these shapes are on the whole respecte also or the close loop optimal system in the more realistic case, when the voltage u(k) is consiere as control variable. Moreover, this aspect is vali also or the ree enpoint optimal control problem. It was stuie the eect o some ierent moiications in the control law or in the unctioning conitions: A signiicant increase o the sampling perio (up to times) only or the corrective component u c (k) o not yiel a signiicant change o the traectory. his act allows reucing o the on-line computing time. he increase o the loa torque leas to a small increase o the maximum value o the current (or instance, or the change o the loa torque rom.5 Nm up to.5 Nm, the maximum value o the current increases only with.6 A). his act shows that the most part o the electromagnetic torque o the motor ensures the acceleration o the system. he ecrease o the impose inal time leas to a signiicant increase o the current (or example, or the ecrease o the inal time t rom.9s to.5s the maximum value o the current increase by.7 times). he change (or an inaccurate estimation) o the loa torque m o not prouce a great variation rom the reerence curves o ω(k) an θ(k). his act is illustrate in the ig. 3 or the change o the loa torque rom.5 Nm up to.5 Nm at the moment k /. he energy consumption was compute in each case an compare with one obtaine in the usual cascae control case. A signiicant ecrease o the energy losses (up to 3%, epening on the weight matrices) is obtaine in the optimal control case. time[s] Fig.. he behavior o the optimal servo rive system on the optimization interval [, t ]

5 time[s] Fig.. he behavior o the optimal servo rive system or t< t an or t > t (t =.9 s) Annual Conerence o the IEEE Inustrial Electronics Society IECON 98, Aachen, 998, pp [3] C. Botan, F. Ostai, S. Dumbrava, A. Onea, Linear Quaratic Optimal Control o an Electrical Servo Drive System, Proceeings o the th International Power Electronics & Motion Control Conerence, EPE-PEMC, Cavtat & Dubrovnik,, pp. 437&CDROM. [4] C. Botan, A. Onea, Discrete-ime Optimal Control o an Electrical Drive System, Bul. Instit. Politehnic Iasi, om XLV(IL), Fasc. -4, A.C., 999, pp [5] S. Komaa, M. Ishia, K. Ohnishi,. Hori, Disturbance Observer-Base Motion Control o Direct Drive Robots, IEEE ransactions on Energy Conversion, 6(3), 99, pp time[s] Fig. 3. he eect o the change o the loa torque rom.5 Nm up to.5 Nm at the moment t=t / 4. Conclusions A new metho or the iscrete optimal control or a servo-rive system is presente. he propose algorithm can be easier implemente than in the classical proceure or the linear quaratic optimal control. he aopte criterion ensures a goo behavior or the system an a signiicant ecrease o the energy consumption. Reerences [] Brian D.O. Anerson, John B. Moore, Optimal Linear Quaratic Methos, Prentice Hall, Englewoo Clis, New Jersey, 99. [] K.S. Low, Y.Z. Deng, X.L. Guo, wo-egreeo-reeom Control o a PMSM Drive without Mechanical Sensor, Proceeings o the 4 th

Energy Time Dichotomy in the Optimal Control of the Electrical Drives

Energy Time Dichotomy in the Optimal Control of the Electrical Drives Proc of the 3r IAS/WSAS Int Conf on nergy, nvironment, cosystems an Sustainable Development, Agios Nikolaos, Greece, July 4-6, 7 54 nergy ime Dichotomy in the Optimal Control of the lectrical Drives CORNLIU

More information

DYNAMIC PERFORMANCE OF RELUCTANCE SYNCHRONOUS MACHINES

DYNAMIC PERFORMANCE OF RELUCTANCE SYNCHRONOUS MACHINES Annals of the University of Craiova, Electrical Engineering series, No 33, 9; ISSN 184-485 7 TH INTERNATIONAL CONFERENCE ON ELECTROMECHANICAL AN POWER SYSTEMS October 8-9, 9 - Iaşi, Romania YNAMIC PERFORMANCE

More information

Nonlinear Backstepping Control of Permanent Magnet Synchronous Motor (PMSM)

Nonlinear Backstepping Control of Permanent Magnet Synchronous Motor (PMSM) International ournal o Systems Control (Vol.1-010/Iss.1) Merzoug an Benalla / Nonlinear Backstepping Control o ermanent... / pp. 30-34 Nonlinear Backstepping Control o ermanent Magnet Synchronous Motor

More information

Robust Control of a Brushless Servo Motor Using Sliding Mode

Robust Control of a Brushless Servo Motor Using Sliding Mode Buletin Teknik Elektro an Inormatika (Bulletin o Electrical Engineering an Inormatics) Vol.1, No.4, December 2012, pp. 295~304 ISSN: 2089-3191 295 Robust Control o a Brushless Servo Motor Using Sliing

More information

Vehicle Stability Improvement Based on Electronic Differential Using Sliding Mode Control

Vehicle Stability Improvement Based on Electronic Differential Using Sliding Mode Control 7th WSEAS International Conference on Electric Power Systems, High Voltages, Electric Machines, Venice, Italy, November 1-3, 007 331 Vehicle Stability Improvement Base on Electronic Differential Using

More information

Non-Superconducting Fault Current Limiter

Non-Superconducting Fault Current Limiter Proceeings o the 5th WEA International Conerence on Applications o Electrical Engineering, Prague, Czech Republic, March -, 6 (pp-7) Non-uperconucting Fault Current Limiter A. CHARMIN*, M. TARAFDAR HAQUE,

More information

An inductance lookup table application for analysis of reluctance stepper motor model

An inductance lookup table application for analysis of reluctance stepper motor model ARCHIVES OF ELECTRICAL ENGINEERING VOL. 60(), pp. 5- (0) DOI 0.478/ v07-0-000-y An inuctance lookup table application for analysis of reluctance stepper motor moel JAKUB BERNAT, JAKUB KOŁOTA, SŁAWOMIR

More information

Experimental Determination of Mechanical Parameters in Sensorless Vector-Controlled Induction Motor Drive

Experimental Determination of Mechanical Parameters in Sensorless Vector-Controlled Induction Motor Drive Experimental Determination of Mechanical Parameters in Sensorless Vector-Controlle Inuction Motor Drive V. S. S. Pavan Kumar Hari, Avanish Tripathi 2 an G.Narayanan 3 Department of Electrical Engineering,

More information

Chapter 31: RLC Circuits. PHY2049: Chapter 31 1

Chapter 31: RLC Circuits. PHY2049: Chapter 31 1 Chapter 31: RLC Circuits PHY049: Chapter 31 1 LC Oscillations Conservation of energy Topics Dampe oscillations in RLC circuits Energy loss AC current RMS quantities Force oscillations Resistance, reactance,

More information

The Application of Euler Lagrange Method of Optimization for Electromechanical Motion Control

The Application of Euler Lagrange Method of Optimization for Electromechanical Motion Control HE ANNAS OF "DUNAREA DE OS" UNIVERSIY OF GAAI FASCICE III, ISSN -454X EECROECHNICS, EECRONICS, AUOMAIC CONRO, INFORMAICS he Application o Euler agrange Metho o Optiization or Electroechanical Motion Control

More information

A Novel Decoupled Iterative Method for Deep-Submicron MOSFET RF Circuit Simulation

A Novel Decoupled Iterative Method for Deep-Submicron MOSFET RF Circuit Simulation A Novel ecouple Iterative Metho for eep-submicron MOSFET RF Circuit Simulation CHUAN-SHENG WANG an YIMING LI epartment of Mathematics, National Tsing Hua University, National Nano evice Laboratories, an

More information

Dynamics of the synchronous machine

Dynamics of the synchronous machine ELEC0047 - Power system ynamics, control an stability Dynamics of the synchronous machine Thierry Van Cutsem t.vancutsem@ulg.ac.be www.montefiore.ulg.ac.be/~vct These slies follow those presente in course

More information

Smith Compensator Using Modified IMC for Unstable Plant with Time Delay

Smith Compensator Using Modified IMC for Unstable Plant with Time Delay 2 International Conerence on Inormation an Electronics Engineering IPCSIT vol.6 (2) (2) IACSIT Press, Singapore Smith Compensator Using Moiie IMC or Unstable Plant with Time Delay Hiroki Shibasaki, Manato

More information

Basic Strategy for Card-Counters: An Analytic Approach. by N. Richard Werthamer

Basic Strategy for Card-Counters: An Analytic Approach. by N. Richard Werthamer Basic Strategy or Car-Counters: An Analytic Approach by N. Richar Werthamer Abstract We evelop an eicient metho, similar to that o Marcus (7) who calls it Counter Basic Strategy, or casino blackack car

More information

A Short Note on Self-Similar Solution to Unconfined Flow in an Aquifer with Accretion

A Short Note on Self-Similar Solution to Unconfined Flow in an Aquifer with Accretion Open Journal o Flui Dynamics, 5, 5, 5-57 Publishe Online March 5 in SciRes. http://www.scirp.org/journal/oj http://x.oi.org/.46/oj.5.57 A Short Note on Sel-Similar Solution to Unconine Flow in an Aquier

More information

Modelling of Permanent Magnet Synchronous Motor Incorporating Core-loss

Modelling of Permanent Magnet Synchronous Motor Incorporating Core-loss Research Journal of Applie Sciences, Engineering an Technology 4(7): 846-85, ISSN: 4-7467 Maxwell Scientific Organization, Submitte: November, Accepte: December 9, Publishe: September, Moelling of Permanent

More information

Predictive control of synchronous generator: a multiciterial optimization approach

Predictive control of synchronous generator: a multiciterial optimization approach Preictive control of synchronous generator: a multiciterial optimization approach Marián Mrosko, Eva Miklovičová, Ján Murgaš Abstract The paper eals with the preictive control esign for nonlinear systems.

More information

Debond crack growth in fatigue along fiber in UD composite with broken fibers

Debond crack growth in fatigue along fiber in UD composite with broken fibers Debon crack growth in atigue along iber in UD composite with broken ibers Johannes Eitzenberger an Janis arna Dept o Applie Physics an Mechanical Engineering Lulea University o Technology, Sween SE 97

More information

A DYNAMIC MODEL OF POLYELECTROLYTE GELS

A DYNAMIC MODEL OF POLYELECTROLYTE GELS A DYNAMIC MODEL OF POLYELECTROLYTE GELS M.CARME CALDERER, HAORAN CHEN, CATHERINE MICEK, AND Y. MORI Abstract. We erive a moel o the couple mechanical an electrochemical eects o polyelectrolyte gels. We

More information

Teaching Fourier optics through ray matrices

Teaching Fourier optics through ray matrices INSTITUTE OF PHYSICS PUBLISHING Eur. J. Phys. 26 (2005 261 271 EUROPEAN JOURNAL OF PHYSICS oi:10.1088/0143-0807/26/2/005 Teaching Fourier optics through ray matrices IMoreno 1,MMSánche-Lópe 1,CFerreira

More information

Lecture 6: Control of Three-Phase Inverters

Lecture 6: Control of Three-Phase Inverters Yoash Levron The Anrew an Erna Viterbi Faculty of Electrical Engineering, Technion Israel Institute of Technology, Haifa 323, Israel yoashl@ee.technion.ac.il Juri Belikov Department of Computer Systems,

More information

Optimal design of reinforced concrete T-sections in bending

Optimal design of reinforced concrete T-sections in bending Engineering Structures 5 (003) 951 964 www.elsevier.com/locate/engstruct Optimal esign o reinorce concrete T-sections in ening C.C. Ferreira a,, M.H.F.M. Barros a, A.F.M. Barros a Department o Civil Engineering,

More information

IPMSM Inductances Calculation Using FEA

IPMSM Inductances Calculation Using FEA X International Symposium on Inustrial Electronics INDEL 24, Banja Luka, November 68, 24 IPMSM Inuctances Calculation Using FEA Dejan G. Jerkan, Marko A. Gecić an Darko P. Marčetić Department for Power,

More information

DOUBLE PENDULUM VIBRATION MOTION IN FLUID FLOW

DOUBLE PENDULUM VIBRATION MOTION IN FLUID FLOW ENGINEERING FOR RURA DEEOPMENT Jelgava,.-.5.5. DOUBE PENDUUM IBRATION MOTION IN FUID FOW Janis iba, Maris Eiuks, Martins Irbe Riga Technical University, atvia janis.viba@rtu.lv, maris.eiuks@rtu.lv, martins.irbe@rtu.lv

More information

ECE 422 Power System Operations & Planning 7 Transient Stability

ECE 422 Power System Operations & Planning 7 Transient Stability ECE 4 Power System Operations & Planning 7 Transient Stability Spring 5 Instructor: Kai Sun References Saaat s Chapter.5 ~. EPRI Tutorial s Chapter 7 Kunur s Chapter 3 Transient Stability The ability of

More information

Research Article Development of Digital Control for High Power Permanent-Magnet Synchronous Motor Drives

Research Article Development of Digital Control for High Power Permanent-Magnet Synchronous Motor Drives Mathematical Problems in Engineering Volume 214, Article ID 926727, 1 pages http://x.oi.org/1.1155/214/926727 Research Article Development of Digital Control for High Power Permanent-Magnet Synchronous

More information

An Upper Bound on the Minimum Distance of Serially Concatenated Convolutional Codes

An Upper Bound on the Minimum Distance of Serially Concatenated Convolutional Codes SUBMITTED TO IEEE TRANSACTIONS ON INFORMATION THEORY, FEBRUARY 2004 1 An Upper Boun on the Minimum Distance o Serially Concatenate Convolutional Coes Alberto Perotti, Member, IEEE, an Sergio Beneetto,

More information

1. Filling an initially porous tube under a constant head imposed at x =0

1. Filling an initially porous tube under a constant head imposed at x =0 Notes on Moving Bounary problems, Voller U o M, volle00@umn.eu. Filling an initially porous tube uner a constant hea impose at x =0 Governing equation is base on calculating the water volume lux by the

More information

arxiv: v1 [math.ca] 9 Jan 2016

arxiv: v1 [math.ca] 9 Jan 2016 Local Weak Observability Conitions of Sensorless AC Drives Mohama Koteich, Stuent Member, IEEE, Abelmalek Maloum, Gilles Duc an Guillaume Sanou arxiv:1601.06129v1 [math.ca] 9 Jan 2016 KEYWORDS Sensorless

More information

Optimal Variable-Structure Control Tracking of Spacecraft Maneuvers

Optimal Variable-Structure Control Tracking of Spacecraft Maneuvers Optimal Variable-Structure Control racking of Spacecraft Maneuvers John L. Crassiis 1 Srinivas R. Vaali F. Lanis Markley 3 Introuction In recent years, much effort has been evote to the close-loop esign

More information

Modeling and analysis of parallel connected permanent magnet synchronous generators in a small hydropower plant

Modeling and analysis of parallel connected permanent magnet synchronous generators in a small hydropower plant Proceeings of the 2006 IASME/WSEAS International Conference on Energy & Environmental Systems, Chalkia, Greece, May 8-10, 2006 (pp83-88) Moeling an analysis of parallel connecte permanent magnet synchronous

More information

A Novel Unknown-Input Estimator for Disturbance Estimation and Compensation

A Novel Unknown-Input Estimator for Disturbance Estimation and Compensation A Novel Unknown-Input Estimator for Disturbance Estimation an Compensation Difan ang Lei Chen Eric Hu School of Mechanical Engineering he University of Aelaie Aelaie South Australia 5005 Australia leichen@aelaieeuau

More information

Peaked Periodic Wave Solutions to the Broer Kaup Equation

Peaked Periodic Wave Solutions to the Broer Kaup Equation Commun. Theor. Phys. 67 (2017) 22 26 Vol. 67, No. 1, January 1, 2017 Peake Perioic Wave Solutions to the Broer Kaup Equation Bo Jiang ( 江波 ) 1, an Qin-Sheng Bi ( 毕勤胜 ) 2 1 Department o Applie Mathematics,

More information

Research on Thin Film Thickness Uniformity for Deposition of Rectangular Planar Sputtering Target

Research on Thin Film Thickness Uniformity for Deposition of Rectangular Planar Sputtering Target Available online at www.scienceirect.com Physics Proceia 3 (01 ) 903 913 18 th International Vacuum Congress (IVC-18) Research on Thin Film Thickness Uniormity or Deposition o Rectangular Planar puttering

More information

Modeling of transport phenomena in a fuel cell anode. Frank A. Coutelieris

Modeling of transport phenomena in a fuel cell anode. Frank A. Coutelieris Moeling o transport phenomena in a uel cell anoe Frank A. Coutelieris Department o Engineering an Management o Energy Resources, University o Western Maceonia, Bakola & Sialvera, 50100 Kozani, Greece,

More information

Reactive Power Compensation in Mechanical Systems

Reactive Power Compensation in Mechanical Systems Reactive Power Compensation in Mechanical Systems Carlos Rengifo, Bassel Kaar, Yannick Aoustin, Christine Chevallereau To cite this version: Carlos Rengifo, Bassel Kaar, Yannick Aoustin, Christine Chevallereau.

More information

Product and Quotient Rules and Higher-Order Derivatives. The Product Rule

Product and Quotient Rules and Higher-Order Derivatives. The Product Rule 330_003.q 11/3/0 :3 PM Page 119 SECTION.3 Prouct an Quotient Rules an Higher-Orer Derivatives 119 Section.3 Prouct an Quotient Rules an Higher-Orer Derivatives Fin the erivative o a unction using the Prouct

More information

Open Access An Exponential Reaching Law Sliding Mode Observer for PMSM in Rotating Frame

Open Access An Exponential Reaching Law Sliding Mode Observer for PMSM in Rotating Frame Sen Orers for Reprints to reprints@benthamscience.ae The Open Automation an Control Systems Journal, 25, 7, 599-66 599 Open Access An Exponential Reaching Law Sliing Moe Observer for PMSM in Rotating Frame

More information

Multirate Feedforward Control with State Trajectory Generation based on Time Axis Reversal for Plant with Continuous Time Unstable Zeros

Multirate Feedforward Control with State Trajectory Generation based on Time Axis Reversal for Plant with Continuous Time Unstable Zeros Multirate Feeforwar Control with State Trajectory Generation base on Time Axis Reversal for with Continuous Time Unstable Zeros Wataru Ohnishi, Hiroshi Fujimoto Abstract with unstable zeros is known as

More information

The Levitation Controller Design of an Electromagnetic Suspension Vehicle using Gain Scheduled Control

The Levitation Controller Design of an Electromagnetic Suspension Vehicle using Gain Scheduled Control Proceeings of the 5th WSEAS Int. Conf. on CIRCUIS, SYSEMS, ELECRONICS, CONROL & SIGNAL PROCESSING, Dallas, USA, November 1-3, 6 35 he Levitation Controller Design of an Electromagnetic Suspension Vehicle

More information

State Space Analysis of Power System Stability Enhancement with Used the STATCOM

State Space Analysis of Power System Stability Enhancement with Used the STATCOM tate pace Analysis of Power ystem tability Enhancement with Use the ACOM M. Mahavian () - G. hahgholian () () Department of Electrical Engineering, Islamic Aza University, Naein Branch, Esfahan, Iran ()

More information

θ x = f ( x,t) could be written as

θ x = f ( x,t) could be written as 9. Higher orer PDEs as systems of first-orer PDEs. Hyperbolic systems. For PDEs, as for ODEs, we may reuce the orer by efining new epenent variables. For example, in the case of the wave equation, (1)

More information

Simple Electromagnetic Motor Model for Torsional Analysis of Variable Speed Drives with an Induction Motor

Simple Electromagnetic Motor Model for Torsional Analysis of Variable Speed Drives with an Induction Motor DOI: 10.24352/UB.OVGU-2017-110 TECHNISCHE MECHANIK, 37, 2-5, (2017), 347-357 submitte: June 15, 2017 Simple Electromagnetic Motor Moel for Torsional Analysis of Variable Spee Drives with an Inuction Motor

More information

New Simple Controller Tuning Rules for Integrating and Stable or Unstable First Order plus Dead-Time Processes

New Simple Controller Tuning Rules for Integrating and Stable or Unstable First Order plus Dead-Time Processes Proceeings of the 3th WSEAS nternational Conference on SYSTEMS New Simple Controller Tuning Rules for ntegrating an Stable or Unstable First Orer plus Dea-Time Processes.G.ARVANTS Department of Natural

More information

Longitudinal Waves in a Rotating Solid Cylinder Immersed in an Inviscid Fluid Using Chebyshev Polynomial

Longitudinal Waves in a Rotating Solid Cylinder Immersed in an Inviscid Fluid Using Chebyshev Polynomial Longituinal Waves in a Rotating Soli Cyliner Immerse in an Invisci Flui Using Chebyshev Polynomial R. Selvamani *1, P.Ponnusamy 1 Department o Mathematics, Karunya University, Coimbatore, TamilNau, Inia

More information

Mathematical Modeling and Dynamic Simulation of a Class of Drive Systems with Permanent Magnet Synchronous Motors

Mathematical Modeling and Dynamic Simulation of a Class of Drive Systems with Permanent Magnet Synchronous Motors Applied and Computational Mechanics 3 (2009) 331 338 Mathematical Modeling and Dynamic Simulation of a Class of Drive Systems with Permanent Magnet Synchronous Motors M. Mikhov a, a Faculty of Automatics,

More information

STABILITY CONTROL FOR SIX-WHEEL DRIVE ARTICULATED VEHICLE BASED ON DIRECT YAW MOMENT CONTROL METHOD

STABILITY CONTROL FOR SIX-WHEEL DRIVE ARTICULATED VEHICLE BASED ON DIRECT YAW MOMENT CONTROL METHOD STABILITY CONTROL FOR SIX-WHEEL DRIVE ARTICULATED VEHICLE BASED ON DIRECT YAW MOMENT CONTROL METHOD 1 YITING KANG, 2 WENMING ZHANG 1 Doctoral Caniate, School of Mechanical Engineering, University of Science

More information

Chapter 6. Electromagnetic Oscillations and Alternating Current

Chapter 6. Electromagnetic Oscillations and Alternating Current hapter 6 Electromagnetic Oscillations an Alternating urrent hapter 6: Electromagnetic Oscillations an Alternating urrent (hapter 31, 3 in textbook) 6.1. Oscillations 6.. The Electrical Mechanical Analogy

More information

Table of Common Derivatives By David Abraham

Table of Common Derivatives By David Abraham Prouct an Quotient Rules: Table of Common Derivatives By Davi Abraham [ f ( g( ] = [ f ( ] g( + f ( [ g( ] f ( = g( [ f ( ] g( g( f ( [ g( ] Trigonometric Functions: sin( = cos( cos( = sin( tan( = sec

More information

THE ACCURATE ELEMENT METHOD: A NEW PARADIGM FOR NUMERICAL SOLUTION OF ORDINARY DIFFERENTIAL EQUATIONS

THE ACCURATE ELEMENT METHOD: A NEW PARADIGM FOR NUMERICAL SOLUTION OF ORDINARY DIFFERENTIAL EQUATIONS THE PUBISHING HOUSE PROCEEDINGS O THE ROMANIAN ACADEMY, Series A, O THE ROMANIAN ACADEMY Volume, Number /, pp. 6 THE ACCURATE EEMENT METHOD: A NEW PARADIGM OR NUMERICA SOUTION O ORDINARY DIERENTIA EQUATIONS

More information

Stability-Guaranteed Impedance Control of Hydraulic Robotic Manipulators

Stability-Guaranteed Impedance Control of Hydraulic Robotic Manipulators Tampere University o Technology Stability-Guarantee Impeance Control o Hyraulic Robotic Manipulators Citation Koivumäki, J., & Mattila, J. (217). Stability-Guarantee Impeance Control o Hyraulic Robotic

More information

G j dq i + G j. q i. = a jt. and

G j dq i + G j. q i. = a jt. and Lagrange Multipliers Wenesay, 8 September 011 Sometimes it is convenient to use reunant coorinates, an to effect the variation of the action consistent with the constraints via the metho of Lagrange unetermine

More information

Harmonic Modelling of Thyristor Bridges using a Simplified Time Domain Method

Harmonic Modelling of Thyristor Bridges using a Simplified Time Domain Method 1 Harmonic Moelling of Thyristor Briges using a Simplifie Time Domain Metho P. W. Lehn, Senior Member IEEE, an G. Ebner Abstract The paper presents time omain methos for harmonic analysis of a 6-pulse

More information

TIME-DELAY ESTIMATION USING FARROW-BASED FRACTIONAL-DELAY FIR FILTERS: FILTER APPROXIMATION VS. ESTIMATION ERRORS

TIME-DELAY ESTIMATION USING FARROW-BASED FRACTIONAL-DELAY FIR FILTERS: FILTER APPROXIMATION VS. ESTIMATION ERRORS TIME-DEAY ESTIMATION USING FARROW-BASED FRACTIONA-DEAY FIR FITERS: FITER APPROXIMATION VS. ESTIMATION ERRORS Mattias Olsson, Håkan Johansson, an Per öwenborg Div. of Electronic Systems, Dept. of Electrical

More information

SWEEP METHOD IN ANALYSIS OPTIMAL CONTROL FOR RENDEZ-VOUS PROBLEMS

SWEEP METHOD IN ANALYSIS OPTIMAL CONTROL FOR RENDEZ-VOUS PROBLEMS J. Appl. Math. & Computing Vol. 23(2007), No. 1-2, pp. 243-256 Website: http://jamc.net SWEEP METHOD IN ANALYSIS OPTIMAL CONTROL FOR RENDEZ-VOUS PROBLEMS MIHAI POPESCU Abstract. This paper deals with determining

More information

'HVLJQ &RQVLGHUDWLRQ LQ 0DWHULDO 6HOHFWLRQ 'HVLJQ 6HQVLWLYLW\,1752'8&7,21

'HVLJQ &RQVLGHUDWLRQ LQ 0DWHULDO 6HOHFWLRQ 'HVLJQ 6HQVLWLYLW\,1752'8&7,21 Large amping in a structural material may be either esirable or unesirable, epening on the engineering application at han. For example, amping is a esirable property to the esigner concerne with limiting

More information

Estimation of Saturation of Permanent-Magnet Synchronous Motors Through an Energy-Based Model

Estimation of Saturation of Permanent-Magnet Synchronous Motors Through an Energy-Based Model Estimation of Saturation of Permanent-Magnet Synchronous Motors Through an Energy-Base Moel Al Kassem Jebai, François Malrait, Philippe Martin an Pierre Rouchon arxiv:110393v1 [mathoc] 15 Mar 011 Mines

More information

Predictive Control of a Laboratory Time Delay Process Experiment

Predictive Control of a Laboratory Time Delay Process Experiment Print ISSN:3 6; Online ISSN: 367-5357 DOI:0478/itc-03-0005 Preictive Control of a aboratory ime Delay Process Experiment S Enev Key Wors: Moel preictive control; time elay process; experimental results

More information

JUST THE MATHS UNIT NUMBER DIFFERENTIATION 2 (Rates of change) A.J.Hobson

JUST THE MATHS UNIT NUMBER DIFFERENTIATION 2 (Rates of change) A.J.Hobson JUST THE MATHS UNIT NUMBER 10.2 DIFFERENTIATION 2 (Rates of change) by A.J.Hobson 10.2.1 Introuction 10.2.2 Average rates of change 10.2.3 Instantaneous rates of change 10.2.4 Derivatives 10.2.5 Exercises

More information

Motion-Copying System Using FPGA-based Friction-Free Disturbance Observer

Motion-Copying System Using FPGA-based Friction-Free Disturbance Observer IEEJ Journal of Inustry Applications Vol.3 No.3 pp.248 259 DOI: 10.1541/ieejjia.3.248 Paper Motion-Copying System Using FPGA-base Friction-Free Disturbance Observer Thao Tran Phuong a) Member, Kiyoshi

More information

MEASUREMENT OF LOSSES IN DIRECT TORQUE CONTROLLED PERMANENT MAGNET SYNCHRONOUS MOTOR BY ANALYSIS AND EXPERIMENTAL SETUP

MEASUREMENT OF LOSSES IN DIRECT TORQUE CONTROLLED PERMANENT MAGNET SYNCHRONOUS MOTOR BY ANALYSIS AND EXPERIMENTAL SETUP IJRET: International Journal of Research in Engineering an Technology eissn: 2319-1163 pissn: 2321-738 MEASUREMENT OF LOSSES IN DIRECT TORQUE CONTROLLED PERMANENT MAGNET SYNCHRONOUS MOTOR BY ANALYSIS AND

More information

Shifted Independent Component Analysis

Shifted Independent Component Analysis Downloae rom orbit.tu.k on: Dec 06, 2017 Shite Inepenent Component Analysis Mørup, Morten; Masen, Kristoer Hougaar; Hansen, Lars Kai Publishe in: 7th International Conerence on Inepenent Component Analysis

More information

MATLAB Simulation Research on Permanent Magnet Synchronous Motor Vector Control

MATLAB Simulation Research on Permanent Magnet Synchronous Motor Vector Control MATLAB Simulation Research on Permanent Magnet Synchronous Motor Vector Control Wei Hanpei 1*, Wei Haifeng 1,2, Zhang Yi 1,2 1 School of Electrical an Information, Jiangsu University of Science an Technology,

More information

A Comparison between a Conventional Power System Stabilizer (PSS) and Novel PSS Based on Feedback Linearization Technique

A Comparison between a Conventional Power System Stabilizer (PSS) and Novel PSS Based on Feedback Linearization Technique J. Basic. Appl. Sci. Res., ()9-99,, TextRoa Publication ISSN 9-434 Journal of Basic an Applie Scientific Research www.textroa.com A Comparison between a Conventional Power System Stabilizer (PSS) an Novel

More information

Monovariable H Robust Controller for a Permanent Magnet Synchronous Machine (PMSM)

Monovariable H Robust Controller for a Permanent Magnet Synchronous Machine (PMSM) Monovariable H Robust Controller for a Permanent Magnet Synchronous Machine (PMSM) J. Kheri # # Automatic Control Unit, National School of Engineers of Sfax, ENIS Roa of soukra, km 3.5 - BP.W, 3038, Sfax,

More information

A Review of Multiple Try MCMC algorithms for Signal Processing

A Review of Multiple Try MCMC algorithms for Signal Processing A Review of Multiple Try MCMC algorithms for Signal Processing Luca Martino Image Processing Lab., Universitat e València (Spain) Universia Carlos III e Mari, Leganes (Spain) Abstract Many applications

More information

PD Controller for Car-Following Models Based on Real Data

PD Controller for Car-Following Models Based on Real Data PD Controller for Car-Following Moels Base on Real Data Xiaopeng Fang, Hung A. Pham an Minoru Kobayashi Department of Mechanical Engineering Iowa State University, Ames, IA 5 Hona R&D The car following

More information

Deriving ARX Models for Synchronous Generators

Deriving ARX Models for Synchronous Generators Deriving AR Moels for Synchronous Generators Yangkun u, Stuent Member, IEEE, Zhixin Miao, Senior Member, IEEE, Lingling Fan, Senior Member, IEEE Abstract Parameter ientification of a synchronous generator

More information

State-Space Model for a Multi-Machine System

State-Space Model for a Multi-Machine System State-Space Moel for a Multi-Machine System These notes parallel section.4 in the text. We are ealing with classically moele machines (IEEE Type.), constant impeance loas, an a network reuce to its internal

More information

6.003 Homework #7 Solutions

6.003 Homework #7 Solutions 6.003 Homework #7 Solutions Problems. Secon-orer systems The impulse response of a secon-orer CT system has the form h(t) = e σt cos(ω t + φ)u(t) where the parameters σ, ω, an φ are relate to the parameters

More information

EC5555 Economics Masters Refresher Course in Mathematics September 2013

EC5555 Economics Masters Refresher Course in Mathematics September 2013 EC5555 Economics Masters Reresher Course in Mathematics September 3 Lecture 5 Unconstraine Optimization an Quaratic Forms Francesco Feri We consier the unconstraine optimization or the case o unctions

More information

Multi-Level Library of Electrical Machines for Aerospace Applications

Multi-Level Library of Electrical Machines for Aerospace Applications Multi-Level Library of Electrical Machines for Aerospace Applications P. Giangrane C.I. Hill C. Geraa S.V. Bozhko University of Nottingham PEMC Group, Nottingham, NG7 RD, UK. p.giangrane@nottingham.ac.uk

More information

the solution of ()-(), an ecient numerical treatment requires variable steps. An alternative approach is to apply a time transformation of the form t

the solution of ()-(), an ecient numerical treatment requires variable steps. An alternative approach is to apply a time transformation of the form t Asymptotic Error Analysis of the Aaptive Verlet Metho Stephane Cirilli, Ernst Hairer Beneict Leimkuhler y May 3, 999 Abstract The Aaptive Verlet metho [7] an variants [6] are time-reversible schemes for

More information

Lie symmetry and Mei conservation law of continuum system

Lie symmetry and Mei conservation law of continuum system Chin. Phys. B Vol. 20, No. 2 20 020 Lie symmetry an Mei conservation law of continuum system Shi Shen-Yang an Fu Jing-Li Department of Physics, Zhejiang Sci-Tech University, Hangzhou 3008, China Receive

More information

Michaelis-Menten Plot

Michaelis-Menten Plot NAM: HAITI CHMISTRY, SPRING, 17 Circle Section Number: 1 11 amination, April 15, 17 Answer each question in the space provie; use back o page i etra space is neee. Answer questions so the graer can RADILY

More information

Circle-criterion Based Nonlinear Observer Design for Sensorless Induction Motor Control

Circle-criterion Based Nonlinear Observer Design for Sensorless Induction Motor Control International Journal of Automation an Computing 11(6), December 214, 598-64 DOI: 1.17/s11633-14-842-1 Circle-criterion Base Nonlinear Observer Design for Sensorless Inuction Motor Control Wafa Bourbia

More information

SYNTHESIS ON THE ASSESSMENT OF CHIPS CONTRACTION COEFFICIENT C d

SYNTHESIS ON THE ASSESSMENT OF CHIPS CONTRACTION COEFFICIENT C d SYNTHESIS ON THE ASSESSMENT OF HIPS ONTRATION OEFFIIENT Marius MILEA Technical University Gheorghe Asachi of Iași, Machine Manufacturing an Inustrial Management Faculty, B-ul D Mangeron, nr 59, A, 700050,

More information

Suppression Method of Rising DC Voltage for the Halt Sequence of an Inverter in the Motor Regeneration

Suppression Method of Rising DC Voltage for the Halt Sequence of an Inverter in the Motor Regeneration Suppression Metho of Rising DC Voltage for the Halt Sequence of an Inverter in the Motor Regeneration Jun-ichi Itoh Wataru Aoki Goh Teck Chiang Akio Toba Nagaoka University of Technology Fuji Electric

More information

Linear Quadratic Regulator (LQR) Design I

Linear Quadratic Regulator (LQR) Design I Lecture 7 Linear Quadratic Regulator LQR) Design I Dr. Radhakant Padhi Asst. Proessor Dept. o Aerospace Engineering Indian Institute o Science - Bangalore LQR Design: Problem Objective o drive the state

More information

Motivation. CS/EE 3700 : Fundamentals of Digital System Design

Motivation. CS/EE 3700 : Fundamentals of Digital System Design Motivation CS/EE 37 : Funamentals o Digital System Design Chris J. Myers Lecture 4: Logic Optimization Chapter 4 Algebraic manipulation is not systematic. This chapter presents methos that can be automate

More information

Lagrangian and Hamiltonian Mechanics

Lagrangian and Hamiltonian Mechanics Lagrangian an Hamiltonian Mechanics.G. Simpson, Ph.. epartment of Physical Sciences an Engineering Prince George s Community College ecember 5, 007 Introuction In this course we have been stuying classical

More information

Position Sensorless Control for an Interior Permanent Magnet Synchronous Motor SVM Drive with ANN Based Stator Flux Estimator

Position Sensorless Control for an Interior Permanent Magnet Synchronous Motor SVM Drive with ANN Based Stator Flux Estimator International Journal of Computer an Electrical Engineering, Vol., No. 3, June, 1 Position Sensorless Control for an Interior Permanent Magnet Synchronous Motor SVM Drive with ANN Base Stator Flux Estimator

More information

The Efficiency Optimization of Permanent Magnet Synchronous Machine DTC for Electric Vehicles Applications Based on Loss Model

The Efficiency Optimization of Permanent Magnet Synchronous Machine DTC for Electric Vehicles Applications Based on Loss Model International Power, Electronics an Materials Engineering Conference (IPEMEC 015) The Efficiency Optimization of Permanent Magnet Synchronous Machine DTC for Electric Vehicles Applications Base on Loss

More information

On interface property characterization and performance of fiber-reinforced cementitious composites

On interface property characterization and performance of fiber-reinforced cementitious composites Concrete Science an Engineering, Vol. 1, September 1999, pp 173-174 On interace property characterization an perormance o iber-reinorce cementitious composites Z. Lin 1, T. Kana an V. C. Li 1 (1 Avance

More information

Performance Evaluation of Synchronous Reluctance Motors With and Without Permanent Magnets

Performance Evaluation of Synchronous Reluctance Motors With and Without Permanent Magnets Performance Evaluation of Synchronous Reluctance Motors With an Without Permanent Magnets M. N. Ibrahim 1,, Stuent Member IEEE, Peter Sergeant 1, Member IEEE an E. M. Rasha, Senior Member IEEE 1 Department

More information

Influence of weight initialization on multilayer perceptron performance

Influence of weight initialization on multilayer perceptron performance Influence of weight initialization on multilayer perceptron performance M. Karouia (1,2) T. Denœux (1) R. Lengellé (1) (1) Université e Compiègne U.R.A. CNRS 817 Heuiasyc BP 649 - F-66 Compiègne ceex -

More information

Interpolated Rigid-Body Motions and Robotics

Interpolated Rigid-Body Motions and Robotics Interpolate Rigi-Boy Motions an Robotics J.M. Selig Faculty of Business, Computing an Info. Management. Lonon South Bank University, Lonon SE AA, U.K. seligjm@lsbu.ac.uk Yaunquing Wu Dept. Mechanical Engineering.

More information

State estimation for predictive maintenance using Kalman filter

State estimation for predictive maintenance using Kalman filter Reliability Engineering an System Safety 66 (1999) 29 39 www.elsevier.com/locate/ress State estimation for preictive maintenance using Kalman filter S.K. Yang, T.S. Liu* Department of Mechanical Engineering,

More information

A Hydraulic Steering Gear Simulator for Analysis and Control

A Hydraulic Steering Gear Simulator for Analysis and Control A Hyraulic teering Gear imulator for Analysis an Control Nikolaos I. Xiros (), Vasilios P. Tsourapas (), Kyriakos K. Mourtzouchos () () chool of Naval Architecture an Marine Engineering National Technical

More information

and from it produce the action integral whose variation we set to zero:

and from it produce the action integral whose variation we set to zero: Lagrange Multipliers Monay, 6 September 01 Sometimes it is convenient to use reunant coorinates, an to effect the variation of the action consistent with the constraints via the metho of Lagrange unetermine

More information

VIRTUAL STRUCTURE BASED SPACECRAFT FORMATION CONTROL WITH FORMATION FEEDBACK

VIRTUAL STRUCTURE BASED SPACECRAFT FORMATION CONTROL WITH FORMATION FEEDBACK AIAA Guiance, Navigation, an Control Conference an Exhibit 5-8 August, Monterey, California AIAA -9 VIRTUAL STRUCTURE BASED SPACECRAT ORMATION CONTROL WITH ORMATION EEDBACK Wei Ren Ranal W. Bear Department

More information

A Numerical Analysis on a Compact Heat Exchanger in Aluminum Foam

A Numerical Analysis on a Compact Heat Exchanger in Aluminum Foam Journal o Physics: Conerence Series PAPER OPEN ACCESS A Numerical Analysis on a Compact Heat Exchanger in Aluminum Foam To cite this article: B Buonomo et al 2016 J. Phys.: Con. Ser. 745 032141 View the

More information

Probabilistic Model of Error in Fixed-Point Arithmetic Gaussian Pyramid

Probabilistic Model of Error in Fixed-Point Arithmetic Gaussian Pyramid Probabilistic Model o Error in Fixed-Point Arithmetic Gaussian Pyramid Antoine Méler John A. Ruiz-Hernandez James L. Crowley INRIA Grenoble - Rhône-Alpes 655 avenue de l Europe 38 334 Saint Ismier Cedex

More information

Modelling of Three Phase Short Circuit and Measuring Parameters of a Turbo Generator for Improved Performance

Modelling of Three Phase Short Circuit and Measuring Parameters of a Turbo Generator for Improved Performance Moelling of Three Phase Short Circuit an Measuring Parameters of a Turbo Generator for Improve Performance M. Olubiwe, S. O. E. Ogbogu, D. O. Dike, L. Uzoechi Dept of Electrical an Electronic Engineering,

More information

Beam Propagation Hazard Calculations for Telescopic Viewing of Laser Beams

Beam Propagation Hazard Calculations for Telescopic Viewing of Laser Beams ILSC 003 Conerence Proceeings Beam Propagation Hazar Calculations or Telescopic Vieing o Laser Beams Ulrie Grabner, Georg Vees an Karl Schulmeister Please register to receive our Laser, LED & Lamp Saety

More information

NON-LINEAR CONTROL STRATEGY FOR STRIP CASTING PROCESSES

NON-LINEAR CONTROL STRATEGY FOR STRIP CASTING PROCESSES NON-LINER CONROL SREGY FOR SRIP CSING PROCESSES V.. Oliveira, R. R. Nascimento, N. S. D. rrifano E. Gesualo, J. P. V. osetti Departamento e Engenharia Elétrica, USP São Carlos CP 359, CEP 3560-970 São

More information

THE SPEED CONTROL OF PERMANENT MAGNET SYNCHRONOUS MOTOR USING FUZZY LOGIC AND SELF TUNING FUZZY PI CONTROLLER

THE SPEED CONTROL OF PERMANENT MAGNET SYNCHRONOUS MOTOR USING FUZZY LOGIC AND SELF TUNING FUZZY PI CONTROLLER THE SPEED CONTROL OF PERMANENT MAGNET SYNCHRONOUS MOTOR USING FUZZY LOGIC AND SELF TUNING FUZZY PI CONTROLLER Abulhakim KARAKAYA Ercüment KARAKAŞ e-mail: akarakaya@kou.eu.tr e-mail: karakas@kou.eu.tr Department

More information

Predictive Cascade Control of DC Motor

Predictive Cascade Control of DC Motor Volume 49, Number, 008 89 Predictive Cascade Control of DC Motor Alexandru MORAR Abstract: The paper deals with the predictive cascade control of an electrical drive intended for positioning applications.

More information

Consideration on new theoretical solutions of special electric machines using specialized soft of electromagnetic field numerical analysis

Consideration on new theoretical solutions of special electric machines using specialized soft of electromagnetic field numerical analysis Recent Researches in Software Engineering, Parallel an Distribute Systems Consieration on new theoretical solutions of special electric machines using specialize soft of electromagnetic fiel numerical

More information

Artificial Neural Network to Improve Speed Control of Permanent Magnet Synchronous Motor

Artificial Neural Network to Improve Speed Control of Permanent Magnet Synchronous Motor Proceeing o the 6th WSEAS/IASME Int. Con. on Electric Power Sytem, High Voltage, Electric Machine, Tenerie, Spain, December 16-18, 2006 94 Artiicial Neural Network to Improve Spee Control o Permanent Magnet

More information